Nothing Special   »   [go: up one dir, main page]

TW201230083A - Composite magnetic material, production method thereof, antenna and communication device - Google Patents

Composite magnetic material, production method thereof, antenna and communication device Download PDF

Info

Publication number
TW201230083A
TW201230083A TW100144103A TW100144103A TW201230083A TW 201230083 A TW201230083 A TW 201230083A TW 100144103 A TW100144103 A TW 100144103A TW 100144103 A TW100144103 A TW 100144103A TW 201230083 A TW201230083 A TW 201230083A
Authority
TW
Taiwan
Prior art keywords
resin
composite magnetic
magnetic
mhz
antenna
Prior art date
Application number
TW100144103A
Other languages
Chinese (zh)
Inventor
Masayuki Ishizuka
Ryo Kikuta
Ryosuke Nakamura
Nobuhiro Hidaka
Takeshi Kawase
Ryuuta Yamaya
Michio Tano
Yoshiki Yoshioka
Original Assignee
Sumitomo Osaka Cement Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority claimed from JP2011254169A external-priority patent/JP6044064B2/en
Application filed by Sumitomo Osaka Cement Co Ltd filed Critical Sumitomo Osaka Cement Co Ltd
Publication of TW201230083A publication Critical patent/TW201230083A/en

Links

Landscapes

  • Soft Magnetic Materials (AREA)
  • Coils Or Transformers For Communication (AREA)

Abstract

The present invention provides a composite magnetic material comprising plate-like magnetic particles which are dispersed in an insulating material, wherein the plate-like magnetic particles have an average thickness of 0.01 μ m or more and 0.5 μ m or less, an average major axis of 0.05 μ m or more and 10 μ m or less, and an average aspect ratio (major axis/thickness) of 5 or more, a production method thereof, an antenna provided with the composite magnetic material, and a communication device provided with the antenna.

Description

201230083 六、發明說明: 【發明所屬之技術領域】 本發明係關於複合磁性體及其製造方法、天線以及通 信裝置,詳細而言,係關於可適當地使用在應用70MHz至 500MHz的頻率波段之VHF波段的電磁波之高頻電路基板、 尚頻電子零件、磁性薄片、電磁波遮敝薄片、樹脂结合磁 石、磁性記錄媒體、天線等,並且具有高複磁導率的實部 /zr’之複合磁性體及其製造方法,及具備該複合磁性體之 天線,以及具備該天線之通信裝置。此外,本發明係關於 在160MHz至222MHz中,可使用在攜帶式終端之安裝有上 述複合磁性體之單極天線。 本申請案係根據2010年11月30日於日本申請之日 本特願2010-266903、2011年3月23日於日本申請之日本 特願201 1-064310、2011年4月25日於日本申請之日本特 願2011-097157、2011年5月31日於日本申請之日本特願 2011-122440、2011年7月29日於日本申請之日本特願 2011-167077、2011年7月29日於日本申請之日本特願 2011-167078、2011年11月21日於日本申請之日本特願 2011-254169、2011年11月25日於日本申請之日本特願 2011-257615、2011年11月25日於日本申請之日本特願 2011-257616而主張優先權,並在此援引其内容。 【先前技術】 磁性材料,就對於電磁波之特性或生產性、使用容易 度等來看,為人所知者有使用作為混合並分散於有機高分 323724 3 4 201230083 子材料等絕緣材料中之複合磁性體者。 該磁性材料,係使用在電子設備中所裝載之電子零 件、磁性薄片、電磁干擾抑制薄片、馬達、變壓器等電氣 製品、錄影帶或軟碟(F i 〇 p p y,註冊商標)等磁性記錄媒體。 近年來隨著^訊通k设備的高速化、高密度化,強 烈地要求電子設備中所裝載之電子零件或電路基板或天 線,尤其是卿式資訊設制天料之小型化及低消耗電 力化。 一般而言,於物質内傳遞之電磁波的波長,可使用 於真空中傳遞之電磁波的波長h與物質之複介電常數的 實部ε r (以下有時略稱為£ r,)以及複磁導率的實部 yr’(以下有時略稱為yr’)而表示如下式(1), λ g= λ 〇/( ε rJ · β r' )1/z · · · (1) 根據式(1),er’及//r’愈大,波長凡8的縮短率愈大。 因此,藉由增大構成電子零件或電路基板或天線等之磁性 材料的ε r’及# r’,增大波長λ g的縮短率,而可達成電子 零件或電路基板或天線等之小型化。 增大波長的縮短率之材料,提出有一種將磁性體粒子 混合並分散於構成電子零件或電路基板之絕緣材料中之複 合磁性體(專利文獻1)。該複合磁性體中,係藉由增大 /z r’,來增大波長的縮短率。 當複合磁性體中使用球狀磁性體粒子時,一般所知 者’由於各磁性體粒子中的去磁場係數(demagnetizing factor)變大,而產生難以增大複合磁性體的,之問題 323724 4 201230083 點 因此,有人提出-種作為使用在此般用途之磁性體粒 子’較佳是厚度以下之平板狀磁性體粒子,且為爲 平狀、鱗片狀、小片(flake)狀等長寬比(長徑/厚度)較大 之各種形狀的磁性體粒子(例如參考專利文獻2、3等)。 此般平板狀磁性體粒子中,可在去磁場係數最低^平 面方向’亦即長軸方向上得到高訂,。因此,將平板狀磁 性體粒子混合並分散於絕緣材料中之複合磁性體,為了有 效地應用去磁場係數的效果來得到高,,必須使平板狀 磁性體粒子在絕緣材料中往單向定向。 使平板狀磁性體粒子定向之方法,係有人提出使形成 於基體上之含有平板狀磁性微粒子之__磁石的磁極 間之方法(專敎獻4),以及❹㈣有永久磁石之成形 模具之方法(專利文獻5)。 此^方法中’使用樹脂作為絕緣材料,並在該樹脂於 :硬化刖或在加齡融下具有流祕之㈣下施加磁場, 藉此使平板狀磁性體粒子定向。 二:利文獻4或專利文獻5所記載之使平板狀磁性 融:且:、1之方法中’即使在樹脂於熱硬化前或在加熱熔 有性之狀態下施加磁如使平板狀磁性體粒子 疋向=具有所得之複合魏體的訂,較小之問題點。 雜診接各個軚磁性的平板狀磁性體粒子本身的訂,, 力大之硬_的平板狀磁性體粒子更高,但 在以在㈣場施加方法巾,·㈣力小之㈣㈣平板狀 323724 5 201230083 磁性體粒子的定向性差’而具有複合磁性體全體所得之# r’較小之問題點。尤其當製造具有100# m以上的厚度之複 合磁性體時,乃具有無法得到良好的#1*’之問題點。 此外,近年來在90至220MHz的VHF波段中,就電波 資源的有效應用之觀點來看,計劃從對類比電視的應用變 更至其他用途。此等用途中,當中較有希望者為攜帶式資 訊終端用途者’該攜帶式資訊終端中’由於VHF波段的電 波波長較長而難以達成天線的小型化’目前仍不得不代用 大型的棒狀天線或耳機線來作為天線。 另一方面’攜帶式資訊終端的用途’在從通話擴大至 通話以外的通信中,必須在即使將攜帶式資訊終端放入於 皮包或口袋中之狀態下亦能夠接收,所以天線於攜帶式資 訊終端之内藏化乃成為必要事項。因此,期待一種波長縮 短效果大’且可使VHF波段的天線達成小型化之磁性材料。 然而,當將以往的磁性材料應用在VHF波段的天線 時’磁性材料的表面會產生渦電流,該渦電流會朝向抵銷 所施加之磁場的變化而產生磁場,因而具有磁性材料的磁 導率明顯降低之問題點。 此外’由於渦電流的增大會產生焦耳熱所形成之能量 才貝耗’故難以將磁性材料用作為天線或電子零件等之材料。 專利文獻6’提出一種將球狀或扁平狀的磁性粉末分 :緣材料中之複合物,且為1GHz之複磁導率的實部 …於1,且複磁導率的損耗正切tan占以(以下有時略 稱為tan占"、兔Λ Ί 以 >>為0· 1以下之複合磁性體。 6 323724 201230083 根據該複合磁性體,可避免因渦電流所造成之磁特性 的劣化’在500MHz至1GHz的頻率波段亦可降低損耗。 另一方面,作為可在VHF波段中使用之磁性材料,提 出一種高頻用肥粒鐵(ferrite)。 然而’專利文獻6所提出之複合磁性體中,雖然可降 低因渴電流所造成之磁特性的劣化和500MHz至1GHz頻率 波段中的損耗,但在低於5 0 0 Μ Η z的頻率中,損耗正切有增 、向尤其100MHz之損耗正切tan (5 #為0· 1以上。 即使將該複合磁性體應用在VHF波段的天線,亦存 難以達成天線的更加小型化之問題點。 VHF t卜’高頻用肥粒鐵雖可使用在VHF波段,但由於該 頻率之共鳴損耗的景彡響較顯著之頻率波段,故訂,對 目依性大,而有電路設計較難進行之問題點。 可靠2,由於肥粒鐵為喊’故具有形狀加工性或機械 會產之問題點’因此’當應用在攜帶式資訊終端時 王♦多限制,故不佳。 如下式特性阻抗Zg,可使用真空的特性阻抗ζ。而表示 Ζ。,(訂’ / ε r,)1/2 · ·.⑵ 性阻浐:式⑵’ η,與#之值的差愈小’真空中的特 -方:與複合磁性體的特性阻抗Zg之值的差亦愈小。另 阻抗z *由於電波所行進之空間的特性阻抗與真空的特性 可抑以°幾乎為相同值,所以^與^,之值的差愈小,命 可抑制用於阻抗匹配之電力損耗。 愈 323724 7 201230083 此外,藉由式⑴,可得知當 田襁短電磁波的波長時, ,、需θ加ει·與#1·之值即可,但 之值的差愈大,所能夠接收傳送之頻率皮:。: 此,為了在寬頻率波段下接收傳送更多資訊獅 r,之值與//r’之值的差。 4雕J ε 因此,作為可達成電子零件或電子設備的小型化並抑 制電力祕’並且在寬頻率波段下接收傳送更多資訊之複 合磁性體’係有人提出—種藉由將球狀磁性體粒子分散於 絕緣材中,使1GHz的頻率之訂,丨5以上^,. er 0.2.ΧΤ» ^(^rVer^)1-^ 〇.5,χ^ ι τ 之複合磁性體(專利文獻7)。 .,、、:而專利文獻7所記載之複合磁性體中,由於使用 球狀磁性體粒子,所以各個磁性體粒子的去磁場係數增 大,使所得之複合磁性體的不足,即使可抑制阻抗匹 配所造成之電力損耗,但仍有電子零件或電子設備的小型 化不足之問題點。 另一方面,專利文獻8所記載之複合磁性體中,由於 使用導電性高的金屬材料作為平板狀磁性體粒子,所以複 合磁性體的yr’之值亦大,但由於該磁性體粒子與絕緣材 料之界面具有靜電電容,會使’之值增加至所需程度以 上’而有阻抗匹配所造成之電力損耗增加之問題點。 s亥電力損耗,例如在天線接收傳送電磁波時會成為電 磁波的輸出損耗,而使天線最重要的性能之發射效率降 低。此外’由於# r’與ε r,之差擴大,故亦存在天線所能 8 323724 201230083 夠接收傳送之頻率波段變窄之問題。 再者’大部分的磁性體粒子中’由於々r,較e r’更小 (μι·’ < ε r’),即使藉由改良磁性體粒子來增大複合磁性 體本身的//r ,亦會使£r’之值增加至所需程度以上,無 法達成電子零件或電子設備的小型化,此外,無法抑制電 力損耗’並存在著無法達成天線所能夠接吹傳送之頻率的 寬波段化之問題點。 此般問題點’在特別要求小型化之電子設備,例如行 動電話、攜帶式資訊終端、多功能型攜帶式資訊設備等攜 帶式資訊設備中所使用之天線等當中,乃成為重大的問題 點。 尤其是,最近顯著地普及之智慧型手機等多功能攜帶 式資訊終端中,由於從與框體為大致相同大小之顯示器部 產生較強電場,所以在該顯示器部上必須卩且隔電磁波。因 此,天線必須設置在不與顯示器重疊之位置上或是設置在 與顯示器隔著間隔之位置上,然而,在框體内可設置天線 之位置有限,並且為極狹窄之區域。 另一方面’攜帶式資訊設備中所使用之Ι-Seg廣播與 多媒體廣播,由於所使用之電磁波的波長較長,故須接收 寬波長區域的電磁波。以往,框體内的小型天線無法得到 充分的接收性能,因此,有人提出—種以此等廣播的接收 為目的,將藉由使天線部分可伸縮自如而能夠延長至框體 ,小的數倍長度之鞭形天線,設置在框體外之搞帶式資訊 '^備。然而,即使使用該鞭形天線,當將攜帶式資訊設備 9 323724 201230083 放入於皮包或口袋等時,無法拉長鞭形天線,而仍具有難 以接收此等廣播之問題點。 此外,近年來攜帶式終端中所使用之電磁波的頻率波 段最低者,為移動體用途之地面數位廣播(卜的 470MHz至770MHz。此外,日本國内正計劃應用2〇7MHz至 222MHz作為攜帶式終端用途的多媒體廣播。此外,韓國欲 將180MHz至210MHz的頻率波段應用在數位廣播中。 此般攜帶式終端中所使用之天線,必須是可裝載於攜 帶式終端之小型天線。然而,由於為了使天線產生共振需 使用波長1/4長度的天線導體,在如160MHz至222MHz般 之頻率低且波長較長之波段中,裝載於攜帶式終端時會有 天線變的過大之問題。 為了解決上述問題,專利文獻9提出一種藉由使用具 有高磁導率之肥粒鐵,而可藉由波長縮短效果使磁性體天 線達成小型化之方法。 然而,專利文獻9所記載之技術中,由於肥粒鐵般的 陶瓷材料在160MHz至222MHz中磁導率小,故波長縮短效 果小,無法充分地達成天線的小型化。再者,由於陶瓷材 料的加工性差,所以存在著可使用之形狀受到限制之問題。 (先前技術文獻) (專利文獻) (專利文獻1)日本特開2004-087627號公報 (專利文獻2)日本特開昭63-35701號公報 (專利文獻3)日本特開平1-188606號公報 10 323724 201230083 ^ (專利文獻4)日本特開昭57-127931號公報 (專利文獻5)日本特開2000-141392號公報 (專利文獻6)日本特開2008-181905號公報 (專利文獻7)日本特開2010-103427號公報 (專利文獻8)日本特開2008-263098號公報 (專利文獻9)日本特開2009-159244號公報 【發明内容】 (發明所欲解決之課題) 本發明係鑒於上述情形而成者’目的在於提供一種可 應用70MHz至5〇〇MHz的頻率波段,且該頻率波段之複磁導 率的實部μ r’大’複磁導率的損耗正切tan占#為〇.丨以 下之具備平板狀磁性體粒子之複合磁性體及其製造方法及 天線以及通信裝置。 此外’該目的在於提供一種在使電子零件或電子設備 達成小型化時,配合該小型化,使複磁導率的實部,充 分地大’且使複磁導率的實部#1·’之值與複介電常數的實 部er’之值的差縮小,結果可使電子零件或電子設備達成 小型化,同時可抑制阻抗匹配所造成之電力損耗並達成寬 波段化之複合磁性體及具備其之天線以及通信裝置。 此外,該目的在於提供一種藉由使上述平板狀磁性體 粒子在樹脂中良好地定向,而提高複磁導率的實部之 複合磁性體及其製造方法及天線以及通信裝置。 再者’該目的在於提供一種亦可應用在1 6〇MHZ至 2 2 2MHz般之低頻率波段’並且可裝載於攜帶式終端之小塑 323724 11 201230083 單極天線。 (用以解決課題之手段) 本發明者們係為了解決上述課題 果得到下列發現。 而進行精心探討201230083 VI. TECHNOLOGICAL FIELD OF THE INVENTION The present invention relates to a composite magnetic body, a method of manufacturing the same, an antenna, and a communication device, and more particularly to a VHF that can be suitably used in a frequency band of 70 MHz to 500 MHz. High-frequency circuit board of electromagnetic wave in band, frequency-frequency electronic part, magnetic sheet, electromagnetic wave concealing sheet, resin-bonded magnet, magnetic recording medium, antenna, etc., and composite magnetic body of real part/zr' with high complex permeability And a method of manufacturing the same, an antenna including the composite magnetic body, and a communication device including the antenna. Further, the present invention relates to a monopole antenna in which the above-described composite magnetic body is mounted on a portable terminal in the range of 160 MHz to 222 MHz. This application is filed in Japan according to Japanese Patent Application 2010-266903, which was filed in Japan on November 30, 2010, Japanese Patent Application No. 201 1-064310, which was filed in Japan on March 23, 2011, and Japan, April 25, 2011. Japan's special offer 2011-097157, Japan's special offer 2011-122440, which was applied for in Japan on May 31, 2011, Japan's special offer 2011-167077, which was applied for in Japan on July 29, 2011, and Japan's application on July 29, 2011. Japan's special wish 2011-167078, Japan's special offer 2011-254169, which was applied for in Japan on November 21, 2011, Japan's special offer 2011-257615, which was applied for in Japan on November 25, 2011, and Japan, November 25, 2011 Priority is claimed on Japanese Patent Application No. 2011-257616, the entire disclosure of which is incorporated herein. [Prior Art] Magnetic materials are known to be used as a compound which is mixed and dispersed in an insulating material such as an organic high-grade 323724 3 4 201230083 sub-material for the characteristics, productivity, ease of use, and the like of electromagnetic waves. Magnetic body. The magnetic material is a magnetic recording medium such as an electronic component mounted on an electronic device, a magnetic sheet, an electromagnetic interference suppression sheet, an electric product such as a motor or a transformer, a video tape or a floppy disk (registered trademark). In recent years, with the increase in speed and density of the device, there is a strong demand for electronic components or circuit boards or antennas mounted in electronic devices, especially for miniaturization and low consumption of the materials. Electricityization. In general, the wavelength of the electromagnetic wave transmitted in the substance allows the wavelength h of the electromagnetic wave transmitted in the vacuum to be the real part ε r of the complex permittivity of the substance (hereinafter sometimes abbreviated as £ r), and the complex magnetic The real part yr' of the conductance (hereinafter sometimes abbreviated as yr') is expressed by the following formula (1), λ g = λ 〇 / ( ε rJ · β r' ) 1 / z · · · (1) (1) The larger the er' and / / r', the larger the shortening rate of the wavelength. Therefore, by increasing the ε r′ and # r′ of the magnetic material constituting the electronic component, the circuit board, or the antenna, the shortening rate of the wavelength λ g can be increased, and the electronic component, the circuit board, the antenna, or the like can be miniaturized. . In the material which increases the shortening rate of the wavelength, a composite magnetic body in which magnetic particles are mixed and dispersed in an insulating material constituting an electronic component or a circuit board has been proposed (Patent Document 1). In the composite magnetic body, the shortening rate of the wavelength is increased by increasing /z r'. When spherical magnetic particles are used in the composite magnetic material, it is generally known that the problem of difficulty in increasing the composite magnetic body due to the large demagnetizing factor in each magnetic particle is 323724 4 201230083 Therefore, it has been proposed to use a magnetic particle having a thickness of less than or equal to the thickness of the flat magnetic particle, and to have a flat aspect, a scale shape, a flake shape, and the like. Magnetic particles of various shapes having a large diameter/thickness (for example, refer to Patent Documents 2 and 3). In such a flat magnetic particle, a high order can be obtained in the direction of the lowest depolarization coefficient, i.e., the direction of the long axis. Therefore, the composite magnetic body in which the flat magnetic particles are mixed and dispersed in the insulating material is high in order to effectively apply the effect of the demagnetization factor, and it is necessary to orient the flat magnetic particles in the insulating material in one direction. A method of orienting a flat magnetic particle, a method of forming a magnetic pole between magnets of a magnet containing a flat magnetic particle formed on a substrate (Special 4), and a method of forming a permanent magnet with a permanent magnet (Patent Document 5). In the method, a resin is used as an insulating material, and a magnetic field is applied to the resin under hardening or under the age of (4), thereby orienting the flat magnetic particles. (2) The magnetic properties of the flat plate described in Patent Document 4 or Patent Document 5 are: and in the method of 1, the magnetic material is applied to the flat magnetic body even before the resin is thermally cured or heated. Particle orientation = the problem with the resulting composite Wei body, which is a minor problem. In the miscellaneous diagnosis, the flat magnetic particles of each of the neodymium magnets are arranged, and the hard magnetic particles of the flat magnetic particles are higher, but the method is applied in the (four) field, and (4) the force is small (four) (four) flat 323724 5 201230083 The magnetic particles have poor orientation, and the #r' obtained by the composite magnetic body is small. In particular, when a composite magnetic body having a thickness of 100 # m or more is produced, there is a problem that a good #1*' cannot be obtained. In addition, in the VHF band of 90 to 220 MHz in recent years, it is planned to change from the application of analog TV to other uses from the viewpoint of effective application of radio wave resources. Among these applications, the more promising ones are portable information terminal users. In the portable information terminal, it is difficult to achieve miniaturization of the antenna due to the long wavelength of the radio wave in the VHF band. The antenna or headphone cable comes as an antenna. On the other hand, the 'purpose of the portable information terminal' must be able to receive the portable information terminal even if the portable information terminal is placed in a leather bag or a pocket, so that the antenna is in the portable information. The internalization of the terminal is a necessary matter. Therefore, it is expected that a magnetic material having a large wavelength reduction effect can be achieved and the antenna of the VHF band can be miniaturized. However, when a conventional magnetic material is applied to an antenna of a VHF band, an eddy current is generated on the surface of the magnetic material, and the eddy current generates a magnetic field toward a change in the applied magnetic field, thereby having a magnetic permeability of the magnetic material. Significantly reduce the problem point. Further, since the increase in the eddy current causes the energy generated by the Joule heat to be consumed, it is difficult to use the magnetic material as a material such as an antenna or an electronic component. Patent Document 6' proposes a composite in which a spherical or flat magnetic powder is divided into a rim material, and is a real part of a complex magnetic permeability of 1 GHz... at 1, and a loss tangent of complex magnetic permeability is occupied by (The following is abbreviated as tan occupant ", rabbit Ί &>> is a composite magnetic body of 0.1 or less. 6 323724 201230083 According to the composite magnetic body, magnetic properties due to eddy current can be avoided. Deterioration 'in the frequency band of 500 MHz to 1 GHz can also reduce the loss. On the other hand, as a magnetic material that can be used in the VHF band, a high-frequency ferrite is proposed. However, the composite proposed in Patent Document 6 In the magnetic body, although the deterioration of the magnetic characteristics due to the thirsty current and the loss in the frequency band of 500 MHz to 1 GHz can be reduced, in the frequency lower than 500 Μ Η z, the loss tangent increases, especially to 100 MHz. Loss tangent tan (5 # is 0·1 or more. Even if the composite magnetic body is applied to an antenna of the VHF band, it is difficult to achieve a problem of further miniaturization of the antenna. VHF tb' Used in the VHF band, but due to the The frequency of resonance noise is more pronounced in the frequency band, so it is more difficult to carry out the problem of circuit design. Reliable 2, because of the fertilization of iron, it has shape processing or The problem of mechanical production is 'so that' when the portable information terminal is used, the king ♦ is more limited, so it is not good. The characteristic impedance Zg is as follows, and the characteristic impedance of the vacuum can be used, and Ζ., (booking ' / ε r,) 1/2 · ·. (2) Sexual resistance: The smaller the difference between the values of equation (2)' η and #, the special-degree in vacuum: the smaller the difference from the value of the characteristic impedance Zg of the composite magnetic body The other impedance z* is almost the same value as the characteristic impedance of the space in which the electric wave travels and the vacuum characteristic, so the smaller the difference between the values of ^ and ^, the power loss for impedance matching can be suppressed. 323724 7 201230083 In addition, by the formula (1), it can be known that when the wavelength of the electromagnetic wave is short, the value of θ plus ει· and #1· is required, but the larger the difference is, the receiver can receive Frequency of transmission:: This, in order to receive and transmit more resources in a wide frequency band The difference between the value of lion r and the value of //r'. 4 eagle J ε Therefore, as a composite that can achieve miniaturization of electronic parts or electronic devices and suppress power secrets, and receive more information in a wide frequency band. The magnetic body has been proposed by dispersing spherical magnetic particles in an insulating material to set a frequency of 1 GHz, 丨5 or more. er 0.2.ΧΤ» ^(^rVer^)1-^ 〇 .5, 复合^ ι τ composite magnetic body (Patent Document 7). In the composite magnetic material described in Patent Document 7, since the spherical magnetic particles are used, the demagnetizing field of each magnetic particle When the coefficient is increased, the resulting composite magnetic body is insufficient, and even if the power loss due to impedance matching can be suppressed, there is still a problem that the electronic component or the electronic device is insufficient in size. On the other hand, in the composite magnetic material described in Patent Document 8, since a highly conductive metal material is used as the flat magnetic particles, the value of yr' of the composite magnetic material is also large, but the magnetic particles and the insulating material are insulated. The interface of the material has an electrostatic capacitance, which causes the value of 'to be increased above the required level' and the power loss caused by impedance matching increases. The power loss of the shai, for example, becomes an output loss of the electromagnetic wave when the antenna receives and transmits the electromagnetic wave, and the emission efficiency of the most important performance of the antenna is lowered. In addition, since the difference between #r' and ε r is widened, there is also a problem that the frequency band of the antenna can be narrowed by receiving the transmission of 8 323724 201230083. Furthermore, in most of the magnetic particles, 々r is smaller than e r' (μι·' < ε r'), and the composite magnetic body itself is increased by modifying the magnetic particles themselves. It will increase the value of £r' to the required level or more, and it is impossible to achieve miniaturization of electronic components or electronic devices. In addition, power loss cannot be suppressed, and there is a wide band that cannot achieve the frequency at which the antenna can transmit and transmit. The problem of the problem. Such a problem has become a major problem in the use of electronic devices such as mobile phones, portable information terminals, and portable information devices such as portable information devices, which are particularly required to be miniaturized. In particular, in a multi-functional portable information terminal such as a smart phone which has been widely used recently, since a strong electric field is generated from a display unit having substantially the same size as a casing, electromagnetic waves are required to be separated from the display unit. Therefore, the antenna must be placed at a position that does not overlap the display or at a position spaced apart from the display. However, the position of the antenna in the frame can be limited and it is an extremely narrow area. On the other hand, the Ι-Seg broadcast and the multimedia broadcast used in the portable information device have to receive electromagnetic waves in a wide wavelength region because the wavelength of the electromagnetic wave used is long. In the past, small antennas in the casing have not been able to obtain sufficient reception performance. Therefore, it has been proposed to extend the antenna portion to the frame for a small number of times for the purpose of receiving such broadcasts. The whip antenna of the length is set in the outside of the frame. However, even when the whip antenna is used, when the portable information device 9 323724 201230083 is placed in a purse or a pocket or the like, the whip antenna cannot be elongated, and there is still a problem that it is difficult to receive such broadcast. In addition, in recent years, the lowest frequency band of electromagnetic waves used in portable terminals is terrestrial digital broadcasting for mobile applications (from 470 MHz to 770 MHz. In addition, Japan is planning to apply 2 to 7 MHz to 222 MHz as a portable terminal. Multimedia broadcasting for use. In addition, Korea wants to apply a frequency band of 180 MHz to 210 MHz in digital broadcasting. The antenna used in such a portable terminal must be a small antenna that can be mounted on a portable terminal. Antenna resonance requires the use of a 1/4-length antenna conductor. In a band with a low frequency and a long wavelength such as 160 MHz to 222 MHz, there is a problem that the antenna becomes too large when it is mounted on a portable terminal. Patent Document 9 proposes a method of miniaturizing a magnetic antenna by a wavelength shortening effect by using ferrite iron having a high magnetic permeability. However, in the technique described in Patent Document 9, due to the fat grain The iron-like ceramic material has a small magnetic permeability in the range of 160 MHz to 222 MHz, so the wavelength shortening effect is small, and the antenna cannot be sufficiently obtained. In addition, the shape of the ceramic material is limited, and the shape of the ceramic material is limited. (Prior Art Document) (Patent Document) (Patent Document 1) Japanese Patent Laid-Open Publication No. 2004-087627 (Patent Literature) (2) Japanese Patent Laid-Open Publication No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. Japanese Laid-Open Patent Publication No. 2008-181092 (Patent Document No.) JP-A-2009-159244 SUMMARY OF INVENTION Technical Problem The present invention has been made in view of the above circumstances, and an object thereof is to provide a frequency band in which a frequency band of 70 MHz to 5 〇〇 MHz can be applied, and the frequency band is The real part of the complex magnetic permeability μ r 'large 'complex permeability loss tangent tan 占 # 丨 丨 丨 丨 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合The purpose In order to reduce the size of the electronic component or the electronic device, the real part of the complex magnetic permeability is sufficiently large and the value of the real part of the complex magnetic permeability #1·' is complex The difference in the value of the real part er' of the dielectric constant is reduced, and as a result, the electronic component or the electronic device can be miniaturized, and the power loss due to impedance matching can be suppressed and the wide-band composite magnetic body and the antenna having the same can be realized. Further, it is an object of the invention to provide a composite magnetic body which is a real part which improves the complex magnetic permeability by orienting the flat magnetic particles in a resin, a method for producing the same, an antenna, and a communication device. Furthermore, the object is to provide a small plastic 323724 11 201230083 monopole antenna which can also be applied in a low frequency band of 16 MHZ to 2 2 2 MHz and can be mounted on a portable terminal. (Means for Solving the Problems) The inventors of the present invention have found the following findings in order to solve the above problems. Carefully explore

