JP2699838B2 - Infrared detector and manufacturing method thereof - Google Patents
Infrared detector and manufacturing method thereofInfo
- Publication number
- JP2699838B2 JP2699838B2 JP5295607A JP29560793A JP2699838B2 JP 2699838 B2 JP2699838 B2 JP 2699838B2 JP 5295607 A JP5295607 A JP 5295607A JP 29560793 A JP29560793 A JP 29560793A JP 2699838 B2 JP2699838 B2 JP 2699838B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- compound semiconductor
- hgcdte
- type
- junction
- Prior art date
- Legal status (The legal status 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 status listed.)
- Expired - Lifetime
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Description
【0001】[0001]
【産業上の利用分野】本発明は禁制帯幅の狭い半導体、
特にHgを含む化合物半導体を用いた赤外線検出器とそ
の製造方法に関するものである。The present invention relates to a semiconductor having a narrow bandgap,
In particular the infrared detector and its using a compound semiconductor containing Hg
And a method for producing the same.
【0002】[0002]
【従来の技術】一般に赤外線検出器においては禁制帯幅
の狭い半導体を用いたものが高感度であることが知られ
ている。その中でも検出部分にpn接合を有する光起電
力型素子は、単素子を二次元に配列した構成を採った赤
外線撮像装置にとって非常に有効である。2. Description of the Related Art It is generally known that an infrared detector using a semiconductor having a narrow band gap has high sensitivity. Among them, a photovoltaic element having a pn junction in a detection portion is very effective for an infrared imaging apparatus having a configuration in which single elements are two-dimensionally arranged.
【0003】その代表的なものであるHgCdTeを用
いた光起電力型赤外線検出器について、図2を用いて簡
単に説明する。CdTe基板1上にMBE法を用いてH
gCdTe層をエピタキシャル成長させ、Hg雰囲気中
での熱処理によりHg空孔よりなるp−HgCdTe層
3を形成する。その後、レジストマスクを用い部分的に
イオン注入を施すことでイオン注入領域4を形成し、さ
らにイオン注入ダメージによる特性劣化を回避するため
に、熱処理を行い格子間のHgを結晶の奥へ拡散させn
- −HgCdTe領域5を形成し、pn接合界面8をダ
メージフリーの領域に移動させる。最後に保護膜6、電
極7を形成し素子は完成する。A typical example of the photovoltaic infrared detector using HgCdTe will be briefly described with reference to FIG. H is formed on the CdTe substrate 1 using the MBE method.
The gCdTe layer is epitaxially grown, and a p-HgCdTe layer 3 composed of Hg vacancies is formed by heat treatment in an Hg atmosphere. Thereafter, ion implantation is performed partially by performing ion implantation using a resist mask, and heat treatment is performed to diffuse Hg between lattices to the back of the crystal in order to avoid deterioration in characteristics due to ion implantation damage. n
- forming a -HgCdTe region 5, to move the pn junction interface 8 to the damage free areas. Finally, a protective film 6 and an electrode 7 are formed to complete the device.
【0004】入射した赤外線はp−HgCdTe層3及
びn- −HgCdTe領域5で吸収され、電子あるいは
ホールとなって拡散し、pn接合部分で電気的に分離さ
れ、信号として電極7(p側の電極はここでは省略し
た)より出力される。The incident infrared light is absorbed by the p-HgCdTe layer 3 and the n − -HgCdTe region 5 and diffuses as electrons or holes, is electrically separated at the pn junction, and is used as a signal at the electrode 7 (p-side). The electrodes are omitted here).
【0005】[0005]
【発明が解決しようとする課題】しかしながら、この様
な赤外線検出器には以下に述べる欠点が存在する。However, such an infrared detector has the following disadvantages.
