JP2006228767A - Mask for extreme ultraviolet ray exposure, mask blank, and exposure method - Google Patents
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- 238000000034 method Methods 0.000 title claims abstract description 11
- 239000010408 film Substances 0.000 claims abstract description 109
- 238000010521 absorption reaction Methods 0.000 claims abstract description 59
- 239000010409 thin film Substances 0.000 claims abstract description 18
- 239000000758 substrate Substances 0.000 claims abstract description 7
- 229910052751 metal Inorganic materials 0.000 claims description 10
- 239000002184 metal Substances 0.000 claims description 10
- 229910052760 oxygen Inorganic materials 0.000 claims description 9
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 claims description 8
- 229910052710 silicon Inorganic materials 0.000 claims description 8
- 230000008033 biological extinction Effects 0.000 claims description 7
- 229910052757 nitrogen Inorganic materials 0.000 claims description 7
- 239000010703 silicon Substances 0.000 claims description 7
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims description 6
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 claims description 6
- 239000001301 oxygen Substances 0.000 claims description 6
- 239000000470 constituent Substances 0.000 claims description 4
- 230000001678 irradiating effect Effects 0.000 claims description 4
- 238000007689 inspection Methods 0.000 abstract description 13
- 238000010894 electron beam technology Methods 0.000 abstract description 10
- 230000007547 defect Effects 0.000 abstract description 7
- 230000003287 optical effect Effects 0.000 description 14
- 239000007789 gas Substances 0.000 description 12
- 238000005546 reactive sputtering Methods 0.000 description 7
- 239000011521 glass Substances 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 4
- 239000000463 material Substances 0.000 description 4
- 239000004065 semiconductor Substances 0.000 description 4
- 238000004544 sputter deposition Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 229910006249 ZrSi Inorganic materials 0.000 description 2
- 238000004364 calculation method Methods 0.000 description 2
- 150000001875 compounds Chemical class 0.000 description 2
- 229920001940 conductive polymer Polymers 0.000 description 2
- 238000010292 electrical insulation Methods 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 239000011261 inert gas Substances 0.000 description 2
- 238000001459 lithography Methods 0.000 description 2
- 229910052750 molybdenum Inorganic materials 0.000 description 2
- 238000000206 photolithography Methods 0.000 description 2
- 238000002310 reflectometry Methods 0.000 description 2
- 101100269850 Caenorhabditis elegans mask-1 gene Proteins 0.000 description 1
- ZOKXTWBITQBERF-UHFFFAOYSA-N Molybdenum Chemical compound [Mo] ZOKXTWBITQBERF-UHFFFAOYSA-N 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000008094 contradictory effect Effects 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 238000001900 extreme ultraviolet lithography Methods 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 230000031700 light absorption Effects 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 239000011733 molybdenum Substances 0.000 description 1
- 150000004767 nitrides Chemical class 0.000 description 1
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Abstract
Description
本発明は、極端紫外線露光用マスク、マスクブランク、及び露光方法に係り、特に、極端紫外線を露光光として用いてパターン露光を行うための反射型のフォトマスク、マスクブランク、及び露光方法に関する。 The present invention relates to an extreme ultraviolet exposure mask, a mask blank, and an exposure method, and more particularly, to a reflective photomask, a mask blank, and an exposure method for performing pattern exposure using extreme ultraviolet light as exposure light.
半導体集積回路の微細化技術の進歩に伴い、微細化のためのフォトリソグラフィ技術に使用される光の波長は次第に短くなってきている。 With the progress of miniaturization technology of semiconductor integrated circuits, the wavelength of light used in photolithography technology for miniaturization has been gradually shortened.
即ち、光源として、これまで使用されて来たKrFエキシマレーザ(波長248nm)からArFエキシマレーザ(波長193nm)に切り替わりつつあり、更にはF2エキシマレーザ(波長157nm)の使用が提案され、開発されている。 That is, as a light source, the KrF excimer laser (wavelength 248 nm) that has been used so far is being switched to an ArF excimer laser (wavelength 193 nm), and the use of an F2 excimer laser (wavelength 157 nm) has been proposed and developed. Yes.