亦即發現到:若是將平均厚度為 以下,平均長徑為以上 比(長徑/厚度)為5以上之平板狀磁性體二:均長寬 材料中而成之複合磁性體,則可使 磁於絕緣 至簡Hz的頻率波段之複磁導率的實复4性體之麵z 磁導率的損耗正切tan5 //為〇· 1以下 大於1 ’且複 合磁性體應用在爾波段的天線,結果P ’可將該複 小型化,以及天線於卿式資訊終端之内2天線的更加 此外,將平板狀磁性體粒子分散於絕緣材料中之複人 磁性體中,當平板狀磁性體粒子為少量時,容㈣句地二 散於絕緣材料中,隨著平板狀磁性體粒子量的增加,由ς 平板狀磁性體粒子彼此纏繞或凝料,於該^板狀磁性 體粒子間產生空間’絕緣材料難以進人於該空間内,結果 在所得之複合磁性體中產生氣孔4外,在使平板狀=性 體粒子往單向定向時’相互平行地配置之平板狀磁性體粒 子間的間隔變得極窄,絕緣材料難以進入於該狹窄空間 内’結果在所得之複合磁性體中產生氣孔。 因此,發現到:當將平板狀磁性體粒子分散於絕緣材 料中時,可藉由減少此等平板狀磁性體粒子間所產生之氣 孔,雖然VI·’之值增大,但ε r,之值幾乎不變,結果可縮 323724 12 201230083 小μι*之值與εΓ’之值的差。 此外,當混合以往的雙酚型環氧樹脂與平板狀磁性體 粒子來作為絕緣材料時,所得之成形材料,該環氧樹脂的 Β旎基吸附於平板狀磁性體粒子的表面,使高分子鏈包圍 磁性體粒子的周圍而成為長長地纏繞之狀態。此般高分子 鏈為長^地纏繞之狀態的成形材料,該高分子鏈有時會成 為立體障礙而阻礙平板狀磁性體粒子的定向。 因此,為了使平板狀磁性體粒子的流動性變佳,即使 增加成形材料中的溶劑量而在巨觀上呈低黏度,高分子鏈 之立體P早礙的影響仍大,仍會阻礙平板狀磁性體粒子的定 向。 一 f方面,#為了降低高分子鏈之立體障礙的影響而 縮门刀子鏈時,向分子鏈彼此的縮合或鍵結反應不足, 結果使所得之複合贿體的機械強度降低,因情況的不同, 甚至有無法轉形狀之疑慮,因而無法使用在電子零件或 電路基枝等。 合 發現到·為了降低高分子鏈之立體障礙的影響 鏈具有平面地且不易纏繞於平板狀磁性體粒子之 Λ所^之,時’可提升平板狀磁性體粒子依據磁場摊 僅V二於ί定向性。再者,藉由使用所聚合之官能基並非 而是具有以單體單位所聚合之官能基之樹 分子鏈較短’亦形成較多鍵結,藉此提升所得 復°磁性體的機械強度,且亦容易維持形狀。 此外’發現到:若是將可撓性及伸縮性佳之樹脂,添 323724 13 201230083 加於主鏈具有不易纏繞於平板狀磁性體粒子之上述環狀結 構之樹脂,則該樹脂可進入於平板狀磁性體粒子彼此的= 隙’藉此可得到進-步提升複合磁性體之複磁導率的實部 #r’,且進一步提升複合磁性體從基材之剝離性,並且生 產性佳之複合磁性體。 再者,發現到·當混合上述樹脂與平板狀磁性體粒子 使成形材料成形並施加磁場時,以使磁力線大致平行於成 形體的表面之方式施加1次或複數次磁場,藉此提升複合 磁性體之複磁導率的實部yr’。 此外,發現到:以上述複合磁性體來被覆單極天線的 導體,可使該天線達成小型化。 亦即,本發明係關於下列内容。 (1) 一種複合磁性體,其係將平板狀磁性體粒子分散 於絕緣材料中而成,前述平板狀磁性體粒子的平均厚度為 0. 01 以上0.5/zm以下,平均長徑為0.05 am以上1〇 ym以下,且平均長寬比(aspect ratio,長徑/厚度)為5 以上。 (2) 如前述(1)所述之複合磁性體,其中,至 500MHz的頻率波段之複磁導率的實部a r,大於1,且複磁 導率的損耗正切tan(5 y為0. 1以下。 (3) 如前述(1)所述之複合磁性體,其中,7〇MHz至 500MHz的頻率波段之複磁導率的實部v r’大於7,且複磁 導率的損耗正切tan 5 //為〇. 1以下。 (4) 如前述(1)所述之複合磁性體’其中,7〇MHz至 323724 14 201230083 5〇〇MHZ的頻率波段之複磁導率的實部"r,大於10,且複磁 導率的損耗正切ta…為〇1以下。 (5) 如别述(1)所述之複合磁性體,其令,前述平板狀 磁性體粒子為含有選自鋁(A1)、鉻(Cr)、錳(Μη) 、鈷(Co)、 銅(Cu)、鋅(Zn)、鈮(Nb)、翻(M〇)、銦(In)、錫(Sn)的群 組之1種或2種以上的金屬元素之鐵_鎳合金。 (6) 如前述(1)所述之複合磁性體,其中,前述平板狀 磁性體粒子是藉由對平均粒徑〇 5#m以下的球狀磁性粒 子施以機械應力,使該球狀磁性粒子彼此變形及熔著而成。 (7) 如則述(1)所述之複合磁性體,其中,至 220MHz的頻率波段之複磁導率的實部訂,大於1,且複磁 導率的損耗正切tan5以為〇· 〇5以下。 (8) 如前述(1)所述之複合磁性體,其中,氣孔率為2〇% 以下。 (9) 如前述(8)所述之複合磁性體,其中,7〇ΜΗζ至 500MHz的頻率波段之複磁導率的實部#『,為7以上,複介 電常數的實部er’為15以上,且(以,…,)—1/2為〇」 以下,(以r’/er,)1/2為0.5以上1以下。 . (10) 如前述(9)所述之複合磁性體,其中,7〇MHz至 500MHz的頻率波段之複磁導率的損耗正切以為〇 〇5 以下,複介電常數的損耗正切以下。· (⑴如前述⑴所述之複合磁性體,其中,前述絶緣 材料係、含有··主鏈具有結構且科料體單位所聚合 之官能基之第1樹脂。 323724 15 201230083 (12) 如前述(11)所述之複合磁性體,其中,前述樹脂 為熱硬化性樹脂。 (13) 如前述(11)所述之複合磁性體,其中,前述樹脂 為環氧樹脂。 (14) 如前述(11)所述之複合磁性體,其中,前述樹脂 為二環戊二烯型環氧樹脂。 (15) 如前述(11)所述之複合磁性體,其中,前述平板 狀磁性體粒子之前述樹脂中的定向方向與該平板狀磁性體 粒子的長軸方向所形成之角度為20°以下。 (16) 如前述(11)所述之複合磁性體,其中,70MHz至 500MHz的頻率波段之複磁導率的實部#r’為7以上。 (17) 如前述(11)所述之複合磁性體,其中,更含有對 前述第1樹脂賦予可撓性之樹脂的第2樹脂。 (18) 如前述(17)所述之複合磁性體,其中,前述第2 樹脂為具有雙酚A型骨架及雙酚F型骨架中的至少1種之 環氧樹脂。 (19) 如前述(17)所述之複合磁性體,其中,前述第2 樹脂為於1分子中含有2個以上的環氧基且具有醚骨架之 環氧樹脂。 (20) 如前述(17)所述之複合磁性體,其中,前述第2 樹脂為具有丙二醇加成雙酚A型骨架及乙二醇加成雙酚A 型骨架中的任一種之環氧樹脂。 (21) 如前述(17)所述之複合磁性體,其中,70MHz至 500MHz的頻率波段之複磁導率的實部/zr’為7以上。 16 323724 201230083 (22)—種複合磁性體的製造方法,該複合磁性體係如 前述(1)至(21)中任一項所述之複合磁性體,其具備有:將 使平均粒徑〇.5am以下的球狀磁性粒子分散於含有界面 活性劑之溶液中而成之漿液(slurry)及分散介質填充於可 雄、閉的容器内,以使前述漿液及前述分散介質的合計體積 ^前述容H内的體積成為相同,在密閉狀態下將該聚液與 則述分散介質—⑽拌,使前述賴磁性粒子彼此變形及 溶著而形成平板狀磁性錄子之第丨步驟;使前述平板狀 磁f生體粗子分散並混合於在溶劑巾簡㈣緣 =成形材料之第2步驟;以及包含有:將前述成: ^枓成L佈於基材上而獲得成形體之成形步驟、 月J述成形體乾燥/硬化之乾燥/硬化步驟之第3步驟。 =3)如前述(22)所述之複合磁性體的製造方法,其 中’則述絕緣材料,為主鏈具有環狀結構且具有以單體」 位所聚合之官能基之樹脂。 早 (24)如前述(22)所述之複合磁性體的製造方法,其 :’在前述第3㈣巾,在料成形步職,進行對所择 =成,體施加磁場錢該成形體巾的前述平板狀磁心 、,早向定向之定向步驟’接著進行前述乾燥/硬化步驟。 …(25)一種天線,係具備如前述(1)至(21)中任一 述之複合磁性體而成。 、 成。⑽-種通信裝置,係具備如前述(25)所述之天線而 (2Ό-種單極天線,係天線導體由如前述⑴所述之 323724 17 201230083 複合磁性體所被覆。 (28) 如前述(27)所述之單極天線,其中,前述複合磁 性體於160MHz至222MHz的頻率波段之複磁導率的實部 y r’為3以上。 (29) 如前述(28)所述之單極天線,其令,前述複合磁 性體的被覆厚度為2. 4min以上l〇mm以下。 (30) 如前述(27)所述之單極天線,其中,前述複合磁 性體於160MHz至222MHz的頻率波段之複磁導率的實部 /z r’為6以上。 (31) 如前述(30)所述之單極天線,其中,前述複合磁 性體的被覆厚度為1. 2mm以上l〇mm以下。 (32) 如前述(27)所述之單極天線,其中,前述天線導 體的長度為200mm以下。 (發明之效果) 根據本發明之複合磁性體,由於使用平均厚度為〇. 01 Vm以上0. 以下,平均長徑為〇. 〇5y m以上5ym以 下’且平均長寬比(長极/厚度)為5以上之平板狀磁性體粒 子,故可使70MHz至500MHz的頻率波段之複磁導率的實部 "r,大於1,且複磁導率的損耗正切tan (5 "為0.1以下, 因此可大幅提1¾該頻率波段之波長的縮短率。 因此,若將該複合磁性體應用在VHF波段的天線,則 可防止該複合磁性體表面之渦電流的產生,防止er’的降 低,而更進一步達成天線的小型化。 因此,若將該複合磁性體應用在VHF波段的天線或電 18 323724 201230083 子零件,則可進一步達成天線或電子零件的小型化。 根據本發明之複合磁性體,由於將具有上述平板狀磁 性體粒子之複合磁性體的氣孔率設為20%以下,雖然使複 磁導率的實部#!’之值增大,但可使複介電常數的實部ε r’之值幾乎不變。因此,可縮小複磁導率的實部#r’之值 與複介電常數的實部ε r’之值的差,結果可使應用該複合 磁性體之電子零件或電子設備達成小型化,並抑制阻抗匹 配所造成之電力損耗。 根據本發明之複合磁性體,因含有:上述平板狀磁性 體粒子、以及主鏈具有環狀結構且具有以單體單位所聚合 之官能基之第1樹脂’由於該樹脂具有平面地且不易纏繞 於平板狀磁性體粒子之結構,所以可減少由樹脂所形成之 立體障礙對該平板狀磁性體粒子所造成的影響。因此,可 得到平板狀磁性體粒子的定向良好,且複磁導率的實部# r’高之複合磁性體。 再者,由於使用具有以單體單位所聚合之官能基之樹 脂,可使樹脂的鍵結變得堅固,而具有可使用作為電子零 件等之成形體的充分機械強度。 根據本發明之複合磁性體,因含有:上述平板狀磁性 體粒子、主鏈具有環狀結構且具有以單體單位所聚合之官 能基之第1樹脂、以及對該第1樹脂賦予可撓性之第2樹 脂,因此,該主鏈具有環狀結構且具有以單體單位所聚合 之官能基之第1樹脂,可減少由樹脂所形成之立體障礙對 該平板狀磁性體粒子所造成的影響。因此,可提升平板狀 19 323724 201230083 磁性體粒子往單向之定向性,而容易得到複磁導率的實部 Μ Γ南之複合磁性體。 此外,由於第2樹脂對該第丨樹脂賦予可撓性,所以 可提升複合磁性體本身的可撓性及伸縮性,結果可得到生 產性佳之複合磁性體。 根據本發明之複合磁性體的製造方法,因具備有:將 使平均粒彳i 町的球狀磁性粒子分散 生劑之溶液中而成之漿液及分散介f,填充於可密閉的 4内,以使前述漿液及前述分散介質的合計體積量與前 述容器内的體積成為相同,在密閉狀態下將該漿液盥前述 分散介質-關拌,使前述球狀磁性粒子彼此變形及炼著 =成平板狀磁性體粒子.之第i步驟;使前述平板狀磁性 體粒子分散並混合於在溶射溶解有絕緣材料之溶 形成成形材料之第2步驟;以及包含右:此合' 成形或塗佈於基材上而得到成频之成形步^述成形^料 成形體乾無/硬化之乾燥/硬化步驟之第3吏〗辻· 容易地製作出70MHz至5GGMHz的頻率波/^ ’因此’可 部"r,大,且複磁導率的損耗正切tand <複磁導率的實 複合磁性體。 々為〇·1以下之 此外 ,當使用主鏈具㈣I轉且㈠ 聚合之官能基之樹脂作為絕緣材料時,可办早體早位) 板狀磁性體粒子的定向良好,複磁 4易地製作出-複合磁性體。 Ά實部灯’高. 進行對所 再者,在第3步驟中’在前述成形步驟後 20 323724 201230083 得之成形體施加磁場以使該成形體中的前述平板狀磁性體 粒子往單向定向之定向步驟,接著當進行前述乾燥/硬化步 驟時,可容易地製作出平板狀磁性體粒子的定向更良好, 且複磁導率的實部#r’更高之複合磁性體。 根據本發明之天線,由於具備上述複合磁性體,可藉 由使用在70MHz至500MHz的頻率波段中之複磁導率的實部 #r’高之複合磁性體,而將天線導體縮短至較波長的1/4 更短,使天線全體達成小型化。因此,可提供進一步達成 小型化之天線。 再者,當具備氣孔率20%以下之複合磁性體時,可提 升發射效率。因此可提供一種小型且抑制阻抗匹配所造成 之電力損耗,小型化且發射效率高,並且可在70MHz至 500MHz的寬波段中使用之天線。 此外,當具備含有主鏈具有環狀結構且具有以單體單 位所聚合之官能基之第1樹脂作為上述絕緣材料之複合磁 性體時,或是具備含有前述第1樹脂以及對前述第1樹脂 賦予可撓性之第2樹脂作為上述絕緣材料之複合磁性體 時,由於可得更高的#r’,故可提供進一步達成小型化之 天線。 根據本發明之通信裝置,由於具備上述天線,故可藉 由使用經小型化後之天線而達成通信裝置全體的小型化。 因此可提供進一步達成小型化之通信裝置。 再者,當具備安裝有上述氣孔率20%以下之複合磁性 體之天線時,藉由使用小型且發射效率高,並可在寬波段 21 323724 201230083 中使用之天線,而可達成通信裝置全體的小型化及通信性 能的提升。因此,可提供進一步達成小型化並可在70MHz 至500MHz的寬波段中使用之通信裝置。 根據本發明之單極天線,由於將上述複合磁性體被覆 於天線導體,所以可將天線導體縮短至較波長的1/4更 短,而得到可接收、傳送、或接收傳送160MHz至222MHz 之低頻率波段的電波,且可裝載於攜帶式終端之小型的單 極天線。 【實施方式】 以下說明用以實施本發明之複合磁性體及其製造方 法及天線以及通信裝置之形態。 並且,該形態係用以更容易理解發明之主旨所具體說 明者,在無特別指定下,本發明並不限定於此。 [第1複合磁性體] 本實施形態之複合磁性體,係將平板狀磁性體粒子分 散於絕緣材料中而成之複合磁性體,且係該平板狀磁性體 粒子的平均厚度為Ο.ΟΙ/zm以上0.5/zm以下,平均長徑為 0.05/zm以上10/zm以下,且平均長寬比(長徑/厚度)為5 以上之複合磁性體。 平均厚度、平均長徑,可藉由測定複數個平板狀磁性 體粒子的各個厚度及長徑(粒子内的最大長度),例如為 100個以上,較佳為500個以上之平板狀磁性體粒子的各 個厚度及長徑,並算出厚度及長徑的各平均值而求取。 此外,該平板狀磁性體粒子的平均長寬比(長徑/厚 22 323724 201230083 fm相同’可藉㈣定複數辦板狀雜體粒子的 ==r例如為_個以上,較佳為_個以上 狀磁性體^子的各個餘及厚度,來求取各個平板 =县=職寬比(長徑/厚度)’然後算出此等長 寬比(長從/厚度)的平均值而求取。 該平板狀磁性體粒子的平均厚度為〇〇1㈣以上〇5 :二下,較佳為0.012_以上〇 3心以That is, it is found that if the average thickness is below, the average long diameter is a flat magnetic body having a ratio of the above ratio (long diameter/thickness) of 5 or more: a composite magnetic body made of a material having a length and a width, the magnetic body can be made magnetic. The surface of the complex magnetic body of the complex magnetic permeability in the frequency band of the insulating to simple Hz z The loss tangent of the magnetic permeability tan5 // is less than 1 ' below 〇·1 and the composite magnetic body is applied to the antenna of the erbium band, As a result, P' can be miniaturized, and the antenna is further integrated into the two antennas in the information terminal, and the flat magnetic particles are dispersed in the complex magnetic body in the insulating material, when the flat magnetic particles are In a small amount, the volume of the four (4) sentences is scattered in the insulating material. As the amount of the flat magnetic particles increases, the flat magnetic particles entangle or condense, creating a space between the plate-shaped magnetic particles. It is difficult for the insulating material to enter the space, and as a result, the gap between the flat magnetic particles arranged in parallel with each other when the flat-shaped body particles are oriented in one direction is generated in the obtained composite magnetic body. Become extremely narrow, absolutely It is difficult for the edge material to enter the narrow space. As a result, pores are generated in the obtained composite magnetic body. Therefore, it has been found that when the flat magnetic particles are dispersed in the insulating material, the pores generated between the flat magnetic particles can be reduced, and although the value of VI·' is increased, ε r, The value is almost constant, and the result can be reduced by the difference between the value of 323724 12 201230083 and the value of εΓ'. Further, when a conventional bisphenol type epoxy resin and flat magnetic particles are mixed as an insulating material, the obtained molding material, the sulfhydryl group of the epoxy resin is adsorbed on the surface of the flat magnetic particles, and the polymer is made of a polymer. The chain surrounds the periphery of the magnetic particles and is wound in a long state. Such a polymer chain is a molding material in a state of being wound up in a long manner, and the polymer chain may become a steric obstacle and hinder the orientation of the flat magnetic particles. Therefore, in order to improve the fluidity of the flat magnetic particles, even if the amount of the solvent in the molding material is increased and the viscosity is high on the macroscopic view, the influence of the three-dimensional P of the polymer chain is still large, and the flat shape is still hindered. Orientation of magnetic particles. In the case of F, in order to reduce the influence of the steric hindrance of the polymer chain and to shrink the knife chain, the condensation or bonding reaction to the molecular chains is insufficient, and as a result, the mechanical strength of the resulting composite bribe is lowered, depending on the situation. There are even doubts about the inability to change shape, so it cannot be used in electronic parts or circuit bases. In order to reduce the influence of the steric obstacle of the polymer chain, the chain has a flat surface and is not easily entangled in the flat magnetic particles. When the flat magnetic particles are lifted, the magnetic particles are only V in the magnetic field. Orientation. Furthermore, by using the polymerized functional group, the tree chain having a functional group polymerized in a monomer unit is shorter, and more bonds are formed, thereby increasing the mechanical strength of the obtained complex magnetic body. It is also easy to maintain the shape. In addition, it was found that: in the case of a resin which is excellent in flexibility and flexibility, 323724 13 201230083 is added to a resin having a ring structure in which the main chain has a tendency to be entangled with the flat magnetic particles, and the resin can enter the flat magnetic state. The gaps between the bulk particles can be used to obtain the real part #r' of the complex magnetic permeability of the composite magnetic body, and further improve the releasability of the composite magnetic body from the substrate, and the composite magnetic body with good productivity . Further, it has been found that when the resin and the flat magnetic particles are mixed and the molding material is molded and a magnetic field is applied, the magnetic field is applied in a substantially parallel manner to the surface of the molded body to increase the composite magnetic property. The real part of the complex magnetic permeability of the body yr'. Further, it has been found that the conductor of the monopole antenna is coated with the above composite magnetic material, and the antenna can be miniaturized. That is, the present invention relates to the following. (1) A composite magnetic body obtained by dispersing flat magnetic particles in an insulating material, wherein the average thickness of the flat magnetic particles is 0.01 or more and 0.5/zm or less, and the average long diameter is 0.05 am or more. 1 〇 ym or less, and the aspect ratio (length ratio / thickness) is 5 or more. (2) The composite magnetic body according to (1) above, wherein the real part ar of the complex magnetic permeability in the frequency band of 500 MHz is larger than 1, and the loss of the complex magnetic permeability is tangent tan (5 y is 0. (1) The composite magnetic body according to the above (1), wherein the real part v r' of the complex magnetic permeability in the frequency band of 7 〇 MHz to 500 MHz is greater than 7, and the loss tangent of the complex magnetic permeability Tan 5 // is 〇. 1 or less. (4) The composite magnetic body as described in (1) above, the real part of the complex magnetic permeability of the frequency band of 7〇MHz to 323724 14 201230083 5〇〇MHZ (r) is greater than 10, and the loss tangent ta of the complex magnetic permeability is 〇1 or less. (5) The composite magnetic body according to (1), wherein the flat magnetic particle is selected from the group consisting of Aluminum (A1), chromium (Cr), manganese (Μη), cobalt (Co), copper (Cu), zinc (Zn), niobium (Nb), turn (M〇), indium (In), tin (Sn) (6) The composite magnetic body according to the above (1), wherein the flat magnetic particles are by an average particle diameter 〇 Spherical magnetic particles below 5#m (7) The composite magnetic body according to (1), wherein the real magnetic body of the complex magnetic frequency in the frequency band of 220 MHz is set, (6) The composite magnetic body according to the above (1), wherein the porosity is 2% or less. (9) As described above (1) 8) The composite magnetic body according to the above, wherein the real part of the complex magnetic permeability in the frequency band of 7 〇ΜΗζ to 500 MHz is 7 or more, and the real part er' of the complex dielectric constant is 15 or more, and (1), 1/2 is 〇 以下 以下 以下 以下 以下 以下 以下 以下 以下 以下 以下 以下 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合 复合The loss tangent of the complex magnetic permeability in the frequency band of the frequency range of from MHz to 500 MHz is 〇〇5 or less, and the complex dielectric constant of the complex dielectric constant is less than or equal to the above. (1) The composite magnetic material according to the above (1), wherein the insulating material is - The first resin having a functional group in which the main chain has a structure and polymerized in the unit body. 323724 15 201230083 (12) The compound as described in the above (11) The above-mentioned resin is a thermosetting resin. The composite magnetic material according to the above (11), wherein the resin is an epoxy resin. (14) The composite magnetic body as described in the above (11) The composite magnetic material according to the above (11), wherein the orientation direction of the resin in the flat magnetic particle is the same as the flat plate The angle formed by the long-axis direction of the magnetic particles is 20 or less. (16) The composite magnetic body according to the above (11), wherein the real part #r' of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz is 7 or more. (17) The composite magnetic material according to the above (11), further comprising a second resin which imparts flexibility to the first resin. (18) The composite magnetic material according to the above (17), wherein the second resin is an epoxy resin having at least one of a bisphenol A type skeleton and a bisphenol F type skeleton. (19) The composite magnetic material according to the above (17), wherein the second resin is an epoxy resin having two or more epoxy groups in one molecule and having an ether skeleton. (20) The composite magnetic material according to the above (17), wherein the second resin is an epoxy resin having any one of a propylene glycol addition bisphenol A type skeleton and an ethylene glycol addition bisphenol A type skeleton. . (21) The composite magnetic body according to the above (17), wherein the real part /zr' of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz is 7 or more. A composite magnetic body according to any one of the above (1) to (21), which is provided with an average particle diameter of 〇. a slurry in which spherical magnetic particles of 5 am or less are dispersed in a solution containing a surfactant, and a dispersion medium are filled in a container which can be filled in a male or a closed container so that the total volume of the slurry and the dispersion medium is as described above. a second step in which the volume in H is the same, and the poly-liquid is mixed with the dispersion medium (10) in a sealed state, and the magnetic particles are deformed and dissolved to form a flat magnetic recording device; The magnetic f raw body is dispersed and mixed in the second step of the solvent towel (four) edge = molding material; and the molding step of obtaining the formed body by the above-mentioned formation: The third step of the drying/hardening step of drying/hardening of the shaped body. (3) The method for producing a composite magnetic material according to the above (22), wherein the insulating material is a resin having a cyclic structure and a functional group polymerized at a monomer position. (24) The method for producing a composite magnetic body according to the above (22), wherein: in the third (fourth) towel, in the step of forming the material, the magnetic field is applied to the body towel. The aforementioned planar core, the orientation step of the early orientation is followed by the aforementioned drying/hardening step. (25) An antenna comprising the composite magnetic body according to any one of the above (1) to (21). , to make. (10) A communication device comprising the antenna according to the above (25), wherein the antenna conductor is covered by the 323724 17 201230083 composite magnetic body as described in the above (1). (28) (27) The monopole antenna according to the above aspect, wherein the complex magnetic body has a real part y r' of a complex magnetic permeability in a frequency band of 160 MHz to 222 MHz of 3 or more. (29) A single sheet as described in the above (28) The monopole antenna according to the above (27), wherein the composite magnetic body has a frequency of 160 MHz to 222 MHz. The thickness of the composite magnetic body is 1. 2mm or more and l〇mm or less. The thickness of the composite magnetic body is 1. 2mm or more and l〇mm or less. (32) The monopole antenna according to the above (27), wherein the length of the antenna conductor is 200 mm or less. (Effect of the invention) The composite magnetic body according to the present invention has an average thickness of 〇. 01 Vm or more. 0. Hereinafter, the average long diameter is 〇. 〇5y m or more and 5ym or less' and the average aspect ratio (long pole/thickness) is a flat magnetic particle of 5 or more, so that the real part of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz can be greater than 1, and the loss of complex magnetic permeability tangent tan ( 5 " is 0.1 or less, so that the shortening rate of the wavelength in the frequency band can be greatly increased. Therefore, if the composite magnetic body is applied to the antenna of the VHF band, the generation of eddy current on the surface of the composite magnetic body can be prevented. In order to prevent the reduction of er', the antenna can be further miniaturized. Therefore, if the composite magnetic body is applied to an antenna of the VHF band or an electric component of the 203724 201230083, the antenna or the electronic component can be further miniaturized. In the composite magnetic material of the present invention, the porosity of the composite magnetic material having the flat magnetic particles is 20% or less, and the value of the real part #!' of the complex magnetic permeability is increased, but the complex magnetic material can be increased. The value of the real part ε r' of the dielectric constant is almost constant. Therefore, the difference between the value of the real part #r' of the complex magnetic permeability and the value of the real part ε r' of the complex permittivity can be reduced. Electron applying the composite magnetic body The device or the electronic device is miniaturized, and the power loss caused by the impedance matching is suppressed. The composite magnetic body according to the present invention contains the above-mentioned flat magnetic particles and the main chain has a cyclic structure and has a monomer unit Since the first resin of the polymerized functional group has a structure in which the resin is flat and is not easily entangled with the flat magnetic particles, the influence of the steric obstacle formed by the resin on the flat magnetic particles can be reduced. A composite magnetic body having a good orientation of the flat magnetic particles and a real part of the complex magnetic permeability #r' can be obtained. Further, since a resin having a functional group polymerized in a monomer unit is used, the bonding of the resin can be made strong, and sufficient mechanical strength can be used as a molded body such as an electronic component. The composite magnetic material according to the present invention contains the above-mentioned flat magnetic particles, a first resin having a cyclic structure in a main chain and having a functional group polymerized in a monomer unit, and flexibility imparted to the first resin. Since the second resin has a cyclic structure and a first resin having a functional group polymerized in a monomer unit, the effect of the steric hindrance formed by the resin on the flat magnetic particles can be reduced. . Therefore, the orientation of the flat-shaped 19 323724 201230083 magnetic particles can be improved, and the composite magnetic body of the real part of the complex magnetic permeability can be easily obtained. Further, since the second resin imparts flexibility to the second resin, the flexibility and stretchability of the composite magnetic body itself can be improved, and as a result, a composite magnetic body excellent in productivity can be obtained. According to the method for producing a composite magnetic material of the present invention, the slurry and the dispersion medium f obtained by dispersing the spherical magnetic particles of the average granules in the raw material are filled in the sealable 4, The total volume of the slurry and the dispersion medium is the same as the volume in the container, and the slurry is kneaded in the sealed medium in a sealed state, and the spherical magnetic particles are deformed and refined into a flat plate. The i-th step of the magnetic particles; the second step of dispersing and mixing the flat magnetic particles in a molten forming material in which an insulating material is dissolved and dissolved; and including the right: forming or coating on the base The forming step of forming the material on the material is described as the third step of the drying/hardening step of the forming and drying of the formed body. The frequency wave of 70 MHz to 5 GG MHz is easily produced. ;r, large, and complex magnetic permeability loss tangent tand < complex magnetic permeability of the composite magnetic body. 々为〇·1 or less, when using a resin with a main chain (4) I and (a) polymerized functional group as an insulating material, the early orientation of the plate can be used.) The orientation of the plate-like magnetic particles is good, and the complex magnetic field is easy. A composite magnetic body was produced. The tamping lamp is 'high.' In the third step, a magnetic field is applied to the molded body obtained after the forming step 20 323724 201230083 to orient the flat magnetic particles in the formed body in one direction. In the orientation step, when the drying/hardening step is carried out, a composite magnetic body in which the orientation of the flat magnetic particles is better and the real part #r' of the complex magnetic permeability is higher can be easily produced. According to the antenna of the present invention, since the composite magnetic body is provided, the antenna conductor can be shortened to a longer wavelength by using a composite magnetic body having a real part #r' of a complex magnetic permeability in a frequency band of 70 MHz to 500 MHz. The 1/4 is shorter, and the entire antenna is miniaturized. Therefore, an antenna for further miniaturization can be provided. Further, when a composite magnetic body having a porosity of 20% or less is provided, the emission efficiency can be improved. Therefore, it is possible to provide an antenna which is small and suppresses power loss due to impedance matching, is miniaturized and has high transmission efficiency, and can be used in a wide band of 70 MHz to 500 MHz. In addition, when the composite magnetic material including the first resin having a cyclic structure in the main chain and having a functional group polymerized in a monomer unit as the insulating material is provided, the first resin and the first resin may be contained. When the flexible second resin is used as the composite magnetic material of the insulating material, a higher #r' can be obtained, so that an antenna which is further miniaturized can be provided. According to the communication device of the present invention, since the antenna is provided, it is possible to achieve miniaturization of the entire communication device by using the miniaturized antenna. Therefore, it is possible to provide a communication device that further achieves miniaturization. In addition, when an antenna having a composite magnetic body having a porosity of 20% or less is mounted, an antenna that is small in size and high in emission efficiency and can be used in a wide band 21 323724 201230083 can be used to realize the entire communication device. Miniaturization and improved communication performance. Therefore, it is possible to provide a communication device which is further miniaturized and can be used in a wide band of 70 MHz to 500 MHz. According to the monopole antenna of the present invention, since the composite magnetic body is coated on the antenna conductor, the antenna conductor can be shortened to be shorter than 1/4 of the wavelength, and can be received, transmitted, or received at a low frequency of 160 MHz to 222 MHz. A radio wave in the frequency band and can be mounted on a small monopole antenna of a portable terminal. [Embodiment] Hereinafter, a composite magnetic body, a method for producing the same, an antenna, and a communication device for carrying out the present invention will be described. It is to be understood that the present invention is not limited thereto, and the present invention is not limited thereto. [First composite magnetic material] The composite magnetic material of the present embodiment is a composite magnetic body in which flat magnetic particles are dispersed in an insulating material, and the average thickness of the flat magnetic particles is Ο.ΟΙ/ A composite magnetic body having an average aspect ratio of 0.5/zm or less and an average aspect ratio of 0.05/zm or more and 10/zm or less and an average aspect ratio (longitudinal diameter/thickness) of 5 or more. The average thickness and the average major axis can be measured by measuring the respective thicknesses and long diameters (maximum lengths in the particles) of the plurality of flat magnetic particles, for example, 100 or more, preferably 500 or more flat magnetic particles. Each thickness and long diameter are calculated, and the average values of the thickness and the long diameter are calculated. Further, the average aspect ratio of the flat magnetic particles (long diameter/thickness 22 323724 201230083 fm is the same), and the == r of the plurality of plate-shaped impurity particles can be, for example, _ or more, preferably _ The respective flatness and thickness of the above-mentioned magnetic body were determined by taking the average value of each of the flatness/county ratio (long diameter/thickness) and calculating the average of these aspect ratios (length/thickness). The average thickness of the tabular magnetic particles is 〇〇1 (four) or more 〇5: two, preferably 0.012 _ 〇 心 3 hearts

為 0. 05 # m 以上 1 〇 &quot; m IV 丁 ., ^ J 下。 1〇_以下,較佳為〇.5&quot;以上5_以 造,=理1=厚度未達時’如後述般難以製 w且處雜㈣得困難,故不佳, 過〇.5,時,會產生起因於粒子彼此的熔著二= :圭使丽波段之複磁導率的損耗正 為5 該平板狀磁性體粒子的平均長寬 以上’尤佳為7以上。 比(長徑/厚度)較佳 降低,故不佳 在此,虽平均長寬比(長徑/厚度)小於5時,平板狀 :_二_係數增大,結果使複合二= 將該平板狀磁性體 由如下所述。 粒子的形狀限定在上述 範圍之理 係與磁性粒子的形狀相 由於去磁場等向地存在, 以在T%頻區域中得到優異 磁性粒子之去磁場的大+ 依。例如當磁性粒子為球狀時, 故所得到之磁導率亦呈等向,難 323724 23 201230083 =平=,當磁性粒子的形狀為上述範圍時, :千板=仃之方向上的去磁場可大幅降低,因此使所得 之/z r增大。 因此,藉由使用上述平板狀磁性體 至500MHz的頻率波段之複磁導率了㈣ λα μ τ ㈣等手的實部β r,大於1,且複 Ο為°,1以下之複合磁性體。 複磁導率的實部W較佳為5以上,尤㈣Μ以上。 二,,磁導率的實部訂,及複磁導率的損耗正切 tanO限疋在上述範圍之理由,在於該範圍是可縮短電磁 波的波長’且可降低渦電流所造叙則員耗,使能量損耗 縮小之範圍之故。 該複合磁性體中,尤佳者是9_422〇的頻率 波段之複磁導率的實部訂,大於i,且損耗正切_ 〇為 0. 05以下。 能量損耗的大小,可藉由下列式(3)所示之複磁導率 的虛部// r&quot;(以下有時略稱為以r&quot;)來表示。 ^r&quot; = ^r, xtand //---(3) 在此,由於複磁導率的虛部以1·&quot;較佳為〇. 5以下,所 以從上述式(3)中,得知當心,冑10時,較佳為 0.05以下,此外,當^^’為15時,tan&lt;5以較佳為1/3〇 以下。 該平板狀磁性體粒子的組成,較佳是在Permall〇y (商 品名稱)等Fe-Ni合金、Supermalloy(商品名稱)等Fe_Ni-M〇 合金、Sendust(商品名稱)等Fe-Si-Al合金、Fe_Si合金、 323724 24 2012300830. 05 # m above 1 〇 &quot; m IV 丁 ., ^ J 下下. 1〇_以下, preferably 〇.5&quot;The above 5_ is made, =1 is 1=the thickness is not reached'. As described later, it is difficult to make w and the miscellaneous (4) is difficult, so it is not good, too much. It is caused by the fusion of the particles with each other. =: The loss of the complex magnetic permeability of the Kelly band is 5, and the average length and width of the flat magnetic particles are more than 7 or more. The ratio (long diameter/thickness) is preferably lowered, so it is not preferable here, although the average aspect ratio (long diameter/thickness) is less than 5, the flat shape: the _ two-factor is increased, and as a result, the composite two = the flat plate The magnetic body is as follows. The shape of the particles is limited to the above range and the shape of the magnetic particles is present in the direction of the demagnetizing field, so that the demagnetizing field of the excellent magnetic particles is obtained in the T% frequency region. For example, when the magnetic particles are spherical, the magnetic permeability obtained is also isotropic, and it is difficult to 323724 23 201230083 = flat =, when the shape of the magnetic particles is in the above range, the demagnetizing field in the direction of the thousand plates = 仃It can be greatly reduced, thus increasing the resulting /zr. Therefore, by using the above-mentioned flat magnetic body to the complex magnetic frequency in the frequency band of 500 MHz, the real part β r of the hand such as (4) λα μ τ (4) is larger than 1, and the complex magnetic material of °, 1 or less is formed. The real part W of the complex magnetic permeability is preferably 5 or more, and particularly (four) Μ or more. Second, the real part of the magnetic permeability, and the loss of the complex permeability tangent tanO is limited to the above range, because the range is that the wavelength of the electromagnetic wave can be shortened and the eddy current can be reduced. The reason for reducing the energy loss. In the composite magnetic body, it is particularly preferable that the real magnetic permeability of the frequency band of 9_422 波段 is greater than i, and the loss tangent _ 〇 is 0.05 or less. The magnitude of the energy loss can be expressed by the imaginary part of the complex magnetic permeability represented by the following formula (3) / / r &quot; (hereinafter sometimes abbreviated as r&quot;). ^r&quot; = ^r, xtand //---(3) Here, since the imaginary part of the complex magnetic permeability is 1·&quot; preferably 〇. 5 or less, from the above formula (3), It is understood that when 胄10, it is preferably 0.05 or less, and when ^^' is 15, tan<5> is preferably 1/3 〇 or less. The composition of the flat magnetic particles is preferably Fe-Ni alloy such as Permall〇y (trade name), Fe_Ni-M〇 alloy such as Supermalloy (trade name), or Fe-Si-Al alloy such as Sendust (trade name). , Fe_Si alloy, 323724 24 201230083