【0006】pn型接合形成には上述したようにイオン
注入法が用いられるのが、制御性、簡便性を考えると最
も有利な方法であり、イオン注入ダメージによる特性劣
化改善のため、その後の工程で熱処理を施すのが一般的
な方法である。この熱処理により、イオン注入で生じた
格子間のHgがp−HgCdTe層3中のHg空孔を介
して拡散し、イオン注入ダメージのない領域にpn接合
を形成するが、その拡散は比較的速く、更にHg空孔の
数にも大きく依存するために、拡散フロント即ちpn接
合界面8を十分に制御するのは困難である。特にエピタ
キシャル結晶でHgCdTe層が10〜15μm程度の
薄い結晶を用いた場合、熱処理により、格子歪の多い基
板との界面近傍までpn接合が移動する可能性もあり、
暗電流の増加等特性劣化を招くことも有り得る。As described above, the ion implantation method is used for forming the pn-type junction, which is the most advantageous method in view of controllability and simplicity. Is a general method of performing heat treatment. By this heat treatment, Hg between lattices generated by ion implantation diffuses through Hg vacancies in the p-HgCdTe layer 3 to form a pn junction in a region where ion implantation is not damaged, but the diffusion is relatively fast. In addition, it is difficult to sufficiently control the diffusion front, that is, the pn junction interface 8, because it largely depends on the number of Hg vacancies. In particular, when a thin HgCdTe layer having a thickness of about 10 to 15 μm is used as an epitaxial crystal, the pn junction may be moved to the vicinity of the interface with the substrate having a large lattice distortion due to the heat treatment.
There is also a possibility that characteristic deterioration such as an increase in dark current may be caused.
【0007】本発明の目的は、これらの欠点を除いた赤
外線検出器とその製造方法を提供することにある。[0007] It is an object of the present invention to provide an infrared detector which eliminates these disadvantages and a method of manufacturing the same.
【0008】[0008]
【課題を解決するための手段】本発明の光起電力赤外線
検出器は、Hgを含む化合物半導体を用いた赤外線検出
器において、基板上にp型ドーパントをドーピングした
第一の化合物半導体層を有し、前記第一の化合物半導体
層上にHg空孔をアクセプタとしたp型の第二の化合物
半導体層を有し、かつ前記第二の化合物半導体層に、格
子間のHgをドナーとしたn型の領域が形成されている
ことを特徴とするものである。Means for Solving the Problems] photovoltaic infrared detector of the present invention, the infrared detector using a compound semiconductor containing Hg, have a first compound semiconductor layer doped with p-type dopant on the substrate And the first compound semiconductor
Has a second compound semiconductor layer of p-type which is an acceptor of Hg vacancies on the layer, and the second compound semiconductor layer, n-type regions as a donor of Hg between grating is formed It is characterized by the following.
【0009】[0009]
【作用】基板上に複数の化合物半導体層を形成した赤外
線検知装置としては、従来よりCdTe基板上にx値の
大きいHg1 - x Cdx Teバッファ層とx値の小さい
Hg1 - x Cdx Te層を積層したダイオードが既に提
案されていた(特開平1−233777号公報等)。こ
れは、ダイオードが形成される部分だけ選択的にキャリ
ア濃度を低減し、各ダイオード(画素)間のクロストー
クを低減することを目的とした装置である。このような
構成においてHgの拡散を制御することは不可能であ
り、本願発明の目的を達成することはできなかった。The infrared detection device in which a plurality of compound semiconductor layer to the action substrate, large Hg 1 x values on CdTe substrate conventionally - x Cd x Te buffer layer and the x value smaller Hg 1 - x Cd x A diode in which a Te layer is laminated has already been proposed (Japanese Patent Laid-Open No. 1-233777, etc.). This is an apparatus aimed at selectively reducing the carrier concentration only in a portion where a diode is formed and reducing crosstalk between diodes (pixels). In such a configuration, it was impossible to control the diffusion of Hg, and the object of the present invention could not be achieved.