Fe-Co 合金、Fe-Cr 、I? r 〇.人 a r 口金、Fe-Cr-Si合金等高磁導 中,^加有細)、鉻(Cr)、猛⑽、靴。)、鋼二金 =)、銳⑽)、_。)、銦(In)、錫⑽等金屬元素之 該平板狀磁性體粒子之上述金屬元素的添 為(M請以上90質量%以下,尤佳為 = 質量%以下’更佳為1質量%以上5質量%以下。 12 在此,將上述金屬元素的添加量限定在上述範圍之理 由,在於當金屬元素的添加量未達Q1質量%時,I法 分的塑性變職力料至磁鋒子,另—方面, :過^量%時,由於金屬元素本身的磁矩小,:二: 之 子全體的飽和魏強度降低,結果使所得之訂,亦變小 故0 尤其就得到高,之觀點來看,較佳為含有i f4% 以上5質量%以下之選自紹⑼、絡(Cr)、M(Mn)、_〇)、° 銅(Cu)、鋅(Zn)、銳⑽、翻(Mo)、銦(In)、錫⑽的群 組之1種或2種以上的金屬元素之鐵—鎳合金。 絕緣材料’只要是絕緣性的材料即;,並無特別限 制’當將本實施形態之複合磁性體使用作為行㈣話用天 線或攜帶式資訊終端用天線時,較佳糸 ⑨領触度高,吸濕 性低,且形狀加工性佳。此般絕緣材料,/ t |何料,例如可適當地使 用聚醯亞胺樹脂、聚苯並卩等唑樹脂、聚妯〜^ 灰伸本樹脂、聚苯並 環丁烯樹脂、聚伸芳基醚樹脂、&amp; ^ ^ . s &quot; 聚矽氧烷樹脂 (polysiloxane resin)、環氧樹脂、聚龄 歇1曰樹脂、氟樹脂、 323724 25 201230083 聚烯烴樹脂、聚環烯烴樹脂、氰酸酯樹脂、聚伸苯基鱗樹 脂、降莰烯樹脂、ABS樹脂、聚苯乙烯樹脂等熱硬化性樹 脂或熱可塑性樹腊。此等樹脂可僅單獨使用1種或組合2 種以上而使用。 當117,熱硬化性樹脂較佳為機械強度及形狀加工性佳 之環氧樹脂,此外,熱可塑性樹脂較佳為聚伸苯樹脂、八跎 樹脂。 [第1複合磁性體的製造方法] 本實施形態之複合磁性體的製造方法,係具備有··將 使平均粒經0.5㈣以下的球狀磁性粒子分散於含有界面 =性劑之㈣巾而成之㈣及分散介f,填充於可密閉的 容,内’以使前述聚液及前述分散介質的合計體積量與前 述容器内的體積成為相同,在密閉狀態下將該毁液與前述 分散介質—_拌,使前述球狀雜粒子彼此變形及炫著 板狀磁性體粒子之第1步驟;使前述平板狀磁性 立分散並混合於在溶劑中溶解有絕緣材料之溶液中而 之第2步驟;以及包含有:將前述成形材料 形體:焯/於基材上而得成形體之成形步驟、及使前述成 乾無/硬化之乾燥/硬化㈣之第3步驟。 以下係詳細說明各步驟。 &lt;第1步驟&gt; 於含均粒徑町的球狀雜粒子分散 、1面,舌性劑之溶液+而構成漿液。 磁性粒子的經成,係與上述平板狀磁性體粒子的組成 323724 26 201230083 * 完全相同。 界面活性劑,較佳是含有與磁性粒子表面的配合性佳 之氮、鱗、硫等元素之界面活性劑,例如可列舉出含氮的 嵌·段共聚物、碳酸鹽、聚乙締*»比u各u定酮等。 、 溶解該界面活性劑之溶劑,由於需防止磁性粒子中所 含有之金屬元素的氧化’故較佳為有機溶劑,特佳為二甲 苯(xylene)、曱苯(toluene)、環戊酮、環己酮等非極性有 機溶劑。 接著將該漿液及分散介質填充於可密閉的容器内,以 使該漿液及分散介質的合計體積與容器内的體積成為相 同’並在密閉狀態下將該漿液與分散介質一同攪拌,使球 狀磁性粒子彼此變形及熔著而形成平板狀磁性體粒子。 分散介質,其硬度必須較球狀磁性粒子更高,例如可 列舉出鋁、鋼(stell)、不鏽鋼、鉛等之金屬球,由氧化鋁、 二氧化鍅、二氧化矽、二氧化鈦等金屬氧化物或無機氧化 物所構成之球狀燒結體,由氮化矽等無機氮化物所構成之 球狀燒結體’由碳化矽等無機碳化物所構成之球狀燒結體, 以及由鈉玻璃、鉛玻璃、高比重玻璃等所構成之稱為珠粒 (bead)的球狀粒子,當中,就效率來看,較佳為比重6以 上的,&quot;&quot;&quot;'氧化錯、鋼、不錄鋼等。 機械應力對球狀磁性粒子的施加,是藉由分散介質碰 撞時的衝擊來進行,隨著分散介質碰撞次數的增加,而提 升球狀磁性粒子彼此的變形及熔著性。 如此,分散介質的平均粒徑愈小,每單位體積所存在 323724 27 201230083 之個數增加,碰撞次數亦增多,而提升變形及炼著性,但 另一方面,當分散介質的平均粒徑過小時,難以從漿液中 分離該分散介質。因此,分散介質的平均粒徑至少須為 0. 03mm以上,較佳需為0. 04mm以上。 此外,當分散介質的平均粒徑過大時,碰撞次數減 少,使球狀磁性粒子彼此的變形及熔著性降低。因此,分 散介質的平均粒徑之上限值為3. 0mm。 可密閉的容器,較佳為可藉由使圓盤(disk)、螺桿、 葉片等之單軸旋轉體高速旋轉而使漿液與分散介質一同高 速旋轉之密閉容器。 由於該密閉容器為單純的單軸旋轉方式,故亦容易達 成大型化,工業生產上亦較有利。 並且,亦可在上述可密閉的容器上設置用以將漿液導 入/導出於容器内之流入口及流出口,並在密閉容器内使漿 液循環。此時,可預先將分散介質容納於密閉容器内,從 流入口投入混合有球狀磁性粒子與界面活性劑與溶劑之漿 液,並填充於容器内以至不存在空間,然後將從流出口所 排出之漿液再次投入於密閉容器内。 在此,漿液及分散介質對上述密閉容器内的填充量, 係設為與密閉容器内的體積相同。換言之,以不存在間隙 之方式將漿液及分散介質填充於密閉容器内。 在此,以不存在間隙之方式將漿液及分散介質填充於 密閉容器内之理由如下所述。 第1圖係顯示藉由單軸旋轉體155,使投入於上部呈 28 323724 201230083 開放的開放容器151之含有球狀磁性粒子152之漿液ι53 以及分散介質154高速旋轉而進行高速攪拌之樣態之圖。 該圖中,當單軸旋轉體155高速旋轉時,漿液153及 分散介質154的液面,由於離心力而成為在中心轴附近較 低且周緣部較高之研钵狀。 藉由單軸旋轉體155而對含有球狀磁性粒子152之聚 液153以及分散介質154所施加之機械應力,會逃往研蛛 狀的空間,使在開放容器151内全體經由分散介質154被 傳送至球狀磁性粒子152之機械應力變得不均勻,而導致 所得之平板狀磁性體粒子的厚度無規律。 此外’在研蛛狀空間的底部附近(中心軸附近)成為平 板狀磁性體粒子之磁性體粒子,係與分散介質一同被釋出 至研缽狀空間而承受不規則的衝擊’而有產生破裂或缺損 等之疑慮。此般磁性體粒子的厚度無規律或破裂或缺損 等,係成為在VHF波段之複磁導率的損耗正切“增 加之因素。 第2圖係顯示藉由單軸旋轉體155,使投入於密閉容 器1511之含有球狀磁性粒子152之漿液153以及分散介 154高速旋轉而進行高速攪拌之樣態之圖。 該圖中,即使單軸旋轉體155高速旋轉,由於密閉容 器1511内被含有球狀磁性粒子152之聚液153以及分散介 質154所填滿,所以並無產生如在開放容器151中所看到 之研钵狀空間之疑慮。因此,藉由單轴旋轉體155而對含 有球狀磁性好152之漿液153以及分散介質154所施加 323724 29 201230083 之機械應力’在密閉容器1511内全體經由分散介質154 被均勻地傳送至球狀磁性粒子152,而不會有所得之平板 狀磁性體粒子的厚度無規律之疑慮。此外,成為平板狀之 磁性體粒子,亦不會承受不規則的衝擊,而不會有產生破 裂或缺損等之疑慮。 單軸旋轉體155的轉數,是由密閉容器1511的大小 來決定。例如為内徑120mm的密閉容器1511時,含有球狀 磁性粒子152之漿液153以及分散介質154於密閉容器 1511内壁附近的流速,較佳為5m/秒以上,尤佳為8〇1/秒 以上。 並且,當密閉容器1511的内容積較小時,會有球狀 磁性粒子152殘留於所得之平板狀磁性體粒子之疑慮。殘 留之球狀磁性粒子152,因球狀磁性粒子152彼此的接觸 或者球狀磁性粒子152與平板狀磁性體粒子之接觸,而有 磁損耗增加或阻礙平板狀磁性體粒子的定向之疑慮。因 此,平板狀磁性體粒子,較佳為磁性粒子全體量的9〇質量 %以上,尤佳為95質量%以上,更佳為99質量%以上,較佳 係實質上不含球狀磁性粒子152。 在此’當密閉容器1511的内容積較小時會使球狀磁 性粒子152殘留之理由,認為係因密閉容器i5u的角落或 旋轉體5與密閉容器i5U的接合部般之機械應力未充分地 傳達的閒置空間(dead space)相對較大之故。因此,當增 大密閉容器1511的内容積時,可相對縮小閒置空間,故機 械應力充分地傳達至球狀粒子2,提升球狀磁性粒子彼此 30 323724 201230083 的變形及熔著性,結果使球狀磁性粒子152的殘留減少, 球狀磁性粒子152實質上不存在。 如此,使球狀磁性粒子152實質上未殘留之密閉容器 1511的體積’較佳為il以上,尤佳為5l以上。 以上,球狀磁性粒子彼此,係藉由單軸旋轉體155所 施加之機械應力產生變形及熔著,而成為平板狀磁性體粒 子0 接著從分散介質及溶劑中分離該平板狀磁性體粒子。 再者,可考量到製作平板狀磁性體粒子時所使用之溶 劑與之後所混合之絕緣性材料的相溶性,來實施適當的聚 液乾燥步驟。 具體而言,當製作平板狀磁性體粒子時所使用之溶劑 與絕緣性材料的相溶性差時,較佳係進行乾燥處理以使上 述溶劑成為4質量%以下,較佳為2質量%以下’尤佳為i 質量%以下。另一方面,當製作平板狀磁性體粒子時所使用 之溶劑與絕緣性材料的相溶性良好時,亦可不進行漿液乾 燥步驟,而在使平板狀磁性體粒子分散於溶劑中之漿液狀 態下直接移往第2步驟。 乾燥方法,只要在製作平板狀磁性體粒子後的漿液中 去除溶劑者即可,並無特別限定,可列舉出加熱乾燥、真 空乾燥、冷束乾燥等,就乾燥效率之觀點來看,較佳為真 空乾燥。此外,為了提高乾燥效率,乾燥步驟前,可藉由 固液分離等手法來去除某種程度的溶劑。固液分離的方 法,可使用壓濾(filter press)或吸引過濾等過濾操作, 323724 31 201230083 或是依據傾析機(decanter)或離心分離機所進行之離心分 離操作等之一般方法。 &lt;第2步驟&gt; 使上述平板狀磁性體粒子分散並混合於在溶劑中溶 解有絕緣材料之溶液中而形成成形材料。 在此,絕緣材料可使用與上述所說明之絕緣材料完全 相同者,故省略說明。 此外,溶劑只要是可溶解上述絕緣材料者即可,並無 特別限定,例如可適當地使用曱醇、乙醇、2-丙醇、丁醇、 辛醇等醇類,乙酸乙酯、乙酸丁酯、乳酸乙酯、丙二醇單 甲醚乙酸酯、丙二醇單乙醚乙酸酯、7-丁内酯等酯類,二 乙趟、乙二醇單曱_1(曱基賽路蘇(11161:1^1〇611〇3〇1乂6))、 乙二醇單乙醚(乙基賽路蘇)、乙二醇單丁醚(丁基赛路蘇)、 二乙二醇單甲醚、二乙二醇單乙醚等醚類,丙酮、丁酮、 甲基異丁基酮、乙醯丙酮、環己酮等酮類,苯、甲苯、二 曱苯、乙基苯等芳香族烴,二曱基曱醯胺、N,N-二曱基乙 醯基乙醯胺、N-曱基吡咯啶酮等醯胺類,此等溶劑可單獨 使用1種或混合2種以上而使用。 分散混合方法並無特別限制,較佳係使用行星研磨 機、砂磨機(sandmill)、球磨機等攪拌裝置。混合條件, 可在不使平板狀磁性體粒子彼此凝聚下適當地調整來實 施。 &lt;第3步驟&gt; 將上述成形材料成形或塗佈於基材上而製作成形體, 32 323724 201230083 接者使所得&lt;成_乾燥及硬化。 成形方法,較適合有一般所知的成形方法,例如模壓 成开 刮刀塗佈法、射出成形法等。藉由使用該 薄膜。/形為任意形狀的薄片狀或薄膜狀,可製作出乾 形為層體時,較佳是藉由刮刀塗佈法成 Α狀或薄膜狀。 濃縮材料,當須進行黏度調整時,使溶劑揮發並 在乾燥前進= 有必要,可在將成形材料塗佈於基材上後, 片或薄膜平,由磁場的定向使平板狀磁性體粒子往與薄 什之方向定向之定向處理。 理或在還f性氣體中或真空中進行熱處 曰此可彳于到本實施形態之複合磁性體。 可塑可將平板狀磁性體粒子與熱硬化性樹脂或熱 曰進行加熱捏揉而混合分散並予以成开^,如此 亦可得到本實_態之複合雜體。 t如此 加熱捏揉(kneading)方法,亦可藉由一般所知的方 法,例如加壓捏揉機、雙軸式捏揉機、喷磨機(blast mill) 等進行混合分散而製得捏揉物。該捏揉物的成形方法,可 藉由一般所知的方法,例如加熱模壓成形、擠壓成形、射 出成形等來製作出成形體。此等方法中,為了使平板狀磁 性體粒子在樹脂中定向’較佳是拉伸為平面狀之加熱模壓 成形。為了進行拉伸時的黏度調整,較佳係添加塑化劑或 是進行平板狀磁性體粒子的表面處理。若有必要,較佳在 323724 33 201230083 加熱而維持流動性之狀態下,進行藉由磁場的定向使平板 狀磁性體粒子定向之定向處理。 [第2複合磁性體] 本實施形態之複合磁性體,係將上述平板狀磁性體粒 子分散於絕緣材料中而成之複合磁性體,該複合磁性體的 氣孔率為20%以下。 在此,複合磁性體的氣孔率,可藉由下列式(4)來求 取。 氣孔率= (1-實測密度/理論密度)χ100· · .(4) 該複合磁性體的理論密度,是根據平板狀磁性體粒子 的理論密度與絕緣材料的理論密度(与實測密度),考量到 平板狀磁性體粒子與絕緣材料之混合比率來算出。 此外,算出平板狀磁性體粒子的理論密度之方法,係 有從平板狀磁性體粒子的X射線繞射圖形中算出晶格常 數,並根據該晶格常數與結晶結構來算出理論密度值之方 法。 另一方面,算出絕緣材料的實測密度之方法,例如當 絕緣材料為樹脂時,係有僅使樹脂硬化並測定外形尺寸及 質量,並從此等測定值來算出實測密度之方法。 此外,算出複合磁性體的實測密度之方法,例如有測 定外形尺寸及質量,並從此等測定值來算出實測密度之方 法,或是使用比重儀法所測定之值之方法。 該複合磁性體,較佳是70MHz至500MHz的頻率波段 之複磁導率的實部#r’為7以上,複介電常數的實部er’ 34 323724 201230083 為15以上,且(以r,· ε r,)-&quot;2為〇. i以下,(# γ £〆)1/2 為0. 5以上1以下。 該複合磁性體中,藉由將複磁導率的實部,及複介 電常數的實部er,設定在上述範圍,可使具備本實施形態 之複合磁性體之電子零件或電子設備達成小型化,並可抑 制阻抗匹配所造成之電力損耗。 以下,係以將該複合磁性體安裝於天線者為例,詳細 地說明在該複合磁性體中將上述之複磁導率的實部#r,、 複介電常數的實部ε r’、( y r,· ε r,)-1/2及(以r,/石『,)1/2 之值設定在上述範圍為佳之理由。 再者,同樣的效果,於上述天線以外之使用高頻之所 有電子零件中均可得到。 首先,較佳為70MHz至500MHz的頻率波段之複磁導 率的實// r為7以上’尤佳為9以上。在此,將# r,設 為7以上之理由,在於複介電常數的實部,通常顯示出 15以上的較大值,當π未達7時,訂,與“,相比成為 極知丨的值,導致因特性阻抗的不一致所造成之電力損耗 增大之故。 該vr’的上限值並無特別限制,就實際上所能夠製造 之平板狀磁性體粒子的長寬比或含有率等來看,較佳為 以下,尤佳為15以下。 複介電常數的實部,較佳為15以上,尤佳為2〇以 上。在此,將ε r’設為15以上之理由,在於依循上述式 而成為達成天線的小型化之有效值之故。 323724 35 201230083 該複合磁性體中,將/zr’及ε r’之值設定在上述範圍 時,(/zr’ . ε r’)—1/2更佳為0. 1以下。其理由如下所述。 該(# r’ . ε r’)_1/2之值,如式(1)所示,為複合磁性 體中之高頻率波長相對於真空令的波長之縮短率。再者, 真空中的波長與一般大氣中的波長,係顯示出幾乎相等之 值。 一般而言,天線通常是由以波長的1/2或1/4長度之 導線等所形成之天線導體所構成。在頻率低之長波長區 域,尤其在70MHz至500MHz的頻率波段中,波長為60cm 以上,當天線導體的長度為30cm以上或15cm以上時,天 線本身會變大。因此,使用匹配電路將長波長信號與電子 電路匹配以進行接收傳送,但當縮短天線長度時,由於天 線導體上的電流量降低,使天線所能夠接收傳送之頻率波 段變窄,或產生天線的發射效率降低等問題。尤其在將天 線長度設為波長的1/10以下時,難以進行電波的接收傳 送,實用上產生問題。 因此,若將(μι·’ . ε r’ V&quot;2為0. 1以下之複合磁性體 安裝於天線,在複合磁性體上,高頻波長理論上幾乎縮短 至1/10以下。因此,並不會產生如使用匹配電路時之天線 所能夠接收傳送之頻率波段變窄或是天線的發射效率降 低,而能夠達成天線大小的小型化。 上述(/zr’/ er’)1/2較佳為0.5以上1以下。其理由如 下所述。 該(/^1'’/£1*’)1/2之值,如上述式(2)所示,為複合磁 36 323724 201230083 性體的特性阻抗^與真空的特性阻抗Zfl之比(Zg/ Zq),故 複合磁性體的特性阻抗Zs為真空的特性阻抗匕之 er,)1/2 倍。 通常,複合磁性體的//!*,較£1·,更小,所以複合磁性 體的特性阻抗Zg較大氣的特性阻抗Ζα (与真空的特性阻抗 Ζ〇)之值更小。並且,高頻信號,為人所知者在從特性阻= 較大的區域往較小的區域傳播時,會產生反射或吸收而衰 減。 因此,當複合磁性體的特性阻抗Zg較大氣的特性阻抗 Za小50%以上時,高頻率的衰減率極大,實用上會產生問 題。因此,當將(//1^’/£]:’)^之值設為〇.5以上時,當電 磁波從大氣傳播至複合磁性體時,可將特性阻抗的變化抑 制在50%以内。因此可抑制高頻信號的衰減。此外,當複 合磁性體的特性阻抗Zg較大氣的特性阻抗Za更大時,即使 此等特性阻抗差極小,電磁波亦會大幅衰減。因此,(“尸/ e r’)1/2之值較佳為1以下。 該複合磁性體之複磁導率的損耗正切較佳為 05以下尤佳為〇 〇4以下。此外,該複合磁性體之 介電常數的損耗正切tanA , ^ 刀tan&lt;5 e (以下有時略稱為tan(5 ε ) 車乂佳為Ο.1以下,尤佳為0.07以下。 如此w tan5 //及tan5 £之值分別超過較佳值時, ^磁性體内,僅高頻率之對應於複磁導率的虛數部#, =讀電常數的虛數部er„之部分被吸收而轉換為熱除 使向頻信號的能量衰減之外,亦有產生s/n比降低或放 323724 37 201230083 熱等問題之疑慮,故不值。 目前,在70MHz至500MHz的頻率波段中,由於電磁 波的波長較長而難以達成天線的小型化,因而在行動電話、 攜帶式資訊終端、多功能型攜帶式資訊設備等特別要求小 型化之用途中,必須將鞭形天線拉長至框體的數倍長度來 使用,或是不得不使用耳機線來作為天線。 另一方面,本實施形態之複合磁性體中,若70MHz至 500MHz的頻率波段之複磁導率的實部yr,等諸項特性滿 足上述範圍,則在70MHz至500MHz,較佳為在9〇MHz至 220MHz的頻率波段中所使用之電子零件或電子設備,例如 行動電話、攜帶式資訊終端、多功能型攜帶式資訊設備等 通信裝置的天線中,亦可同時達成小型化與電力損耗的降 低。 再者,在500MHZ為止的頻率波段中,與超過5〇〇MHz 之頻率波段相比,tan (5 //及tan (5 ε較低,所以天線的增 益提高,故較佳。 本實施形態之複合磁性體中,藉由將上述平板狀磁性 體粒子分散於絕緣材料中而使所得之複合磁性體的氣孔率 成為20%以下,雖然提高複合磁性體的以r,,但£ r,幾乎 不變。藉此,可使應用該複合磁性體之電子零件或電子設 備’例如行動電話、攜帶式資訊終端、多功能型攜帶式資 訊設備等通信裝置的天線達成小型化,並可抑制阻抗匹配 所造成之電力損耗。 得到此般效果之機制可考量如下。 323724 38 201230083 當複合磁性體中的氣孔 位體積的磁性體粒子量變小a f體之母早 灰 夕,使以r’變小。另一方面,由 之;面上呈Γ靜::緣材料相同’在與平板狀磁性體粒子 有静電電容’故即使氣孔率增大,…亦 此外,當複合磁性體中 ^ ^ 的氧孔率減少時,複合磁性體 之母早位體積的磁性體粒子 置變多’使# r’變大。另一方 面,如上述般,ε r,之佶继Fe-Co alloy, Fe-Cr, I?r 〇. Human a r gold, Fe-Cr-Si alloy and other high magnetic permeability, ^ added fine), chromium (Cr), fierce (10), boots. ), steel two gold =), sharp (10)), _. The addition of the metal element of the flat magnetic particle of the metal element such as indium (In) or tin (10) is (M: 90% or more, more preferably = % by mass or less), more preferably 1% by mass or more The reason why the amount of the metal element added is limited to the above range is that when the amount of the metal element added is less than Q1% by mass, the plasticity of the I method is changed to the magnetic front. On the other hand, when the amount of % is too large, the magnetic moment of the metal element itself is small, and the second one: the saturation strength of the whole part of the child is lowered, and as a result, the obtained order is also small, so that 0 is particularly high. It is preferable that the content of i f4% or more and 5% by mass or less is selected from the group consisting of Shao (9), complex (Cr), M (Mn), _〇, ° copper (Cu), zinc (Zn), sharp (10), and An iron-nickel alloy of one or two or more metal elements of Mo), indium (In), and tin (10). The insulating material 'is not particularly limited as long as it is an insulating material. 'When the composite magnetic body of the present embodiment is used as a row (four) speech antenna or a portable information terminal antenna, it is preferable that the 糸9 has a high degree of touch. It has low hygroscopicity and good shape processability. Such an insulating material, for example, may be suitably used, such as a polyimide resin, an azole resin such as polybenzopyrene, a polyfluorene~^ ash resin, a polybenzocyclobutene resin, and a poly-strand. Ether Resin, & ^ ^ . s &quot; Polysiloxane Resin, Epoxy Resin, Polyester Resin, Fluoro Resin, 323724 25 201230083 Polyolefin Resin, Polycycloolefin Resin, Cyanic Acid A thermosetting resin such as an ester resin, a polyphenylene resin, a norbornene resin, an ABS resin, or a polystyrene resin, or a thermoplastic wax. These resins may be used alone or in combination of two or more. In the case of 117, the thermosetting resin is preferably an epoxy resin excellent in mechanical strength and shape processability, and the thermoplastic resin is preferably a polyphenylene resin or an octagonal resin. [Manufacturing method of the first composite magnetic material] The method for producing a composite magnetic material according to the present embodiment includes dispersing spherical magnetic particles having an average particle size of 0.5 (four) or less in a (four) towel containing an interface=agent. And (4) and the dispersion medium f are filled in the sealable medium, so that the total volume of the liquid and the dispersion medium is the same as the volume in the container, and the decomposed liquid is dispersed in the sealed state a first step of deforming the spherical heteroparticles and squeezing the slab-shaped magnetic particles with each other, and dispersing the spheroidal magnetic particles in a solution in which a solution of the insulating material is dissolved in a solvent And the third step of forming the shaped body: the forming step of the molded body on the substrate, and the drying/hardening (4) of drying/hardening. The following is a detailed description of each step. &lt;First Step&gt; A slurry is formed by dispersing spherical heteroparticles containing a uniform particle size, and a solution of a lingual agent on one side. The formation of the magnetic particles is identical to the composition of the above-mentioned flat magnetic particles 323724 26 201230083 *. The surfactant is preferably a surfactant containing an element such as nitrogen, scale, or sulfur which is excellent in compatibility with the surface of the magnetic particle, and examples thereof include a nitrogen-containing in-segment copolymer, a carbonate, and a polyethylene-based ratio. u each ketone and the like. The solvent for dissolving the surfactant is preferably an organic solvent because it is required to prevent oxidation of a metal element contained in the magnetic particles, and particularly preferably xylene, toluene, cyclopentanone, or ring. A non-polar organic solvent such as ketone. Then, the slurry and the dispersion medium are filled in a closable container so that the total volume of the slurry and the dispersion medium is the same as the volume in the container, and the slurry is stirred together with the dispersion medium in a sealed state to form a spherical shape. The magnetic particles are deformed and fused together to form flat magnetic particles. The dispersion medium must have a higher hardness than the spherical magnetic particles, and examples thereof include metal spheres such as aluminum, stell, stainless steel, and lead, and metal oxides such as alumina, ceria, cerium oxide, and titanium oxide. Or a spherical sintered body made of an inorganic oxide, a spherical sintered body made of an inorganic nitride such as tantalum nitride, a spherical sintered body made of inorganic carbide such as tantalum carbide, and a soda glass or lead glass. A spherical particle called a bead, which is composed of a high-specific gravity glass. Among them, in terms of efficiency, it is preferably a specific gravity of 6 or more, &quot;&quot;&quot; 'oxidation error, steel, non-recorded steel Wait. The application of the mechanical stress to the spherical magnetic particles is carried out by the impact when the dispersion medium collides, and as the number of collisions of the dispersion medium increases, the deformation and the fusion property of the spherical magnetic particles are improved. Thus, the smaller the average particle size of the dispersion medium, the more the number of 323724 27 201230083 per unit volume increases, the number of collisions increases, and the deformation and refining properties are improved, but on the other hand, when the average particle size of the dispersion medium is excessive In hours, it is difficult to separate the dispersion medium from the slurry. 01毫米以上。 The average particle size of the dispersion medium must be at least 0. 03mm or more, preferably 0. 04mm or more. Further, when the average particle diameter of the dispersion medium is too large, the number of collisions is reduced, and the deformation and the meltability of the spherical magnetic particles are lowered. 0毫米。 The upper limit of the average particle size of the dispersion medium is 3. 0mm. The hermetically sealable container is preferably a hermetic container which can rotate the slurry and the dispersion medium at a high speed by rotating a uniaxial rotating body such as a disk, a screw or a blade at a high speed. Since the sealed container is a simple uniaxial rotation method, it is easy to be enlarged, and it is advantageous in industrial production. Further, an inlet and an outlet for introducing and discharging the slurry into the container may be provided in the sealable container, and the slurry may be circulated in the sealed container. In this case, the dispersion medium may be contained in a sealed container in advance, and a slurry in which spherical magnetic particles, a surfactant, and a solvent are mixed may be introduced from the inlet, filled in the container so that there is no space, and then discharged from the outlet. The slurry is again placed in a closed container. Here, the filling amount of the slurry and the dispersion medium in the sealed container is the same as the volume in the sealed container. In other words, the slurry and the dispersion medium are filled in the sealed container in such a manner that no gap exists. Here, the reason why the slurry and the dispersion medium are filled in the sealed container so as not to have a gap is as follows. 1 is a view showing a state in which the slurry ι 53 containing the spherical magnetic particles 152 and the dispersion medium 154 which are placed in the open container 151 opened at the upper portion of 28 323 724 201230083 by the uniaxial rotating body 155 are rotated at a high speed to perform high-speed stirring. Figure. In the figure, when the uniaxial rotating body 155 is rotated at a high speed, the liquid surface of the slurry 153 and the dispersion medium 154 is formed in a mortar shape which is low in the vicinity of the central axis and high in the peripheral portion due to the centrifugal force. The mechanical stress applied to the poly-liquid 153 containing the spherical magnetic particles 152 and the dispersion medium 154 by the uniaxial rotating body 155 escapes into a spider-like space, so that the entire open container 151 is passed through the dispersion medium 154. The mechanical stress transmitted to the spherical magnetic particles 152 becomes uneven, resulting in irregular thickness of the resulting flat magnetic particles. In addition, in the vicinity of the bottom of the spider-shaped space (near the central axis), the magnetic particles of the flat magnetic particles are released into the mortar-like space together with the dispersion medium to withstand an irregular impact. Or doubts such as defects. As a result, the thickness of the magnetic particles is irregular or broken or defective, and is a factor of increase in the loss tangent of the complex magnetic permeability in the VHF band. Fig. 2 shows that the uniaxial rotating body 155 is used to make the sealing The slurry 153 containing the spherical magnetic particles 152 of the container 1511 and the dispersion medium 154 are rotated at a high speed to perform high-speed stirring. In the figure, even if the uniaxial rotating body 155 rotates at a high speed, the sealed container 1511 contains a spherical shape. Since the liquid 153 of the magnetic particles 152 and the dispersion medium 154 are filled, there is no doubt that the mortar-like space as seen in the open container 151 is generated. Therefore, the uniaxial rotating body 155 is spherical. The mechanical stress ' 323 724 29 201230083 applied to the slurry 153 of the magnetic good 152 and the dispersion medium 154 is uniformly transferred to the spherical magnetic particles 152 through the dispersion medium 154 in the entire closed container 1511 without the resulting flat magnetic body. There is no doubt about the thickness of the particles. In addition, the magnetic particles that are flat will not withstand irregular impacts, and there will be no doubt that cracks or defects will occur. The number of revolutions of the uniaxial rotating body 155 is determined by the size of the hermetic container 1511. For example, in the case of the hermetic container 1511 having an inner diameter of 120 mm, the slurry 153 containing the spherical magnetic particles 152 and the dispersion medium 154 are located near the inner wall of the closed container 1511. The flow rate is preferably 5 m/sec or more, and more preferably 8 Å/sec or more. Further, when the internal volume of the hermetic container 1511 is small, the spherical magnetic particles 152 remain in the obtained flat magnetic particles. It is a concern that the residual spherical magnetic particles 152 are in contact with the spherical magnetic particles 152 or the spherical magnetic particles 152 are in contact with the flat magnetic particles, and the magnetic loss is increased or the orientation of the flat magnetic particles is hindered. Therefore, the flat magnetic particles are preferably 9% by mass or more, more preferably 95% by mass or more, and still more preferably 99% by mass or more, and preferably substantially free of spherical magnetic properties. Particle 152. Here, the reason why the spherical magnetic particle 152 remains when the internal volume of the sealed container 1511 is small is considered to be due to the corner of the closed container i5u or the rotating body 5 and the closed container i5U. The dead space that is not sufficiently conveyed by the mechanical stress is relatively large. Therefore, when the internal volume of the closed container 1511 is increased, the idle space can be relatively reduced, so that the mechanical stress is sufficiently transmitted to the ball. The particles 2 enhance the deformation and the fusion property of the spherical magnetic particles 30 323724 201230083, and as a result, the residual of the spherical magnetic particles 152 is reduced, and the spherical magnetic particles 152 are substantially absent. Thus, the spherical magnetic particles 152 are substantially The volume ' of the closed container 1511 which does not remain on is preferably il or more, and more preferably 5 l or more. As described above, the spherical magnetic particles are deformed and fused by the mechanical stress applied by the uniaxial rotating body 155, and become the flat magnetic particles 0. Then, the flat magnetic particles are separated from the dispersion medium and the solvent. Further, an appropriate liquid drying step can be carried out by considering the compatibility of the solvent used in the production of the flat magnetic particles with the insulating material to be mixed later. Specifically, when the solvent used for producing the flat magnetic particles is inferior in compatibility with the insulating material, it is preferred to carry out a drying treatment so that the solvent is 4% by mass or less, preferably 2% by mass or less. It is especially good for i mass% or less. On the other hand, when the compatibility between the solvent used for the production of the flat magnetic particles and the insulating material is good, the slurry drying step may be carried out without dispersing the flat magnetic particles in the solvent. Move to step 2. The drying method is not particularly limited as long as the solvent is removed from the slurry after the production of the flat magnetic particles, and examples thereof include heat drying, vacuum drying, and cold beam drying. From the viewpoint of drying efficiency, it is preferred. Dry for vacuum. Further, in order to improve the drying efficiency, a certain degree of solvent can be removed by a method such as solid-liquid separation before the drying step. The solid-liquid separation method may be a filtration operation such as a filter press or a suction filtration, 323724 31 201230083 or a general method such as a centrifugal separation operation by a decanter or a centrifugal separator. &lt;Second Step&gt; The flat magnetic particles are dispersed and mixed in a solution in which an insulating material is dissolved in a solvent to form a molding material. Here, the insulating material can be completely the same as the insulating material described above, and thus the description thereof will be omitted. Further, the solvent is not particularly limited as long as it can dissolve the insulating material, and for example, an alcohol such as decyl alcohol, ethanol, 2-propanol, butanol or octanol, ethyl acetate or butyl acetate can be suitably used. Ethyl lactate, propylene glycol monomethyl ether acetate, propylene glycol monoethyl ether acetate, 7-butyrolactone and other esters, diethyl hydrazine, ethylene glycol monoterpene _1 (曱基赛路苏(11161:1) ^1〇611〇3〇1乂6)), ethylene glycol monoethyl ether (ethyl celecoxib), ethylene glycol monobutyl ether (butyl seduce), diethylene glycol monomethyl ether, diethyl Ethers such as diol monoethyl ether, ketones such as acetone, methyl ethyl ketone, methyl isobutyl ketone, acetamidine acetone, cyclohexanone, aromatic hydrocarbons such as benzene, toluene, diphenylbenzene, and ethylbenzene; A guanamine such as guanamine, N,N-dimercaptoacetamide or N-decylpyrrolidone, and these solvents may be used alone or in combination of two or more. The dispersion mixing method is not particularly limited, and a stirring device such as a planetary mill, a sand mill, or a ball mill is preferably used. The mixing conditions can be suitably adjusted without agglomerating the flat magnetic particles. &lt;Third Step&gt; The above-mentioned molding material is molded or applied onto a substrate to prepare a molded body, and 32 323 724 201230083 is obtained by drying and curing the resultant. The molding method is suitable for a generally known molding method such as a die-casting blade coating method, an injection molding method, or the like. By using the film. The shape of the sheet is in the form of a sheet or a film having an arbitrary shape. When the layer is formed into a dry form, it is preferably formed into a shape of a crucible or a film by a doctor blade method. Concentrated material, when viscosity adjustment is required, volatilize the solvent and advance in drying. = If necessary, after the forming material is applied to the substrate, the sheet or film is flat, and the magnetic field is oriented to cause the flat magnetic particles to Orientation processing oriented with the direction of the thin. The heat may be carried out in a gas or in a vacuum, and the composite magnetic body of the present embodiment may be used. The plastic magnetic particles can be kneaded with a thermosetting resin or a hot crucible, mixed and dispersed, and formed into a composite body. Thus, a composite body of the actual state can be obtained. The kneading method may be carried out by heating and kneading by a generally known method such as a pressure kneader, a biaxial kneader, a blast mill or the like to obtain a kneaded product. In the method for molding the kneaded product, a molded body can be produced by a generally known method such as hot press molding, extrusion molding, injection molding or the like. In these methods, in order to orient the flat magnetic particles in the resin, it is preferably a heat-molded molding which is stretched into a flat shape. In order to adjust the viscosity at the time of stretching, it is preferred to add a plasticizer or to perform surface treatment of the flat magnetic particles. If necessary, it is preferred to carry out the orientation treatment of the orientation of the flat magnetic particles by the orientation of the magnetic field while heating and maintaining the fluidity in 323724 33 201230083. [Second composite magnetic material] The composite magnetic material of the present embodiment is a composite magnetic body in which the flat magnetic particles are dispersed in an insulating material, and the composite magnetic material has a porosity of 20% or less. Here, the porosity of the composite magnetic body can be obtained by the following formula (4). Porosity = (1 - measured density / theoretical density) χ 100 · · (4) The theoretical density of the composite magnetic material is based on the theoretical density of the flat magnetic particles and the theoretical density (and measured density) of the insulating material. The ratio of the mixture of the flat magnetic particles and the insulating material was calculated. Further, a method of calculating the theoretical density of the flat magnetic particles is a method of calculating a lattice constant from an X-ray diffraction pattern of the flat magnetic particles, and calculating a theoretical density value based on the lattice constant and the crystal structure. . On the other hand, a method of calculating the measured density of the insulating material, for example, when the insulating material is a resin, is a method of calculating the measured density from the measured values by merely curing the resin and measuring the outer dimensions and mass. Further, a method of calculating the measured density of the composite magnetic material, for example, a method of measuring the outer shape and the mass, and calculating the measured density from the measured values, or a method using the value measured by the pycnometer method. Preferably, the composite magnetic body has a real partial permeability #r' of 7 or more in a frequency band of 70 MHz to 500 MHz, and a real part er' 34 323724 201230083 of a complex dielectric constant of 15 or more, and (in r, · ε r,)-&quot;2 is 〇. i is below, (# γ £〆) 1/2 is 0.5 or more and 1 or less. In the composite magnetic body, by setting the real part of the complex magnetic permeability and the real part er of the complex permittivity to the above range, the electronic component or the electronic device including the composite magnetic body of the embodiment can be made small. It can suppress the power loss caused by impedance matching. Hereinafter, the composite magnetic body is attached to the antenna as an example, and the real part #r of the complex magnetic permeability described above and the real part ε r' of the complex permittivity are described in detail in the composite magnetic body. ( yr, · ε r,) - 1/2 and (the reason that r, / stone ",) 1/2 is set in the above range is preferable. Furthermore, the same effect can be obtained in all electronic components other than the above-mentioned antennas using high frequencies. First, it is preferable that the real//r of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz is 7 or more', and particularly preferably 9 or more. Here, the reason why #r is set to 7 or more is that the real part of the complex permittivity generally exhibits a large value of 15 or more, and when π is less than 7, the order is compared with "," The value of 丨 causes an increase in power loss due to inconsistency in characteristic impedance. The upper limit of the vr' is not particularly limited, and the aspect ratio or content of the flat magnetic particles that can be actually produced can be obtained. In view of the ratio, etc., it is preferably 15 or less. The real part of the complex dielectric constant is preferably 15 or more, and more preferably 2 or more. Here, the reason why ε r' is 15 or more is used. According to the above formula, the effective value of miniaturization of the antenna is achieved. 323724 35 201230083 When the values of /zr' and ε r' are set in the above range in the composite magnetic body, (/zr'. ε r ') - 1/2 is more preferably 0.1 or less. The reason is as follows. The value of (# r' . ε r')_1/2, as shown in the formula (1), is in the composite magnetic body. The rate of shortening of the high-frequency wavelength with respect to the wavelength of the vacuum. Furthermore, the wavelength in the vacuum and the wavelength in the general atmosphere are shown. Almost equal values. In general, an antenna is usually composed of an antenna conductor formed by a wire having a length of 1/2 or 1/4 of a wavelength, etc. In a long wavelength region with a low frequency, especially at a frequency of 70 MHz to 500 MHz. In the wavelength band, the wavelength is 60 cm or more, and when the length of the antenna conductor is 30 cm or more or 15 cm or more, the antenna itself becomes large. Therefore, the matching circuit is used to match the long-wavelength signal with the electronic circuit for reception and transmission, but when the antenna length is shortened When the amount of current on the antenna conductor is lowered, the frequency band in which the antenna can receive and transmit is narrowed, or the emission efficiency of the antenna is lowered. In particular, when the length of the antenna is set to be 1/10 or less of the wavelength, it is difficult to perform. The reception and transmission of radio waves have practical problems. Therefore, if a composite magnetic body (μι·'. ε r' V&quot;2 is 0.1 or less is mounted on the antenna, the high-frequency wavelength is theoretically almost the same on the composite magnetic body. Shortened to less than 1/10. Therefore, there is no narrowing of the frequency band that the antenna can receive and transmit when the matching circuit is used or the emission efficiency of the antenna is lowered. It is low, and the size of the antenna can be reduced. The above (/zr'/ er') 1/2 is preferably 0.5 or more and 1 or less. The reason is as follows. (/^1''/£1*') The value of 1/2, as shown in the above formula (2), is the ratio of the characteristic impedance of the composite magnetic 36 323724 201230083 to the characteristic impedance Zfl of the vacuum (Zg/Zq), so the characteristic impedance Zs of the composite magnetic body is The characteristic impedance of the vacuum is er, 1/2 times. Usually, the composite magnetic body ///* is smaller than £1·, so the characteristic impedance of the composite magnetic body Zg is larger than the characteristic impedance Ζα (with vacuum) The characteristic impedance Ζ〇) has a smaller value. Further, when a high-frequency signal is known to propagate from a region having a large characteristic resistance to a small region, reflection or absorption occurs and is attenuated. Therefore, when the characteristic impedance Za of the composite magnetic body is larger than 50% of the characteristic impedance Za of the gas, the high frequency attenuation rate is extremely large, and practical problems occur. Therefore, when the value of (//1^'/£]:')^ is set to 〇.5 or more, when the electromagnetic wave propagates from the atmosphere to the composite magnetic body, the change in the characteristic impedance can be suppressed to within 50%. Therefore, the attenuation of the high frequency signal can be suppressed. Further, when the characteristic impedance Za of the composite magnetic material having a large characteristic impedance Zg is larger, even if the characteristic impedance difference is extremely small, the electromagnetic wave is largely attenuated. Therefore, the value of ("corporate / e r') 1/2 is preferably 1 or less. The loss tangent of the complex magnetic permeability of the composite magnetic body is preferably at most 05 or less than 〇〇4. Further, the composite The loss of the dielectric constant of the magnetic body tangent tanA , ^ knife tan &lt; 5 e (hereinafter sometimes abbreviated as tan (5 ε ) 乂 乂 preferably Ο.1 or less, especially preferably 0.07 or less. So w tan5 // and When the value of tan5 £ exceeds the preferred value, respectively, in the magnetic body, only the high frequency corresponds to the imaginary part of the complex magnetic permeability #, = the part of the imaginary part of the reading constant is absorbed and converted into heat removal. In addition to the energy attenuation of the frequency signal, there is also a doubt that the s/n ratio is lowered or the heat of the 323724 37 201230083 is lowered, so it is not worthwhile. Currently, in the frequency band of 70 MHz to 500 MHz, the wavelength of the electromagnetic wave is long. It is difficult to achieve miniaturization of the antenna. Therefore, in applications where special requirements such as mobile phones, portable information terminals, and multi-functional portable information devices are required to be miniaturized, the whip antenna must be stretched to several times the length of the frame to be used. Or you have to use the headphone cable as an antenna. On the other hand, this In the composite magnetic body of the embodiment, if the real part yr of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz satisfies the above range, the frequency is from 70 MHz to 500 MHz, preferably from 9 〇 MHz to 220 MHz. In the antennas of electronic components or electronic devices used in the band, such as mobile phones, portable information terminals, and multi-functional portable information devices, miniaturization and power loss can be achieved at the same time. In the frequency band up to 500 MHz, tan (5 // and tan (5 ε is lower than the frequency band exceeding 5 〇〇 MHz, so the gain of the antenna is improved, which is preferable. In the composite magnetic body of the present embodiment) By dispersing the above-mentioned flat magnetic particles in an insulating material, the porosity of the obtained composite magnetic material is 20% or less, and although the composite magnetic material is increased by r, it is hardly changed. The antenna of the electronic component or the electronic device using the composite magnetic body, such as a mobile phone, a portable information terminal, and a multi-functional portable information device, can be miniaturized. The power loss caused by impedance matching can be suppressed. The mechanism for obtaining such an effect can be considered as follows. 323724 38 201230083 When the amount of magnetic particles in the pore volume of the composite magnetic body becomes smaller, the mother of the af body is grayish, so that r' On the other hand, it is immersed on the surface; the edge material is the same 'has an electrostatic capacitance with the flat magnetic particles', so even if the porosity is increased, ... in addition, when the composite magnetic body is ^ When the oxygen porosity is reduced, the magnetic particles of the mother's early volume of the composite magnetic body are multiplied to make #r' larger. On the other hand, as mentioned above, ε r

之值為幾乎相同之值。手不受氣孔率的影響,故K 亦即’藉由減少複合磁性體中的氣孔率,雖&quot;r,之值 變大,但ε r之值幾手不繳 沾兰hei ^ u ^,故縮小Mr,之值與ε r,之值 的差。因此,藉由將平均長會 1 ^ 我莧比(長徑/厚度)為5以上之平 板狀磁性體粒子分散於絕緣材料中而成之複合磁性體的氣 孔率設為2咖下’可使_該複合郝狀電子零件或 電子設備達成小型化,並可抑制阻抗匹配所造成之電力損 耗。 再者,減少複合磁性體的氣孔率之方法,只要是可將 複合磁性體的氣孔率減少至20%以下之方法即可,並無特 別限制。例如有藉由提升平板狀磁性體粒子對絕緣材料之 分散性,來防止平板狀磁性體粒子彼此凝聚之方法,藉由 使硬化劑的種類和量達到最適化以提升絕緣材料的硬化性 之方法’選擇流動性高的絕緣材料,使絕緣材料容易進入 於平板狀磁性體粒子與平板狀磁性體粒子間的間隙之方 法,藉由將所得之複合磁性體予以加壓來減少内部氣孔之 323724 39 201230083 方法等,此外’料_心合料方 &lt;絕緣材料&gt; 犮哥 絕緣材料,只要是絕緣性的材料即可,可使用與上述 第1複合磁性體的項目令所說明之絕緣 亦即,當將本實施形態之複合磁性 濕性低,且形狀加工性佳。此二=機械強度高,吸 版絕緣材料,例如可適當地 使=聚醯亞胺樹脂、聚苯並•樹脂、聚伸、聚苯 並環丁烯樹脂、聚伸芳基_脂、聚石夕氧燒樹卜日产氧 脂、聚醋樹脂、氟樹脂、聚稀煙樹 曰衣、 酸醋樹脂、聚伸苯細樹脂、降获㈣婦烴樹脂、乱 苯乙稀樹脂等熱硬化性樹脂或熱 :、ABS樹脂、聚 僅單獨使用i種或組合2種以樹脂。此等樹脂可 當中,主鏈具有環狀結構且呈有 官能基之樹脂,由於不易與平板狀磁^ =所聚合之 無阻礙平板狀磁性體粒子的Μ之疑慮,且所以並 故較佳。此般樹脂例如可列舉出二環 易传到商, :使用如二環戊二烯型樹墙般之較硬:: :: 低複合磁性體的氣孔率,於此般較硬 f為了降 予伸縮性或可撓性之絕緣性樹〗旨 :’可混合賦 絕緣性樹脂,種上述樹脂巾適#地=或可撓性之 狀環氧樹脂或雙酚型環氧樹脂。 ’特佳為液 當將該二環戊二烯型樹脂與上述液 酚型環氧樹脂組合使用時,較佳係 =ί脂或雙 一展戊一烯型樹脂相 323724 40 201230083 對於樹脂全體量之含有率設為5G f量%以上⑽質量%以 下。藉由將該二環戊二烯型樹脂的含有率設定在上述範圍, 可提升平板狀磁性體粒子的定向性,並且可得到高^,。 此外,由於含有10質量%以上50質量%以下之賦予伸 縮性或可撓性之絕緣性樹脂,所以樹脂容易地進入於平板 狀磁性體粒子彼此的間隙,可抑制複合磁性體之氣孔的生 成,並可降低氣孔率,故較佳。 [第2複合磁性體的製造方法] 接著說明本實施形態之複合磁性體的製造方法。 、該複合磁性體的製造方法,係具備有:使上述平板狀 磁i1 生體粒子刀政並混合於絕緣材料而製作出成形材料之步 驟,將所付之成形材料成形為既定形狀之成形步驟;以及 使所得之卿體絲/硬狀絲/硬化步驟。 &lt;成形材料的製作步驟〉 該步驟係合上述平板狀磁性體粒子、絕緣材料、溶 齊J以及因應必要之硬化劑,而製作出使平板狀磁性體粒 子分散於絕緣材料中之成形材料之步驟。 %緣材料已如上所敘述,故省略該說明。 田使用熱硬化性樹脂作為絕緣材料時,關於硬化劑的 種類和添加里,可因應所使用之熱硬化性樹脂的種類和量 來適當地調整。 田使用環氧樹脂作為上述熱硬化性樹脂時,就促進環 氧土彼此的縮合反應,並防止複合磁性體的成形體之硬化 不良所造成之氣孔的產生之觀點來看,較佳為三級胺。 41 323724 201230083 三級胺例如可列舉出1-異丁基-2-曱基咪唑、1-苄基 -2-曱基咪唑、卜氰基乙基-2-曱基咪唑、卜氰基乙基-2-乙基-4-曱基咪唑等。 硬化劑的添加量,考量到促進官能基的縮合反應,可 添加相對於熱硬化性樹脂與硬化劑的全體質量為0.5質量 %以上3質量%以下。 溶劑,只要是可溶解上述絕緣材料者即可,並無特別 限定,例如可適當地使用丙酮、丁酮、曱基異丁基酮、乙 醯丙酮、環己酮等酮類,苯、甲苯、二甲苯、乙基苯等芳 香族烴,二乙醚、乙二醇單曱醚(曱基赛路蘇)、乙二醇單 乙醚(乙基賽路蘇)、乙二醇單丁醚(丁基賽路蘇)、二乙二 醇單曱醚、二乙二醇單乙醚、丙二醇單曱醚等醚類,二曱 基曱醯胺、N,N-二曱基乙醯胺、N-曱基吡咯啶酮等醯胺類。 此等溶劑可單獨使用1種或混合2種以上而使用。尤 其是環己酮或二曱苯等高沸點的溶劑,可抑制因溶劑的揮 發所造成之成形材料的增黏,故較佳。 溶劑較佳係混合成形材料中的30質量%以上,尤佳為 35質量%以上。 藉由混合30質量%以上的溶劑,使所得之成形材料的 黏度降低,即使在混合時平板狀磁性體粒子彼此凝聚,仍 消除凝聚而提升絕緣材料中的分散性。藉此可降低複合磁 性體的氣孔率。 再者,當溶劑的量過多時,後述乾燥將會花費時間, 乾燥時有生成氣孔之疑慮,故溶劑的量較佳為50質量%以 42 323724 201230083 下。 該成形材料中之平板狀磁性體粒子的含有率,相對於 絕緣材料與硬化劑與平板狀磁性體粒子的合計量,較佳為 10體積%以上60體積%以下,尤佳為3〇體積%以上別體積 %以下。 在此,當平板狀磁性體粒子的含有率未達1〇體積% 時,平板狀磁性體粒子過少,使作為複合魏體的磁特性 降低’故不佳。另—方面,當該平板狀磁性體粒子的含有 率超過60體積%時,平板狀磁性體粒子過多,使含有該平 板狀磁性體粒子與絕緣材料與硬化劑與 流動性降低’因此,使用該成形材料成形時之成成形::的 故不佳。 _ 以及 混合此等平板狀磁性體粒子、絕緣材料、溶劑 因應必要之硬化劑,而得到成形材料。 混合裝置,只要可均勻地混合並分散此等平板狀磁性 體粒子、絕緣材料、硬化劑、及溶劑而形成狀成形材 料者即可,並無特別限制,例如可列舉出㈣機、自轉公 轉式混合機、均質機、超音波均質機、麟機等。以此等 褒置進行混合時mx不會使平板狀雜體粒子過度 凝聚而均勾地分散於絕緣材料巾之方式,來適當地調整混 合條件即可。 &lt;成形步驟&gt; 此係將上述步驟巾所得之成形材料,成形為既定形狀 的薄片狀、薄膜狀或塊(bulk)狀之步驟。 43 323724 201230083 成形法,只要是可將成形材料成形為一定形狀並保持 成形後的形狀者即可,並無特別限制。 此外,成形體的形狀或大小亦無特別限制,例如可成 形為薄片狀或薄膜狀,或是成形為直方體狀等具有厚度的 形狀,例如塊狀。 當成形為薄片狀或薄膜狀時,可藉由將上述成形材料 塗佈於薄片狀或薄膜狀的基體上而容易得到。該方法的量 產性佳,故較佳。 成形為薄片狀或薄膜狀之方法,可列舉出刮刀塗佈 法、棒塗佈法、模具塗佈法(die coating)、模壓法等。此 外,當成形為薄板狀等具有厚度的形狀時,例如使成形材 料流入於任意形狀的模具之方法等。 此外,當積層複合磁性體來構成積層構造體時,較佳 係藉由刮刀塗佈法來積層成形為薄片狀或薄膜狀之複合磁 性體。 &lt;定向步驟&gt; 此係使上述成形步驟中所得之成形體中之平均長寬 比(長徑/厚度)為5以上的平板狀磁性體粒子往單向定向 之步驟。 上述成形步驟中所得之成形體,當具有期望的# r’ 時,乃不需進行此定向步驟,但為了得到;f/r’更高的複合 磁性體,較佳係進行對所得之成形體施加磁場以使成形體 中的平板狀磁性體粒子往單向定向之定向步驟。 使成形體中的平板狀磁性體粒子定向之方法,只要施 44 323724 201230083 的平板狀磁性體粒子可往單向定向即 形二=====粒子施加磁場時,當成 : = 產生的磁力線相對於成形體 ,。當磁場達=二=二:: :成::中的平板狀磁性體粒子充分往單向定 板狀,由於細場,會有平 h 、— 彼此凝^而與絕緣材料分離之疑;t,使所 H=l轉組叫―佳 後之上述定向步驟中使平板狀磁性體粒子定向 =讀切㈣/硬化,㈣錢合魏體之步驟。 燥,接著藉ΓΓΓ板狀磁性體粒子定向後之成形體進行乾 乾燥/硬二、㈣料料硬化。 伟田4 , 牛(處理&amp;度、處理時間等),可因岸所 料或溶劑的種類而適當地調整。 下;燥Γ驟中所得之成形體的氣孔率為20%以 或欲更降^成=模壓步驟,當成形體的氣孔率超過20% 施行=體,率時’較佳係在上述乾燥步驟後 仃模壓之步驟。模壓裝置可適當地使用 323724 45 201230083 一般所知者。 以模壓展置對成形體施加壓力時,當使用樹脂作為絕 緣材料時’為了有效地減少氣孔,較佳是在樹脂的軟化溫 度以上且硬化起始溫度以下施加壓力。 模壓時的壓力可適當地調整,較佳係施加5MPa至 20MPa左右的壓力。 藉由上述方法,可製得本實施形態之複合磁性體。 [第3複合磁性體] 本實施形態之複合磁性體,係在前述第1複合磁性體 中’前述絕緣材料含有主鏈具有環狀結構且具有以單體單 位所聚合之官能基之第1樹脂之複合磁性體。 &lt;第1樹脂&gt; 上述第1樹脂,為主鏈具有環狀結構且具有以單體單 位所聚合之官能基之樹脂。該樹脂,只要是在與平板狀磁 性體粒子混合時可得到低黏度且具有流動性之成形材料之 樹脂即可,並無特別限定,可使用熱硬化性樹脂、熱可塑 性樹脂、紫外線硬化樹脂。 此般樹脂,可列舉出環氧樹脂、聚矽氧樹脂(silic〇ne resin)、酚樹脂、聚醯亞胺樹脂、聚苯並噚唑樹脂、聚伸 苯樹脂、聚苯並環丁烯樹脂、聚伸芳基醚樹脂、聚環己貌 樹脂、聚酯樹脂、氟樹脂、聚烯烴樹脂、聚環烯烴樹脂、 氰酸酯樹脂、聚伸苯基醚樹脂、聚苯乙烯樹脂、丙烯酸樹 脂、甲基丙烯酸樹脂、胺基甲酸酯樹脂、胺基甲酸酯_丙烯 酉文樹知知·氧-丙稀酸樹脂等。此孝樹脂可僅單獨使用1 46 323724 201230083 種或組合2種以上而使用。 此等當中,就相對於多數的溶劑具有溶解性且容易調 整黏度之觀點來看,較佳為熱硬化性樹脂,熱硬化性樹脂 中,較佳為環氧樹脂或聚環烯烴樹脂。 在此,主鏈具有環狀結構之樹脂,以環氧樹脂為例來 說明時,可適當地使用主鏈僅具有環狀結構之二環戊二烯 型環氧樹脂(式(1))或萘型環氧樹脂(式(2))。The value is almost the same value. The hand is not affected by the porosity, so K is also 'by reducing the porosity in the composite magnetic body, although the value of &quot;r, becomes larger, but the value of ε r does not pay dim blue hei ^ u ^, Therefore, the difference between the value of Mr and the value of ε r is reduced. Therefore, the porosity of the composite magnetic body obtained by dispersing the flat magnetic material having an average length of 1 ^1 (long diameter/thickness) of 5 or more in the insulating material can be made 2" _ The composite Hao-like electronic parts or electronic devices have been miniaturized, and the power loss caused by impedance matching can be suppressed. Further, the method of reducing the porosity of the composite magnetic material is not particularly limited as long as it can reduce the porosity of the composite magnetic body to 20% or less. For example, a method of preventing the dispersibility of the flat magnetic particles against the insulating material to prevent the flat magnetic particles from aggregating with each other, and improving the hardenability of the insulating material by optimizing the type and amount of the curing agent 'Selecting a highly fluid insulating material to allow the insulating material to easily enter the gap between the flat magnetic particles and the flat magnetic particles, and pressurizing the obtained composite magnetic body to reduce internal pores 323724 39 201230083 Method, etc., in addition, the material of the material of the first composite magnetic body, that is, the insulation described in the item of the first composite magnetic body, that is, the insulating material. When the composite magnetic permeability of the present embodiment is low, the shape processability is good. These two = high mechanical strength, suction plate insulation material, for example, can be appropriately made = polyimide resin, polybenzo resin, poly-stretch, polybenzocyclobutene resin, poly-arylene-lipid, poly stone Oxygen-burning tree, such as oxygen-producing resin, vinegar resin, fluororesin, poly-smoke tree smear, vinegar resin, poly- benzene fine resin, (4) maternity resin, styrene resin, etc. Or heat: ABS resin, poly, only use i alone or in combination with two kinds of resins. Among these resins, a resin having a cyclic structure in a main chain and having a functional group is preferable because it is difficult to cope with the flatness of the plate-like magnetic particles which are polymerized. Such a resin can be exemplified by the fact that the two rings are easily transported to the quotient: using a harder wall such as a dicyclopentadiene type wall:: :: a porosity of a low composite magnetic body, which is harder to reduce Insulating or flexible insulating tree is intended to be: 'mixable insulating resin, epoxy resin or bisphenol epoxy resin in the above-mentioned resin towel. 'Specially good liquid When the dicyclopentadiene type resin is used in combination with the above liquid phenol type epoxy resin, it is preferably a gluten or a bis- pentylene type resin phase 323724 40 201230083 The content ratio is set to 5 G f % by volume or more (10) by mass or less. By setting the content of the dicyclopentadiene type resin in the above range, the orientation of the flat magnetic particles can be improved, and a high yield can be obtained. In addition, since the insulating resin which imparts stretchability or flexibility is contained in an amount of 10% by mass or more and 50% by mass or less, the resin easily enters the gap between the flat magnetic particles, and the generation of pores of the composite magnetic body can be suppressed. It is preferable because the porosity can be lowered. [Method for Producing Second Composite Magnetic Body] Next, a method for producing the composite magnetic body of the present embodiment will be described. In the method for producing a composite magnetic body, the step of forming the molding material by forming the flat magnetic i1 green particles into a insulating material and mixing the molding material into a predetermined shape is provided. And the resulting filament/hard wire/hardening step. &lt;Step of Producing Molding Material&gt; This step is to produce a molding material in which flat magnetic particles are dispersed in an insulating material by combining the above-mentioned flat magnetic particles, an insulating material, a solvent J, and a curing agent necessary for the coating. step. Since the % edge material has been described above, the description is omitted. When a thermosetting resin is used as the insulating material in the field, the type and amount of the curing agent can be appropriately adjusted depending on the type and amount of the thermosetting resin to be used. When an epoxy resin is used as the thermosetting resin, it is preferably three-stage from the viewpoint of promoting condensation reaction between the epoxy earth and preventing generation of pores due to poor curing of the composite body of the composite magnetic body. amine. 41 323724 201230083 The tertiary amine may, for example, be 1-isobutyl-2-mercaptoimidazole, 1-benzyl-2-mercaptoimidazole, cyanoethyl-2-mercaptoimidazole or cyanoethyl 2-Ethyl-4-mercaptoimidazole and the like. The amount of the curing agent to be added is adjusted to promote the condensation reaction of the functional group, and may be added in an amount of 0.5% by mass or more and 3% by mass or less based on the total mass of the thermosetting resin and the curing agent. The solvent is not particularly limited as long as it can dissolve the insulating material. For example, ketones such as acetone, methyl ethyl ketone, decyl isobutyl ketone, acetamidine acetone, and cyclohexanone, benzene, toluene, and the like can be suitably used. Aromatic hydrocarbons such as xylene and ethylbenzene, diethyl ether, ethylene glycol monoterpene ether (methicone), ethylene glycol monoethyl ether (ethyl stilbene), ethylene glycol monobutyl ether (butyl Ethers such as sulphide), diethylene glycol monoterpene ether, diethylene glycol monoethyl ether, propylene glycol monoterpene ether, dimethyl decylamine, N,N-dimercaptoacetamide, N-fluorenyl Amidoxime such as pyrrolidone. These solvents may be used alone or in combination of two or more. In particular, a solvent having a high boiling point such as cyclohexanone or diphenylbenzene can suppress the increase in viscosity of the molding material due to the evaporation of the solvent, which is preferable. The solvent is preferably 30% by mass or more, and more preferably 35% by mass or more in the mixed molding material. By mixing 30% by mass or more of the solvent, the viscosity of the obtained molding material is lowered, and even when the flat magnetic particles are agglomerated during mixing, the aggregation is eliminated and the dispersibility in the insulating material is improved. Thereby, the porosity of the composite magnetic body can be lowered. Further, when the amount of the solvent is too large, it takes time to dry as described later, and there is a concern that pores are formed during drying. Therefore, the amount of the solvent is preferably 50% by mass to 42 323724 201230083. The content of the flat magnetic particles in the molding material is preferably 10% by volume or more and 60% by volume or less, and particularly preferably 3% by volume based on the total amount of the insulating material and the curing agent and the flat magnetic particles. The above is less than the volume %. When the content of the tabular magnetic particles is less than 1% by volume, the amount of the flat magnetic particles is too small, and the magnetic properties of the composite WE body are lowered, which is not preferable. On the other hand, when the content of the tabular magnetic particles exceeds 60% by volume, the tabular magnetic particles are excessively large, and the flat magnetic particles, the insulating material, and the curing agent are reduced in fluidity. When the forming material is formed into a shape: it is not preferable. _ and a molding material obtained by mixing these flat magnetic particles, an insulating material, and a solvent with a hardening agent necessary for the solvent. The mixing device is not particularly limited as long as it can uniformly form and disperse the flat magnetic particles, the insulating material, the curing agent, and the solvent to form a molding material, and examples thereof include a (four) machine and a self-rotating type. Mixer, homogenizer, ultrasonic homogenizer, Lin machine, etc. When mixing is carried out in such a manner, mx does not excessively agglomerate the tabular particles, and is uniformly dispersed in the insulating material to adjust the mixing conditions appropriately. &lt;Molding step&gt; This is a step of forming the molding material obtained in the above-mentioned step towel into a sheet shape, a film shape or a bulk shape having a predetermined shape. 43 323724 201230083 The molding method is not particularly limited as long as it can shape the molding material into a constant shape and maintain the shape after molding. Further, the shape or size of the molded body is not particularly limited, and for example, it may be formed into a sheet shape or a film shape, or may be formed into a shape having a thickness such as a rectangular parallelepiped shape, for example, a block shape. When it is formed into a sheet shape or a film shape, it can be easily obtained by applying the above-mentioned molding material to a sheet-like or film-like substrate. This method is preferred because of its good mass productivity. Examples of the method of forming into a sheet shape or a film form include a doctor blade coating method, a bar coating method, a die coating method, a molding method, and the like. Further, when it is formed into a shape having a thickness such as a thin plate shape, for example, a method of allowing a molding material to flow into a mold of an arbitrary shape or the like. Further, when the composite magnetic body is laminated to form a laminated structure, it is preferable to form a composite magnetic body formed into a sheet shape or a film shape by a doctor blade method. &lt;Orientation Step&gt; This is a step of aligning the flat magnetic particles having an average aspect ratio (long diameter/thickness) of 5 or more in the molded body obtained in the above-described molding step in one direction. The shaped body obtained in the above forming step does not need to perform this orientation step when it has a desired #r', but in order to obtain a composite magnetic body having a higher f/r', it is preferred to carry out the obtained shaped body. A direction in which a magnetic field is applied to orient the flat magnetic particles in the shaped body in one direction. The method of orienting the flat magnetic particles in the formed body is as long as the flat magnetic particles of 44 323724 201230083 can be oriented in one direction, that is, when the magnetic field is applied to the particles =====, when the magnetic field is applied to: = In the molded body, When the magnetic field reaches = two = two:: :::: The flat magnetic particles in the form are fully unidirectionally plated, and due to the fine field, there will be a flat h, a mutual condensation and separation from the insulating material; The H=l group is called the step of aligning the flat magnetic particles in the above-mentioned orientation step = read-cut (four)/hardening, and (iv) the step of merging the Wei body. After drying, the formed body oriented by the slab-shaped magnetic particles is subjected to dry drying/hardening, and (iv) material hardening. Weitian 4, cattle (treatment &amp; degree, treatment time, etc.) can be appropriately adjusted depending on the type of material or solvent. The porosity of the formed body obtained in the drying step is 20% or more desirably = molding step, and when the porosity of the formed body exceeds 20%, the body is subjected to the drying step. The step of molding. The molding device can be suitably used as described in 323724 45 201230083. When pressure is applied to the molded body by press-fitting, when resin is used as the insulating material, in order to effectively reduce the pores, it is preferred to apply pressure above the softening temperature of the resin and below the hardening start temperature. The pressure at the time of molding can be appropriately adjusted, and it is preferred to apply a pressure of about 5 MPa to 20 MPa. The composite magnetic body of the present embodiment can be obtained by the above method. [3rd composite magnetic material] The composite magnetic material of the present embodiment is characterized in that the insulating material contains a first resin having a cyclic structure and having a functional group polymerized in a monomer unit. Composite magnetic body. &lt;First resin&gt; The first resin is a resin having a cyclic structure and having a functional group polymerized in a monomer unit as a main chain. The resin is not particularly limited as long as it is a resin which can obtain a molding material having a low viscosity and fluidity when it is mixed with the flat magnetic particles, and a thermosetting resin, a thermoplastic resin, or an ultraviolet curable resin can be used. Examples of the resin include an epoxy resin, a silica resin, a phenol resin, a polyimide resin, a polybenzoxazole resin, a polyphenylene resin, and a polybenzocyclobutene resin. , poly-arylene ether resin, polycyclohexene resin, polyester resin, fluororesin, polyolefin resin, polycycloolefin resin, cyanate resin, polyphenylene ether resin, polystyrene resin, acrylic resin, A methacrylic resin, a urethane resin, a urethane, a propylene propylene tree, an oxy-acrylic resin, and the like. This filial resin can be used alone or in combination of two or more types of 1 46 323 724 201230083. Among these, from the viewpoint of solubility in a large amount of solvent and easy adjustment of viscosity, a thermosetting resin is preferable, and among the thermosetting resins, an epoxy resin or a polycycloolefin resin is preferable. Here, the main chain has a resin having a cyclic structure, and when an epoxy resin is used as an example, a dicyclopentadiene type epoxy resin having a cyclic structure of a main chain (formula (1)) or Naphthalene type epoxy resin (formula (2)).

式(2)中,h為氫或曱基。 此外,主鏈具有直鏈結構之樹脂,可列舉出在曱紛盼 醛型環氧樹脂的直鏈中具有C=1至3的短直鏈結構之樹脂 (式(3))。式(3)中,X為具有C=1至3的短院基鏈之直鏈 結構,較佳為C=1的直鏈結構。 47 323724 201230083In the formula (2), h is hydrogen or a fluorenyl group. In addition, the resin having a linear structure in the main chain, and a resin having a short linear structure of C = 1 to 3 in the linear chain of the aldehyde type epoxy resin is exemplified (formula (3)). In the formula (3), X is a linear structure having a short-length base chain of C = 1 to 3, preferably a linear structure of C = 1. 47 323724 201230083

式(3)中,X為ΟΙ至3的烷基鏈,R2為氫、分子量位 於15至180的範圍之烷基、芳基中的任一種。 該X例如可列舉出曱基、乙基、丙基、異丙基、丁基、 異丁基、三級丁基、苯基、苄基、甲苯基(tolyl)等。 此外,主鏈具有直鏈結構之樹脂,亦可使用在二環戊 二烯型環氧樹脂的直鏈中具有〇1至3的短直鏈結構之樹 脂(式(4))。 式(4)中,X為具有ΟΙ至3的烷基鏈之直鏈結構。 該X,與式(3)相同,例如可列舉出曱基、乙基、丙基、 異丙基、丁基、異丁基、三級丁基、苯基、苄基、曱苯基 等。In the formula (3), X is an alkyl chain of ΟΙ to 3, and R2 is any one of hydrogen and an alkyl group or an aryl group having a molecular weight of from 15 to 180. Examples of the X include a mercapto group, an ethyl group, a propyl group, an isopropyl group, a butyl group, an isobutyl group, a tertiary butyl group, a phenyl group, a benzyl group, a tolyl group, and the like. Further, as the resin having a linear structure in the main chain, a resin having a short linear structure of 〇1 to 3 in the linear chain of the dicyclopentadiene type epoxy resin (formula (4)) can also be used. In the formula (4), X is a linear structure having an alkyl chain of ΟΙ to 3. The X is the same as the formula (3), and examples thereof include a mercapto group, an ethyl group, a propyl group, an isopropyl group, a butyl group, an isobutyl group, a tertiary butyl group, a phenyl group, a benzyl group, and a fluorenylphenyl group.

即使上述結構的樹脂為不易纏繞於平板狀磁性體粒 子之樹脂,當高分子鏈較長時,有時會使複合磁性體之複 磁導率的實部#r’變小。因此,上述式(1)、式(3)、式(4) 的η較佳為0至3,更佳為n=0。 48 323724 201230083 亦即,較佳係單獨使用單體或是適當地組合單體及低 聚物而使用。 該複合磁性體全體量中之平板狀磁性體粒子的含有 率,較佳為10質量%以上60質量%以下,尤佳為30質量°/〇 以上50質量%以下。 在此,當平板狀磁性體粒子的含有率未達10質量% 時,平板狀磁性體粒子的比率過少,使所得之複合磁性體 的从r’過低,結果有無法確保期望的/zr’之疑慮,故不佳。 另一方面,當平板狀磁性體粒子的含有率超過60質 量%時,平板狀磁性體粒子的比率過多,使樹脂的量相對變 得過少,在混合平板狀磁性體粒子與樹脂時,無法得到低 黏度且具有流動性之成形材料,在後續步驟中之平板狀磁 性體粒子的定向不足,故不佳。 該平板狀磁性體粒子於複合磁性體中之定向方向與 該平板狀磁性體粒子的長轴方向所形成之角度,較佳為 20°以下,尤佳為0°以上15°以下,更佳為0°以上10°以下。 藉由使平板狀磁性體粒子的長軸方向相對於該平板 狀磁性體粒子的定向方向在上述範圍内傾斜,可得到/zr’ 更高之複合磁性體。 在此所謂的「定向方向」,是指平板狀磁性體粒子的 長軸所定向之方向,亦即當觀察複合磁性體的剖面時,與 複數個平板狀磁性體粒子的長軸方向所形成之角度的標準 偏差為最小之方向。 該複合磁性體的//r’,在70MHz至500MHz的頻率波 49 323724 201230083 段中’較佳為7以上,尤佳為1〇以上。 在此,將設為7以上之理由,在於訂,命大 長的驗率愈大,所以可達職㈣複合磁性體 件或電路基板等之進一步的小型化之故。 [第3複合磁性體的製造方法] 製、體的製造方法’係在第1複合磁性體的 “方去中之第2步驟中’含有主鏈具有環狀結構且具 以單體單位所聚合之官能基之第i樹脂作為絕緣材料^形 成成形材料,除此之外,其他與第!複合磁性體 法元全相同。 在此,為了得到从r,更高的複合磁性體,在第1 磁性體的製造総t之第3步㈣,健係在”成= 驟後,進行對所得之成形體施加磁場以使該絲體中的前 述平板狀磁性體粒子往單向定向之定向步驟,然 前述乾燥/硬化步驟。 仃 接著詳細說明第3複合磁性體的製造方法。 &lt;成形材料的製作步驟&gt; 首先,混合主鏈具有環狀結構且具有以單體單位所聚 合之官能基之樹脂、平板狀磁性體粒子、溶劑、以及因應 必要之硬化劑’而製作出成形材料。 μ 該主鏈具有環狀結構且具有以單體單位所聚合之官 能基之樹脂,只要是在與平板狀磁性㈣子混合^得到 低黏度且具有流動性之成形材料之樹❹阿,並無特別限 定,可使用熱硬化性職、熱可錢⑽旨、料線硬化樹 323724 50 201230083 脂0 此般樹脂,可列舉出環氧樹赌、聚石夕氧樹脂、齡樹腊 聚醯亞胺樹脂、聚苯並噚唑樹脂、聚伸苯樹脂、聚苯並環 丁烯樹脂、聚伸芳基_脂、聚環己域脂、聚賴脂、 氟樹脂、聚稀烴樹脂、聚環稀烴樹脂、氰酸醋樹脂、聚伸 苯基崎脂、聚苯乙烯樹脂、丙__、甲基丙雜樹 脂、胺基甲酸_脂、胺基f酸自旨—丙稀酸樹脂、環氧_丙 烯酸樹脂等。此等樹脂可僅單獨使用丨種或組合2種以上 ^等當中,就相對於多數的溶劑具有溶解性且容易調 中,點來看’較佳為熱硬化性樹脂,熱硬化性樹脂 中較佳為環氧樹脂或聚環烯烴樹脂。 述式主鏈具有環狀結構之環氧樹脂,可列舉出由上 从及由式(2)表示之萘型環氧樹脂。 匕外,主鏈具有直鏈結構之環 述式(3)表示之具有C=1 5 q^ *枒脂,可列舉出由上 脂,以及由十矣- 、丑直鏈之甲酚酚醛型環氧樹 烯型壤氡_具有&amp;1至3的短直鏈之二環戍二 體的// 至3,更隹因:二上述式⑴、式(3)、式⑷…佳為 子之::上!,的樹脂為不易纏繞於平板狀磁性體粒 r,變小。長時’有時會使複合磁性 =0 亦即 ,較佳係翔❹㈣或4#触合單體及低 323724 51 201230083 聚物而使用。 硬化劑的種類和添加量,可因應所使用之樹脂來適當 地調整。 當使用環氧樹脂作為上述樹脂時,就促進環 的縮合反應,並提升複合趣體之成形體 二 點來看,較佳為三級胺。 螞強度之觀 9三級胺例如可列舉出1、異丁基-2-甲基麵、卜节基 -2-曱基咪唑、i-氰基乙基、2_ &amp; 乙基-4-曱基咪唑等。 土 ’、〜氘基乙基-2- 硬化劑的添加量,考量到促進官能基 添加相對於樹脂與硬化#丨 闱〇反應,可 質量%以下。 劑的全體質量為〇.5質伽上3 此外’就降低立體障礙 ,提升複合磁性體的財,之觀點來看之 為具有環狀結構之硬化·; 匕叙具有核狀結構之硬化劑,例 型硬化劑、新紛傲歹丨舉出酚類酚醛 用何酚树脂(xylok)型 劑等。此等硬化劑^ 環戍二烯型硬化 更弱,故較佳係丄,:於使樹脂聚合之驅動力較三級胺等 ^ 係杰加與樹脂同等程度的量。 :谷劑’只要是可溶解上述樹脂者 ^例如可適當地使用丙酮、丁鲷、甲基=特別限 妳環己酮等綱類,苯、,苯 :、丁基酮、乙醯 族烴,二乙醚、 乙基苯等芳香 驗(乙基赛路蘇)醇單甲鍵(甲基赛路蘇)、乙二醇單乙 穌)、乙二醇單丁醚(丁基赛路蘇)、二乙二醇 323724 52 201230083 單曱醚、二乙二醇單乙醚、丙二醇單甲料μ %專皱類,-甲其 甲醯胺、Ν,Ν-二甲基乙醯胺、Ν-甲基一 τ丞 此等溶劍可單獨使用1種或混合2種、_等酿胺類。 其是環己酮或二甲苯等高沸點的溶劑,凡 』抑制因溶劑的槿 發所造成之成形材料的增黏,故較佳。 的禪 該成形材料中之平板狀磁性體粒子的八 备有率,相對·於Even if the resin of the above structure is a resin which is hard to be wound around the flat magnetic particles, when the polymer chain is long, the real part #r' of the complex magnetic permeability of the composite magnetic body may become small. Therefore, η of the above formula (1), formula (3), and formula (4) is preferably 0 to 3, more preferably n=0. 48 323724 201230083 That is, it is preferred to use a monomer alone or a combination of a monomer and an oligomer as appropriate. The content of the flat magnetic particles in the total amount of the composite magnetic material is preferably 10% by mass or more and 60% by mass or less, and more preferably 30% by mass or more and 50% by mass or less. When the content of the tabular magnetic particles is less than 10% by mass, the ratio of the tabular magnetic particles is too small, and the obtained composite magnetic material is too low from r', and as a result, the desired /zr' cannot be ensured. The doubts are not good. On the other hand, when the content of the tabular magnetic particles is more than 60% by mass, the ratio of the tabular magnetic particles is too large, and the amount of the resin is relatively small. When the flat magnetic particles and the resin are mixed, the ratio cannot be obtained. The molding material having low viscosity and fluidity is insufficient in the orientation of the flat magnetic particles in the subsequent step, which is not preferable. The angle between the orientation direction of the flat magnetic particles in the composite magnetic body and the long axis direction of the flat magnetic particles is preferably 20 or less, more preferably 0 or more and 15 or less, and more preferably 0° or more and 10° or less. By inclining the long-axis direction of the flat magnetic particles with respect to the orientation direction of the flat magnetic particles in the above range, a composite magnetic body having a higher /zr' can be obtained. The term "orientation direction" as used herein refers to a direction in which the long axis of the flat magnetic particles is oriented, that is, when the cross section of the composite magnetic body is observed, and the longitudinal direction of the plurality of flat magnetic particles is formed. The standard deviation of the angle is the smallest direction. The //r' of the composite magnetic body is preferably 7 or more, more preferably 1 or more, in the frequency wave of 49 MHz to 500 MHz in the period of 49 323 724 201230083. Here, the reason for setting it to 7 or more is that the larger the inspection rate is, the further the miniaturization of the composite magnetic body or the circuit board is achieved. [Method for Producing Third Composite Magnetic Body] The method for producing a body and the body is a method in which the main composite has a cyclic structure and is polymerized in a monomer unit in the second step of the first composite magnetic body. The i-th resin of the functional group is formed as a molding material as an insulating material, and the other is the same as the first compound magnetic element. Here, in order to obtain a higher composite magnetic body from r, the first one is obtained. In the third step (4) of the production of the magnetic body, after the "forming" step, a step of applying a magnetic field to the obtained shaped body to orient the flat magnetic particles in the filament in a unidirectional direction is performed. The aforementioned drying/hardening step.仃 Next, a method of manufacturing the third composite magnetic body will be described in detail. &lt;Production Step of Molding Material&gt; First, a mixed resin having a cyclic structure and having a functional group polymerized in a monomer unit, a flat magnetic particle, a solvent, and a curing agent required thereto are prepared. Forming material. μ The resin having a cyclic structure and having a functional group polymerized in a monomer unit, as long as it is mixed with a flat magnetic (tetra) substrate to obtain a low-viscosity and fluid-forming molding material, In particular, it is possible to use a heat-curing job, a heat-curable (10), a wire hardening tree 323724 50 201230083, a grease, and the like, and examples thereof include an epoxy tree gambling, a polyglycol, and an indomethacin. Resin, polybenzoxazole resin, polyphenylene resin, polybenzocyclobutene resin, polyarylene-lipid, polycyclohexyl ester, polylysate, fluororesin, poly-saturated resin, polycyclic ring Hydrocarbon resin, cyanate vinegar resin, polyphenylene resin, polystyrene resin, propylene, methacrylic resin, amino carboxylic acid _ lipid, amino acid f acid, acrylic acid resin, epoxy _Acrylic resin, etc. These resins may be used alone or in combination of two or more kinds, and have solubility in many solvents and are easy to adjust. From the viewpoint, it is preferably a thermosetting resin or a thermosetting resin. It is preferably an epoxy resin or a polycycloolefin resin. The epoxy resin having a cyclic structure in the main chain is a naphthalene type epoxy resin represented by the above formula (2). In addition, the main chain has a linear structure, and the cyclic formula (3) indicates that it has C=1 5 q^* rouge, and it can be exemplified by a grease, and a cresol novolac type. Epoxy-arc-type locus _ having a short-chain bicyclic quinone dimer of &amp; 1 to 3 // to 3, more causes: two of the above formula (1), formula (3), formula (4)... The resin of the above:: upper! is not easily entangled in the flat magnetic particle r, and becomes small. The long-term 'sometimes makes the composite magnetic =0, that is, it is preferably used as a sputum (4) or 4# contact monomer and a low 323724 51 201230083 polymer. The type and amount of the hardener can be appropriately adjusted depending on the resin to be used. When an epoxy resin is used as the above-mentioned resin, the condensation reaction of the ring is promoted, and the molded body of the composite fungus is promoted. From the viewpoint of the above, a tertiary amine is preferred. Examples of the strength of the turmeric strength 9 tertiary amines include, for example, isobutyl-2-methyl surface, phenethyl-2-mercaptoimidazole, i-cyanoethyl, 2_ &amp; ethyl-4-anthracene Imidazole and the like. The addition amount of the earth's ~-mercaptoethyl-2-hardener is considered to promote the reaction of the functional group with respect to the resin and the hardening, and the mass % or less. The total mass of the agent is 〇.5 伽加上3 In addition, it reduces the steric obstacle and enhances the financial properties of the composite magnetic material. From the viewpoint of the hardening of the ring structure, the hardening agent having a nuclear structure is described. The type of hardener, the new one is proud of the phenolic phenolic phenolic resin (xylok) type agent. These hardeners are less hardened by the cyclodecadiene type, so it is preferred to be a ruthenium. The driving force for polymerizing the resin is the same as that of the tertiary amine or the like. : the granules are as long as they are soluble in the above-mentioned resin. For example, acetone, butyl hydrazine, methyl group, particularly limited to cyclohexanone, benzene, benzene, butyl ketone, and ethyl hydrazine may be suitably used. Aromatic test (ethyl celecoxib) alcohol monomethyl bond (methyl serotonin), ethylene glycol monoethyl sulphate, ethylene glycol monobutyl ether (butyl sulbac), diethyl ether, ethyl benzene, etc. Diethylene glycol 323724 52 201230083 Monoterpene ether, diethylene glycol monoethyl ether, propylene glycol monomethacrylate μ% wrinkle, methionamide, hydrazine, hydrazine-dimethylacetamide, hydrazine-methyl One such squirting sword can be used alone or in combination with two kinds, _, etc. It is a solvent having a high boiling point such as cyclohexanone or xylene, and is preferred because it suppresses the viscosity of the molding material due to the burst of the solvent. Zen, the ratio of the flat magnetic particles in the forming material, relative to

成形材料中的揮發成分以外者硬化而成為固體狀穑 (樹脂+硬化劑+平板狀磁性體粒子),較佳I * V A U *S3 Qc 1' t · 60體積%以下,尤佳為30體積%以上5〇體積%以。 在此,當平板狀磁性體粒子的含有率未達丨〇體 時,平板狀磁性體粒子過少,使作為複合磁性體的磁特性。 降低,另一方面,當該平板狀磁性體粒子的含有率超 體時,平板狀磁性體粒子過多,使含有該平板狀磁 粒子與樹脂與硬化劑與溶劑之成形材料的流動性降低, 此,成形性降低,故不佳。 _ 因 〜混合此等平板狀磁性體粒子、樹脂、硬化劑及溶劑, 而侍到成形材料。此時,藉由適當地調整溶劑的添加窃, 可調整成形材料的黏度。 垔 、混=裝置,只要可均勻地混合此等平板狀磁性體粒 子、樹脂、硬化劑及溶劑而形成漿液狀成形材料者即可, 並&quot;’、特別限制,例如可列舉出親磨機、自轉公轉式現合 均質機、、超音波均質機、攪拌機等。 以 該成形材料的黏度較佳為0. IPa . S以上l〇6pa . 下尤佳為〇. 3 pa · S以上i〇4pa · s以下。 323724 53 201230083 在此’當黏度未達〇· 1 Pa · S時’流動性變得過大而 使乾燥步驟的生產性惡化’另一方面’當黏度超過106Pa . S時,黏性過高而難以進行平板狀磁性體粒子的定向,結 果使複合磁性體之爭板狀磁性體粒子的定向性降低,故不 佳。 如此,藉由將平板狀磁性體粒子的含有率設為10體 積%以上60體積%以下’且成形材料的黏度設為〇. 1Pa · s 以上106Pa · S以下’可得到以r與成形體的機械強度達到 均衡之複合磁性體。 &lt;成形&gt; 成形法’只要是在對成形材料施加磁場之步驟時可保 持為一定形狀者即可,並無特別限定。 此外 成形體的形狀双穴小亦無特別限制,例如可成 形為薄片狀或薄膜狀’或是成形為直方體狀等I有厂 、 形狀 由將上述成形材料塗 且置產性佳,故較 成形為薄片狀或薄膜狀者,可藉 佈於薄片或薄膜的基體上而容易得到 佳。 當成形為薄片狀或薄膜狀時,例如當成形材 為lOPa.S以下時,可使用刮刀塗佈法、棒塗佈々、-又 外,當成形材料的黏度超過10Pa . s時, 法等,此 法:。此外,當成形為具有厚度的形狀時,例如 料流入於任意形狀的模具之方法等。 y 在成形材料成形為薄片狀、薄膜狀或是成形為直方體 323724 54 201230083 狀等之狀態下,平板狀磁性體粒子有時會分別朝向不規則 方向而使定向不足。 々因此,對該成形為薄片狀、薄膜狀或是成形為直方體 狀等之成形體施加磁場,使該成雜巾的平板狀磁性體粒 子定向。 &lt;定向&gt; 使成形體中的平板狀磁性體粒子定向之方法,只要施 ^礤場以使成形體中的平板狀磁性體粒子可往單向定向即 可,並無特別限定,當成形體中磁力線彎曲時,無法使平 板狀磁性體粒子往單向定向。因此,磁場必須是以使所產 生的磁力線相對於成形體的表面大致平行之方式來施加。 此般定向方法,有下列所列舉之4種定向方法。The volatile component in the molding material is hardened to become a solid ruthenium (resin + hardener + flat magnetic particle), preferably I * VAU * S3 Qc 1' t · 60 vol% or less, and particularly preferably 30 vol% Above 5〇% by volume. When the content of the tabular magnetic particles is less than that of the ruthenium, the flat magnetic particles are too small to exhibit magnetic properties as a composite magnetic material. On the other hand, when the content rate of the flat magnetic particles is excessive, the flat magnetic particles are excessively large, and the fluidity of the molding material containing the flat magnetic particles and the resin and the curing agent and the solvent is lowered. The formability is lowered, so it is not good. _ Because the flat magnetic particles, resin, hardener and solvent are mixed, the molding material is applied. At this time, the viscosity of the molding material can be adjusted by appropriately adjusting the addition of the solvent. The 垔 and the mixing device may be formed by uniformly mixing the flat magnetic particles, the resin, the curing agent, and the solvent to form a slurry-like molding material, and are particularly limited, and examples thereof include a pro-grinding machine. , self-rotating and revolving type homogenizer, ultrasonic homogenizer, mixer, etc. The viscosity of the forming material is preferably 0. IPa. S or more l〇6pa. The lower part is 〇. 3 pa · S or more i〇4pa · s or less. 323724 53 201230083 Here, when the viscosity is less than 1 Pa · S, the fluidity becomes too large to deteriorate the productivity of the drying step. On the other hand, when the viscosity exceeds 106 Pa. S, the viscosity is too high and difficult. When the orientation of the flat magnetic particles is performed, the orientation of the plate-like magnetic particles of the composite magnetic body is lowered, which is not preferable. In this manner, the content of the flat magnetic particles is 10% by volume or more and 60% by volume or less and the viscosity of the molding material is set to 〇1 Pa·s or more and 106 Pa·s or less. A composite magnetic body with a balanced mechanical strength. &lt;Forming&gt; The molding method is not particularly limited as long as it can maintain a constant shape when a magnetic field is applied to the molding material. Further, the shape of the molded body is not particularly limited, and may be, for example, formed into a sheet shape or a film shape, or formed into a rectangular parallelepiped shape, etc., and the shape is coated by the above-mentioned molding material and has good productivity. Those formed into a sheet shape or a film shape can be easily obtained by being attached to a substrate of a sheet or a film. When it is formed into a sheet shape or a film shape, for example, when the molding material is 10 or less, it is possible to use a doctor blade coating method, a bar coating method, and/or, when the viscosity of the molding material exceeds 10 Pa·s, the method, etc. This method: Further, when formed into a shape having a thickness, for example, a method of flowing a material into a mold of an arbitrary shape or the like. y In the state in which the molding material is formed into a sheet shape, a film shape, or a shape formed into a rectangular parallelepiped shape, the flat magnetic particles may be oriented in an irregular direction and insufficiently oriented. Therefore, a magnetic field is applied to the molded body formed into a sheet shape, a film shape, or a rectangular parallelepiped shape, and the flat magnetic particles of the formed napkin are oriented. &lt;Orientation&gt; The method of orienting the flat magnetic particles in the molded body is not particularly limited as long as the field is applied so that the flat magnetic particles in the molded body can be oriented in one direction. When the magnetic field lines are bent, the flat magnetic particles cannot be oriented in one direction. Therefore, the magnetic field must be applied in such a manner that the magnetic lines of force generated are substantially parallel with respect to the surface of the formed body. As such a directional method, there are four orientation methods listed below.

(1)定向方法A 、第3圖係顯示用以實施本發明之複合磁性體的製造方 套中之疋向方法A之定向裝置之概略構成圖,為藉由對將 上述成形材料(圖式省略)塗佈於薄片狀或薄膜狀基體1的 上面之塗佈膜2施加磁場所產生之磁力線H,使塗佈膜2 中的平板狀磁性體粒子定向之裝置的例子。 κ该定向裝置11,是由:具備有將上述成形材料(圖式 Τ略)塗佈於往圖中箭頭方向g行進之基體1的上面而形成 塗佈膜2之分注器(dispenser)之塗佈手段12 ;分別設置 亥塗佈膜2的寬度方向兩侧,並藉由沿著該寬度方向對 塗佈臈2施加磁場所產生之磁力線H而使塗佈膜2中的平 板狀磁性體粒子定向之一對磁石l3a、13b ;以及將藉由磁 55 323724 201230083 力線Η使平板狀磁性體粒子定向後之塗佈膜2進行乾燥之 乾燥手段14所構成。磁石13a、13b,係配置為使相對向 的極彼此互成為異極。 該定向裝置11中,磁場從磁石13 a的N極朝向磁石 13b的S極產生,所以在通過磁石13a、13b間之塗佈膜2 上,會產生平行於從磁石13a的N極朝向磁石13b的S極 之方向之磁力線Η。藉由該磁力線Η,使塗佈膜2中的平板 狀磁性體粒子平行於磁力線Η而定向。 藉由上述方式,可使塗佈膜2中的平板狀磁性體粒子 平行於磁力線Η而定向。 (2)定向方法Β 第4圖係顯示用以實施本發明之複合磁性體的製造方 法中之定向方法Β之定向裝置之概略構成圖,該定向裝置 21與第3圖的定向裝置11不同之處,在於分別設置在塗 佈膜2的上側及下側之一對磁石22a、22b是配置為使相對 向的極彼此互成為同極者。 該定向裝置21中,當藉由一對磁石22a、22b對塗佈 膜2施加磁場時,從一方的磁石22a所產生之磁力線與從 另一方的磁石22b所產生之磁力線,由於在塗佈膜2的位 置上相斥,所以產生對該塗佈膜2的表面施加平行的磁場 之磁力線HI、H2。藉由該磁力線HI、H2,使塗佈膜2中的 平板狀磁性體粒子平行於磁力線Η1、H2而定向。 藉由上述方式,可使塗佈膜2中的平板狀磁性體粒子 平行於磁力線HI、Η2而定向。 56 323724 201230083(1) Orientation Method A and FIG. 3 are schematic structural views showing an orientation device of the method A of the method for manufacturing the composite magnetic body of the present invention, by using the above-mentioned molding material (pattern) An example of a device for applying a magnetic field line H generated by a magnetic field to a coating film 2 coated on the upper surface of a sheet-like or film-like substrate 1 to orient the flat magnetic particles in the coating film 2 is omitted. The aligning device 11 is provided with a dispenser that forms the coating film 2 by applying the molding material (schematically) to the upper surface of the substrate 1 that travels in the direction of the arrow g in the drawing. Coating means 12; each of the two sides in the width direction of the coating film 2 is provided, and the flat magnetic body in the coating film 2 is made by applying a magnetic field line H generated by applying a magnetic field to the coating crucible 2 along the width direction. One of the particle orientation pairs of the magnets l3a, 13b; and a drying means 14 for drying the coating film 2 obtained by orienting the flat magnetic particles by magnetic 55 323724 201230083. The magnets 13a, 13b are arranged such that the opposing poles become mutually different poles. In the orienting device 11, since the magnetic field is generated from the N pole of the magnet 13a toward the S pole of the magnet 13b, the coating film 2 passing between the magnets 13a and 13b is generated in parallel with the N pole from the magnet 13a toward the magnet 13b. The magnetic field line in the direction of the S pole. By the magnetic force line 平板, the flat magnetic particles in the coating film 2 are oriented parallel to the magnetic lines of force. By the above manner, the flat magnetic particles in the coating film 2 can be oriented parallel to the magnetic lines of force. (2) Orientation method Β Fig. 4 is a schematic block diagram showing an orientation device for performing the orientation method in the method for producing a composite magnetic body of the present invention, which is different from the orientation device 11 of Fig. 3. The magnets 22a and 22b are disposed on the upper side and the lower side of the coating film 2 so that the opposing poles are equal to each other. In the orientation device 21, when a magnetic field is applied to the coating film 2 by the pair of magnets 22a and 22b, magnetic lines of force generated from one of the magnets 22a and magnetic lines of force generated from the other of the magnets 22b are applied to the coating film. Since the position of 2 is repelled, magnetic lines HI and H2 which apply a parallel magnetic field to the surface of the coating film 2 are generated. The plate-like magnetic particles in the coating film 2 are oriented parallel to the magnetic lines Η1 and H2 by the magnetic lines HI and H2. By the above manner, the flat magnetic particles in the coating film 2 can be oriented parallel to the magnetic lines HI and Η2. 56 323724 201230083

(3 )定向方法C 第5圖係顯示用以實施本發明之複合磁性體的製造方 法中之疋向方法C之定向裝置之概略構成圖,該定向裝置 31與第4圖的定向裝置21不同之處,在於分別設置在該 塗佈膜2的上侧及下側之各一對的磁石32a、32b、磁石 33a、33b及磁石34a、34b,係以各個相對向的極彼此互成 為同極之方式’隔著一定間隔,例如相鄰接之磁石彼此的 磁力線不會相互抵銷之間隔而配置者。 例如’第4圖所示之定向裝置21中,由於從磁石22a、 22b的各N極所產生之磁力線H1、H2返回s極,所以在磁 石22a、22b之水平方向的兩端附近,磁力線垂直於塗佈膜 2的表面’而在未平行於塗佈膜2之方向上亦產生磁力線, 結果有時會使平板狀磁性體粒子的定向性降低。 另一方面’第5圖所示之定向裝置31中,如第6圖 所顯示,塗佈膜2在通過一對磁石32a、32b間之前,塗佈 膜2中的平板狀磁性體粒子41 ’雖然定向方向處於無秩序 狀態,但藉由通過磁石32a、32b間,藉由相對於該塗佈膜 2的表面平行地產生之磁力線hi、H2,使塗佈膜2中的平 板狀磁性體粒子41,成為沿著磁力線HI、H2而定向之平 板狀磁性體粒子41。 然而,若僅通過最初的磁石32a、32b間,則平板狀 磁性體粒子41的定向有時會不足。因此,藉由通過磁石 33a、33b間,修正平板狀磁性體粒子41不足的定向,而 提升定向性。在通過最後的磁石34a、34b間後,平板狀磁 323724 57 201230083(3) Orientation Method C Fig. 5 is a schematic block diagram showing the orientation device of the method C of the method for manufacturing the composite magnetic body of the present invention, which is different from the orientation device 21 of Fig. 4. Each of the pair of magnets 32a and 32b, the magnets 33a and 33b, and the magnets 34a and 34b provided on the upper side and the lower side of the coating film 2 are formed so that the opposite poles become mutually the same pole. The method is such that, for example, the magnetic lines of the adjacent magnets are not mutually offset at intervals. For example, in the orientation device 21 shown in Fig. 4, since the magnetic lines H1 and H2 generated from the respective N poles of the magnets 22a and 22b return to the s pole, the magnetic lines of force are perpendicular to both ends in the horizontal direction of the magnets 22a and 22b. Magnetic field lines are also generated on the surface ' of the coating film 2 in a direction not parallel to the coating film 2, and as a result, the orientation of the flat magnetic particles may be lowered. On the other hand, in the orientation device 31 shown in Fig. 5, as shown in Fig. 6, the coating film 2 is coated with the flat magnetic particles 41' in the film 2 before passing between the pair of magnets 32a and 32b. Although the orientation direction is in an unordered state, the flat magnetic particles 41 in the coating film 2 are caused by the magnetic lines of force hi, H2 generated in parallel with the surface of the coating film 2 between the magnets 32a and 32b. The flat magnetic particles 41 oriented along the magnetic lines HI and H2 are formed. However, if only the first magnets 32a and 32b pass between the first magnets 32a and 32b, the orientation of the flat magnetic particles 41 may be insufficient. Therefore, the orientation of the flat magnetic particles 41 is corrected by the difference between the magnets 33a and 33b. After passing between the last magnets 34a, 34b, the flat magnet 323724 57 201230083

性體粒子41不足的定向祜攸 ...L 铍修正,使其成為定向性高者。 如此,藉由對塗佈祺? Z施加稷數次磁場,可提升塗佈 膜2中之平板狀磁性體粒子41的定向性。The orientation of the traits of the traits 41 is insufficient, so that it becomes a highly directional. So, by coating? When the magnetic field is applied a plurality of times by Z, the orientation of the flat magnetic particles 41 in the coating film 2 can be improved.