【0010】これに対し、本発明の赤外線検出器は、基
板との界面近傍にはAs等のp型ドーパントをドーピン
グした層、その上にHg空孔をアクセプタとしたp型の
層があるp型HgCdTe結晶を用い、イオン注入によ
るpn接合ダイオード形成、注入後の熱処理等を含む通
常のプロセスを行っている。上記二層構造のp型HgC
dTe結晶を用いているため、熱処理によりHg空孔を
介して拡散する格子間のHgはHg空孔の殆ど存在しな
いp型ドーパントをドーピングした層で止まる。従って
pn接合位置は格子歪が多く存在する基板との界面近傍
まで達することはなく、それによる暗電流増加等のダイ
オード特性の劣化もみられない。On the other hand, in the infrared detector of the present invention, a layer doped with a p-type dopant such as As is provided near the interface with the substrate, and a p-type layer having Hg vacancies as an acceptor is provided thereon. Using a type HgCdTe crystal, a normal process including formation of a pn junction diode by ion implantation, heat treatment after implantation, and the like are performed. The p-type HgC of the above two-layer structure
Since the dTe crystal is used, Hg between lattices diffused through Hg vacancies due to the heat treatment stops at the layer doped with the p-type dopant having almost no Hg vacancies. Therefore, the pn junction position does not reach the vicinity of the interface with the substrate where a large amount of lattice distortion is present, and deterioration of diode characteristics such as an increase in dark current due to the pn junction position is not observed.
【0011】[0011]
【実施例】次に、本発明の実施例を図面を用いて説明す
る。Next, embodiments of the present invention will be described with reference to the drawings.
【0012】図1は本発明の実施例を示す図である。ア
クセプタの種類の異なる2層のp型HgCdTe結晶上
にフォトダイオードを形成した本発明の製造方法につい
て簡単に述べる。FIG. 1 is a diagram showing an embodiment of the present invention. The manufacturing method of the present invention in which a photodiode is formed on two layers of p-type HgCdTe crystals having different types of acceptors will be briefly described.
【0013】CdTe基板1上にAsをドーピングした
p−HgCdTe層2を5μm、ノンドープのHgCd
Teを5μm、順次MBE法により成長し、Hg雰囲気
中のp化アニールによりノンドープのHgCdTe中に
Hg空孔を作りHg空孔によるp−HgCdTe層3を
形成する。その後、約50μmφのマスクを通してホウ
素(B)を部分的にイオン注入しpn接合を形成する。
イオン注入エネルギーは150keV程度でよい。この
ときn型のドナーとなっているのは活性化したBとイオ
ン注入によって生じた格子間にあるHgである。イオン
注入領域4近傍にあるイオン注入ダメージ領域からpn
接合を遠ざけるために150〜200℃で1時間程度熱
処理を行う。このとき格子間のHgはp−HgCdTe
層3中のHg空孔を介して拡散し、n- −HgCdTe
領域5を形成しながらpn接合位置は全体的に外側に移
動するが、深さ方向の拡散はAsドーピングされたp−
HgCdTe層2との界面で止まる。これは格子間のH
gの拡散を助けるHg空孔がp−HgCdTe層2にほ
とんどないからである。またこの界面は一連の成長で形
成され、格子定数のズレもないことから格子欠陥等によ
り生じる界面準位やトラップ準位が非常に少ない領域で
ある。その後保護膜6、電極7を形成し素子は完成す
る。An As-doped p-HgCdTe layer 2 is formed on a CdTe substrate 1 by a 5 μm, non-doped HgCd
Te is grown by MBE in order of 5 μm, Hg vacancies are formed in non-doped HgCdTe by p-annealing in an Hg atmosphere, and the p-HgCdTe layer 3 is formed by the Hg vacancies. Thereafter, boron (B) is partially ion-implanted through a mask of about 50 μmφ to form a pn junction.
The ion implantation energy may be about 150 keV. At this time, the activated B and Hg between the lattices generated by the ion implantation serve as the n-type donor. Pn from the ion implantation damage region near the ion implantation region 4
Heat treatment is performed at 150 to 200 ° C. for about 1 hour to keep the junction away. At this time, Hg between lattices is p-HgCdTe
Diffused through the Hg vacancies in layer 3 to form n − -HgCdTe
While the region 5 is formed, the position of the pn junction is moved outward as a whole, but the diffusion in the depth direction is made of As-doped p-type.