(4)定向方法D 第7圖係,J不用以實施本發明之複合磁性體的製造方 法中之疋向方法D之定向|置之概略構成圖,該定向裝置 51與第4圖的定向裝置21不同之處,在於在磁力線m、 H2平行於塗佈膜2中的平板狀磁性體粒子4i之位置上, 設置用以預備乾燥塗佈膜2之乾燥手段52者。 乾燥手&amp; 52’只要是具備可使塗佈膜2固化之程度的 乾燥功此者即可’並師別限定’例如可列舉出連接於暖 風供給源之暖風吹出喷嘴等。 該定向裝置51中’當藉由一對磁石22a、22b對塗佈 膜2施加磁場時’產生對該塗佈M 2的表面施加平行的磁 場之磁力線Η卜H2。藉由該磁力線耵、H2,使塗佈膜2 中的平板狀磁性體粒子平行於磁力線Μ、H2而定向。此 時,若藉減料段52預備賴塗佈膜2,駭使塗佈膜 2固化而將以平行於磁力線H1、H2之方式定向之平板狀磁 性體粒子的定向狀態固定。 藉由上述方式,可使塗佈膜2中的平板狀磁性體粒子 平行於磁力線HI、H2而定向。 如上所述,可僅單獨進行定向方法A至D中的任一 種,或是組合2種以上來進行,藉此可提升塗佈膜2中之 平板狀磁性體粒子的定向性。 323724 58 201230083 即使將塗佈膜2取代為既定形狀的成形體時,亦可藉 由適當地應用定向方法A至D中的一種以上,而提升成形 體中之平板狀磁性體粒子的定向性。 上述磁石13a、13b……,可列舉出電磁石、永久磁石 等。磁石的配置或對數並無特別限定,可配合塗佈膜或成 形體的形狀或所要求之磁特性來適當地調整。 所施加之磁場的大小,在如第3圖所示之定向裝置般 使異極互相面對時,較佳為100高斯以上1000高斯以下。 當磁場的大小未達100高斯時,磁場過小而有時無法使成 形體中的平板狀磁性體粒子充分地定向。另一方面,當超 過1000高斯時,磁場過大,而有平板狀磁性體粒子與樹脂 分離之疑慮,結果使所得之複合磁性體的磁特性產生不均 勻。 此外,在如第4圖所示之定向裝置般使同極互相面對 時,由於不易引起平板狀磁性體粒子與樹脂之分離,故較 佳為100高斯以上3000高斯以下。 &lt;乾燥/硬化&gt; 係將使平板狀磁性體粒子定向後之成形體進行乾 燥,接著藉由加熱或是紫外線照射等使樹脂硬化。乾燥/ 硬化條件(處理溫度、處理時間等),可因應所使用之樹脂 或溶劑的種類而適當地調整。 藉由上述方法,可製得第3複合磁性體。 [第4複合磁性體] 本實施形態之複合磁性體,係在前述第1複合磁性體 59 323724 201230083 中’前述絕緣材料含有主鏈具有環狀結構且具有以單體單 位所聚合之官能基之第1樹脂,並且更含有對該第1樹脂 賦予可撓性之第2樹脂之複合磁性體。 該複合磁性體之70MHz至500MHz的頻率波段之複磁 導率的實部/zr,較佳為7以上,尤佳為1〇以上。 在此,將該複合磁性體之70MHz至500MHz的頻率波 段之複磁導率的實部&quot;r,設為7以上之理由,在於v r,愈 大,波長的縮短率愈大,所以可達到應用該複合磁性體之 電子零件或電路基板等之進一步的小型化之故。 該複合磁性體之複磁導率的損耗正切tan &lt;5 /z較佳為 0. 05以下,尤佳為〇.〇4以下。在此’當tan &lt;5 //超過0.05 時’複合磁性體内,僅高頻率之對應於複磁導率的虛數部 β r”之部分被吸收而轉換為熱’除了使高頻信號的能量衰 減之外,亦產生S/N比降低或放熱等問題,有時會使增益 降低,故不佳。 在此係詳細說明構成本實施形態之複合磁性體之第2 樹脂。 第2樹脂,為對主鏈具有環狀結構且具有以單體單位 所聚合之官能基之第1樹脂賦予可撓性之樹脂。 該第2樹脂,當混合第1樹脂與平板狀磁性體粒子並 成形/硬化時,只要是可將可撓性及伸縮性賦予至所得之硬 化體之樹脂即可,並無特別限定’較佳例如為環氧樹脂、 聚矽氧樹脂、胺基甲酸酯樹脂、聚醢胺樹脂等可撓性佳之 樹脂。 60 323724 201230083 此外,亦可使用:使用胺基曱酸酯、聚乙烯、乙烯丙 烯等而對環氧樹脂進行改質之改質環氧樹脂,或是將環氧 丙烧(propylene oxide)加成於環氧樹脂之環氧丙炫加成 環氧樹脂。 此般賦予可撓性之樹脂,較佳為環氧樹脂,尤佳例如 為具有雙酚A型、雙酚B型、雙酚F型等雙酚骨架之環氧 樹脂。 具有雙酚A型骨架之環氧樹脂,可列舉出亞異丙基雙 酚、亞異丙基雙(鄰甲酚)、四溴雙盼A、1,3-雙(4-羥基異 丙苯基苯)、1,4-雙(4-羥基異丙苯基苯)等。 具有雙酚B型骨架之環氧樹脂,可列舉出2, 2-雙(羥 基苯基)丁烷等。 具有雙酚F型骨架之環氧樹脂,可列舉出亞曱基雙 酚、亞曱基雙(鄰曱酚)等。 該具有雙酚骨架之環氧樹脂中,較佳為具有雙酚A型 骨架及雙酚F型骨架中的至少1種之環氧樹脂。當中,就 伸縮性、剪切強度之觀點來看,較佳為具有雙酚A型骨架 之環氧樹脂。 此外,上述具有雙酚骨架之環氧樹脂中,較佳是於1 分子中含有2個以上的環氧基且具有醚骨架之環氧樹脂。 於1分子中含有2個以上的環氧基之結構,例如可列舉出 二縮水甘油驗(diglycidyl ether)、二縮水甘油酯、二縮 水甘油胺等。 上述醚骨架,只要是含有1個以上的醚部分結構之化 61 323724 201230083 合物者即可,並無特別限定。此般醚骨架,例如可列舉出 烧二醇。 該烧二醇,伸烧基的碳數較佳為2至6,尤佳為2至 5,更佳為2至4。 該醚骨架可為直鏈狀或具有分枝鏈者,較佳為來自乙 二醇或丙二醇之醚骨架。 此外,具有雙酚A型骨架、於1分子中含有2個以上 的環氧基且具有醚骨架之結構,例如可列舉出將由丙二醇 所構成之醚骨架導入於雙酚A型的骨架,並將縮水甘油醚 導入於該雙酚A型骨架的末端之丙二醇加成雙酚A型結構 (化學式(5))。(4) Orientation Method D Fig. 7 is a schematic diagram of the orientation of the method of the method of manufacturing the composite magnetic body of the present invention, and the orientation device of the orientation device 51 and the fourth embodiment The difference of 21 is that the magnetic force lines m and H2 are parallel to the flat magnetic particles 4i in the coating film 2, and the drying means 52 for preparing the dried coating film 2 is provided. The drying hand &amp; 52' can be a drying blower having a degree to which the coating film 2 can be cured, and can be exemplified, for example, a warm air blowing nozzle connected to a warm air supply source. In the orienting device 51, when a magnetic field is applied to the coating film 2 by the pair of magnets 22a, 22b, a magnetic field line H2 which applies a parallel magnetic field to the surface of the coating M 2 is generated. The flat magnetic particles in the coating film 2 are oriented parallel to the magnetic lines Μ and H2 by the magnetic lines 耵 and H2. At this time, if the coating film 2 is prepared by the reduction section 52, the coating film 2 is cured to fix the orientation state of the flat magnetic particles oriented in parallel with the magnetic lines H1 and H2. By the above manner, the flat magnetic particles in the coating film 2 can be oriented parallel to the magnetic lines of force HI, H2. As described above, it is possible to carry out only one of the alignment methods A to D alone or two or more of them, whereby the orientation of the flat magnetic particles in the coating film 2 can be improved. 323724 58 201230083 When the coating film 2 is replaced with a molded body having a predetermined shape, the orientation of the flat magnetic particles in the molded body can be improved by appropriately applying one or more of the orientation methods A to D. Examples of the magnets 13a and 13b include magnetite, permanent magnet, and the like. The arrangement or the number of pairs of the magnets is not particularly limited, and can be appropriately adjusted in accordance with the shape of the coating film or the shaped body or the required magnetic properties. The magnitude of the applied magnetic field is preferably 100 gauss or more and 1000 gauss or less when the opposite poles face each other as in the orientation device shown in Fig. 3. When the magnitude of the magnetic field is less than 100 gauss, the magnetic field is too small and the flat magnetic particles in the shaped body may not be sufficiently oriented. On the other hand, when the value exceeds 1000 gauss, the magnetic field is excessively large, and there is a concern that the flat magnetic particles are separated from the resin, and as a result, the magnetic properties of the obtained composite magnetic body are uneven. Further, when the same poles are faced to each other as in the orientation apparatus shown in Fig. 4, since the separation of the flat magnetic particles and the resin is less likely to occur, it is preferably 100 gauss or more and 3,000 gauss or less. &lt;Drying/hardening&gt; The molded body obtained by orienting the flat magnetic particles is dried, and then the resin is cured by heating or ultraviolet irradiation. The drying/hardening conditions (treatment temperature, treatment time, etc.) can be appropriately adjusted depending on the type of the resin or solvent to be used. By the above method, the third composite magnetic body can be obtained. [4th composite magnetic body] The composite magnetic material of the present embodiment is the first composite magnetic material 59 323724 201230083. The insulating material contains a functional group having a main chain having a cyclic structure and polymerized in a monomer unit. The first resin further contains a composite magnetic material of a second resin that imparts flexibility to the first resin. The real part /zr of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz of the composite magnetic body is preferably 7 or more, and more preferably 1 or more. Here, the reason why the real part of the complex magnetic permeability of the composite magnetic body in the frequency band of 70 MHz to 500 MHz is 7 or more is that the larger the vr is, the larger the wavelength shortening rate is, and thus the achievable Further miniaturization of electronic components or circuit boards using the composite magnetic body is employed. The loss tangent of the complex magnetic permeability of the composite magnetic body is preferably &lt; 5 /z is preferably 0.05 or less, and more preferably 〇.〇4 or less. Here, 'when tan &lt;5 // exceeds 0.05', in the composite magnetic body, only the portion of the imaginary part β r" corresponding to the complex magnetic permeability of the high magnetic permeability is absorbed and converted into heat 'except for the high frequency signal. In addition to the energy attenuation, problems such as a decrease in the S/N ratio or heat generation may occur, which may cause a decrease in gain, which is not preferable. The second resin constituting the composite magnetic body of the present embodiment will be described in detail. A resin which imparts flexibility to a first resin having a cyclic structure and a functional group polymerized in a monomer unit. The second resin is formed by molding a first resin and a flat magnetic particle. In the case of a resin which can impart flexibility and stretchability to the obtained cured body, it is not particularly limited. Preferably, for example, an epoxy resin, a polyoxyxylene resin, a urethane resin, or a polyfluorene is used. A flexible resin such as an amine resin. 60 323724 201230083 In addition, a modified epoxy resin modified with an amino phthalate, polyethylene, ethylene propylene or the like may be used, or a ring may be used. Add propylene oxide to the ring The epoxy resin of the resin is added to the epoxy resin. The resin which is imparted with flexibility is preferably an epoxy resin, and particularly preferably a bisphenol such as bisphenol A type, bisphenol B type or bisphenol F type. Epoxy resin of the skeleton. Epoxy resin having a bisphenol A type skeleton, and examples thereof include isopropylidene bisphenol, isopropylidene bis(o-cresol), tetrabromo-p-A, and 1,3-double ( 4-hydroxycumylbenzene), 1,4-bis(4-hydroxycumylbenzene), etc. Epoxy resin having a bisphenol B-type skeleton, and 2,2-bis(hydroxyphenyl) Butane, etc. The epoxy resin having a bisphenol F-type skeleton may, for example, be an anthracenyl bisphenol or a fluorenylene bis (o-nonylphenol). An epoxy resin having at least one of a bisphenol A type skeleton and a bisphenol F type skeleton. Among them, an epoxy resin having a bisphenol A type skeleton is preferable from the viewpoint of stretchability and shear strength. Further, among the epoxy resins having a bisphenol skeleton, an epoxy resin having two or more epoxy groups and having an ether skeleton is preferably contained in one molecule. Examples of the structure of the epoxy group include diglycidyl ether, diglycidyl ester, diglycidylamine, etc. The ether skeleton is a compound containing at least one ether moiety 61 323724 The composition of the ether skeleton is not particularly limited. For example, the ether skeleton may be a calcined diol. The calcined diol has a carbon number of preferably 2 to 6, more preferably 2 to 5, More preferably, it is 2 to 4. The ether skeleton may be linear or branched, preferably an ether skeleton derived from ethylene glycol or propylene glycol. Further, it has a bisphenol A type skeleton and contains 2 molecules in one molecule. The structure which has an epoxy group and has an ether skeleton, for example, is a propylene glycol which introduces the ether skeleton which consists of propylene glycol to the bisphenol A type, and introduces a glycidyl ether in the terminal of the bisphenol A type skeleton. Addition of bisphenol A type structure (chemical formula (5)).

/CH 3 h2c&gt;ch-ch2-o^ch-ch2-o;/CH 3 h2c&gt;ch-ch2-o^ch-ch2-o;

JH-CH,JH-CH,

V _(5) 該化學式(5)中,p+q之值為1至5,該p+q之較佳的 值為2至4,更佳的值為2至3。 · 此外,該結構的其他例子,可列舉出將由乙二醇所構 成之醚骨架,來取代由丙二醇所構成之醚骨架而導入於雙 酚A型的骨架,並將縮水甘油醚導入於該雙酚A型骨架的 末端之由化學式(6)表示之乙二醇加成雙酚A型結構。 H2v c -c-o{ch2-ch2o)|&lt;^^-|-^^(och2-ch2)-o -c- c-ch2 (6) 62 323724 201230083 該化學式(6)中 的值為4至8,争社 7,η+πι之值為1至10,該n+m之較佳 為4至8 ’更佳的值為6。 具有雙紛A刑辱加¥ w ^ L .V _ (5) In the chemical formula (5), the value of p + q is from 1 to 5, and the preferred value of the p + q is from 2 to 4, and more preferably from 2 to 3. In addition, as another example of the structure, an ether skeleton composed of ethylene glycol is substituted for the ether skeleton composed of propylene glycol and introduced into a bisphenol A type skeleton, and glycidyl ether is introduced into the double The ethylene glycol addition bisphenol A type structure represented by the chemical formula (6) at the end of the phenol A type skeleton. H2v c -co{ch2-ch2o)|&lt;^^-|-^^(och2-ch2)-o -c- c-ch2 (6) 62 323724 201230083 The value in the chemical formula (6) is 4 to 8 The value of η+πι is 1 to 10, and the value of n+m is preferably 4 to 8'. The better value is 6. Have a double-discriminate A torture plus ¥ w ^ L.

此專第1树脂與第2樹脂的混合比率,相對於第1樹 脂與第2樹脂之合計質量,較佳係含有5質量%以上3〇質 量%以下之第2樹脂。 藉由在上述範圍内將第2樹脂混合於第丨樹脂,者將 複合磁性體成形於基材上0造時,由於可職基材:剝 離性為良好之程度的伸縮性及可撓性賦予至該複合磁性 體,故較佳。 [第4複合磁性體的製造方法] 接著說明第4複合磁性體的製造方法。 第4複合磁性體的製造方法,係在第3複合磁性體的 製造方法+之第2步射’含有域具有環狀結構且具有 以單體單位所聚合之官能基之第1樹脂作為絕緣材料了且 更含有對前述第1樹脂賦予可撓性之樹脂的第2樹脂而形 成成形材料,除此之外,其他與第3複合磁性體的製造方 法完全相同。 323724 63 201230083 &lt;成形材料的製作步驟&gt; 該步驟中’係混合主鏈具有環狀結構且具有以單體單 位所聚合之官能基之第1樹脂、對該第丨樹脂賦予可撓性 之第2樹脂、平板狀磁性體粒子、溶劑、以及因應必要之 硬化劑’而製作出成形材料之步驟。 此等第1樹脂、第2樹脂及平板狀磁性體粒子的各組 成、形狀、特性、製造方法等既已說明,故省略該說明。 再者,第1樹脂及第2樹脂可藉由一般所知的方法來 合成,亦可使用市售品。 此外,第2樹脂的市售品,較佳為商品名稱「Adeka Resin EP-4000」(Adeka公司製(上述化學式(5)中p+q=2 者)、商品名稱「RikaresinBPO-20E」(新日本理化股份有 限公司製(上述化學式(5)中p+q=2者)、商品名稱 「RikaresinBPO-60E」(新日本理化股份有限公司製(上述 化學式(6)中n+m=6者)等。 使用上述第1樹脂及第2樹脂時之硬化劑的種類和添 加量’可因應所使用之樹脂的種類和量來適當地調整。 當使用壤氧樹脂作為上述樹脂時,就促進譬氧某彼此 的縮合反應’並提升複合磁性體之成形體的機械強度之觀 點來看,較佳為三級胺。 三級胺例如可列舉出1-異丁基-2-曱基坐、丨_节基 -2-甲基咪°坐、1-氰基乙基-2-曱基咪唾、說夷乙夷_2一 乙基-4-甲基°米唾等。 硬化劑的添加量’考量到促進官能基的縮合反應,可 323724 64 201230083 於樹脂與硬化劑的全體質量為〇.5質量%以上3 此外,料低立輯礙對平板狀雜體 ^響以提升複合师體的〆之觀點來看,與上述樹= 5 述更化劑較佳為主鏈具有環狀結構之硬化劑。 此般具有環狀結構之硬化劑,例如可列舉出齡類祕 !硬化劑、新_^(xylQk)型硬化劑、二環戊二烯型硬化 劑等此等硬化劑’由於使樹脂聚合之_力較三級胺等 更弱,故較佳係添加與樹脂同等程度的量。 /奋劑可列舉出與上述第3複合磁性體中所列舉者為相 同者。 該成形材料中之平板狀磁性體粒子的含有率,相對於 成形材料中的揮發成分以外者硬化而成為固體狀時之第1 樹脂的體積VI與第2樹脂的體積V2與硬化劑的體積V3 與平板狀磁性體粒子的體積V4之和(BV1+V2+V3+V4),較佳 為10體積%以上60體積%以下,尤佳為30體積%以上50 體積%以下。 在此’當平板狀磁性體粒子的含有率未達1〇體積% 時’平板狀磁性體粒子過少,使作為複合磁性體的磁特性 降低,故不佳’另一方面,當該平板狀磁性體粒子的含有 率超過60體積%時’平板狀磁性體粒子過多,使含有該平 板狀磁性體粒子與樹脂與硬化劑與溶劑之成形材料的流動 性降低,因此’當藉由該成形材料來形成成形體時,不易 進行平板狀磁性體粒子的定向,結果使複合磁性體中之平 65 323724 201230083 板狀磁性體粒子的定向性降低,故不佳。 混合此等平板狀磁性體粒子、第1樹脂、第2樹脂、 硬化劑及溶劑,而製作成形材料。此時,藉由適當地調整 溶劑的添加量,可調整成形材料的黏度。 混合裝置可列舉出與上述第1複合磁性體中所列舉者 為相同者。 所得之成形材料的黏度較佳為0. IPa · S以上106Pa · S以下,尤佳為0. 3 Pa · S以上104Pa · S以下。 在此,當黏度未達0. IPa · S時,流動性變得過大而 使乾燥步驟的生產性惡化,故不佳,另一方面,當黏度超 過106Pa · S時,黏性過高而難以進行平板狀磁性體粒子的 定向,結果使複合磁性體中之平板狀磁性體粒子的定向性 降低,故不佳。 如此,藉由將該成形材料中之平板狀磁性體粒子的含 有率設為10體積%以上60體積%以下,且將該成形材料的 黏度設為0. IPa · S以上106Pa · S以下,可得到# r’與成 形體的機械強度達到均衡之複合磁性體。 &lt;成形步驟&gt; 此係將上述步驟中所得之成形材料成形為既定形狀 之步驟。 成形法,只要是可將成形材料成形為一定形狀,且於 成形後施加磁場時可保持為一定形狀者即可,並無特別限 定。 此外,成形體的形狀或大小亦無特別限制,例如可成 66 323724 201230083 形為薄片狀或薄膜狀,或是成形為直方體狀等具有厚度的 形狀,例如為塊狀。 成形為薄片狀或薄膜狀時,可藉由將上述成形材料塗 佈於薄片狀或薄膜狀的基體上而容易得到。該方法的量產 性佳,故較佳。 當成形為薄片狀或薄膜狀時,例如當成形材料的黏度 為10Pa · S以下時,可使用刮刀塗佈法、棒塗佈法等。此 外,當成形材料的黏度超過l〇Pa · S時,可使用模具塗佈 法等。此外,當成形為具有厚度的形狀時,例如可列舉使 成形材料流入於任意形狀的模具之方法等。 在僅使成形材料成形為薄片狀、薄膜狀或是成形為直 方體狀等之狀態下,平板狀磁性體粒子有時會分別朝向不 規則方向而使定向不足。 因此,對該成形為薄片狀、薄膜狀或是成形為直方體 狀等成形體施加磁場,使成形體中的平板狀磁性體粒子往 单向定向。 &lt;定向步驟&gt; 第4複合磁性體的定向步驟,與上述第3複合磁性體 中所記載之定向步驟相同。 &lt;乾燥/硬化步驟&gt; 將藉由上述定向步驟而使平板狀磁性體粒子定向後 之成形體進行乾燥/硬化而形成複合磁性體之步驟。 該乾燥/硬化步驟,係與上述第3複合磁性體的乾燥/ 硬化步驟相同。 67 323724 201230083 &lt;模壓步驟&gt; 當欲更降低上述乾燥步驟中所得之成形體的氣孔率 時,較佳係在上述乾燥步驟後,進行對此成形體施以楔壓 之步驟。模壓裝置可適當地使用一般所知者。 以模壓裝置對成形體施加壓力時,為了有效地減少氣 孔,較佳是在樹脂的軟化溫度以上且硬化起始溫度以下施 加壓力。 模壓時的壓力可適當地調整,較佳係施加5仙&amp;至 20MPa左右的壓力。 藉由上述方法,可製得本實施形態之複合磁性體。 [天線] 本實施形態之天線,具備上述第丨至第4中的任〜 複合磁性體。 該天線的一項形態,為安裝有上述複合磁性體 線。 天 將上述複合磁性體安裝於該天線之方法並無特別限制 可藉由-般所知的方法而安|,將上述複合磁性體被覆於 構成天線之銅線等導體(以下稱為「天線導體」)。 、 天線的麵或形狀並無特別限制,可適當地使用單極 天線、環形天線、螺形天線(helical她麵)、平板天線 (Patch antenna)、F形天線、L·形天線等。此外,亦可為 了使天線達到更小型化而與匹配電路併用。 例如,單極天線或L形天線,係以天線導體為中心, 將上述複合磁性體加工成棒狀或長條板狀並予以爽持天線 323724 68 201230083 導體而形成而得。 此外’螺形天線,可在將上述複合磁性體加工成棒狀 之棒狀複合磁性體的周圍以由銅線等所構成之長條且極細 之天線導體捲繞成線圈狀而得。 此等天線中,可藉由波長縮短效果而得到長度較期望 波長的1/4更短之小型天線。 第8圖係顯示本實施形態之天線的一例之單極天線的 供電方法之示意圖,該單極天線61係具備:棒狀天線導體 62、以及藉由埋入該天線導體62而被覆其表面之板狀複合 磁性體63。 該單極天線61,係經由同軸連接器等而連接於由既定 形狀的導體所構成之底板64,並以將該同軸連接器等作為 内導體的連接部65用作為供電點之方式連接有交流信號 發送機66。 其他種類及形狀之天線的供電方法亦與上述相同,天 線經由連接器等連接於底板64,並以將該連接部65用作 為供電點之方式連接有交流信號發送機66。該成為供電點 之連接。卩65與底板,係呈現電絕緣。 [通信裝置] 本實施形癌之通信裝置係具備上述天線。 該通#衷置’只要是經由電磁波來進行各種資訊的接 收傳送、及接收傳送中的任一項之裝置即可,並無特別 ,疋:例如可列舉4個人電腦、行動電話、㈣式資訊終 端、智慧型手機等多功能攜帶式資訊終端,PDA(Personal 69 323724 201230083The mixing ratio of the first resin and the second resin is preferably 5% by mass or more and 3% by mass or less based on the total mass of the first resin and the second resin. When the second resin is mixed in the second resin in the above range, when the composite magnetic material is molded on the substrate, the stretchability and flexibility of the workable base material are excellent. It is preferred to the composite magnetic body. [Method for Producing Fourth Composite Magnetic Body] Next, a method for producing the fourth composite magnetic body will be described. In the second method of producing the third composite magnetic material, the first resin having a cyclic structure and having a functional group polymerized in a monomer unit is used as the insulating material in the second step of the third method of producing the third composite magnetic material. In addition, the second resin which is a resin which imparts flexibility to the first resin is formed to form a molding material, and other methods for producing the third composite magnetic body are completely the same. 323724 63 201230083 &lt;Production step of molding material&gt; In this step, the first resin having a cyclic structure and having a functional group polymerized in a monomer unit is mixed, and flexibility is imparted to the second resin. A step of preparing a molding material from the second resin, the flat magnetic particles, the solvent, and the curing agent required. The composition, shape, characteristics, production method, and the like of the first resin, the second resin, and the flat magnetic particles are described, and thus the description thereof is omitted. Further, the first resin and the second resin can be synthesized by a generally known method, and a commercially available product can also be used. In addition, the commercial product of the second resin is preferably the product name "Adeka Resin EP-4000" (manufactured by Adeka Co., Ltd. (p+q=2 in the above chemical formula (5)), and the product name "Rikaresin BPO-20E" (new Manufactured by Nippon Physicochemical Co., Ltd. (p+q=2 in the above chemical formula (5)), and the product name "Rikaresin BPO-60E" (manufactured by Nippon Chemical and Chemical Co., Ltd. (n+m=6 in the above chemical formula (6)) The type and amount of the curing agent when the first resin and the second resin are used can be appropriately adjusted depending on the type and amount of the resin to be used. When a resin is used as the resin, oxygen is promoted. From the viewpoint of the condensation reaction of each other and the mechanical strength of the molded body of the composite magnetic body, a tertiary amine is preferred. The tertiary amine may, for example, be 1-isobutyl-2-indenyl or oxime.节基-2-methylmi-sit, 1-cyanoethyl-2-indenyl sulphate, sulphate, sulphate, sulphate, etc. Considering the condensation reaction that promotes the functional group, 323724 64 201230083 The total mass of the resin and the hardener is 〇.5% by mass. In addition, in view of the fact that the flat-shaped hybrid body is used to enhance the entanglement of the composite body, it is preferable that the modifier is a hardening agent having a cyclic structure in the main chain. Examples of the hardening agent having a cyclic structure include a curing agent, a curing agent, a xylQk type curing agent, and a dicyclopentadiene type curing agent. The force is weaker than that of the tertiary amine, and is preferably added in an amount equivalent to that of the resin. The agent is the same as those listed in the third composite magnetic material. The content ratio of the magnetic particles is such that the volume VI of the first resin and the volume V2 of the second resin and the volume V3 of the curing agent and the flat magnetic particles are solidified when they are solidified with respect to the volatile component in the molding material. The sum of the volumes V4 (BV1+V2+V3+V4) is preferably 10% by volume or more and 60% by volume or less, and more preferably 30% by volume or more and 50% by volume or less. Here, the content of the flat magnetic particles is When the volume is less than 1% by volume, the amount of flat magnetic particles is too small, so that it is compounded. When the magnetic properties of the magnetic material are lowered, the content of the flat magnetic particles is more than 60% by volume. When the content of the flat magnetic particles is too large, the flat magnetic particles are excessively contained, and the flat magnetic particles and the resin are hardened. Since the fluidity of the molding material of the solvent and the solvent is lowered, when the molded body is formed by the molding material, the orientation of the flat magnetic particles is less likely to occur, and as a result, the composite magnetic body is flat 65 323724 201230083 plate-shaped magnetic body It is not preferable that the orientation of the particles is lowered. The flat magnetic particles, the first resin, the second resin, the curing agent, and the solvent are mixed to form a molding material. At this time, the viscosity of the molding material can be adjusted by appropriately adjusting the amount of addition of the solvent. The mixing device is the same as those listed in the above first composite magnetic body. The viscosity of the obtained molding material is preferably 0. IPa · S or more and 106 Pa · S or less, and more preferably 0.3 Pa · S or more and 104 Pa · S or less. Here, when the viscosity is less than 0. IPa · S, the fluidity becomes too large to deteriorate the productivity of the drying step, which is not preferable. On the other hand, when the viscosity exceeds 106 Pa · S, the viscosity is too high and it is difficult. When the orientation of the flat magnetic particles is performed, the orientation of the flat magnetic particles in the composite magnetic material is lowered, which is not preferable. In this manner, the content of the flat magnetic particles in the molding material is 10% by volume or more and 60% by volume or less, and the viscosity of the molding material is set to 0. IPa · S or more and 106 Pa · S or less. A composite magnetic body in which the mechanical strength of the molded body is balanced with #r' is obtained. &lt;Forming Step&gt; This is a step of forming the molding material obtained in the above step into a predetermined shape. The molding method is not particularly limited as long as it can form a molding material into a constant shape and can maintain a constant shape when a magnetic field is applied after molding. Further, the shape or size of the molded body is not particularly limited. For example, it may be in the form of a sheet or a film, or may be formed into a rectangular shape such as a rectangular shape, for example, in a block shape. When it is formed into a sheet shape or a film shape, it can be easily obtained by coating the above-mentioned molding material on a sheet-like or film-like substrate. This method is preferred because of its good mass productivity. When it is formed into a sheet shape or a film shape, for example, when the viscosity of the molding material is 10 Pa·s or less, a doctor blade coating method, a bar coating method, or the like can be used. Further, when the viscosity of the molding material exceeds 10 ÅPa · S, a die coating method or the like can be used. Further, when it is formed into a shape having a thickness, for example, a method of causing a molding material to flow into a mold of an arbitrary shape or the like is exemplified. In a state where only the molding material is formed into a sheet shape, a film shape, or a rectangular shape, the flat magnetic particles may be oriented in an irregular direction and may be insufficiently oriented. Therefore, a magnetic field is applied to the molded body formed into a sheet shape, a film shape, or a rectangular parallelepiped shape, and the flat magnetic particles in the molded body are oriented in one direction. &lt;Orientation Step&gt; The orientation step of the fourth composite magnetic body is the same as the orientation step described in the above third composite magnetic body. &lt;Drying/hardening step&gt; The step of drying/hardening the molded body obtained by orienting the flat magnetic particles by the above-described orientation step to form a composite magnetic body. This drying/hardening step is the same as the drying/hardening step of the above third composite magnetic body. 67 323724 201230083 &lt;Molding step&gt; When it is desired to further reduce the porosity of the formed body obtained in the above drying step, it is preferred to carry out a step of applying a wedge pressure to the formed body after the drying step. The molding device can be suitably used as generally known. When pressure is applied to the molded body by the press device, in order to effectively reduce the pores, it is preferred to apply a pressure above the softening temperature of the resin and below the hardening start temperature. The pressure at the time of molding can be appropriately adjusted, and it is preferred to apply a pressure of about 5 sen &amp; to about 20 MPa. The composite magnetic body of the present embodiment can be obtained by the above method. [Antenna] The antenna of the present embodiment includes any of the above-described composite magnetic bodies of the fourth to fourth. One form of the antenna is to mount the above composite magnetic body wire. The method of attaching the composite magnetic body to the antenna is not particularly limited, and the composite magnetic body is coated on a conductor such as a copper wire constituting an antenna (hereinafter referred to as an "antenna conductor"). "). The surface or shape of the antenna is not particularly limited, and a monopole antenna, a loop antenna, a helical antenna (helical her face), a patch antenna, an F-shaped antenna, an L-shaped antenna, or the like can be suitably used. Further, it is also possible to use the matching circuit in order to make the antenna smaller. For example, a monopole antenna or an L-shaped antenna is formed by processing the composite magnetic body into a rod shape or a long strip shape centering on the antenna conductor and holding the antenna 323724 68 201230083 conductor. Further, the 'stud antenna' can be obtained by winding a long and extremely thin antenna conductor made of a copper wire or the like around the rod-shaped composite magnetic body in which the composite magnetic body is processed into a rod shape. Among these antennas, a small antenna having a length shorter than 1/4 of a desired wavelength can be obtained by the wavelength shortening effect. Fig. 8 is a view showing a power supply method of a monopole antenna which is an example of an antenna according to the present embodiment, and the monopole antenna 61 includes a rod antenna conductor 62 and a surface covered by the antenna conductor 62. A plate-like composite magnetic body 63. The monopole antenna 61 is connected to a bottom plate 64 made of a conductor having a predetermined shape via a coaxial connector or the like, and is connected to the ground by a connection portion 65 having the coaxial connector or the like as an internal conductor. Signal transmitter 66. The power supply method of the antenna of other types and shapes is also the same as described above, and the antenna is connected to the bottom plate 64 via a connector or the like, and the AC signal transmitter 66 is connected by using the connection portion 65 as a power supply point. This becomes the connection of the power supply point. The 卩65 and the bottom plate are electrically insulated. [Communication device] The communication device of the present invention has the antenna described above. It is not particularly limited as long as it is a device for receiving and transmitting various kinds of information via electromagnetic waves, and receiving and transmitting it. For example, four personal computers, mobile phones, and (four) information can be cited. Multi-functional portable information terminal such as terminal and smart phone, PDA (Personal 69 323724 201230083

Digital Assistant ;個人數位助理)等通信設備,音訊設 備(audio equipment)、視訊設備、攝像設備等各種電子設 備等。 本實施形態之通信裝置中,除了上述各種設備之外, 亦包含安裝有將上述天線設置在此等各種設備中所隨附之 保護蓋等各種附件(輔助用具)的辅助天線之通信裝置。 此等通信裝置中,上述天線可設置在通信裝置的外部 或是内藏於通信裝置,任一種均可。 在此’係以將行動電話用作為通信裝置者為例,來說 明上述天線的各種安裝方式。 第9圖係顯示本實施形態之通信裝置的一種之行動電 話的一例之斜視圖,該行動電話71,係在框體72的前面 設置有由液晶顯示器或有機電激發光顯示器等所構成之具 有顯示功能的顯示部73,在該顯示部73的内面側設置有 底板(圖式省略)’並經由連接器等將配設在棒狀單極天線 74内之天線導體75連接於該底板,經由該連接部而連接 有行動電話71的電子電路(圖式省略)。該單極天線74的 天線導體75是由複合磁性體76所被覆。 該單極天線74,可從框體72取出或容納於框體^, 通信時,可因應必要從框體72拉“進行通信,未通信 時,可塞入於框體72而容納。 該單極天線74不4須為棒狀,可伸縮自如。 該單極天線74,考量到提升天線增益 不與顯示部73等重疊之位置。再者,當將單極天1㈣ 323724 70 201230083 •置在與顯示部73等重疊之位置時,該單極天線74與顯示 部73之間,較佳係空出間隔。 第1〇圖係顯示本實施形態之通信裝置的一種之行動 電=的其他一例之斜視圖,該行動電話8卜係在框體82 的刖面叹置有由液晶顯示器或有機電激發光顯示器等所構 ^之具有顯示功能的顯示部⑽,於側面設置有外部天線用 端子84,。又置在棒狀單極天線85的侧面之連接端子祁被 嵌入於》亥外部天線用端子84,配設在該單極天線Μ内之 天線導體87,經由連接端子86及外部天線用端子84而連 接於在顯示部83的内面側上所設置之底板(圖式省略),經 由,連接部而連接有行動電話81的電子電路(圖式省略)。 。單極天線85的天線導體87是由複合磁性體88所被覆。 該行動電話81中,藉由將單極天線85的連接端子86 插入於外部天線用端子84或從外部天線用端子以卸 而可裝著及卸下。 第11圖係顯示本實施形態之通信裝置的一種之行動 電話的另外-例之部分斜視圖,該行動電話91,係在框體 92的前面之由液晶顯示器或有機電激發光顯示器等所構 成之具有顯示功能的顯示部⑽式省略)的背面側設置有底 板93’在未與該底板93重叠之位置(第^圖中為底板卯 的上方)上設置有L形天線94,配設在該L形天線%内且 由銅線等導體所構成之天線導體95,係經由連接器等連接 於底板93,並經由該連接部而連接有行動電話91的電子 電路(圖式省略)。該L形天線94的天線導體95是由複合 323724 71 201230083 磁性體9 6所被覆。 第12圖係顯示本實施形態之通信裝置的一種之行動 電話的另外一例之部分斜視圖,該行動電話101,係在框 體102的前面之由液晶顯示器或有機電激發光顯示器等所 構成之具有顯示功能的顯示部(圖式省略)的背面側設置有 底板103,在未與該底板103重疊之位置(第12圖中為底 板103的上方)上設置有螺形天線1〇4,該螺形天線中 捲繞於棒狀複合磁性體105之螺旋狀天線導體1〇6,係經 由連接器等連接於底板1〇3,並經由該連接部而連接有行 動電話101的電子電路(圖式省略)。 忒螺形天線1〇4,係以捲取棒狀複合磁性體1〇5之方 式,將由銅線等導體所構成之天線導體1〇6捲繞成螺旋狀。 第13圖係顯示本實施形態之通信裝置的一種之附有 保護蓋的行動電話的一例之斜視圖,該附有保護蓋的行動 電話ill,是由行動電話112及裝著於該行動電話112之 附件的一種之保護蓋113所構成。該行動電話112,係在 框體114的前面設置有由液晶顯示器或有機電激發光顯示 态等所構成之具有顯示功能的顯示部115,該框體114之 一邊的側面上,設置有連接於在顯示部115的内面側上所 设置之底板(圖式省略)之外部天線用端子116。 另一方面,保護蓋113是由具有柔軟性之樹脂等所構 成並且可變形者,並以覆蓋框體114之扣除顯示部115後 的周緣部及背面之方式所設置,於該保護蓋113之一邊的 侧部,設置有雙極天線121,該雙極天線121是藉由複合 72 323724 201230083 磁性體123來被覆由銅線等導體所構成之天線導體 ㈣雙極天線121’設置有用以將該雙極天線i2i連接於 外部天線用端子116之連接端子ι24。 雙極天線12卜係具備成對的2個單極天線 護蓋nu著於㈣餘112時,較麵餅未與顯示部 15重*之位置。再者’當設置在與顯示部⑴重疊之位 置時,較佳係增加保護蓋113的料,並在保護蓋ιΐ3内 部使雙極天線121與顯示部115之間空出適當的間隔。 該附有保護蓋的行動電話lu,該雙極天線i2i係經 由連接端子124及外紅_料116而連接於在顯示部 115的内面侧上所設置之底板(圖式省略),並經由該連接 部而連接有行動電話的電子電路(圖式省略)。 該附有保護蓋的行動電話lu中,將保護蓋113的連 接端子124插入於行動電話112的外部天線用端子ιΐ6 中,並在簡該狀態下將㈣蓋113覆蓋在行動電話 藉此可將雙極天線121連接於行動電話112。 此外,藉由從行動電話112中卸下保護蓋113,而可 從行動電話112中卸下雙極天線12ι。 第14圖係顯示本實施形態之通信裝置的一種之附有 保濩蓋的行動電話的其他一例之俯視圖,第15圖為沿著第 圖的A —A線之剖面圖,該附有保護蓋的行動電話131, 是由行動電話132及保護蓋133所構成,該行動電話132, 係在框體134的前面設置有由液晶顯示器或有機電激發光 顯示器等所構成之具有顯示功能的顯示部135,在該框體 323724 73 201230083 134的上面,設置有連接於在顯示部135的内面側上所設 置之底板(圖式省略)之外部天線用端子136。 另一方面,保護蓋133是由具有柔軟性之樹脂等所構 成並且可變形者,並以覆蓋框體134的周緣部及背面之方 式所設置,於該保護蓋133之背面的上部,設置有螵線天 線(spiral antenna)141。該螺線天線141,係藉由複合磁 性體143來被覆構成為螺線狀之天線導體142,於該嫘線 天線141,設置有用以連接於外部天線用端子136之連接 端子144。 該螺線天線141’當將保護蓋133裝著於行動電話132 時,較佳係位於未與顯示部135重疊之位置。再者,當設 置在與顯示部135重疊之位置時,較佳係增加保護蓋133 的厚度’並在保護蓋133内部使螺線天線141與顯示部135 之間空出適當的間隔。 該附有保護蓋的行動電話131,該螺線天線141係經 由連接端子144及外部天線用端子136而連接於在顯示部 135的内面侧上所設置之底板(圖式省略),並經由該連接 部而連接有行動電話的電子電路(圖式省略)。 該附有保護蓋的行動電話131中,將保護蓋133的連 接端子144插入於行動電話132的外部天線用端子136 中’並在保持該狀態下將保護蓋133覆蓋在行動電話132, 藉此可將螺線天線141連接於行動電話132。 此外’藉由從行動電話132令卸下保護蓋133,而可 從行動電話132中卸下螺線天線141。 323724 201230083Communication equipment such as Digital Assistant; personal digital assistant, various electronic equipment such as audio equipment, video equipment, and video equipment. In addition to the various devices described above, the communication device of the present embodiment includes a communication device in which an auxiliary antenna such as a protective cover or the like which is provided in various devices such as the above-described antenna is mounted. In these communication devices, the antenna may be provided outside the communication device or may be incorporated in the communication device. Here, the use of a mobile phone as a communication device is taken as an example to illustrate various mounting methods of the antenna described above. FIG. 9 is a perspective view showing an example of a mobile phone according to the communication device of the present embodiment. The mobile phone 71 is provided with a liquid crystal display, an organic electroluminescence display or the like provided on the front surface of the casing 72. The display unit 73 of the display function is provided with a bottom plate (not shown) on the inner surface side of the display unit 73, and the antenna conductor 75 disposed in the rod-shaped monopole antenna 74 is connected to the bottom plate via a connector or the like. An electronic circuit (not shown) of the mobile phone 71 is connected to the connection portion. The antenna conductor 75 of the monopole antenna 74 is covered by a composite magnetic body 76. The monopole antenna 74 can be taken out from the housing 72 or housed in the housing. When communicating, it is necessary to pull the communication from the housing 72 as needed. When the communication is not performed, the monopole antenna 74 can be inserted into the housing 72 and accommodated. The pole antenna 74 is not required to be rod-shaped and is retractable. The monopole antenna 74 is considered to have a position where the boost antenna gain does not overlap with the display portion 73. Further, when the monopole day 1 (four) 323724 70 201230083 is placed When the position is overlapped with the display unit 73 or the like, it is preferable that the monopole antenna 74 and the display unit 73 are spaced apart from each other. Fig. 1 is a view showing another example of the action power of the communication device of the present embodiment. In the oblique view, the mobile phone 8 is provided with a display unit (10) having a display function constituted by a liquid crystal display or an organic electroluminescence display or the like, and a terminal for external antenna is provided on the side surface of the frame 82. 84. The connection terminal 置 placed on the side of the rod-shaped monopole antenna 85 is embedded in the external antenna terminal 84, and the antenna conductor 87 disposed in the monopole antenna is connected via the connection terminal 86 and the external antenna. Connected to the display portion 83 by the terminal 84 The bottom plate provided on the front side (omitted from the drawing) is connected to the electronic circuit of the mobile phone 81 via the connection portion (the drawing is omitted). The antenna conductor 87 of the monopole antenna 85 is covered by the composite magnetic body 88. In the mobile phone 81, the connection terminal 86 of the monopole antenna 85 is inserted into or removed from the external antenna terminal 84. Fig. 11 shows the communication of the present embodiment. Another embodiment of a mobile phone of the device, the mobile phone 91 is a display portion (10) having a display function constituted by a liquid crystal display or an organic electroluminescence display or the like in front of the casing 92. The back side of the back side is provided with a bottom plate 93' disposed at a position that is not overlapped with the bottom plate 93 (above the bottom plate 第 in the figure), and an L-shaped antenna 94 is disposed in the L-shaped antenna % and is provided by the copper wire The antenna conductor 95 composed of an equal conductor is connected to the bottom plate 93 via a connector or the like, and an electronic circuit (not shown) of the mobile phone 91 is connected via the connection portion. The antenna conductor 95 of the L-shaped antenna 94 is composed of Compound 32 3724 71 201230083 The magnetic body 9.6 is covered. Fig. 12 is a partial perspective view showing another example of a mobile phone of the communication device of the embodiment, the mobile phone 101 being in front of the casing 102 by a liquid crystal display The bottom surface side of the display portion (not shown) having a display function constituted by an organic electroluminescence display or the like is provided with a bottom plate 103, and is not overlapped with the bottom plate 103 (above the bottom plate 103 in Fig. 12). A helical antenna 1〇4 is provided in which the helical antenna conductor 1〇6 wound around the rod-shaped composite magnetic body 105 is connected to the bottom plate 1〇3 via a connector or the like, and is connected via the connection portion. An electronic circuit (illustration omitted) to which the mobile phone 101 is connected. The spiral antenna 1〇4 is formed by winding a rod-shaped composite magnetic body 1〇5, and winding an antenna conductor 1〇6 made of a conductor such as a copper wire into a spiral shape. Fig. 13 is a perspective view showing an example of a mobile phone with a protective cover of a communication device of the present embodiment, the mobile phone ill with a protective cover attached to the mobile phone 112 and the mobile phone 112. A protective cover 113 of one of the attachments is constructed. The mobile phone 112 is provided with a display unit 115 having a display function, such as a liquid crystal display or an organic electroluminescence display state, on the front surface of the housing 114. The side surface of one side of the housing 114 is provided with a connection. An external antenna terminal 116 (not shown) provided on the inner surface side of the display unit 115. On the other hand, the protective cover 113 is made of a flexible resin or the like and is deformable, and is provided so as to cover the peripheral portion and the back surface of the casing 114 after the display portion 115 is removed, and the protective cover 113 is provided. On one side, a dipole antenna 121 is provided. The dipole antenna 121 is covered with a conductor such as a copper wire by a composite 72 323724 201230083 magnetic body 123. The dipole antenna 121 ′ is provided to The dipole antenna i2i is connected to the connection terminal ι24 of the external antenna terminal 116. The dipole antenna 12 is provided with a pair of two monopole antennas. When the cover nu is at (iv) 112, the face cake is not at the position of the display portion 15. Further, when it is disposed at a position overlapping the display portion (1), it is preferable to increase the material of the protective cover 113, and to provide an appropriate space between the dipole antenna 121 and the display portion 115 inside the protective cover ι3. The mobile phone with the protective cover, the bipolar antenna i2i is connected to the bottom plate (not shown) provided on the inner surface side of the display unit 115 via the connection terminal 124 and the outer red material 116. An electronic circuit (not shown) for connecting a mobile phone to the connection unit. In the mobile phone lu with the protective cover, the connection terminal 124 of the protective cover 113 is inserted into the external antenna terminal ΐ6 of the mobile phone 112, and the (four) cover 113 is covered in the mobile phone in this state. The dipole antenna 121 is connected to the mobile phone 112. Further, the dipole antenna 12i can be removed from the mobile phone 112 by removing the protective cover 113 from the mobile phone 112. Fig. 14 is a plan view showing another example of a mobile phone with a cover provided in the communication device of the embodiment, and Fig. 15 is a cross-sectional view taken along line A-A of the figure, with a protective cover The mobile phone 131 is composed of a mobile phone 132 and a protective cover 133. The mobile phone 132 is provided with a display unit having a display function including a liquid crystal display or an organic electroluminescence display or the like on the front surface of the casing 134. 135. On the upper surface of the casing 323724 73 201230083 134, an external antenna terminal 136 connected to a bottom plate (not shown) provided on the inner surface side of the display unit 135 is provided. On the other hand, the protective cover 133 is made of a flexible resin or the like and is deformable so as to cover the peripheral portion and the back surface of the casing 134, and is provided on the upper portion of the back surface of the protective cover 133. A spiral antenna 141. The helical antenna 141 is covered with a helical antenna conductor 142 by a composite magnetic body 143, and a connection terminal 144 for connecting to the external antenna terminal 136 is provided in the twisted antenna 141. When the protective cover 133 is attached to the mobile phone 132, the helical antenna 141' is preferably located at a position that does not overlap the display portion 135. Further, when it is disposed at a position overlapping the display portion 135, it is preferable to increase the thickness ' of the protective cover 133' and to provide an appropriate space between the spiral antenna 141 and the display portion 135 inside the protective cover 133. The mobile phone 131 with the protective cover is connected to the bottom plate (not shown) provided on the inner surface side of the display unit 135 via the connection terminal 144 and the external antenna terminal 136, and is connected thereto. An electronic circuit (not shown) for connecting a mobile phone to the connection unit. In the mobile phone 131 with the protective cover, the connection terminal 144 of the protective cover 133 is inserted into the external antenna terminal 136 of the mobile phone 132, and the protective cover 133 is covered on the mobile phone 132 while being held therein. The helical antenna 141 can be connected to the mobile phone 132. Further, the helical antenna 141 can be detached from the mobile phone 132 by removing the protective cover 133 from the mobile phone 132. 323724 201230083

各例,由於所裝載之單極天線74、單極天線 94、螺形天線104、雙極天線121及螺線天 製’故可將天線配置在行動電話内的狹小空 到電磁波不會被天線以外的零件所阻隔之天 動電話。 框體内區域下 性能。 L极天線121及螺線天線141由於可設置在如 133般之附件内,所以可在不佔有行動電話的 將輔助天線設置在行動電話而提升天線的 根據本實施形態之複合磁性體,由於將平板狀磁性體 粒子的平均厚度設為〇.〇1/iin以上〇.5em以下,平均長徑 設為0.05am以上10/zm以下,且平均長寬比(長徑/厚度) 設為5以上’故可使70MHz至5〇〇MHz的頻率波段之複磁導 率的實部er,大於1,且損耗正切tan(5 #為〇.丨以下因 此可大幅提高該頻率波段之波長的縮短率。 因此,若將該複合磁性體應用在VHF波段的天線,則 可防止該複合磁性體表面之渦電流的產生,防止複磁導率 的實部yr’的降低,而可更進一步達成天線的小型化。 根據本實施形態之複合磁性體的製造方法,係具備 有·將使平均粒徑〇. 5# in以下的球狀磁性粒子分散於含有 界面活性劑之溶液中而成之漿液及分散介f,填充於可密 閉的容器内,以使前述漿液及前述分散介質的合計體積量 與前述容器内的體積成為相JS],在密閉狀態下將該衆液與 前述分散介質一同擾拌,使前述球狀磁性粒子彼此變形及 323724 75 201230083 熔著而形成平板狀磁性體粒子之第1步驟;使前述平板狀 磁性體粒子分散並混合於在溶劑中溶解有絕緣材料之溶液 中而形成成形材料之第2步驟;以及包含有:將前述成形 材料成形或塗佈於基材上而得到成形體之成形步驟、及使 前述成形體乾燥/硬化之乾燥/硬化步驟之第3步驟,因此, 可容易地製作出70MHz至500MHz的頻率波段之複磁導率的 實部yr’大,且複磁導率的損耗正切tan5 &quot;為0. 1以下 之複合磁性體。 此外’根據將本實施形態之複合磁性體的氣孔率設為 20%以下時之複合磁性體,可提升複磁導率的實部,之 值,並且使複介電常數的實部er,之值幾乎不變。因此, 可使應用該複合磁性體之電子零件或電子設備達成小型 化,並可抑制阻抗匹配所造成之電力損耗。 此外’當將70MHz至500MHZ之複磁導率的損耗正切 tan&lt;5/z设為0.05以下,複介電常數的損耗正切tan(j ε 設為0. 1以下時,可提升電子零件或電子設備的增益。 此外,根據含有主鍵具有環狀結構且具有以單體單位 所聚合之g肖b基之第1樹脂作為絕緣材料之複合磁性體, 可減少由樹脂所形成之立體障礙對平板狀磁性體粒子所造 成的影響。因此’可提供-種複磁導率的實部〆高且機 械強度佳之複合磁性體。 並且由於使用具有以單體單位所聚合之官能基之樹 脂,可使樹脂的鍵結變得堅固,而可具有使用作為電子零 件等之成形體的充分機械強度。 323724 76 201230083 根據本實施形態之複合磁性體的製造方法,由於且備 有:混合主鍵具有環狀結構且具有以單體單位所聚合^官 能基之樹脂、平板狀磁性體粒子、溶劑、以及因應必要之 硬化劑,㈣到成形材料之步驟;對該成形材料施加磁場 以使平板狀磁性錄子定向之步驟;以及將使平板狀磁性 體粒子疋向後之成形體進行乾燥/硬化之步驟,所以可容易 地製作出複磁導率的實部以r ’高且機械強度佳之複合磁性 體。 再者,藉由對塗佈膜施加1次或複數次的磁場,可提 升塗佈膜中之平板狀磁性體粒子的定向性。 此外,根據含有下述者之複合磁性體:主鏈具有環狀 結構且具有以單體單位所聚合之官能基之第丨樹脂作為絕 緣材料、以及對該第丨樹脂賦予可撓性之第2樹脂,可減 J由樹脂所形成之立體障礙對平板狀磁性體粒子所造成的 影響,提高平板狀磁性體粒子對於單向之定向性,而提高 !ΐτ’。 此外,由於第2樹脂對第1樹脂賦予可撓性,所以可 提升複合磁性體本身的可撓性及伸縮性。 因此,可提供一種yr’高且機械強度佳,具有可捲取 於輥般之程度的柔軟性,且生產性佳之複合磁性體。 並且由於使用具有以單體單位所聚合之官能基之第1 樹脂,可使樹脂的鍵結變得堅固,而可具有使用作為電子 零件等之成形體的充分機械強度。 再者,即使是微米等級或奈米等級的大小,亦具有可 77 323724 201230083 撓性及伸縮性,所以榭 此的間隙,而減少成:易進入於平板狀磁性體粒子彼 的氣孔。 ·、、' 降低的原因之複合磁性體中 此外,藉由併用笫】 樹脂所形成之立體障礙,因::第2樹脂’可減缓由第1 平板狀磁性體粒子間所產 I減少樹脂 '樹脂間成樹脂- 土〈氣孔。 藉此,可提供一種且古古 , 根據本實施形態之複合:二之複合磁性體。 有:混合主鏈具有環狀結構 的!造方法,由於具備 能基之第1 旨、對該第二以單體單位所聚合之官 平板狀磁性體粒子、以及飞勢可撓性之第2樹脂、 該成形材料成形為既定形:製作成形材料之步驟;將 施加磁場以使成形體中之 ^步驟,對所得之成形體 定向步驟;以及將定板狀磁性體粒子往單向定向之 &quot; °後之成形體進行乾燥/輝介夕於鹿/ 硬化步驟,所以可容易地製作出進二餘/硬化之她/ 軟且生產性佳之複合磁性體。&quot;…機械強度佳’柔 再者,藉由對塗佈膜施加丨 升塗佈膜中之平板狀磁性體粒子人的磁% ’可提 灯’高之複合磁性體。+^向性°因此可製造出 根據本實施形態之天線’由於安裝本實施形態之複合 體,來接收、傳送、或接收傳送7〇MHz至5〇_z的頻 率波段之電磁波,故可達成天線進—步的小型化。亦即, 藉由波長縮短效果’可得到長度―望波長的1/4更短 小型天線。 323724 78 201230083 再者,當具備本實施形態之氣孔率20%以下之複合磁 性體時,在70MHz至500MHz的頻率波段中,可得到複磁導 率的實部為7以上,複介電常數的實部εΓ,為15以 上,且(Vr’ . ε r,)—1/2為 〇. 1 以下,(//r,/ £ Γ,)1/2為 〇 5 以上1以下之性能。 因此,藉由波長縮短效果,可提供一種達到長度較期 望波長的1/4更短之小型,抑制阻抗匹配所造成之電力損 耗,且發射效率高之天線。因此,即使是如多媒體廣播般 之VHF波段之波長較長的電磁波,亦可藉由波長縮短效 果,而提供一種能夠以行動電話的框體大小來進行接收之 小型天線。 根據本實施形態之通信裝置,由於具備本實施形態之 小型天線,所以將天線配置在不易受到阻斷電波之其他電 子設備的影響之場所的自由度高,而可得到能夠良^地接 收傳送之小型通信裝置。 [單極天線] 第16圖Α係顯示本發明之一實施形態之單極天線的 示意圖(斜視圖),第16圖B為沿著第16圖人的A —a線之 位置上的剖面圖。 本實施形態之單極天線1620 ’係具有:棒狀天線導體 1622以及被覆在天線導體1622的表面之本實施形態之複 合磁性體1621。本實施形態中,如第16圖B所示:係於 圓柱狀天線導冑1622的周面形成有剖面呈正方形狀的複 合磁性體1621,而使全體呈四角柱狀之單極天線。單極天 323724 79 201230083 線^20 ’典型如第16圖a所示,係經由連接器等連接於 既疋尺寸之導體底板1624的中央,並以該連接部1626作 為供電點而連接於交流信號發送機丨625。 單極天線1620中所使用之天線導體1622的形狀並無 特別限定,可使用直線狀的桿天線、鞭形天線或是曲線 狀的螺形天線、曲折(meander)形天線等一般所知的形狀。 此等當中,就不易在天線導體間產生靜電電容而可得到高 天線增益之觀點來看,較佳為直線狀天線。 门 再者,本實施形態之「直線狀」,係意味著天線的共 振部為正直之棒狀或板狀。因此,直線狀單極天線162〇 的形狀,不僅是通常的角柱狀,亦可為角柱狀或細長平板 狀。此外’關於成為芯材之天線導體1622亦相同,可為圓 柱狀、角柱狀、及平板狀的任一種。 天線導體1622較佳係使用導電性金屬或合金。此般 金屬,例如可列舉出銅(Cu)、銀(Ag)、鎳(Ni)、鉑(pt)、 金(Au)等’合金較佳係選自此等中之2種以上金屬的合金。 天線導體1622的剖面形狀’只要是可裝载於攜帶式 終端之大小的程度即可,並無特別限定,例如可形成為直 棱D為0· 5mm至2min左右之方形或圓形的剖面形狀。 再者’由於160MHz至222MHz的電波會在導電體表面 流通,故將天線導體1622構成為表面積大之帶(tape)狀者 亦為有效。帶狀天線導體1622,較佳係其寬度為〇.5min至 2_ ’ 厚度為 0.05 至 0.2mm» 天線導體1622的長度L,只要是可容易裝載於攜帶式 80 323724 201230083 終^程度的長度即可,並無特別Μ,較佳為4g丽以上 __ π ϋ 以下。藉由將長度l 設定在上述範圍’而可容易裝载於攜帶式終端,並可構成 為_在16_2至2·ζ的_波段中 1620。 &lt;複合磁性體&gt; 本實施形態之複合磁性體1621,可使用上述複合磁性 體的任一個。 複合磁性體1621,該160MHz至222MHz的頻率波段之 複磁導率的實部# r’較佳為3以上,更佳為6以上。 若複合磁性體1621之複磁導率的實部#『,為3以 上,則可藉由設為2. 4mm以上的被覆厚度,而可得到即使 使用長度200mm的天線導體1622時,亦可在2〇〇MHz的頻 率引起共振之單極天線1620。 若複合磁性體1621之複磁導率的實部&quot;1&gt;,為6以 上,由於得到更進一步的波長縮短效果,即使將對於天線 導體1622的被覆厚度薄化至1. 2mm,亦可得到使用長度 200mm的天線導體1622而可在200MHz的頻率引起共振之 單極天線1620。 複合磁性體1621的被覆厚度d,過厚時天線變粗,就 攜帶式終端的裝置構成或設計關係上,乃變得難以裝載。 因此,實用上,複合磁性體的被覆厚度d於l〇mm以下之範 圍。 再者,複合磁性體1621與天線導體1622不需密著, 323724 201230083 例如可構成為將天線導體1622配置在圓筒狀複合磁性體 1621的内部,外觀上呈被覆之形態。 本實施形態之複合磁性體1621,160MHz至222MHz的 頻率波段之複磁導率的損耗正切tan5較佳 下。藉一 W〇.〇5以下,可防止二= 222MHz的頻率波段之信號損耗所起因之天線的增益降低。 &lt;單極天線的製造方法&gt; 本實施形態之單極天線1620的製造方法,係具備有: 將球狀磁性粒子加工為平板狀以製作上述平板狀磁性體粒 子之第1轉U前述平板狀磁性體㈣與絕緣材料而 製作成形材料之第2步驟;以及將含有上述平板狀磁性體 粒子之成形材料被覆於天線導體之第3步驟。 以下說明各步驟。 &lt;第1步驟&gt; 步驟,係與上述第j複 1步驟完全相同,故省 製作平板狀磁性體粒子之第i 合磁性體的製造方法中所說明之第 略该說明。 &lt;第2步驟&gt; 接著在》2步財,解板狀雜雜子 2 =射溶解有絕緣材料之溶液中㈣成絲材料。當 緣材料^化時’係成為平板狀魏錄子分散於絕 緣材料中之複合磁性體1621。 制, 323724 82 201230083 恢;氏,用天線時’較佳為機械強度高,吸濕 用聚酿亞胺2 材料,例如可適當地使 環丁歸樹J!旨、^㈣本並%销脂、聚伸苯樹脂、聚苯並 聚㉛樹月匕曰/ _樹月旨、聚石夕氧燒樹脂、環氧樹脂、 -曰樹月曰、氟樹脂、聚烯烴樹脂 =、聚伸笨基_、降莰 = 脂或熱可塑性樹脂。此等樹脂可 使用1種或組合2種以上而使用。 切較佳為機械強度及形狀加工性佳 樹月旨氣_日’此外,熱可塑性樹脂較佳為聚伸笨樹脂、咖 _:當種類和量等’可因應所使用之樹脂的 特別^卜’上述溶劑只要是可溶解上述樹脂者即可,並無 2疋,例如可適當地使用甲醇、乙醇、2H t無 C乙酸乙醋、乙酸丁醋、乳酸乙酿、内二:單 蜒乙酉“旨、丙二醇單乙醚乙酸酯、卜丁 醇早 二醇單甲基賽路蘇)、乙二醇單乙‘ 己二醇單單丁鍵(丁基赛路蘇)、二乙二醇單曱崎… ㈣乙峻等賴,丙酮、丁 _、甲基異丁基_、乙: 鲷、%己酮等酮類,笨、甲苯、 醯 姨趣,二甲基甲酿胺、Ν,Ν-二甲基乙酿基乙酿ς本專芳香 咯啶_等醯胺類,此等溶 ^ ^甲基 以上而使用。 早獨使用1種或處合2種 323724 83 201230083 上述成形材料中之平板狀磁性體粒子的含有率,相對 於成形材料中的揮發成分以外者硬化而成為複合磁性體 1621時之體積,較佳為20體積%以上50體積%以下,尤佳 為30體積%以上40體積%以下。 在此,當平板狀磁性體粒子的含有率未達20體積% 時,平板狀磁性體粒子過少,使複合磁性體1621的磁導率 降低,故不佳,當超過50體積%時,平板狀磁性體粒子過 多,使成形材料的流動性降低,結果使成形材料中之平板 狀磁性體粒子的定向性降低,有時會使複合磁性體1621 的磁導率降低,故不佳。 使平板狀磁性體粒子分散並混合於絕緣材料之方法 並無特別限制,可使用行星研磨機、砂磨機、球磨機等攪 拌裝置。此外,亦可使用加壓捏揉機、雙軸式捏揉機、喷 磨機等捏揉裝置。使用熱可塑性樹脂時,可因應必要進行 加熱。 &lt;第3步驟&gt; 第3步驟中,係將第2步驟中所製作之成形材料塗佈 於天線導體1622的外周面,並使該成形材料硬化而形成複 合磁性體1621。藉此可得本實施形態之單極天線1620。 將成形材料塗佈於天線導體1622而被覆複合磁性體 1621之方法,只要可被覆期望被覆厚度d之複合磁性體 1621的方法即可,無特別限制。 複合磁性體1621的被覆厚度d,係根據天線導體的長 度L及複合磁性體1621的磁導率來決定。複合磁性體1621 84 323724 201230083 的被覆方法,例如可列舉出藉由加熱模墨法、射出成形法、 擠壓成形法’將天線導體體夾持於上述成形材料的内側 並予以成形及硬化㈣覆之方法。再者,使用熱硬化性樹 脂時,較佳是在還原性氣體中或真空中藉由熱處理或加熱 模壓處理使成形材料硬化。 此外,亦可藉由將上述成形材料成形為任意形狀的薄 片狀或薄膜狀者積層複數片以成為期望的被覆厚度,而將 天線導體體夾持而被覆。將成形材料成形為薄片狀或薄 膜狀之成形方法,例如可適當地使用加熱模壓法、到刀愛 佈法、射出成形法等。 此等方法中’就容易使平板狀磁性體粒子在絕緣材料 中定向之觀點來看,較佳是拉伸為平面狀之加轉壓成形 法。為了進行拉伸時的黏度調整,較佳是添加塑化劑或是 進仃平板狀磁性體粒子的表面處理。若心要,較佳是在 1口2維持流動性之狀態下,藉由磁場的定向來進行使不 板狀磁性體粒子定向之處理。 中所板狀磁性體粒子定向之方向,較佳是使天線1620 生之磁場,在平板狀磁性體粒子中通過長距離而得 線導^二步的波長縮短效果者。亦即,較佳敎向為使天 ^ 22^ffl^^^(circumferential direction)^ 平板狀磁性體粒子的長軸大致呈平行。 此外’複合雜體1621 _成時,t必須進行上述 =料的黏度調整時,可使成形材料中所含有之溶劑揮 發並/農縮後再進行成形。 323724 85 201230083 此外’當必須進行平板狀磁性體粒子的定向處理時, 在將天線導體1622夾持於内侧使成形材料成形後,乾燥前 對成形材料施加磁場,使平板狀磁性體粒子定向為使天線 導體1622之圓周方向與平板狀磁性體粒子的長軸大致呈 平行。 如以上所說明般,根據本實施形態之單極天線,藉由 絕緣材料中分散有平板狀磁性體粒子而成之複合磁性體來 被覆天線導體,所以可達成能夠裝載於攜帶式終端之程度 的小型化,而可在160MHz至222MHz的低頻率波段中使用^ 此外,當160MHz至222MHz的頻率波段之複磁導率的 實部為3以上時,藉由將本實施形態之複合磁性體 1621被覆2.4賴以上,即使天線導體為2〇〇mm以下,亦可 在200MHz的頻率下共振。 此外,當160MHz至222MHz的頻率波段之複磁導率的 實部er為6以上時,藉由將本實施形態之複合磁性體 1621被覆l.2mm以上,即使天線導體為2〇〇丽以下,亦可 在200MHz的頻率下共振。 本實施形態之直線狀單極天線162〇,藉由與匹配電路 併用’可達到更加小型化。 (實施例) 以下係藉由實施例及比較例來具體說明本發明,本發 明並不限定於此等實施例。 再者,各例的諸項特性係藉由下列方法進行評估。 (1)平板狀磁性體粒子的觀察 323724 86 201230083 以掃描型電子顯微鏡s_4000(Hitachi High_Tech公 司製)來觀察。 (3) 電磁特性(// r’、# r&quot;、tan 占 #、e r,、ε r',、 tan 6 ε )的測定 以磁導率測疋農置Material Analyzer Ε4991Α型 (Agilent Technologies 公司製),在大氣中室溫(25〇c)t 進行策定。然後根據此等以r,及ε r,來算出(以Γ,· ε r’)’1/2 及(a r,/ ε r’)1/2。 (4) 氣孔率 測定複合磁性體的尺寸及質量’根據此等測定值來算 出實測密度。 另一方面’樹脂的理論密度(与實測密度),係測定僅 有樹脂之硬化體的尺寸及質量,並從此等測定值來算出。 此外,平板狀磁性體粒子的理論密度,係使用從平板狀磁 性體粒子的X射線繞射圖形中所求取之X射線理論密度。 將此等值代入式(4),算出複合磁性體的氣孔率。 [實施例1] 將含有4質量%的辞之平均粒徑0.25//m的Permalloy (商品名稱)磁性粒子200g,混合於溶解有作為界面活性劑 之含氮的接枝聚合物之二曱苯400g及異丙醇400g的混合 液中,而製作出漿液。 接著使用如第2圖所示之循環密閉型且容器體積為5L 之砂磨機Ultra Apex Mill UAM-5(壽工業公司製)作為密 閉容器’將作為分散介質之平均粒徑200 # m的二氧化錘珠 87 323724 201230083 粒投入於該密閉容器内 容器内。在此,係—二 ==密閉 入並進行循環之方式構成配管。 以之為再次投 該狀態下’以使密閉容器内 秒之轉數’攪拌至漿液於密。、、速成為心/ 分鐘為止,而製作出平板狀磁= =使所得之平板狀磁_粒子乾燥並使 =將斜板狀磁性體粒子的既Μ,添加於將環氧樹月1 形份比㈣嶋之樹脂清漆(varnish)中,“ 藉由到刀塗·,騎得之成形㈣朗為硬化後呈 3〇mm見方、厚度100/zra之正方形薄膜。 接著在9(TC、大氣中將該薄膜乾燥1小時而構成乾薄 膜,然後在減壓模壓裝置中進行模壓燒成。模壓條件為常 壓下以20分鐘升溫至130ΐ,其次施加2Mpa的壓力並保 持5分鐘,然後升溫至16〇艺並保持4〇分鐘使樹脂硬化, 而彳于30mm見方、厚度50//m之正方形薄膜狀複合磁性體。 藉由Material Analyzer測定該複合磁性體的複磁導 率’結果為90MHz之複磁導率的實部#r,為13,損耗正切 tan 6 #為0. 02,且220 MHz之複磁導率的實部/zr,為13, 損耗正切tan5 //為0.04。 此外,以掃描型電子顯微鏡(SEM)來觀察該複合磁性 體的形狀,平板狀磁性體粒子50個的平均厚度為〇. 08# m ’平均長徑為〇. 5 // m,平均長寬比為6. 2 5。此外,球狀 88 323724 201230083 磁性粒子或是並非厚度為0. 01 β m以上〇· 5 # m以下’長徑 為0.05&quot;m以上10#m以下,且長寬比為5以上之磁性體 粒子,實質上並未觀查到。 第17圖係顯示該複合磁性體的複磁導率(實部/zr,、 虛部A rn)及損耗正切(tan &lt;5 μ ),第18圖係顯示該複合磁 性體的掃描型電子顯微鏡(SEM)照片。 [比較例1] 將含有4質量%的鋅之平均粒徑〇. 25 Μ 01的Permalloy (商品名稱)磁性粒子20g,混合於溶解有作為界面活性劑 之含氮的接枝聚合物之二曱苯4〇g及異丙醇40g的混合液 中,而製作出漿液。 接著使用如第1圖所示之上部開放塑的砂磨機作為開 放容器,將作為分散介質之平均粒徑200/ΖΠ1的一氧化錯珠 粒投入於該開放容器的器皿(vessel)内,接者才又入上述榮· 液。在此,係以使器皿内之最外周的流速成為l〇m/秒之轉 數授拌30分鐘,而製作出磁性體粒子。 接著使用所得之磁性體粒子’與實施例1進行相同操 作而得到比較例1的薄膜狀複合磁性體。 藉由Material Analyzer測定該複合磁性體的複磁導 率,結果為90MHz之複磁導率的實部//r’為2.6 ’損耗正 切tan &lt;5 &quot;為〇. 〇9,且220 MHz之複磁導率的實部A r’為 2. 8,損粍正切tan (5 #為0.11。 此外,以掃描型電子顯微鏡(SEM)來觀察該複合磁性 體的形狀,磁性體粒子係互相不規則地重疊,得知實質上 89 323724 201230083 存在許多厚度0. 5以m以上者。長徑及長寬比亦不均勻。 第19圖係顯示該複合磁性體的複磁導率(實部er,、 虛部/zr&quot;)及損耗正切(tan 5以),第20圖係顯示該複合磁 性體的掃描型電子顯微鏡(SEM)照片。 [實施例2] 藉由與實施例1相同之方法,製作出12片長250mm、 寬30mm、厚60# m的乾薄膜。 接著積層此等乾薄膜,在第6片與第7片之間夾持直 徑0. 6imn、長250mm的銅線作為天線,然後使用減壓模壓 裝置,在與實施例1相同之條件下進行模壓燒成,而製作 出如第8圖所示之在由長25〇mm、寬3〇mm、厚0. 8mm之乾 薄膜的積層體所構成之複合磁性體63中夾持有由銅線所 構成之天線導體63之單極天線61。 然後將該單極天線61連接於5〇〇mm見方之導體底板 64的中央,藉由交流信號發送機66,以連接部65為供電 點供電50Ω。 在此,測定該單極天線61的共振頻率,此外,為了 比較測疋僅為直徑0. 6mm、長250mm的銅線的共振頻 率〇 其結果為,共振頻率,僅為銅線時為273MHz,相對於 此三安裝有實施例2的複合磁性體之單極天料疆&amp;, 換算為波長之縮短率_ 從該結.果中,得知藉由安 裝本發明之複合磁性體,使丽波段的180MHz之天線長度 達成約34%的小型化。 323724 90 201230083 [實施例3] 將二J哀戊二烯型環氧樹脂EPICLON HP-7200L(DIC股 份有限公司製)、作為硬化劑之相對於環氧樹脂與硬化劑的 全體量為1質量%之1-異丁基曱基咪唑、由相對於樹脂 與硬化劑與平板狀磁性體粒子的全體量為4〇體積%之則75 質量%-Fe20質量%-Zn5質量%之Ni-Fe-Zn合金所構成之平 均長徑2.5#m且平均厚度〇.3/zm且平均長寬比8. 3之平 板狀磁性體粒子、以及相對於平板狀磁性體粒子與樹脂與 硬化劑的合計質量為40質量%之環己酮,投入於行星攪拌 機,混合15分鐘而得到漿液狀成形材料。該成形材料的黏 度為 0. 4Pa · S。 接著藉由棒塗佈機將該成形材料塗佈於聚對苯二曱 酸乙二酯(PET)薄膜上,以使硬化後成為長50mmx寬50mmx 厚0. 1mm之方式進行薄片成形。 薄片成形後,於該薄片的面上,在水平方向上施加900 高斯的磁場6分鐘。其次吹送80°C的暖風以進行風乾。接 著在樹脂的軟化點之ll〇°C下施加l〇MPa的模壓壓力後’ 在16(TC下進行2小時的硬化反應’而得實施例3的複合 磁性體。 第1表係顯示實施例3之複合磁性體的氣孔率以及在 200MHz中藉由Material Analyzer所測得之磁特性的結 果。 此外,第21圖係顯示實施例3的複合磁性體從10MHz 至1GHz之複磁導率的實部及tan6 &quot; ’第22圖係顯 91 323724 201230083 示複介電常數的實部er’及tan 5 ε。 [實施例4] 使用以85:15的質量比來混合二環戊二烯型樹脂與 液狀環氧樹脂Rikaresin ΒΡΟ-20(新日本理化股份有限公 司製)之樹脂’來取代二環戊二烯型樹脂,並且將施加模壓 壓力時的溫度設為l6『c,除此之外,其他依據實施例3 而製得實施例4的複合磁性體。 第1表係顯不實施例4之複合磁性體的氣孔率以及在 200MHz中藉由Material Analyzer所測得之磁特性的結 果。 此外’第23圖係顯示實施例4的複合磁性體從10MHz 至1GHz之複磁導率的實部//r,及tan5 //,第24圖係顯 示複介電常數的實部er,及tan5 ε。 [實施例5] 製得漿液狀的成形材料時,將行星攪拌機的混合時間 從15分鐘改為5分鐘,除此之外,其他依據實施例3而製 得實施例5的複合礤性體。 第1表係顯示該複合磁性體的氣孔率以及在200MHz 中藉由Material Analyzer所測得之磁特性的結果。 [實施例6] 將對成形體進行模壓時的溫度設為16(TC,除此之外, 其他依據實施例3而製得實施例6的複合磁性體。 第1表係顯示該複合磁性體的氣孔率以及在200MHz 中藉由Material Analyzer所測得之磁特性的結果。 92 323724 201230083 , [比較例2] 使用平均長徑1.2/zm、平均厚度0.3/zm、平均長寬 比4之磁性體粒子來取代平均長徑2. 5//m、平均厚度〇. 3 V m、平均長寬比8. 3之平板狀磁性體粒子,除此之外,其 他依據實施例3而製得比較例2的複合磁性體。 第1表係顯示該複合磁性體的氣孔率以及在200MHz 中藉由Material Analyzer所測得之磁特性的結果。 第1表 氣孔率(¾) βτ' tan 5 u ε r* tan δ ε Ur’ · er’), {βτ' / εν )1/z 實施例3 13.3 9.8 0.035 26.5 0.052 0.06 0. 61 實施例4 11.1 9.3 0.017 32.3 0.074 0.06 0.54 實施例5 29.4 7.2 0.024 30.5 0.16 0. 07 0.49 實施例6 26.0 7.1 0. 038 30.8 0.13 0. 07 0.48 比較例2 12.5 3.7 0. 037 19.2 0.066 0.12 0.44 根據第1表’得知實施例3、4之複合磁性體,其氣 孔率與實施例5、6之複合磁性體相比為2〇%以下。因此, 確認到實施例3、4之複合磁性體與實施例5、6之複合磁 性體相比’雖然# r’增大,但ε r’幾乎不變。 此外’比較例2中’即使複合磁性體的氣孔率為2〇% 以下’但由於使用平均長寬比未達5之磁性體粒子,故確 認到複合磁性體的//r’小,無法得到使電子零件或電子設 備達成小型化之充分的ar,。 [實施例7] 將二環戊二烯型環氧樹脂EPICLON HP-7200L(DIC股 份有限公司製)、作為硬化劑之相對於環氧则旨與硬化劑的 全體量為1質量%之1~異丁其9田甘, 兴]基-2-甲基咪唑、由相對於樹脂 323724 93 201230083 與硬化劑與平板狀磁性體粒子的全體量為30體積%之Ni75 質量%-Fe20質量%-Zn5質量%之合金所構成之平均長徑2. 5 且平均厚度0. 3/zm且平均長寬比8. 3且平均保持力為 35厄斯特(0e)之平板狀磁性體粒子、以及環己酮,投入於 行星攪拌機,混合5分鐘而得漿液狀成形材料。該成形材 料的黏度為0. 4Pa · S。 接著藉由棒塗佈機將該成形材料塗佈於聚對笨二曱 酸乙二酯(PET)薄膜上,以使硬化後成為長50mmx寬50mmx 厚0. 1mm之方式進行薄片成形。 薄片成形後,在第3圖所示之定向裝置11上,以2m/ 分鐘的速度傳送該薄片並施加1200高斯的磁場。其次吹送 80°C的暖風以進行風乾,接著在160°C下進行2小時的硬 化反應,而得實施例7的複合磁性體。 使用掃描型電子顯微鏡(SEM)來觀察該複合磁性體中 的平板狀磁性體粒子,並對50個平板狀磁性體粒子,測定 出平板狀磁性體粒子的長軸方向相對於與薄片面呈水平之 方向(定向方向)所形成之角(相對於水平方向之斜率)。其 結果為50個斜率的平均值為8. 2度,平板狀磁性體粒子幾 乎往與薄片面呈水平之方向定向,確認到定向性良好。 此外,該複合磁性體於大氣中、室溫下之200MHz的 y r,為 8. 5。 [實施例8] 將平板狀磁性體粒子的含量設成相對於樹脂與硬化 劑與平板狀磁性體粒子的全體量為40體積%,除此之外, 94 323724 201230083 其他與實施例7進行相同操作而製得實施例8的複合磁性 體。 與實施例7相同,對50個平板狀磁性體粒子,測定 出該複合磁性體中的平板狀磁性體粒子相對於與薄片面呈 水平之方向之斜率,結果為斜率的平均值為8. 5度,平板 狀磁性體粒子幾乎往與薄片面呈水平之方向定向,確認到 定向性良好。 此外,與實施例7相同地測定該複合磁性體的複磁導 率,於大氣中、室溫下之200MHz的/z r’為9. 3。 [實施例9] 相對於環氧樹脂的全體量等量地混合酚類酚醛樹脂 TD-2131 (DIC股份有限公司製)作為硬化劑,來取代混合相 對於環氧樹脂的全體量為1質量%之1-異丁基-2-甲基咪 唑,除此之外,其他與實施例7進行相同操作而製得實施 例9的複合磁性體。 與實施例7相同,對50個平板狀磁性體粒子,測定 出該複合磁性體中的平板狀磁性體粒子相對於與薄片面呈 水平之方向之斜率,結果為斜率的平均值為8. 6度,平板 狀磁性體粒子幾乎往與薄片面呈水平之方向定向,確認到 定向性良好。 此外,與實施例7相同地測定該複合磁性體的複磁導 率,於大氣中、室溫下之200MHz的/z r’為8. 3。 [實施例10] 將實施例7中施加於薄片之磁場從1200高斯變更為 95 323724 201230083 1000高斯,除此之外,其他與實施例7進行相同操作而製 得實施例10的複合磁性體。 與實施例7相同,對50個平板狀磁性體粒子,測定 出該複合磁性體中的平板狀磁性體粒子相對於與薄片面呈 水平之方向之斜率,結果為斜率的平均值為12. 5度,平板 狀磁性體粒子幾乎往與薄片面呈水平之方向定向,確認到 定向性良好。 此外,與實施例7相同地測定該複合磁性體的複磁導 率,於大氣中、室溫下之200MHz的// r’為7. 7。 [實施例11] 將實施例7中施加於薄片之磁場從1200高斯變更為 900高斯,除此之外,其他與實施例7進行相同操作而製 得實施例11的複合磁性體。 與實施例7相同,對5G個平板狀磁性體粒子,測定 出該複合磁性體中的平板狀磁性體粒子相對於與薄片面呈 水平之方向之斜率,結果為斜率的平均值為17. 9度,確認 到平板狀磁性體粒子大致上往與薄片面呈水平之方向定向。 此外,與實施例7相同地測定該複合磁性體的複磁導 率,於大氣中、室溫下之200MHz的# r’為7. 2。 [實施例12] 實施例8中,薄片成形後,在第4圖所示之定向裝置 21上,以2m/分鐘的速度傳送該薄片並施加900高斯的磁 場,以取代在第3圖所示之定向裝置11者,除此之外,其 他均相同而得實施例12的複合磁性體。 96 323724 201230083 與實施例7相同,對50個平板狀磁性體粒子,測定 出該複合磁性體中的平板狀磁性體粒子相對於與薄片面呈 水平之方向之斜率,結果為斜率的平均值為16. 4度,平板 狀磁性體粒子幾乎往與薄片面呈水平之方向定向,確認到 定向性良好。 此外,該複合磁性體於大氣中、室溫下之200MHz的 # r’ 為 7. 5。 [實施例13] 實施例9中,薄片成形後,在第4圖所示之定向裝置 21上,以lm/分鐘的速度傳送該薄片並施加900高斯的磁 場,以取代在第3圖所示之定向裝置11者,除此之外,其 他均相同而得實施例13的複合磁性體。 與實施例7相同,對50個平板狀磁性體粒子,測定 出該複合磁性體中的平板狀磁性體粒子相對於與薄片面呈 水平之方向之斜率,結果為斜率的平均值為17. 0度,平板 狀磁性體粒子幾乎往與薄片面呈水平之方向定向,確認到 定向性良好。 此外,該複合磁性體於大氣中、室溫下之200MHz的 # r’ 為 7. 3。 [實施例14] 實施例12中,薄片成形後,在第5圖所示之定向裝 置31上,以2m/分鐘的速度傳送該薄片並且每1對磁石施 加300高斯的磁場,以取代在第4圖所示之定向裝置21 者。其次吹送80°C的暖風以進行風乾,接著在160°C下進 97 323724 201230083 行2小時的硬化反應’而得實施例η的複合磁性體。 與實施例7相同,對50個平板狀磁性體粒子,測定 出該複合磁性體中的平板狀磁性體粒子相對於與薄片面呈 水平之方向之斜率,結果為斜率的平均值為8. 3度,平板 狀磁性體粒子幾乎往與薄片面呈水平之方向定向,續認到 定向性良好。 此外,該複合磁性體於大氣中、室溫下之2〇〇MHz的 /z r’ 為 9. 0。 [實施例15] 將二環戍一稀型環氧樹脂EPICLON HP-7200L(DIC股 份有限公司製)取代為雙酚型環氧樹脂1256(三菱化學股 份有限公司製)’除此之外,其他與實施例7進行相同操作 而製得實施例15的複合磁性體。 與實施例7相同,對5〇個平板狀磁性體粒子,測定 出該複合磁性體中的平板狀磁性體粒子相對於與薄片面呈 水平之方向之斜率,結果為斜率的平均值為215度,此等 平板狀磁性體粒子未整合於單向上,確認到定向性降低。 此外,與實施例7相同地測定該複合磁性體的複磁導 率,於大氣中、室溫下之2〇〇mHz的# r,為5. 6。 [實施例16] 以相對於此等環氧樹脂的全體質量為10質量%,將雙 酚A雙(丙二醇縮水甘油醚)醚型液狀環氧樹脂Rikaresin BPO-20(新日本理化公司製)混合於二環戊二婦型環氧樹脂 EPICLON HP-72GGL(DIC股份有限公司製),而得環氧樹脂 323724 98 201230083 混合物。 接著,於該環氧樹脂混合物中,將作為硬化劑之相對 於環氧樹脂混合物與硬化劑的全體質量為1質量%之丨—異 丁基-2 -甲基咪唑、由相對於該環氧樹脂混合物與硬化劑與 平板狀磁性體粒子的全體量為40體積%之以75質量%-Fe20 質量%-Zn5質量%之合金所構成之平均長徑2. 5且平均 厚度0.3以111且平均長寬比8.3之平板狀磁性體粒子、以及 相對於該環氧樹脂混合物與硬化劑與平板狀磁性體粒子的 全體質量為40質量%之環己酮,投入於行星攪拌機,混人 5分鐘而得到漿液狀成形材料。 接著藉由棒塗佈機將該漿液狀成形材料塗佈於聚胃 苯二甲酸乙二酯(PET)薄臈上,以使硬化後成為長1〇〇mmx 寬200mmx厚0. 1mm之方式進行薄片成形,而製得實施例16 之附有成形體薄片的薄膜。 然後在該薄片成形後,於該成形體薄片上,在水平方 向上施加900高斯的磁場6分鐘。其次吹送80¾的暖風以 進行風乾後,從PET薄膜將成形體薄片剝離,然後在11〇 °C下施加lOMPa的模壓壓力後,在16ITC下進行2小時的 硬化反應,而得實施例16之l〇〇mmx200min的薄片形狀複合 磁性體。從PET薄膜將該薄片形狀複合磁性體剝離時,薄 片形狀複合磁性體並未產生破損。 接著測定該複合磁性體的電磁特性及氣孔率,結果為 複合磁性體於200MHz時之複磁導率的實部# r,為8·9,複 介電常數的實部ε r’為30. 4,氣孔率為19%。 323724 99 201230083 [實施例17] 使用第3圖所示之定向裝置丨丨,以2m/分鐘的速度傳 送該成形體薄片並施加12〇〇高斯的磁場,來取代於成形體 薄片上在水平方向上施加900高斯的磁場6分鐘者,然後 在乾燥/硬化步驟中,以不施加模壓壓力而在160°C下進行 2小時的硬化反應,來取代在11(rc下施加1〇MPa的模壓壓 力後’在16(TC下進行2小時的硬化反應者’除此之外, 其他與實施例16進行相同操作而製得實施例17的複合磁 性體。 在此,從PET薄膜將所得之薄片形狀複合磁性體剝離 時’薄片形狀複合磁性體並未產生破損。 接著測定該複合磁性體的磁特性及氣孔率,結果為複 合磁性體於200MHz時之複磁導率的實部,為9· 〇,複介 電常數的實部ε r’為27· 1 ’氣孔率為19%。 [實施例18] 係將20質量%的液狀環氧樹脂Rikaresin Bp〇_2〇混 。於二環戊二烯型環氧樹脂EpiCL〇N Hp_72〇〇L,來取代將 Μ質置%的液狀環氧樹脂RikaresinBp〇_2〇混合於二環戊 二婦型環氧樹脂EPICLON HP〜72〇ql者,除此之外,其他盥 實施例15進行相同操作㈣得實施例18的複合磁性體:、 在此,從PET薄膜將所得之薄片形狀複合磁性體剝離 時,薄片形狀複合磁性體並未產生破損。 人接著測定該複合磁性體的磁特性及氣孔率,結果為複 合磁性體於2_Hz時之複磁導率的實部〆為9. 3,複介 loo 323724 201230083 電常數的實部ε r’為31. 0,氣孔率為11%。 此外’藉由Material Analyzer,在大氣中、室溫(25 °C)下測定該複合磁性體於70至1000MHz的頻率波段之複 磁導率的實部yr’及複磁導率的損耗正切tan 5 β。此等 的測定結果如第2 5圖所示。 根據第25圖,70至1000MHz的頻率波段之複磁導率 的實部Mr’為7以上。 [實施例19] 使用雙酚Α二縮水甘油醚型環氧樹脂Adeka Resin EP-4010S(Adeka公司製)來取代雙酚a雙(丙二醇縮水甘油 醚)醚型液狀環氧樹脂,除此之外,其他與實施例16進行 相同操作而製得實施例19的複合磁性體。 在此,從PET薄膜將所得之薄片形狀複合磁性體剝離 時’薄片形狀複合磁性體並未產生破損。 接著測定該複合磁性體的磁特性及氣孔率,結果為複 合磁性體於200MHz時之複磁導率的實部以r,為9· 3,複介 電常數的實部ε r’為29. 7,氣孔率為IQ%。 [實施例20] 係混合20質量%的雙酚a二縮水甘油醚型環氧樹脂In each case, due to the loaded monopole antenna 74, the monopole antenna 94, the helical antenna 104, the dipole antenna 121, and the spiral antenna system, the antenna can be placed in the mobile phone with a small space to the electromagnetic wave without being transmitted by the antenna. The mobile phone that is blocked by parts other than the one. Performance under the inner body of the frame. Since the L-pole antenna 121 and the helical antenna 141 can be disposed in an accessory such as 133, the composite magnetic body according to the present embodiment can be lifted without the mobile phone having the auxiliary antenna installed in the mobile phone. The average thickness of the flat magnetic particles is 〇.〇1/iin or more 〇5em or less, and the average long diameter is 0.05am or more and 10/zm or less, and the average aspect ratio (long diameter/thickness) is 5 or more. 'Therefore, the real er of the complex permeability of the frequency band from 70MHz to 5〇〇MHz can be greater than 1, and the loss tangent tan (5# is 〇.丨 below, thus greatly shortening the wavelength shortening rate of the frequency band) Therefore, if the composite magnetic body is applied to an antenna of a VHF band, generation of eddy current on the surface of the composite magnetic body can be prevented, and the real part yr' of the complex magnetic permeability can be prevented from being lowered, and the antenna can be further realized. The method for producing a composite magnetic material according to the present embodiment includes a slurry obtained by dispersing spherical magnetic particles having an average particle diameter of 〇. 5# in or less in a solution containing a surfactant, and dispersion. F, fill In a closable container, the total volume of the slurry and the dispersion medium is in phase with the volume in the container, and the liquid is scrambled together with the dispersion medium in a sealed state to form the spherical shape. The first step of deforming the magnetic particles and forming a flat magnetic particle by 323724 75 201230083; dispersing and mixing the flat magnetic particles in a solution in which an insulating material is dissolved in a solvent to form a second forming material And a third step of forming a molded material by molding or applying the molding material to a substrate to obtain a molded body, and drying/hardening the drying/hardening step of the molded body, thereby being easily produced The complex magnetic body of the complex magnetic permeability of the frequency band of 70 MHz to 500 MHz is large, and the loss tangent of the complex magnetic permeability tan5 &quot; is a composite magnetic body of 0.1 or less. Further, 'the composite magnetic body according to the present embodiment When the porosity of the body is set to 20% or less, the composite magnetic body can increase the real part of the complex magnetic permeability, and the value of the real part er of the complex permittivity is almost constant. Thus, the application of electronic parts or make the electronic apparatus of the composite magnetic body to achieve miniaturization, and can suppress the power loss caused by the impedance matching. Further 'When the 70MHz to 500MHZ multiplexing loss of magnetic permeability tangent tan &lt;5/z is set to 0.05 or less, and the loss tangent of the complex dielectric constant is tan (j ε is set to 0.1 or less, and the gain of the electronic component or the electronic device can be improved. Further, the main bond has a ring structure and has a ring structure The composite magnetic material in which the first resin of the g-b group based on the monomer unit is used as the insulating material can reduce the influence of the steric hindrance formed by the resin on the flat magnetic particles. A composite magnetic body having a high magnetic permeability and a high mechanical strength. Further, since a resin having a functional group polymerized in a monomer unit is used, the bonding of the resin can be made strong, and it can be used as an electronic component or the like. 323724 76 201230083 According to the method for producing a composite magnetic material of the present embodiment, a mixed primary bond having a cyclic structure and having a resin and a flat plate polymerized in a monomer unit are provided. Magnetic particles, solvent, and necessary hardener, (iv) to the forming material; applying a magnetic field to the forming material to orient the flat magnetic recording And a step of drying/hardening the molded body in which the flat magnetic particles are turned backward, so that a composite magnetic body having a high r 'h' and a high mechanical strength can be easily produced. The orientation of the flat magnetic particles in the coating film can be improved by applying a magnetic field to the coating film once or plural times. Further, according to the composite magnetic body containing the main chain, the main chain has a cyclic structure and has The second resin which is a functional material of a functional group polymerized in a monomer unit and the second resin which imparts flexibility to the second resin can reduce the steric hindrance formed by the resin from the flat magnetic particles. The effect of the slab-shaped magnetic particles on the unidirectional orientation is improved, and ΐτ' is improved. Further, since the second resin imparts flexibility to the first resin, the flexibility and expansion of the composite magnetic body itself can be improved. Therefore, it is possible to provide a composite magnetic body which is high in yr' and mechanically strong, has flexibility to be wound up to a roll-like degree, and is excellent in productivity. The first resin of the polymerized functional group can strengthen the bonding of the resin, and can have sufficient mechanical strength using a molded body such as an electronic component. Further, even if it is a micron or nano grade, It also has the flexibility and flexibility of 77 323724 201230083, so it can be reduced to a hole that easily enters the flat magnetic particles. ·, · The composite magnetic body that causes the decrease The steric obstacle formed by the resin is as follows: the second resin' can reduce the amount of resin produced by the first flat magnetic particles to reduce the resin's resin-to-resin to the pores. Further, the ancient composite according to the present embodiment is a composite magnetic material of the second embodiment. The method for producing a mixed main chain having a cyclic structure is the first method of the energy base and the polymerization of the second monomer unit. The slab-shaped magnetic particles and the second flexible resin of the flying-flexible shape, the molding material is formed into a predetermined shape: a step of preparing a molding material; and a magnetic field is applied to make the step in the molded body The step of orienting the formed body; and drying the shaped body after the unidirectionally oriented magnetic particles are oriented in a unidirectional manner, so that the deer/hardening step can be easily produced. She is a soft and productive composite magnetic body. &quot;...Mechanical strength is good&apos;. Further, by applying a magnetic % of the flat magnetic particles in the coating film to the coating film, the composite magnetic body having a high height can be provided. Therefore, the antenna of the present embodiment can be manufactured by receiving, transmitting, or receiving electromagnetic waves of a frequency band of 7 〇 MHz to 5 〇 _z by mounting the composite of the present embodiment. The antenna is further miniaturized. That is, a small antenna having a length 1/4 of a shorter wavelength can be obtained by the wavelength shortening effect. 323724 78 201230083 When the composite magnetic material having a porosity of 20% or less in the present embodiment is provided, the real part of the complex magnetic permeability can be obtained in the frequency band of 70 MHz to 500 MHz, and the complex dielectric constant is 7 or more. The real part εΓ is 15 or more, and (Vr′ . ε r,)−1/2 is 〇. 1 or less, (//r, / £ Γ,) 1/2 is a performance of 〇5 or more and 1 or less. Therefore, by the wavelength shortening effect, it is possible to provide an antenna which is smaller in length than 1/4 of the desired wavelength, suppresses power loss caused by impedance matching, and has high transmission efficiency. Therefore, even a long wavelength electromagnetic wave in the VHF band like a multimedia broadcast can provide a small antenna capable of receiving the size of a mobile phone by the wavelength shortening effect. According to the communication device of the present embodiment, since the small antenna of the present embodiment is provided, the degree of freedom in the place where the antenna is less likely to be affected by other electronic devices that block the radio wave is high, and the transmission can be received and transmitted. Small communication device. [Monopolar Antenna] Fig. 16 is a schematic view (oblique view) showing a monopole antenna according to an embodiment of the present invention, and Fig. 16B is a cross-sectional view taken along line A-a of the figure 16 . The monopole antenna 1620' of the present embodiment has a rod-shaped antenna conductor 1622 and a composite magnetic body 1621 of the present embodiment which is coated on the surface of the antenna conductor 1622. In the present embodiment, as shown in Fig. 16B, a composite magnetic body 1621 having a square cross section is formed on the circumferential surface of the cylindrical antenna guide 1622, and a monopole antenna having a quadrangular prism shape is formed as a whole. Monopole day 323724 79 201230083 Line ^20 'Typically as shown in Fig. 16a, it is connected to the center of the conductor bottom plate 1624 of the overall size via a connector or the like, and is connected to the AC signal by using the connection portion 1626 as a power supply point. Transmitter 丨 625. The shape of the antenna conductor 1622 used in the monopole antenna 1620 is not particularly limited, and a generally known shape such as a linear rod antenna, a whip antenna, a curved spiral antenna, or a meander antenna can be used. . Among these, a linear antenna is preferable because it is difficult to generate an electrostatic capacitance between the antenna conductors and a high antenna gain can be obtained. Further, the "straight line" in the present embodiment means that the resonance portion of the antenna has a straight rod shape or a plate shape. Therefore, the shape of the linear monopole antenna 162A is not only a normal angular column shape but also a prismatic shape or an elongated flat plate shape. Further, the antenna conductor 1622 which is a core material is also the same, and may be any of a cylindrical shape, a prismatic shape, and a flat plate shape. The antenna conductor 1622 is preferably a conductive metal or alloy. Examples of the metal include, for example, copper (Cu), silver (Ag), nickel (Ni), platinum (pt), gold (Au), and the like. The alloy is preferably an alloy selected from two or more of these metals. . The cross-sectional shape ' of the antenna conductor 1622 is not particularly limited as long as it can be mounted on the size of the portable terminal, and may be, for example, a square or circular cross-sectional shape in which the straight edge D is about 0.5 mm to 2 min. . Further, since radio waves of 160 MHz to 222 MHz flow on the surface of the conductor, it is also effective to configure the antenna conductor 1622 as a tape having a large surface area. The strip antenna conductor 1622 preferably has a width of 〇.5min to 2_' thickness of 0.05 to 0.2mm» the length L of the antenna conductor 1622, as long as it can be easily loaded to the length of the portable 80 323724 201230083 There is no particular flaw, preferably 4g 丽 or more __ π ϋ or less. By setting the length l to the above range ', it can be easily mounted on the portable terminal, and can be configured as _ 1620 in the _ band of 16_2 to 2·ζ. &lt;Composite magnetic body&gt; The composite magnetic body 1621 of the present embodiment can be any of the above composite magnetic bodies. In the composite magnetic body 1621, the real part # r' of the complex magnetic permeability in the frequency band of 160 MHz to 222 MHz is preferably 3 or more, more preferably 6 or more. When the real part of the complex magnetic material 1621 is 3 or more, the thickness of the coating of 2.4 mm or more can be used, and even when the antenna conductor 1622 having a length of 200 mm is used, A frequency of 2 〇〇 MHz causes a resonant monopole antenna 1620. And the thickness of the composite conductor 1622 is reduced to 1.2 mm, even if the thickness of the composite conductor 1622 is reduced to 1.2 mm. A monopole antenna 1620 that can resonate at a frequency of 200 MHz is used using the antenna conductor 1622 having a length of 200 mm. When the coating thickness d of the composite magnetic body 1621 is too thick, the antenna becomes thick, and it becomes difficult to mount the device configuration or design relationship of the portable terminal. Therefore, practically, the coating thickness d of the composite magnetic body is in the range of 10 mm or less. Further, the composite magnetic body 1621 and the antenna conductor 1622 need not be adhered to each other, and 323724 201230083, for example, may be configured such that the antenna conductor 1622 is disposed inside the cylindrical composite magnetic body 1621 and is covered in appearance. In the composite magnetic body 1621 of the present embodiment, the loss tangent tan 5 of the complex magnetic permeability in the frequency band of 160 MHz to 222 MHz is preferable. By borrowing a W〇.〇5 or less, the gain of the antenna due to the signal loss in the frequency band of the second=222 MHz can be prevented from being lowered. &lt;Manufacturing Method of Monopole Antenna&gt; The method for manufacturing the monopole antenna 1620 of the present embodiment includes: processing the spherical magnetic particles into a flat shape to form the first transfer U of the flat magnetic particles The second step of forming the molding material by the magnetic material (4) and the insulating material, and the third step of coating the molding material containing the flat magnetic particles on the antenna conductor. The steps are explained below. &lt;First Step&gt; The step is the same as the above-described step j-th step, and therefore the description of the method for producing the i-th magnetic body of the flat magnetic particles is omitted. &lt;Second Step&gt; Next, in the "2 steps", the plate-like heteromixes 2 = the solution in which the insulating material is dissolved (4) the filament forming material. When the edge material is chemicalized, it becomes a composite magnetic body 1621 in which a flat Weibo is dispersed in an insulating material. System, 323724 82 201230083 Recovering, when using an antenna, 'it is better to have high mechanical strength, and the material for the hygroimin 2 for moisture absorption, for example, the ring can be appropriately returned to the tree J!, ^ (4) and % sold , benzene resin, polyphenylene poly 31 tree 匕曰 / _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _, 莰 = fat or thermoplastic resin. These resins may be used alone or in combination of two or more. It is preferable to cut the mechanical strength and the shape processing property. The thermoplastic resin is preferably a polystyrene resin, and the coffee type: the type and amount of the resin can be used in response to the special use of the resin. The solvent is not particularly limited as long as it can dissolve the resin. For example, methanol, ethanol, 2H t-free ethyl acetate, acetic acid, butyl acetate, lactic acid, and internal two: monomethyl hydrazine can be suitably used. , propylene glycol monoethyl ether acetate, butanol early glycol monomethyl serotonol), ethylene glycol monoethyl hexylene glycol single butyl bond (butyl sulco), diethylene glycol mono saki... (4) Ethylene, etc., acetone, butyl, methyl isobutyl _, B: ketone, hexanone and other ketones, stupid, toluene, stimulant, dimethyl ketoamine, hydrazine, hydrazine-dimethyl The base is brewed with a special aromatic arsenic amide, such as anthraceneamine, which is used in the above-mentioned lyomethyl group. It is used alone or in combination with two kinds of 323724 83 201230083 The content of the bulk particles is hardened to become a composite magnetic body 1621 with respect to the volatile component in the molding material. It is preferably 20% by volume or more and 50% by volume or less, and more preferably 30% by volume or more and 40% by volume or less. When the content of the flat magnetic particles is less than 20% by volume, the flat magnetic particles are too small. When the magnetic permeability of the composite magnetic material 1621 is lowered, it is not preferable. When the magnetic permeability exceeds 50% by volume, the amount of the flat magnetic particles is too large, and the fluidity of the molding material is lowered. As a result, the orientation of the flat magnetic particles in the molding material is caused. The decrease in the magnetic properties of the composite magnetic material 1621 may be lowered, which may be undesirable. The method of dispersing and mixing the flat magnetic particles with the insulating material is not particularly limited, and a planetary grinder, a sand mill, or the like may be used. A stirring device such as a ball mill, or a kneading device such as a pressure kneader, a biaxial kneader, or a jet mill can be used. When a thermoplastic resin is used, heating can be performed as necessary. &lt;Third Step&gt; In the third step, the molding material produced in the second step is applied to the outer peripheral surface of the antenna conductor 1622, and the molding material is cured to form a composite magnetic body 1621. Thereby, the monopole antenna 1620 of the present embodiment can be obtained. The method of applying the molding material to the antenna conductor 1622 and coating the composite magnetic body 1621 is not particularly limited as long as it can cover the composite magnetic body 1621 which is desired to be coated with the thickness d. The coating thickness d of the composite magnetic body 1621 is determined according to the length L of the antenna conductor and the magnetic permeability of the composite magnetic body 1621. For the coating method of the composite magnetic body 1621 84 323724 201230083, for example, the antenna conductor body is sandwiched between the inside of the molding material by a heated molding method, an injection molding method, or an extrusion molding method, and is formed and cured (4). The method. Further, when a thermosetting resin is used, it is preferred to cure the molding material by heat treatment or heat molding in a reducing gas or in a vacuum. Further, the above-mentioned molding material may be formed into a sheet-like or film-like shape of an arbitrary shape to form a desired coating thickness, and the antenna conductor body may be sandwiched and covered. The molding method for forming the molding material into a sheet shape or a film shape can be suitably used, for example, by a hot press method, a knife-to-knife method, or an injection molding method. In the above methods, from the viewpoint of easily orienting the flat magnetic particles in the insulating material, it is preferred to apply a roll forming method which is stretched into a planar shape. In order to adjust the viscosity at the time of stretching, it is preferred to add a plasticizer or a surface treatment of the slab-shaped magnetic particles. If desired, it is preferable to carry out the process of orienting the non-plate-shaped magnetic particles by the orientation of the magnetic field while maintaining the fluidity of the one port 2. The direction in which the plate-like magnetic particles are oriented is preferably a magnetic field generated by the antenna 1620, and the effect of shortening the wavelength of the two-step line by the long distance in the flat-shaped magnetic particles. That is, it is preferable that the longitudinal direction is such that the long axis of the flat magnetic particles is substantially parallel. Further, when the composite composite 1621 is formed, when t is required to adjust the viscosity of the material described above, the solvent contained in the molding material can be volatilized and/or frozen, and then molded. 323724 85 201230083 In addition, when the orientation treatment of the flat magnetic particles is necessary, the molding material is formed by sandwiching the antenna conductor 1622 inside, and a magnetic field is applied to the molding material before drying to orient the flat magnetic particles. The circumferential direction of the antenna conductor 1622 is substantially parallel to the long axis of the flat magnetic particles. As described above, according to the monopole antenna of the present embodiment, the antenna conductor is covered by the composite magnetic body in which the flat magnetic particles are dispersed in the insulating material, so that it can be mounted on the portable terminal. The miniaturization can be used in a low frequency band of 160 MHz to 222 MHz. Further, when the real part of the complex magnetic permeability in the frequency band of 160 MHz to 222 MHz is 3 or more, the composite magnetic body 1621 of the present embodiment is covered. 2.4 or more, even if the antenna conductor is 2 〇〇 mm or less, it can resonate at a frequency of 200 MHz. In addition, when the real part er of the complex magnetic permeability in the frequency band of 160 MHz to 222 MHz is 6 or more, the composite magnetic body 1621 of the present embodiment is covered by 1.2 mm or more, and even if the antenna conductor is 2 or less, It can also resonate at a frequency of 200MHz. The linear monopole antenna 162A of the present embodiment can be further reduced in size by using a matching circuit. (Examples) Hereinafter, the present invention will be specifically described by way of Examples and Comparative Examples, and the present invention is not limited to the Examples. Furthermore, the characteristics of each example were evaluated by the following methods. (1) Observation of flat magnetic particles 323724 86 201230083 It was observed with a scanning electron microscope s_4000 (manufactured by Hitachi High-Tech Co., Ltd.). (3) Electromagnetic characteristics (//r', #r&quot;, tan 占#, er, ε r', tan 6 ε ) were measured by magnetic permeability, and the Material Analyzer Ε4991Α type (made by Agilent Technologies) ), set at room temperature (25 〇 c) t in the atmosphere. Then, based on these, r and ε r are used to calculate (Γ, · ε r')' 1/2 and (a r, / ε r') 1/2. (4) Porosity ratio The size and quality of the composite magnetic body were measured. The measured density was calculated from these measured values. On the other hand, the theoretical density (and measured density) of the resin is measured by measuring the size and mass of the cured body of only the resin, and is calculated from the measured values. Further, the theoretical density of the flat magnetic particles is the theoretical density of X-rays obtained from the X-ray diffraction pattern of the flat magnetic particles. This value is substituted into the formula (4), and the porosity of the composite magnetic body is calculated. [Example 1] 200 g of Permalloy (trade name) magnetic particles containing 4% by mass of an average particle diameter of 0.25/m was mixed with diphenylbenzene in which a nitrogen-containing graft polymer as a surfactant was dissolved. A slurry of 400 g and 400 g of isopropyl alcohol was prepared to prepare a slurry. Next, a sand mill Ultra Apex Mill UAM-5 (manufactured by Shou Industrial Co., Ltd.) having a circulating seal type as shown in Fig. 2 and having a container volume of 5 L was used as a closed container, and the average particle diameter of the dispersion medium was 200 #m. The oxidized hammer beads 87 323724 201230083 pellets are placed in the inner container of the closed container. Here, the system is constructed in such a manner that the system is closed and looped. In order to re-inject the state in this state, the number of revolutions in the closed container is stirred until the slurry is dense. And the speed becomes a heart/minute, and a flat magnet is produced = = the obtained flat magnetic particle is dried and the slanted magnetic particle is added to the epoxy resin In the resin varnish of (4) ,, “by the knife coating, the formation of the ride (four) is a square film of 3〇mm square and 100/zra thick after hardening. Then at 9 (TC, atmosphere) The film was dried for 1 hour to form a dry film, and then compression-molded in a vacuum molding apparatus. The molding conditions were such that the temperature was raised to 130 Torr in 20 minutes under normal pressure, and the pressure of 2 MPa was applied for 5 minutes, and then the temperature was raised to 16 The resin is cured for 4 minutes to harden the resin, and the square film-like composite magnetic body of 30 mm square and 50/m thick is used. The complex magnetic permeability of the composite magnetic body is measured by a Material Analyzer. The real part of the magnetic permeability is #r, which is 13, and the loss tangent tan 6 # is 0.02, and the real part of the complex permeability of 220 MHz/zr is 13, and the loss tangent tan5 // is 0.04. Scanning electron microscope (SEM) to observe the shape of the composite magnetic body, flat The average thickness of 50 particles of morphological particles is 〇. 08# m 'the average length is 〇. 5 // m, and the average aspect ratio is 6.2. In addition, the spherical 88 323724 201230083 magnetic particles are either not thick 0. 01 β m or more 〇· 5 # m The following magnetic particles having a length of 0.05 &quot;m or more and 10#m or less and an aspect ratio of 5 or more are not substantially observed. The complex magnetic permeability (real part / zr, imaginary part A rn) and loss tangent (tan) of the composite magnetic body are shown &lt;5 μ), Fig. 18 is a scanning electron microscope (SEM) photograph showing the composite magnetic body. [Comparative Example 1] 20 g of Permalloy (trade name) magnetic particles having an average particle diameter of 4. 25 Μ 01 containing 4% by mass of zinc was mixed with a nitrogen-containing graft polymer as a surfactant. A slurry of benzene 4 g and 40 g of isopropyl alcohol was prepared to prepare a slurry. Next, using an upper open-type sand mill as shown in Fig. 1 as an open container, the oxidized error beads having an average particle diameter of 200/ΖΠ1 as a dispersion medium are placed in a vessel of the open container, and then connected. Only then entered the above Rong·Li. Here, the magnetic particles were produced by mixing the flow rate at the outermost circumference in the vessel at a number of revolutions of 10 μm/sec for 30 minutes. Then, the obtained magnetic particle ’ was used in the same manner as in Example 1 to obtain a film-like composite magnetic body of Comparative Example 1. The complex magnetic permeability of the composite magnetic body was measured by a Material Analyzer, and as a result, the real part of the complex magnetic permeability of 90 MHz / / r' was 2.6 ′ loss tangent tan &lt;5 &quot;为〇. 〇9, and the real part of the complex permeability of 220 MHz is 2.8, and the tangent tangent tan (5# is 0.11. In addition, by scanning electron microscope (SEM) The shape of the composite magnetic body was observed, and the magnetic particles were irregularly overlapped with each other, and it was found that substantially 89 323 724 201230083 has a thickness of 0.5 or more. The long diameter and the aspect ratio are also uneven. The complex magnetic permeability (real part er, imaginary part/zr&quot;) and loss tangent (tan 5) of the composite magnetic body are shown, and Fig. 20 shows a scanning electron microscope (SEM) photograph of the composite magnetic body. [Example 2] 12 dry films each having a length of 250 mm, a width of 30 mm, and a thickness of 60 #m were produced by the same method as in Example 1. Then, these dry films were laminated, between the sixth and seventh sheets. A copper wire having a diameter of 0.6 μm and a length of 250 mm was used as an antenna, and then compression-molding was carried out under the same conditions as in Example 1 using a vacuum molding apparatus, and a length of 25 was produced as shown in FIG. A composite magnetic body 63 composed of a laminate of 〇mm, a width of 3 mm, and a thickness of 0.8 mm of a dry film is sandwiched by a copper wire. The monopole antenna 61 of the antenna conductor 63 is constructed. Then, the monopole antenna 61 is connected to the center of the conductor bottom plate 64 of the 5 mm square, and the AC signal transmitter 66 supplies 50 Ω with the connection portion 65 as a power supply point. Here, the resonance frequency of the monopole antenna 61 is measured. Further, in order to compare the resonance frequency of the copper wire having a diameter of only 0.6 mm and a length of 250 mm, the resonance frequency is 273 MHz only for the copper wire. Compared with the three-pole material of the composite magnetic body of the second embodiment, the ratio of the shortening rate of the wavelength is calculated. From the result, it is known that the composite magnetic body of the present invention is used to make the composite magnetic body The length of the antenna of the band of 180 MHz is reduced by about 34%. 323724 90 201230083 [Example 3] The second J pentadiene type epoxy resin EPICLON HP-7200L (manufactured by DIC Corporation) was used as a hardener. The amount of 1-isobutylimidazole which is 1% by mass based on the total amount of the epoxy resin and the hardener is 75 mass% based on the total amount of the resin, the hardener, and the flat magnetic particles. -Fe20% by mass-Zn5 mass% of Ni-Fe-Zn The total mass of the flat magnetic particles composed of gold having an average length of 2.5 mm and an average thickness of 3.3/zm and an average aspect ratio of 8.3 and the total mass of the flat magnetic particles and the resin and the hardener is The viscous material is 0. 4Pa · S. The viscous material is 0. 4Pa · S. Then, the molding material was applied onto a polyethylene terephthalate (PET) film by a bar coater to form a sheet so as to have a length of 50 mm x a width of 50 mm x a thickness of 0.1 mm after hardening. After the sheet was formed, a magnetic field of 900 gauss was applied to the surface of the sheet for 6 minutes in the horizontal direction. Next, a warm air of 80 ° C was blown for air drying. Next, a molding pressure of 10 MPa was applied at DL ° C of the softening point of the resin, and then the composite magnetic body of Example 3 was obtained at 16 (hardening reaction for 2 hours under TC). The first watch shows the examples. The porosity of the composite magnetic body of 3 and the magnetic properties measured by the Material Analyzer at 200 MHz. Further, Fig. 21 shows the complex magnetic permeability of the composite magnetic body of Example 3 from 10 MHz to 1 GHz. Department and tan6 &quot; 'Fig. 22 shows 91 323724 201230083 showing the real part er' and tan 5 ε of the complex permittivity. [Example 4] Mixing a dicyclopentadiene type with a mass ratio of 85:15 Resin and liquid epoxy resin Rikaresin ΒΡΟ-20 (resin made by Nippon Chemical & Chemical Co., Ltd.) replaced the dicyclopentadiene type resin, and the temperature at which the molding pressure was applied was set to 16 "c". Further, the composite magnetic body of Example 4 was obtained in the same manner as in Example 3. The first table shows the porosity of the composite magnetic body of Example 4 and the magnetic properties measured by the Material Analyzer at 200 MHz. In addition, '23 shows the compound of Example 4 The real part of the complex magnetic permeability from 10 MHz to 1 GHz // r, and tan 5 //, Fig. 24 shows the real part er of the complex permittivity, and tan 5 ε. [Example 5] Preparation of a slurry In the case of the molding material, the mixing time of the planetary mixer was changed from 15 minutes to 5 minutes, and the composite inert body of Example 5 was obtained according to Example 3. The first surface showed the composite magnetic body. The porosity and the magnetic properties measured by the Material Analyzer at 200 MHz. [Example 6] The temperature at which the molded body was molded was set to 16 (TC, otherwise, according to Example 3 The composite magnetic body of Example 6 was obtained. The first surface shows the porosity of the composite magnetic body and the magnetic properties measured by a Material Analyzer at 200 MHz. 92 323724 201230083, [Comparative Example 2] The average length of the magnetic field of the average long diameter of 2. 5 / / m, the average thickness of 3. 3 V m, the average aspect ratio of 8. 3 A composite magnetic piece of Comparative Example 2 was produced in the same manner as in Example 3 except for the flat magnetic particles. The first table shows the porosity of the composite magnetic body and the magnetic properties measured by the Material Analyzer at 200 MHz. The first table porosity (3⁄4) βτ' tan 5 u ε r* tan δ ε Ur' · er'), {βτ' / εν )1/z Example 3 13.3 9.8 0.035 26.5 0.052 0.06 0. 61 Example 4 11.1 9.3 0.017 32.3 0.074 0.06 0.54 Example 5 29.4 7.2 0.024 30.5 0.16 0. 07 0.49 Example 6 26.0 7.1 0. 038 30.8 0.13 0. 07 0.48 Comparative Example 2 12.5 3.7 0. 037 19.2 0.066 0.12 0.44 According to the first table ', the composite magnetic bodies of Examples 3 and 4 were found to have porosity and examples. The composite magnetic body of 5 and 6 is 2% or less. Therefore, it was confirmed that the composite magnetic bodies of Examples 3 and 4 had an increase in θ r' as compared with the composite magnetic bodies of Examples 5 and 6. In addition, in Comparative Example 2, even if the porosity of the composite magnetic material is 2% or less, the magnetic particles having an average aspect ratio of less than 5 are used. Therefore, it was confirmed that the //r' of the composite magnetic material was small and could not be obtained. A sufficient ar for miniaturization of electronic parts or electronic equipment. [Example 7] The dicyclopentadiene type epoxy resin EPICLON HP-7200L (manufactured by DIC Corporation) was used as a curing agent, and the total amount of the curing agent was 1% by mass with respect to the epoxy. Isobutan 9 saponin, succinyl-2-methylimidazole, from the total amount of the hardener and the flat magnetic particles relative to the resin 323724 93 201230083, 30% by volume of Ni75% by mass-Fe20% by mass-Zn5 a flat magnetic particle composed of a mass % of an alloy having an average major diameter of 2.5 and an average thickness of 0.3/zm and an average aspect ratio of 8.3 and an average holding force of 35 Å (0e), and a ring The ketone was put into a planetary mixer and mixed for 5 minutes to obtain a slurry-like molding material. The viscosity of the molded material is 0. 4Pa · S. Then, the formed material was applied onto a polyethylene terephthalate (PET) film by a bar coater to form a sheet having a length of 50 mm x a width of 50 mm x a thickness of 0.1 mm after hardening. After the sheet was formed, the sheet was conveyed at a speed of 2 m/min on the orienting device 11 shown in Fig. 3 and a magnetic field of 1200 gauss was applied. Next, a warm air of 80 ° C was blown for air drying, followed by a hardening reaction at 160 ° C for 2 hours to obtain a composite magnetic body of Example 7. The flat magnetic particles in the composite magnetic body were observed by a scanning electron microscope (SEM), and the long-axis direction of the flat magnetic particles was measured to be horizontal with respect to the sheet surface for 50 flat magnetic particles. The angle formed by the direction (orientation direction) (relative to the slope in the horizontal direction). As a result, the average value of the 50 slopes was 8.2 degrees, and the flat magnetic particles were oriented in a direction substantially horizontal to the sheet surface, and it was confirmed that the orientation was good. Further, the composite magnetic body has a y r of 200 MHz at room temperature in the atmosphere of 8.5. [Example 8] The content of the tabular magnetic particles was 40% by volume based on the total amount of the resin, the curing agent, and the flat magnetic particles, and 94 323724 201230083 was the same as in Example 7. The composite magnetic body of Example 8 was produced by operation. The average value of the slope is 8.5. The average value of the slope is 8.5. The average value of the slope is 8.5. The flat magnetic particles were oriented almost horizontally with respect to the sheet surface, and it was confirmed that the orientation was good. Further, the complex magnetic permeability of the composite magnetic material was measured in the same manner as in Example 7, and the /z r' at 200 MHz in the atmosphere at room temperature was 9.3. [Example 9] A phenolic novolac resin TD-2131 (manufactured by DIC Corporation) was added as a curing agent in an amount equal to the total amount of the epoxy resin, and the total amount of the epoxy resin was 1% by mass in place of the epoxy resin. A composite magnetic body of Example 9 was obtained in the same manner as in Example 7 except that 1-isobutyl-2-methylimidazole was used. The average value of the slope is 8.6. The average value of the slope is 6.8. The average value of the slope is 8.6. The flat magnetic particles were oriented almost horizontally with respect to the sheet surface, and it was confirmed that the orientation was good. Further, the complex magnetic permeability of the composite magnetic material was measured in the same manner as in Example 7, and the /z r' at 200 MHz in the atmosphere at room temperature was 8.3. [Example 10] A composite magnetic body of Example 10 was produced in the same manner as in Example 7 except that the magnetic field applied to the sheet in Example 7 was changed from 1200 Gauss to 95 323724 201230083 1000 Gauss. In the same manner as in Example 7, the slope of the plate-like magnetic particles in the composite magnetic material was measured in a direction perpendicular to the surface of the sheet, and the average value of the slope was 12.5. The flat magnetic particles were oriented almost horizontally with respect to the sheet surface, and it was confirmed that the orientation was good. The compositive magnetic permeability of the composite magnetic material was 7.7 in the atmosphere at room temperature of 200 MHz. [Example 11] A composite magnetic body of Example 11 was produced in the same manner as in Example 7 except that the magnetic field applied to the sheet in Example 7 was changed from 1200 gauss to 900 gauss. In the same manner as in Example 7, the slope of the plate-like magnetic particles in the composite magnetic material was measured in a direction perpendicular to the surface of the sheet, and the average value of the slope was 17.9. It was confirmed that the flat magnetic particles were oriented substantially in a direction horizontal to the sheet surface. Further, the complex magnetic permeability of the composite magnetic material was measured in the same manner as in Example 7, and the #r' at 200 MHz in the atmosphere at room temperature was 7.2. [Embodiment 12] In Example 8, after the sheet was formed, the sheet was conveyed at a speed of 2 m/min on the orienting device 21 shown in Fig. 4 and a magnetic field of 900 Gauss was applied instead of the one shown in Fig. 3. The composite magnetic body of Example 12 was obtained in the same manner as the orientation device 11 described above. 96 323724 201230083 In the same manner as in the example 7, the slope of the flat magnetic particles in the composite magnetic body with respect to the direction perpendicular to the sheet surface was measured for 50 flat magnetic particles, and the average value of the slope was 16. At 4 degrees, the flat magnetic particles were oriented almost horizontally with the sheet surface, and it was confirmed that the orientation was good. Further, the composite magnetic body was 7.5 in 200 Hz at room temperature in the atmosphere. [Embodiment 13] In Example 9, after the sheet was formed, the sheet was conveyed at a speed of lm/min on the orienting device 21 shown in Fig. 4 and a magnetic field of 900 Gauss was applied instead of the one shown in Fig. 3. The composite magnetic body of Example 13 was obtained in the same manner as the orientation device 11 described above. In the same manner as in Example 7, the slope of the flat magnetic particles in the composite magnetic material was measured in a direction perpendicular to the sheet surface, and the average value of the slope was 17.0. The flat magnetic particles were oriented almost horizontally with respect to the sheet surface, and it was confirmed that the orientation was good. Further, the #r' of the composite magnetic body at 200 MHz in the atmosphere at room temperature was 7.3. [Embodiment 14] In the embodiment 12, after the sheet is formed, the sheet is conveyed at a speed of 2 m/min on the orienting device 31 shown in Fig. 5, and a magnetic field of 300 Gauss is applied to each pair of magnets instead of the first 4 is the orientation device 21 shown. Next, a warm air of 80 ° C was blown for air drying, followed by a hardening reaction of 97 323 724 201230083 at 160 ° C for 2 hours to obtain a composite magnetic body of Example η. The average value of the slope was 8.3. The average value of the slope was 8. 3 as a result of the slope of the flat magnetic particles in the composite magnetic material. The flat magnetic particles were oriented almost horizontally with the sheet surface, and the orientation was improved. Further, the composite magnetic body has a /z r' of 9.0 MHz at room temperature in the atmosphere of 9.0. [Example 15] A bicyclic fluorene-based epoxy resin EPICLON HP-7200L (manufactured by DIC Corporation) was replaced with a bisphenol type epoxy resin 1256 (manufactured by Mitsubishi Chemical Corporation). The composite magnetic body of Example 15 was obtained in the same manner as in Example 7. In the same manner as in Example 7, the slope of the flat magnetic particles in the composite magnetic body with respect to the direction perpendicular to the sheet surface was measured for 5 sheets of the flat magnetic particles, and the average value of the slope was 215 degrees. These flat magnetic particles were not integrated in one direction, and it was confirmed that the orientation was lowered. 5。 The complex magnetic permeability of the composite magnetic body was measured in the same manner as in Example 7 at room temperature of 2 〇〇 mHz # 。, 5.6. [Example 16] A bisphenol A bis(propylene glycol glycidyl ether) ether type liquid epoxy resin Rikaresin BPO-20 (manufactured by Nippon Chemical and Chemical Co., Ltd.) was used in an amount of 10% by mass based on the total mass of the epoxy resin. The mixture was mixed with a bicyclopentadienyl epoxy resin EPICLON HP-72GGL (manufactured by DIC Corporation) to obtain an epoxy resin 323724 98 201230083 mixture. Next, in the epoxy resin mixture, the total mass of the hardening agent relative to the epoxy resin mixture and the hardener is 1% by mass of oxime-isobutyl-2-methylimidazole, from the epoxy The average length of the resin mixture and the total amount of the hardener and the flat magnetic particles is 40% by volume, and the average long diameter is 2.5 and the average thickness is 0.3 and the average thickness is 0.3. The flat magnetic particles having an aspect ratio of 8.3 and the cyclohexanone having a total mass of 40% by mass based on the epoxy resin mixture and the curing agent and the flat magnetic particles are put into a planetary mixer and mixed for 5 minutes. A slurry-like shaped material was obtained. 5毫米进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行进行。 The sheet was formed to obtain a film of the molded article sheet of Example 16. Then, after the sheet was formed, a magnetic field of 900 Gauss was applied to the formed sheet for 6 minutes in the horizontal direction. Next, after blowing 803⁄4 of warm air for air drying, the formed body sheet was peeled off from the PET film, and then a molding pressure of 10 MPa was applied at 11 ° C, and then a hardening reaction was performed at 16 ITC for 2 hours, and Example 16 was obtained. l 〇〇 mmx200min sheet-shaped composite magnetic body. When the sheet-shaped composite magnetic body was peeled off from the PET film, the sheet-shaped composite magnetic body was not damaged. Next, the electromagnetic properties and the porosity of the composite magnetic body were measured. As a result, the real part of the complex magnetic body at 200 MHz was #9, and the real part ε r' of the complex permittivity was 30. 4. The porosity is 19%. 323724 99 201230083 [Example 17] Using the orientation device 第 shown in Fig. 3, the formed body sheet was conveyed at a speed of 2 m/min and a magnetic field of 12 Å Gauss was applied instead of the formed body sheet in the horizontal direction. A magnetic field of 900 Gauss was applied for 6 minutes, and then in the drying/hardening step, a hardening reaction was performed at 160 ° C for 2 hours without applying a molding pressure instead of applying a molding pressure of 1 MPa at 11 rc. The composite magnetic body of Example 17 was obtained by the same operation as in Example 16 except that the "hardening reaction was carried out for 2 hours under TC". Here, the obtained sheet shape was obtained from the PET film. When the composite magnetic material was peeled off, the sheet-shaped composite magnetic material was not damaged. Next, the magnetic properties and the porosity of the composite magnetic body were measured, and as a result, the real part of the complex magnetic permeability of the composite magnetic body at 200 MHz was 9·〇. The real part ε r' of the complex permittivity is 27·1' porosity is 19%. [Example 18] 20% by mass of liquid epoxy resin Rikaresin Bp〇_2 was mixed. Diene type epoxy resin EpiCL〇N Hp_72〇〇 L, in place of the liquid epoxy resin Rikaresin Bp 〇 2 Μ which is set to % by mass, is mixed with the dicyclopentadiene epoxy resin EPICLON HP~72〇ql, except for the other example 15 In the same operation (4), the composite magnetic body of Example 18 was obtained. Here, when the obtained sheet-shaped composite magnetic body was peeled off from the PET film, the sheet-shaped composite magnetic body was not damaged. The magnetic properties of the composite magnetic body were then measured. And the porosity of the composite magnetic body at 9.0 Hz is 9.3. The real part ε r' of the electrical constant of the complex loo 323724 201230083 is 31.0, and the porosity is 11%. In addition, the real yr' of the complex magnetic permeability of the composite magnetic body in the frequency band of 70 to 1000 MHz and the loss tangent of the complex magnetic permeability were measured by the Material Analyzer in the atmosphere at room temperature (25 ° C). 5 β. The measurement results of these are shown in Fig. 25. According to Fig. 25, the real part Mr' of the complex magnetic permeability in the frequency band of 70 to 1000 MHz is 7 or more. [Example 19] Using bisphenol quinone A diglycidyl ether epoxy resin Adeka Resin EP-4010S (manufactured by Adeka Co., Ltd.) A composite magnetic body of Example 19 was obtained in the same manner as in Example 16 except that the phenol a bis(propylene glycol glycidyl ether) ether type liquid epoxy resin was used. Here, the PET film was obtained. When the sheet-shaped composite magnetic material was peeled off, the sheet-shaped composite magnetic material was not damaged. Next, the magnetic properties and the porosity of the composite magnetic body were measured, and as a result, the real part of the complex magnetic permeability at 200 MHz was r, The porosity of the real part of the complex permittivity is 2.9, and the porosity is IQ%. [Example 20] 20% by mass of bisphenol a diglycidyl ether type epoxy resin was mixed