It stops at the interface with the HgCdTe layer 2. This is the interstitial H
This is because there is almost no Hg vacancy in the p-HgCdTe layer 2 that assists in the diffusion of g. Further, this interface is formed by a series of growths, and there is no deviation of the lattice constant, so that the interface level and the trap level caused by lattice defects are very small. Thereafter, a protective film 6 and an electrode 7 are formed to complete the device.
【0014】次に動作を簡単に説明する。入射した赤外
線はAsをドーピングしたp−HgCdTe層2、Hg
空孔によるp−HgCdTe層3及びn- −HgCdT
e領域5で吸収され、電子あるいはホールとなって拡散
し、pn接合部分で電気的に分離され、信号として電極
7(p側の電極はここでは省略した)より出力される。
このとき、前述したように本発明の構造では暗電流の原
因となるpn接合近傍での格子欠陥が非常に少ないこと
から、良好な特性のダイオードが得られる。Next, the operation will be briefly described. The incident infrared light is the As-doped p-HgCdTe layer 2, Hg
P-HgCdTe layer 3 and n -- HgCdT by vacancies
It is absorbed in the e-region 5, diffuses as electrons or holes, is electrically separated at the pn junction, and is output as a signal from the electrode 7 (the p-side electrode is omitted here).
At this time, as described above, in the structure of the present invention, since a lattice defect near the pn junction which causes dark current is very small, a diode having excellent characteristics can be obtained.
【0015】以上述べたように本発明を用いれば、歪等
格子欠陥の多いCdTe基板との界面近傍から離れた所
に制御性良くpn接合を形成できるため、熱処理の不確
定さによる素子の歩留まり低下もなく良好な特性のHg
CdTeダイオードを再現良く作製することができる。As described above, according to the present invention, a pn junction can be formed with good controllability away from the vicinity of the interface with the CdTe substrate having many lattice defects such as strains. Hg with good characteristics without reduction
A CdTe diode can be manufactured with good reproducibility.
【0016】本実施例では狭禁制帯幅の化合物半導体と
してp−HgCdTe層を用いた場合について示した
が、Hgの拡散が関与したpn接合形成機構が同等であ
れば材料、プロセス条件等はこれに限るものではない。In this embodiment, the case where a p-HgCdTe layer is used as a compound semiconductor having a narrow band gap is shown. However, if the pn junction formation mechanism involving the diffusion of Hg is equivalent, the material and the process conditions are the same. It is not limited to.
【0017】[0017]
【発明の効果】以上詳細に説明したように、本発明は熱
処理の不確定さによる素子の歩留まり低下もなく、良好
な特性のHgCdTeダイオードを提供し、赤外線検出
器の高性能化に十分貢献するものである。つまり、本発
明においては歪等格子欠陥の多いCdTe基板との界面
近傍から離れた所に制御性良くpn接合を形成でき、そ
の結果として、暗電流の原因となるpn接合近傍での格
子欠陥とにより生じる界面準位やトラップ準位が非常に
少なく、良好な特性のダイオードが得られる。加えて熱
処理の不確定さによる素子の歩留まり低下もなく良好な
特性のHgCdTeダイオードを再現良く作製すること
ができる。 As described above in detail, the present invention provides a HgCdTe diode having good characteristics without a decrease in the yield of the device due to the uncertainty of the heat treatment, and sufficiently contributes to the high performance of the infrared detector. Things. In other words,
In the light, interface with CdTe substrate with many lattice defects such as strain
A pn junction can be formed with good controllability away from the vicinity,
As a result, the case near the pn junction causing dark current
Interface states and trap states caused by
Diodes with few and good characteristics can be obtained. Plus heat
Good device yield without reduction in process uncertainty
Producing HgCdTe Diodes with High Reproducibility
Can be.