Adeka Resin EP-4010S(Adeka 公司製),來取代混合 1〇 質 量%的雙紛A雙(丙二醇縮水甘_)醚型液狀環氧樹月旨 Rikaresin BPO-20者,除此之外,其他與實施例16進行 相同操作而製得實施例20的複合磁性體。 在此,從PET薄膜將所得之薄片形狀複合磁性體制離 323724 101 201230083 時,薄片形狀複合磁性體並未產生破損。 接著測定該複合磁性體的磁特性及氣孔率,結果為複 合磁性體於200MHz時之複磁導率的實部,為9. 5,複介 電常數的實部’為28. 9 ’氣孔率為12%。 [實施例21 ] 使用第4圖所示之定向裝置21,以2m/分鐘的速度傳 送該成形體薄片並對該成形體薄片施加900高斯的磁場, 來取代於成形體薄片上在水平方向上施加900高斯的磁場 6分鐘者,除此之外’其他與實施例16進行相同操作而製 得實施例21的複合磁性體。 在此,從PET薄膜將所得之薄片形狀複合磁性體剝離 時,薄片形狀複合磁性體並未產生破損。 接著與實施例16相同地測定該複合磁性體的磁特性 及氣孔率,結果為複合磁性體於200MHz時之複磁導率的實 部// r,為7· 3 ’複介電常數的實部e r’為22. 8,氣孔率為 19%。 [實施例22] 使用第5圖所示之定向裝置31,以2m/分鐘的速度傳 送成形體薄片,並且每1對磁石分別施加300高斯的磁場, 來取代於成形體薄片上在水平方向上施加900高斯的磁場 6分鐘者’除此之外’其他與實施例16進行相同操作而製 得實施例22的複合磁性體。 在此’從PET薄膜將所得之薄片形狀複合磁性體剝離 時,薄片形狀複合磁性體並未產生破損。 102 323724 201230083 灰接著與實施例16相同地測定該複合磁性體的磁特性 及亂孔率’結果為複合磁性體於2q·時之複磁導率的實 «Mr | 9.0 ’複介電常數的實部e ^為3〇. 4,氣孔率為 19%。 [實施例23] ―係=40質的液狀環氧樹脂Rik⑽如腳_2〇混 口於一%戊一烯型環氧樹脂epicl〇n Hp_72〇〇L,來取代混 合質量%的液狀環氧樹脂RikaresinBPO_20者,除此之 外’其他與實施例16進行相同操作而製得實施例23的複 合磁性體。 在此’從PET薄膜將所得之薄片形狀複合磁性體剝離 時,薄片形狀複合磁性體並未產生破損。 接著測定該複合磁性體的磁特性及氣孔率,結果為複 合磁性體於200MHz時之複磁導率的實部,為7. 5,複介 電常數的實部ε r’為23. 9,氣孔率為9%。 [實施例24] 未將液狀環氧樹脂Rikaresin BPO-20混合於二環戊 二稀型環氧樹脂EPICLON HP-7200L ’除此之外,其他與實 施例21進行相同操作而製得實施例24的複合磁性體。 在此’從PET薄膜將所得之薄片形狀複合磁性體剝離 時’無法完整地剝離而產生破損,無法得到丨00mmx2〇〇mmx 〇. lmm之薄片形狀複合磁性體。 接著在160°C下對破損之複合磁性體的破片進行2小 時的硬化反應’並與實施例18相同地測定所得之破片狀複 103 323724 201230083 合磁性體的磁特性及氣孔率,結果為複合磁性體於2〇〇MHz 時之複磁導率的實部# r,為7.0,複介電常數的實部εΓ, 為32. 4,氣孔率為26%。 [實施例25] 將平均厚度〇.19#ιη、平均長徑1.63/zm、平均長寬 比8.6之平板狀磁性體粒子(Ni76質量%-Fe20質量%-Zn4 質量/〇分散於環氧樹脂中而得到成形材料。將所得之成形 材料放入於模具中予以成形,進行熱硬化而得複合磁性體。 以厚度1.7mm將該複合磁性體被覆於天線導體,而製 作出第16圖A所示之四角柱狀單極天線。該單極天線,當 將天線長度设為200mm時,在180MHz產生共振,將天線長 度δ史為較200mm短時,在180MHz以上的頻率產生共振,將 天線長度設為180匪時,在200MHz產生共振。該天線於第 16圖A中之X-Z平面上的平均增益為_5. 5dBd。該複合磁 性體之複磁導率的實部Vr,及損耗正切tan(5 #的測定結 果如第26圖所示。所得之複合磁性體於16〇至222MHz之 複磁導率的實部#!·,為6以上,複磁導率的損耗正切乜11 β从為0. 05以下。 [實施例2 6 ] 實施例2 5中,除了將複合磁性體的被覆厚度設為 2. 5mm之外,其他均同樣而製作出實施例26的單極天線。 該單極天線,當將天線長度設為2〇〇mm時,在1 2〇mjjz產生 共振’將天線長度設為較200mm短時,在120MHz以上的頻 率產生共振’设為150_時’在200MHz產生共振。該天線 104 323724 201230083 於x-z平面上的平均增益為_6.5dBd。 [實施例27] 將平均厚度〇.35//m、平均長徑2.49//m、平均長寬 比7. 3之平板狀磁性體粒子(Ni76質量%-Fe20質量%-Zn4Adeka Resin EP-4010S (manufactured by Adeka Co., Ltd.), in place of a mixture of 1% by mass of double bis (A propylene glycol glycidyl) ether type liquid epoxy tree Rikaresin BPO-20, in addition to other The composite magnetic body of Example 20 was obtained in the same manner as in Example 16. Here, when the obtained sheet-shaped composite magnetic system was separated from the PET film by 323724 101 201230083, the sheet-shaped composite magnetic body was not damaged. The porosity of the composite magnetic body is 8.9. The real part of the complex dielectric constant is 28.9. The porosity of the composite magnetic body is 9.5. It is 12%. [Example 21] Using the orienting device 21 shown in Fig. 4, the formed body sheet was conveyed at a speed of 2 m/min and a magnetic field of 900 Gauss was applied to the formed body sheet instead of the horizontally oriented sheet. A composite magnetic body of Example 21 was obtained by the same operation as in Example 16 except that a magnetic field of 900 gauss was applied for 6 minutes. Here, when the obtained sheet-shaped composite magnetic body was peeled off from the PET film, the sheet-shaped composite magnetic body was not damaged. Then, the magnetic properties and the porosity of the composite magnetic material were measured in the same manner as in Example 16. As a result, the real part of the complex magnetic permeability at 200 MHz was /r, which was a solid dielectric constant of 7·3'. The portion e r ' is 22.8, and the porosity is 19%. [Example 22] Using the orienting device 31 shown in Fig. 5, a formed body sheet was conveyed at a speed of 2 m/min, and a magnetic field of 300 Gauss was applied to each pair of magnets in place of the formed body sheet in the horizontal direction. The composite magnetic body of Example 22 was obtained by the same operation as in Example 16 except that a magnetic field of 900 gauss was applied for 6 minutes. Here, when the obtained sheet-shaped composite magnetic body is peeled off from the PET film, the sheet-shaped composite magnetic body is not damaged. 102 323724 201230083 Ash, then, the magnetic properties and the porosity of the composite magnetic body were measured in the same manner as in Example 16. The result was the complex dielectric constant of the complex magnetic permeability of the composite magnetic body at 2q·. The real part e ^ is 3〇. 4, and the porosity is 19%. [Example 23] ― system = 40-mass liquid epoxy resin Rik (10), such as foot _2 〇 mixed with one% pentene type epoxy resin epicl 〇 n Hp_72 〇〇 L, in place of the mixed mass% of the liquid The composite magnetic body of Example 23 was obtained by the same operation as in Example 16 except that the epoxy resin Rikaresin BPO_20 was used. Here, when the obtained sheet-shaped composite magnetic body is peeled off from the PET film, the sheet-shaped composite magnetic body is not damaged. Next, the magnetic properties and the porosity of the composite magnetic body are measured, and the real part of the complex magnetic permeability at the 200 MHz is 7.5, and the real part ε r' of the complex permittivity is 23.9. The porosity was 9%. [Example 24] The same procedure as in Example 21 was carried out except that the liquid epoxy resin Rikaresin BPO-20 was mixed with the dicyclopentadiene type epoxy resin EPICLON HP-7200L'. 24 composite magnetic body. Here, when the obtained sheet-shaped composite magnetic material is peeled off from the PET film, it is not completely peeled off and is broken, and a sheet-shaped composite magnetic body of 丨00 mm x 2 mmx 〇.1 mm cannot be obtained. Subsequently, the fragment of the damaged composite magnetic material was subjected to a curing reaction for 2 hours at 160 ° C. The magnetic properties and porosity of the obtained fragment-like composite 103 323724 201230083 magnetic material were measured in the same manner as in Example 18, and the result was a composite. The real part of the complex magnetic permeability at 2 〇〇MHz is 7.0, the real part of the complex permittivity is εΓ, which is 32.4, and the porosity is 26%. [Example 25] Flat magnetic particles (Ni 76% by mass - Fe 20% by mass - Zn4 mass / 〇 dispersed in epoxy resin) having an average thickness of 19.19#ιη, an average major axis of 1.63/zm, and an average aspect ratio of 8.6 A molding material is obtained in the mold, and the obtained molding material is molded in a mold and thermally cured to obtain a composite magnetic body. The composite magnetic body is coated on the antenna conductor at a thickness of 1.7 mm to produce a pattern of Fig. 16 a quadrilateral columnar monopole antenna. When the antenna length is set to 200 mm, resonance occurs at 180 MHz, and when the antenna length δ is shorter than 200 mm, resonance occurs at a frequency of 180 MHz or more, and the antenna length is obtained. When set to 180 ,, resonance occurs at 200 MHz. The average gain of the antenna in the XZ plane in Fig. 16A is _5. 5 dBd. The real part of the complex magnetic permeability of the composite magnetic body Vr, and the loss tangent tan (The measurement result of 5 # is shown in Fig. 26. The obtained composite magnetic body has a real part of the complex magnetic permeability of 16 〇 to 222 MHz, which is 6 or more, and the loss of the complex magnetic permeability is 乜 11 β from It is below 0.05. [Embodiment 2 6] In Example 2, except for The monopole antenna of Example 26 was produced in the same manner except that the coating thickness of the magnetic material was 2. 5 mm. The monopole antenna was produced at 12 〇mjjz when the antenna length was set to 2 〇〇 mm. When the resonance 'sets the length of the antenna to be shorter than 200 mm, resonance occurs at a frequency of 120 MHz or more' when it is set to 150_, and resonance occurs at 200 MHz. The average gain of the antenna 104 323724 201230083 on the xz plane is _6.5 dBd. Example 27] Flat magnetic particles (Ni 76% by mass-Fe 20% by mass-Zn4) having an average thickness of 35.35//m, an average major axis of 2.49/m, and an average aspect ratio of 7.3.