【図1】本発明の実施例であるHgCdTeダイオード
を説明するための図である。FIG. 1 is a diagram for explaining an HgCdTe diode according to an embodiment of the present invention.
【図2】従来例のHgCdTeダイオードを説明するた
めの断面図である。FIG. 2 is a cross-sectional view illustrating a conventional HgCdTe diode.
1 CdTe基板 2 Asをドーピングしたp−HgCdTe層 3 Hg空孔によるp−HgCdTe層 4 イオン注入領域 5 n- −HgCdTe領域 6 保護膜 7 電極 8 pn接合界面REFERENCE SIGNS LIST 1 CdTe substrate 2 As-doped p-HgCdTe layer 3 p-HgCdTe layer with Hg vacancies 4 Ion-implanted region 5 n − -HgCdTe region 6 Protective film 7 Electrode 8 pn junction interface
Claims (2)
出器において、基板上にp型ドーパントをドーピングし
た第一の化合物半導体層を有し、前記第一の化合物半導
体層上にHg空孔をアクセプタとしたp型の第二の化合
物半導体層を有し、かつ前記第二の化合物半導体層に、
格子間のHgをドナーとしたn型の領域が形成されてい
る光起電力型赤外線検出器。1. A infrared detector using a compound semiconductor containing Hg, comprises a first compound semiconductor layer doped with p-type dopant on the substrate, wherein the first compound semiconductor
A p-type second compound semiconductor layer having Hg vacancies as an acceptor on the body layer , and the second compound semiconductor layer
A photovoltaic infrared detector in which an n-type region having Hg between lattices as a donor is formed.
ピングして第一の化合物半導体層とする工程と、前記第Ping to form a first compound semiconductor layer;
一の化合物半導体層上にノンドープの化合物半導体層をNon-doped compound semiconductor layer on one compound semiconductor layer
形成しこれをp型化アニールを行うことでHg空孔をアHg vacancies are formed by performing p-type annealing
クセプタとしたp型の第二の化合物層を形成する工程Forming a p-type second compound layer as a ceptor
と、イオン注入及びイオン注入後に熱処理を行うことでAnd heat treatment after ion implantation.
前記第二の化合物層中にpn接合ダイオード形成する工Forming a pn junction diode in the second compound layer
程と、からなることを特徴とする請求項1記載の赤外線2. The infrared ray according to claim 1, wherein the infrared ray comprises:
検出器の製造方法。Manufacturing method of detector.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5295607A JP2699838B2 (en) | 1993-11-25 | 1993-11-25 | Infrared detector and manufacturing method thereof |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5295607A JP2699838B2 (en) | 1993-11-25 | 1993-11-25 | Infrared detector and manufacturing method thereof |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH07147425A JPH07147425A (en) | 1995-06-06 |
JP2699838B2 true JP2699838B2 (en) | 1998-01-19 |
Family
ID=17822819
Family Applications (1)
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JP5295607A Expired - Lifetime JP2699838B2 (en) | 1993-11-25 | 1993-11-25 | Infrared detector and manufacturing method thereof |
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JP (1) | JP2699838B2 (en) |
Families Citing this family (2)
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FR2983351B1 (en) * | 2011-11-28 | 2014-01-24 | Commissariat Energie Atomique | DIODE P / N HOSTRUCTURE CONTROLLED AUTOPOSITIONED ON HGCDTE FOR INFRARED IMAGERS |
CN112582293B (en) * | 2020-12-09 | 2021-08-13 | 北京智创芯源科技有限公司 | Ion activation detection method |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0330479A (en) * | 1989-06-28 | 1991-02-08 | Fujitsu Ltd | Infrared detector |
JPH0555620A (en) * | 1991-08-27 | 1993-03-05 | Mitsubishi Electric Corp | Manufacture of infrared ray sensor element |
JPH05267707A (en) * | 1992-03-18 | 1993-10-15 | Fujitsu Ltd | Semiconductor device |
-
1993
- 1993-11-25 JP JP5295607A patent/JP2699838B2/en not_active Expired - Lifetime
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