貝里%)力散於環氧樹脂中而得到成形材料。將該成形材料 放入於模具中&amp; L 以成形,進行熱硬化而得複合磁性體。以 厚度2. 5mm將讀複合磁性體被覆於棒狀天線導體的周圍,Berry%) is dispersed in an epoxy resin to obtain a shaped material. This molding material is placed in a mold &amp; L to be molded and thermally cured to obtain a composite magnetic body. The read composite magnetic body is coated around the rod antenna conductor with a thickness of 2.5 mm.

而製作出第16圖Λ &amp; ^ L _ ^ α圖A所示之四角柱狀單極天線。 °亥單極天線,當將天線長度設為200mm時,在197MHz 產生共振’將天線長度設為較200mm短時,在197MHz以上 的頻率產生共振,設為195mm時,在2GGMHz產生共振。該 Z平面上的平均增益為-5. OdBd。 該複合趟性體於160至222MHz之複磁導率的實部&quot;r, 為3以上,複礤導率的損耗正切tan (5〆為〇. 03。 [實施例28] 實鉍例25中,除了將複合磁性體的被覆厚度設為 〇. 8_之外’其他均同樣而製作出實施例28的單極天線。 §單極天、線冑將天線長度設$测mm時,在230MHz產生 八振,為了在222mhz以下的頻率產生共振,天線長度必須 «又為200mm以上,天線長度為22〇mm時,在200MHz產生共 振。 [實施例29] 實施例27 +,除了將複合磁性體的被覆厚度設為 1.7mm之外,其他均同樣而製作出實施例29的單極天線。 323724 105 201230083 s亥單極天線,當將天線長度設為2〇〇mm時,在236mHz產生 共振,為了在222MHz以下的頻率產生共振,天線長度必須 没為200mra以上,天線長度為23〇mm時,在2〇〇mhz產生共 振。 接著以第16圖A所示之單極天線作為模型,對於以 複磁導率的實部vr’=3, tan(5 “=〇 〇2的複合磁性體來被 覆天線導體之單極天線,以及以#r,=6, tan〇=().〇2的 複合磁性體來被覆天線導體之單極天線,藉由電磁場模擬 器HFSS來計算出複合磁性體的被覆厚度與在2〇〇MHz產生 共振之最小天線長度之關係。第27圖中’計算結果係以直 線表不。上述各實施例及參考例的結果,亦在第27圖中點 綠出(plot)。 如第27圖所示,由於實測值與計算值的直線上幾乎 一致,故得知藉由複磁導率的實部以r,= 3與6之複合磁性 體的被覆,使天線導體長度成為2〇〇mm以下,且為了在 200MHz以下的頻率產生共振,被覆厚度必需為2 4mm或 1. 2mm以上。 【圖式簡單說明】 第1圖係顯示使用開放容器將含有球狀磁性粒子之漿 液及分散介質進行高速攪拌之樣態之圖。 第2圖係顯示使用密閉容器將含有球狀磁性粒子之漿 液及分散介質進行高速擾拌之樣態之圖。 第3圖係顯示用以實施本發明的定向方法A之定向裝 置之概略構成圖。 106 323724 201230083 第4圖係顯示用以實施本發明的定向方法B之定向裝 置之概略構成圖。 第5圖係顯示用以實施本發明的定向方法C之定向裝 置之概略構成圖。 第6圖係顯示用以實施本發明的定向方法C之定向裝 置的動作之示意圖。 第7圖係顯示用以實施本發明的定向方法D之定向裝 置之概略構成圖。 第8圖係顯示本發明的一項實施形態之天線的一例之 單極天線的供電方法之示意圖。 第9圖係顯示本發明的一項實施形態之通信裝置的一 種之行動電話的一例之斜視圖。 第10圖係顯示本發明的一項實施形態之通信裝置的 種之行動電話的其他一例之斜視圖。 第11圖係顯示本發明的一項實施形態之通信裝置的 種之行動電話的另外一例之斜視圖。 第12圖係顯示本發明的一項實施形態之通信裝置的 種之行動電話的另外一例之斜視圖。 第13圖係顯示本發明的一項實施形態之通信裝置的 一種之附有保護蓋的行動電話的一例之斜視圖。 第14圖係顯不本發明的一項實施形態之通信裝置的 -種之附有賴蓋的行動電話的其他—例之俯視圖。 第15圖為沿著第14圖的a —A線之剖面圖。 第16圖A係顯示本實施形態之單極天線的構造及供 323724 107 201230083 電方法之示意圖。 第16圖B為沿著第16圖a的A. ~ A線之位置上的剖 面圖。 第17圖係顯示本發明的實施例1之複合磁性體的複 磁導率及損耗正切之圖。 第18圖係顯示本發明的實施例1之複合磁性體的構 造之掃描型電子顯微鏡(SEM)圖像。 第19圖係顯示比較例1之複合磁性體的複磁導率及 滹耗正切之圖。 第20圖係顯示比較例1之複合磁性體的構造之掃描 裂電子顯微鏡(SEM)圖像。 第21圖係顯示本發明的實施例3之複合磁性體在各 多負率中之複磁導率的實部// r’及複磁導率的損耗正切tan 5 #之圖。 第22圖係顯示本發明的實施例3之複合磁性體在各 礦率中之複介電常數的實部ε r’及複介電常數的損耗正切 tan&lt;5 ε 之圖。 第23圖係顯示本發明的實施例4之複合磁性體在各 鷓率中之複磁導率的實部/zr’及複磁導率的損乾正切tan 5 Μ之圖。 第24圖係顯示本發明的實施例4之複合磁性體在各 頻率中之複介電常數的實部ε r’及複介電常數的損耗正切 tan δ ε之圖。 第25圖係顯示本發明的實施例I8之複合磁性體在10 108 323724 201230083 至1000MHz的頻率波段中之複磁導率的實部/zr’及複磁導 率的損耗正切tan 5 #之圖。 第26圖係顯示實施例25之複合磁性體在各頻率中之 複磁導率的實部//r’及複磁導率的損耗正切tan 5 //之 圖。 第27圖係顯示複合磁性體的被覆厚度與產生共振之 天線長度的關係之圖。 【主要元件符號說明】 1 基體 2 塗佈膜 11、21、31、51定向裝置 12 塗佈手段 13a、13b、22、22a、22b、32a、32b、33a、33b、34a、34b 磁石 14、52 乾燥手段 41 平板狀磁性體粒子 61、 74、85、1620 單極天線 62、 75、87、95、106、122、142、1622 天線導體 63、 76、88、96、105、123、143、1621 複合磁性體 64、 93、103、1624 底板 65、1626 連接部 66、1625 交流信號發送機 71、 81、91、HH、112、132 行動電話 72、 82、92、102、114、134 框體 73、 83、115、135 顯示部84、116、136 外部天線用端子 86、124、144 連接端子 94 L形天線 104、141 螺形天線 111 ' 131 附有保護蓋的行動電話 113、133 保護蓋 121 雙極天線 109 323724 201230083 151 開放容器 152 球狀磁性粒子 153 漿液 154 分散介質 155 單軸旋轉體 1511 密閉容器 Η、HI 、H2 磁力線 g 行進方向 110 323724The four-corner cylindrical monopole antenna shown in Fig. 16 is produced in Fig. 16 &amp; ^ L _ ^ α. In the case of the monopole antenna, when the antenna length is 200 mm, resonance occurs at 197 MHz. When the antenna length is shorter than 200 mm, resonance occurs at a frequency of 197 MHz or more, and when it is 195 mm, resonance occurs at 2 GG MHz. The average gain on the Z plane is -5.0 dBn. The composite body of the complex magnetic body at 160 to 222 MHz has a real part &quot;r, which is 3 or more, and the loss tangent of the complex enthalpy tan is tan (5 〆 is 〇. 03. [Example 28] Example 25 In the above, the monopole antenna of the twenty-eighth embodiment was produced in the same manner except that the coating thickness of the composite magnetic material was set to 〇. 8_. § The unipolar day and the wire 胄 when the antenna length was set to $mm, At 230 MHz, eight resonances are generated. In order to generate resonance at a frequency below 222 mhz, the antenna length must be «200 mm or more, and when the antenna length is 22 〇mm, resonance occurs at 200 MHz. [Embodiment 29] Example 27 + except for composite magnetic The monopole antenna of Example 29 was produced in the same manner except that the coating thickness of the body was set to 1.7 mm. 323724 105 201230083 shai monopole antenna, when the antenna length is set to 2 〇〇 mm, resonance occurs at 236 mHz. In order to generate resonance at a frequency below 222 MHz, the length of the antenna must not be 200 mra or more, and when the length of the antenna is 23 〇mm, resonance occurs at 2 〇〇 mhz. Next, the monopole antenna shown in Fig. 16A is used as a model. The real part of the complex permeability vr'=3, tan(5 “=〇 a composite magnetic body of 2 to cover a monopole antenna of an antenna conductor, and a monopole antenna of an antenna conductor coated with a composite magnetic body of #r,=6, tan〇=().〇2, by an electromagnetic field simulator HFSS The relationship between the coating thickness of the composite magnetic body and the minimum antenna length at which resonance occurs at 2 〇〇 MHz is calculated. In Fig. 27, the calculation results are shown by straight lines. The results of the above respective examples and reference examples are also at the 27th. In the figure, the dot is green. As shown in Fig. 27, since the measured value and the calculated value are almost identical on the straight line, it is found that the real part of the complex magnetic permeability is a composite magnetic of r, = 3 and 6. The coating of the body is such that the length of the antenna conductor is 2 mm or less, and in order to resonate at a frequency of 200 MHz or less, the thickness of the coating must be 24 mm or 1.2 mm or more. [Simplified description of the drawing] Fig. 1 shows the use of the opening The container is a diagram in which a slurry containing spherical magnetic particles and a dispersion medium are stirred at a high speed. Fig. 2 is a view showing a state in which a slurry containing spherical magnetic particles and a dispersion medium are subjected to high-speed scrambling using a closed container. Figure 3 shows the display A schematic diagram of an orientation apparatus for carrying out the orientation method A of the present invention. 106 323724 201230083 FIG. 4 is a schematic configuration diagram showing an orientation apparatus for carrying out the orientation method B of the present invention. FIG. 5 is a diagram showing the implementation of the present invention. A schematic diagram of the orientation device of the orientation method C. Fig. 6 is a schematic view showing the operation of the orientation device for implementing the orientation method C of the present invention. Fig. 7 is a diagram showing the orientation of the orientation method D for implementing the present invention. A schematic diagram of the device. Fig. 8 is a view showing a power supply method of a monopole antenna which is an example of an antenna according to an embodiment of the present invention. Fig. 9 is a perspective view showing an example of a mobile phone of a communication device according to an embodiment of the present invention. Fig. 10 is a perspective view showing another example of a mobile phone of the communication device according to the embodiment of the present invention. Fig. 11 is a perspective view showing another example of a mobile phone of the communication device according to the embodiment of the present invention. Fig. 12 is a perspective view showing another example of a mobile phone of the communication device according to the embodiment of the present invention. Fig. 13 is a perspective view showing an example of a mobile phone with a protective cover of a communication device according to an embodiment of the present invention. Fig. 14 is a plan view showing another example of a mobile phone to which a communication device according to an embodiment of the present invention is attached. Fig. 15 is a cross-sectional view taken along line a - A of Fig. 14. Fig. 16 is a view showing the structure of a monopole antenna of the present embodiment and an electrical method for 323724 107 201230083. Fig. 16B is a cross-sectional view taken along the line A. to A of Fig. 16a. Fig. 17 is a view showing the complex magnetic permeability and loss tangent of the composite magnetic body of Example 1 of the present invention. Fig. 18 is a scanning electron microscope (SEM) image showing the constitution of the composite magnetic body of Example 1 of the present invention. Fig. 19 is a graph showing the complex magnetic permeability and the tangent tangent of the composite magnetic body of Comparative Example 1. Fig. 20 is a scanning electron microscope (SEM) image showing the structure of the composite magnetic body of Comparative Example 1. Fig. 21 is a view showing the real part / / r' of the complex magnetic permeability and the loss tangent tan 5 # of the complex magnetic permeability of the composite magnetic body of Example 3 of the present invention. Fig. 22 is a view showing the real part ε r' of the complex permittivity and the loss tangent tan &lt; 5 ε of the complex permittivity of the composite magnetic body of Example 3 of the present invention. Fig. 23 is a view showing the real part /zr' of the complex magnetic permeability and the loss tangent tan 5 复 of the complex magnetic permeability of the composite magnetic body of Example 4 of the present invention. Fig. 24 is a view showing the real part ε r' of the complex permittivity and the loss tangent tan δ ε of the complex permittivity of the composite magnetic body of Example 4 of the present invention. Figure 25 is a diagram showing the real part /zr' of the complex magnetic permeability and the loss tangent tan 5 # of the complex magnetic permeability in the frequency band of 10 108 323724 201230083 to 1000 MHz of the composite magnetic body of Example I8 of the present invention. . Fig. 26 is a view showing the real part /w of the complex magnetic permeability at each frequency of the composite magnetic body of Example 25 and the loss tangent tan 5 of the complex magnetic permeability. Fig. 27 is a view showing the relationship between the coating thickness of the composite magnetic body and the length of the antenna in which resonance occurs. [Description of main component symbols] 1 Base 2 Coating film 11, 21, 31, 51 Orientation device 12 Coating means 13a, 13b, 22, 22a, 22b, 32a, 32b, 33a, 33b, 34a, 34b Magnet 14, 52 Drying means 41 flat magnetic particles 61, 74, 85, 1620 monopole antennas 62, 75, 87, 95, 106, 122, 142, 1622 antenna conductors 63, 76, 88, 96, 105, 123, 143, 1621. Composite magnetic body 64, 93, 103, 1624 Base plate 65, 1626 Connection portion 66, 1625 AC signal transmitter 71, 81, 91, HH, 112, 132 Mobile phone 72, 82, 92, 102, 114, 134 Frame 73 , 83, 115, 135 Display parts 84, 116, 136 External antenna terminals 86, 124, 144 Connection terminal 94 L-shaped antenna 104, 141 Spiral antenna 111 ' 131 Mobile phone 113, 133 with protective cover Protective cover 121 Dipole antenna 109 323724 201230083 151 Open container 152 Spherical magnetic particles 153 Slurry 154 Dispersion medium 155 Single-axis rotating body 1511 Closed container Η, HI, H2 Magnetic field line g Direction of travel 110 323724

Claims (1)

201230083 七、申請專利範圍: 絕緣 、复δ磁J·生體,其係將平板狀磁性體粒子分散於 材料中而成, 前述平板狀磁性體粒子的平均厚度為〇 〇1em以 上5# m以下’平均長徑為0. 05# ra以上10# m以下, 且平均長寬比(長徑/厚度)為5以上。 2·如申請專利範圍第1項所述之複合磁性體,其中,70MHz 至500MHz的頻率波段之複磁導率的實部#『,大於1, 且複磁導率的損耗正切tanS以為0. 1以下。 3. 如申請專利範圍第1項所述之複合磁性體,其中,7〇ΜΗζ 至500MHz的頻率波段之複磁導率的實部以r,大於7, 且複磁導率的損耗正切tan 5 β為0.1 以下。 4. 如申請專利範圍第1項所述之複合磁性體,其中,70MHz 至500MHz的頻率波段之複磁導率的實部,大於1〇, 且複磁導率的損耗正切tand #為0· 1 以下。 5. 如申請專利範圍第1項所述之複合磁性體,其中,前述 平板狀磁性體粒子為含有選自鉛(A1)、鉻(Cr)、錳 (Μη)、鈷(C〇)、鋼(Cu)、鋅(zn)、鈮(Nb)、铜(Mo)、銦 (In)、錫(Sn)的群組之1種或2種以上的金屬元素之鐵 _鎳合金。 6.如申請專利範圍第1項所述之複合磁性體,其中,前述 平板狀磁性體粒子是藉由對平均粒徑〇. 5/zm以下的球 狀磁性粒子施以機械應力,使該球狀磁性粒子彼此變形 及 '熔著而成。 1 323724 201230083 7. 如申請專利範圍第1項所述之複合磁性體,其中,90MHz 至220MHz的頻率波段之複磁導率的實部/zr’大於1, 且複磁導率的損耗正切tan&lt;5 #為0. 05以下。 8. 如申請專利範圍第1項所述之複合磁性體,其中,氣孔 率為20%以下。 9. 如申請專利範圍第8項所述之複合磁性體,其中,70MHz 至500MHz的頻率波段之複磁導率的實部#!·’為7以 上,複介電常數的實部ε r’為15以上,且(// r’ · ε r’)M/2 為0. 1以下,(y r’ / ε r’)1/2為0. 5以上1以下。 10. 如申請專利範圍第9項所述之複合磁性體,其中,70MHz 至500MHz的頻率波段之複磁導率的損耗正切tan&lt;5 # 為0. 05以下,複介電常數的損耗正切tan&lt;5 ε為0. 1 以下。 11. 如申請專利範圍第1項所述之複合磁性體,其中,前述 絕緣材料係含有:主鏈具有環狀結構且具有以單體單位 聚合之官能基之第1樹脂。 12. 如申請專利範圍第11項所述之複合磁性體,其中,前 述樹脂為熱硬化性樹脂。 13. 如申請專利範圍第11項所述之複合磁性體,其中,前 述樹脂為環氧樹脂。 14. 如申請專利範圍第11項所述之複合磁性體,其中,前 述樹脂為二環戊二烯型環氧樹脂。 15. 如申請專利範圍第11項所述之複合磁性體,其中,前 述平板狀磁性體粒子之前述樹脂中的定向方向與該平 2 323724 201230083 板狀磁性體粒子的長軸方向所形成之角度為20°以下。 16. 如申請專利範圍第11項所述之複合磁性體,其中, 70MHz至500MHz的頻率波段之複磁導率的實部#r’為7 以上。 17. 如申請專利範圍第11項所述之複合磁性體,其中,更 含有對前述第1樹脂賦予可撓性之樹脂的第2樹脂。 18. 如申請專利範圍第17項所述之複合磁性體,其中,前 述第2樹脂為具有雙酚A型骨架及雙酚F型骨架中的至 少1種之環氧樹脂。 19. 如申請專利範圍第17項所述之複合磁性體,其中,前 述第2樹脂為於1分子中含有2個以上的環氧基且具有 醚骨架之環氧樹脂。 20. 如申請專利範圍第17項所述之複合磁性體,其中,前 述第2樹脂為具有丙二醇加成雙酚A型骨架及乙二醇加 成雙酚A型骨架中的任一種之環氧樹脂。 21. 如申請專利範圍第17項所述之複合磁性體,其中, 70MHz至500MHz的頻率波段之複磁導率的實部/zr’為7 以上。 22. —種複合磁性體的製造方法,該複合磁性體係如申請專 利範圍第1至21項中任一項所述之複合磁性體,其具 備下列步驟: 將使平均粒徑0. 5# m以下的球狀磁性粒子分散於 含有界面活性劑之溶液中而成之漿液及分散介質填充 於可密閉的容器内,以使前述漿液及前述分散介質的合 3 323724 201230083 計體積與前述容器内的體積成為相同,在密閉狀態下將 該漿液與前述分散介質一同攪拌,使前述球狀磁性粒子 彼此變形及熔著而形成平板狀磁性體粒子之第1步驟; 使前述平板狀磁性體粒子分散並混合於在溶劑中 溶解有絕緣材料而成之溶液中,形成成形材料之第2 步驟;以及 包含有:將前述成形材料成形或塗佈於基材上而獲 得成形體之成形步驟、及使前述成形體乾燥/硬化之乾 燥/硬化步驟之第3步驟。 23. 如申請專利範圍第22項所述之複合磁性體的製造方 法,其中,前述絕緣材料為主鏈具有環狀結構且具有以 單體單位聚合之官能基之樹脂。 24. 如申請專利範圍第22項所述之複合磁性體的製造方 法,其中,在前述第3步驟中,在前述成形步驟後,進 行對所獲得之成形體施加磁場而使該成形體中的前述 平板狀磁性體粒子往單向定向之定向步驟,接著進行前 述乾燥/硬化步驟。 25. —種天線,係具備如申請專利範圍第1至21項中任一 項所述之複合磁性體而成。 26. —種通信裝置,係具備如申請專利範圍第25項所述之 天線而成。 27. —種單極天線,係天線導體由如申請專利範圍第1項所 述之複合磁性體所被覆。 28. 如申請專利範圍第27項所述之單極天線,其中,前述 4 323724 201230083 複合磁性體於160MHz至222MHz的頻率波段之複磁導率 的實部# I·’為3以上。 29. 如申請專利範圍第28項所述之單極天線,其中,前述 複合磁性體的被覆厚度為2. 4mm以上10匪以下。 30. 如申請專利範圍第27項所述之單極天線,其中,前述 複合磁性體於160MHz至222MHz的頻率波段之複磁導率 的實部# r’為6以上。 31. 如申請專利範圍第30項所述之單極天線,其中,前述 複合磁性體的被覆厚度為1. 2mm以上10mm以下。 32. 如申請專利範圍第27項所述之單極天線,其中,前述 天線導體的長度為200mm以下。 5 323724201230083 VII. Patent application scope: Insulation, complex δ magnetic J·batter, which is obtained by dispersing flat magnetic particles in a material, and the average thickness of the flat magnetic particles is 〇〇1em or more and 5# m or less. 'The average long diameter is 0. 05# ra or more and 10# m or less, and the average aspect ratio (long diameter/thickness) is 5 or more. 2. The composite magnetic body according to claim 1, wherein the real part of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz is greater than 1, and the loss tangent tanS of the complex magnetic permeability is 0. 1 or less. 3. The composite magnetic body according to claim 1, wherein the real part of the complex magnetic permeability in the frequency band of 7 至 to 500 MHz is r, greater than 7, and the loss tangent of the complex magnetic permeability is tan 5 β is 0.1 or less. 4. The composite magnetic body according to claim 1, wherein the real part of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz is greater than 1 〇, and the loss tangent tand # of the complex magnetic permeability is 0· 1 below. 5. The composite magnetic body according to claim 1, wherein the flat magnetic particles are selected from the group consisting of lead (A1), chromium (Cr), manganese (Mn), cobalt (C〇), and steel. An iron-nickel alloy of one or two or more metal elements of (Cu), zinc (zn), niobium (Nb), copper (Mo), indium (In), and tin (Sn). 6. The composite magnetic body according to claim 1, wherein the flat magnetic particles are subjected to mechanical stress by a spherical magnetic particle having an average particle diameter of 0.5/zm or less to cause the ball. The magnetic particles are deformed and 'fused together. 1 323724 201230083 7. The composite magnetic body according to claim 1, wherein the real part of the complex magnetic permeability in the frequency band of 90 MHz to 220 MHz/zr' is greater than 1, and the loss of the complex magnetic permeability tangent tan &lt;; 5 # is 0. 05 or less. 8. The composite magnetic body according to claim 1, wherein the porosity is 20% or less. 9. The composite magnetic body according to claim 8, wherein the real part of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz is 7 or more, and the real part of the complex dielectric constant ε r ' 5以上以下以下。 (/ / r ' · ε r ') M / 2 is 0. 1 or less, (y r ' / ε r ') 1/2 is 0.5 or more and 1 or less. 10. The composite magnetic body according to claim 9, wherein the loss of the complex magnetic permeability of the frequency band of 70 MHz to 500 MHz is tan &lt;5 # is 0.05 or less, and the loss of the complex dielectric constant tangent tan &lt;;5 ε is 0.1 or less. The composite magnetic material according to claim 1, wherein the insulating material contains a first resin having a cyclic structure and a functional group polymerized in a monomer unit. 12. The composite magnetic body according to claim 11, wherein the resin is a thermosetting resin. 13. The composite magnetic body according to claim 11, wherein the resin is an epoxy resin. 14. The composite magnetic body according to claim 11, wherein the resin is a dicyclopentadiene type epoxy resin. The composite magnetic body according to claim 11, wherein an orientation direction of the resin in the flat magnetic particle is an angle formed by a longitudinal direction of the plate-shaped magnetic particle of the flat 2 323 724 201230083 It is 20° or less. 16. The composite magnetic body according to claim 11, wherein the real part #r' of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz is 7 or more. 17. The composite magnetic material according to claim 11, further comprising a second resin which imparts flexibility to the first resin. 18. The composite magnetic material according to claim 17, wherein the second resin is an epoxy resin having at least one of a bisphenol A type skeleton and a bisphenol F type skeleton. 19. The composite magnetic material according to claim 17, wherein the second resin is an epoxy resin having two or more epoxy groups in one molecule and having an ether skeleton. 20. The composite magnetic material according to claim 17, wherein the second resin is an epoxy having any one of a propylene glycol addition bisphenol A type skeleton and an ethylene glycol addition bisphenol A type skeleton. Resin. 21. The composite magnetic body according to claim 17, wherein the real part /zr' of the complex magnetic permeability in the frequency band of 70 MHz to 500 MHz is 7 or more. _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ The slurry and the dispersion medium in which the spherical magnetic particles are dispersed in the solution containing the surfactant are filled in the sealable container, so that the volume of the slurry and the dispersion medium is 3,323,724,300,300,300, and the volume of the container a first step in which the volume is the same, and the slurry is stirred together with the dispersion medium to deform and melt the spherical magnetic particles to form flat magnetic particles. The flat magnetic particles are dispersed. a second step of forming a molding material in a solution obtained by dissolving an insulating material in a solvent; and a molding step of forming or coating the molding material on a substrate to obtain a molded body, and The third step of the drying/hardening step of the shaped body drying/hardening. The method of producing a composite magnetic material according to claim 22, wherein the insulating material is a resin having a cyclic structure and having a functional group polymerized in a monomer unit. The method of producing a composite magnetic material according to claim 22, wherein in the third step, after the molding step, a magnetic field is applied to the obtained molded body to cause the molded body to be in the molded body. The orientation step of aligning the planar magnetic particles into one direction is followed by the aforementioned drying/hardening step. A type of antenna comprising the composite magnetic body according to any one of claims 1 to 21. 26. A communication device comprising an antenna as described in claim 25 of the patent application. 27. A monopole antenna, the antenna conductor being covered by a composite magnetic body as described in claim 1 of the patent application. 28. The monopole antenna according to claim 27, wherein the real part # I·' of the complex magnetic permeability of the 4 323 724 201230083 composite magnetic body in the frequency band of 160 MHz to 222 MHz is 3 or more. The singularity of the composite magnetic body is 2. 4 mm or more and 10 Å or less. The monopole antenna according to claim 27, wherein the composite magnetic body has a real part #r' of a complex magnetic permeability of 6 or more in a frequency band of 160 MHz to 222 MHz. The thickness of the composite magnetic body is 1. 2 mm or more and 10 mm or less, as described in the above-mentioned. The monopole antenna according to claim 27, wherein the length of the antenna conductor is 200 mm or less. 5 323724
TW100144103A 2010-11-30 2011-11-30 Composite magnetic material, production method thereof, antenna and communication device TW201230083A (en)

Applications Claiming Priority (9)

Application Number Priority Date Filing Date Title
JP2010266903 2010-11-30
JP2011064310 2011-03-23
JP2011097157 2011-04-25
JP2011122440 2011-05-31
JP2011167077 2011-07-29
JP2011167078 2011-07-29
JP2011254169A JP6044064B2 (en) 2010-11-30 2011-11-21 Composite magnetic body, method for manufacturing the same, antenna, and communication apparatus
JP2011257616 2011-11-25
JP2011257615 2011-11-25

Publications (1)

Publication Number Publication Date
TW201230083A true TW201230083A (en) 2012-07-16

Family

ID=46934106

Family Applications (1)

Application Number Title Priority Date Filing Date
TW100144103A TW201230083A (en) 2010-11-30 2011-11-30 Composite magnetic material, production method thereof, antenna and communication device

Country Status (1)

Country Link
TW (1) TW201230083A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI673731B (en) * 2016-05-31 2019-10-01 南韓商Skc股份有限公司 Method of preparing conductive magnetic composite sheet and antenna device
TWI685857B (en) * 2015-03-19 2020-02-21 美商羅傑斯公司 Magneto-dielectric substrate, circuit material, and assembly having the same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI685857B (en) * 2015-03-19 2020-02-21 美商羅傑斯公司 Magneto-dielectric substrate, circuit material, and assembly having the same
TWI673731B (en) * 2016-05-31 2019-10-01 南韓商Skc股份有限公司 Method of preparing conductive magnetic composite sheet and antenna device

Similar Documents

Publication Publication Date Title
TWI343872B (en)
JP5368281B2 (en) Core-shell magnetic material, core-shell magnetic material manufacturing method, device apparatus, and antenna apparatus
EP2851910B1 (en) Metal powder and its use
JP5085595B2 (en) Core-shell magnetic material, method for manufacturing core-shell magnetic material, device device, and antenna device.
WO2020174864A1 (en) Power feeding member, magnetic sheet used for coil arrangement, and production method for magnetic sheet used for coil arrangement
CN108353524B (en) Magnetic field shielding unit for wireless power transmission and wireless power transmission module including the same
JP2013253122A (en) Composite magnetic material, method for manufacturing the same, antenna, and communication device
CN103999170B (en) The soft magnetic metal powder that magnetic part and magnetic part use and manufacture method thereof
JP2019504482A (en) Magnetic shielding material, method for producing the same, and device including the same
US20060099454A1 (en) Method for producing electromagnetic wave absorbing sheet, method for classifying powder, and electromagnetic wave absorbing sheet
JP6471015B2 (en) Fe-Co alloy powder and antenna, inductor and EMI filter
TW201230083A (en) Composite magnetic material, production method thereof, antenna and communication device
JP6044064B2 (en) Composite magnetic body, method for manufacturing the same, antenna, and communication apparatus
JP7318422B2 (en) Resin composition and molded product
JP6167560B2 (en) Insulating flat magnetic powder, composite magnetic body including the same, antenna and communication device including the same, and method for manufacturing composite magnetic body
WO2012074024A1 (en) Composite magnet and production method therefor, antenna, and communication device
JP2014029936A (en) Method of producing composite magnetic body and composite magnetic body
JP2013253123A (en) Composite magnetic material, antenna equipped with the same, communication device, and method for manufacturing the composite magnetic material
JP6167533B2 (en) Composite magnetic body, antenna including the same, and RFID tag
WO2013077285A1 (en) Composite magnet, antenna provided therewith, and non-contact ic card
JP2009290067A (en) Magnetic material for high frequency and method for manufacturing magnetic material for high frequency
JP2013254757A (en) Composite magnetic material, and antenna having the same, and communication device
JP2014064258A (en) Antenna, unbalanced feeding type antenna, and communication device
JP2013247352A (en) Composite magnetic material, its manufacturing method, antenna, and communication device
JP2012212980A (en) Antenna component and manufacturing method of the same