しかし、F2エキシマレーザによっても、将来的な50nm以下の線幅を有するデバイスを作製するためのリソグラフィ技術として用いるには、露光機やレジストの課題もあり、容易ではない。このため、エキシマレーザ光より波長が一桁以上短い(10〜15nm)極端紫外線(Extreme UV、以下EUVと略記)を用いた、EUVリソグラフィの研究開発が進められている。 However, even with the F2 excimer laser, it is not easy to use it as a lithography technique for manufacturing a device having a line width of 50 nm or less in the future due to exposure apparatus and resist problems. For this reason, research and development on EUV lithography using extreme ultraviolet (Extreme UV, hereinafter abbreviated as EUV) whose wavelength is one or more orders of magnitude shorter than that of excimer laser light (10 to 15 nm) is being advanced.
EUV露光は、特に、45nm以下の線幅を有するデバイスを作製するための有力なリソグラフィの候補であり、2010年頃からのデバイス量産への適用が予測されている。 EUV exposure is particularly a promising lithography candidate for producing devices having a line width of 45 nm or less, and application to device mass production from around 2010 is predicted.
EUV露光では、上述のように波長が短いため、物質の屈折率が殆ど真空の値に近く、材料間の光吸収の差も小さい。このため、EUV領域では、従来の透過型の屈折光学系を組むことが出来ず、反射光学系となり、従ってマスクも反射型マスクとなる。これまで開発されてきた一般的なEUVマスクは、Siウェハーやガラス基板上に、例えばMoとSiからなる2層膜を40対ほど積層した多層膜部分を高反射領域とし、その上に低反射領域(吸収膜)として金属膜のパターンを形成した構造を有する。 In EUV exposure, since the wavelength is short as described above, the refractive index of a substance is almost close to the value of vacuum, and the difference in light absorption between materials is also small. For this reason, in the EUV region, a conventional transmissive refractive optical system cannot be assembled, resulting in a reflective optical system, and thus the mask is also a reflective mask. A general EUV mask that has been developed so far is a highly reflective region in which a multilayer film part of, for example, about 40 pairs of two-layer films made of Mo and Si is stacked on a Si wafer or glass substrate, and a low-reflection film on the multilayer film. It has a structure in which a metal film pattern is formed as a region (absorption film).
このようなEUVマスクのパターンの欠陥検査においては、線幅が小さいため、波長の短いDUV(遠紫外線)による反射光が用いられる。検査精度を上げるには、DUV光に対する多層膜部の反射率をR1、吸収膜部の反射率をR2とするときのコントラストC=(R1−R2)/(R1+R2)×100%を、少なくとも50%以上とする必要がある。 In such a defect inspection of the EUV mask pattern, since the line width is small, reflected light by DUV (far ultraviolet) having a short wavelength is used. In order to increase the inspection accuracy, the contrast C = (R1−R2) / (R1 + R2) × 100% when the reflectance of the multilayer film portion with respect to DUV light is R1 and the reflectance of the absorption film portion is R2 is at least 50%. % Or more is necessary.
また、マスク作製プロセスにおける電子線描画時に電子線レジストの下地である吸収膜の電気絶縁性が大きいと、チャージアップが生じ、描画パターンの位置ずれが起きるので、吸収膜のシート抵抗Rsは低くする必要がある。 In addition, if the electric insulation of the absorption film, which is the base of the electron beam resist, is large during electron beam drawing in the mask manufacturing process, charge-up occurs and the drawing pattern is displaced, so the sheet resistance Rs of the absorption film is lowered. There is a need.
しかし、多層膜とのコントラストを高くし、しかも電気絶縁性の低い吸収膜材料は、これまで見出されていない。
本発明は、以上の事情に鑑みてなされ、DUV露光による欠陥検査性能を向上させるとともに、電子線描画の際に位置ずれが生ずることのない極端紫外線露光用マスク、そのためのマスクブランク、及びそのようなマスクを用いた露光方法を提供することを目的とする。 The present invention has been made in view of the above circumstances, improves the defect inspection performance by DUV exposure, and does not cause misalignment during electron beam drawing, an extreme ultraviolet exposure mask, and a mask blank therefor, and so on. An object of the present invention is to provide an exposure method using a simple mask.
本発明者らは、上記課題を解決するため、検討を重ねた結果、DUV露光による欠陥検査性能を向上させるために、多層膜とのコントラストを大きくとることが出来るとともに、電子線描画の際に位置ずれが生ずることがないように、電気絶縁性の低い、吸収膜の材質及び膜構造を見出した。本発明は、このような知見に基づくものである。 As a result of repeated studies to solve the above-mentioned problems, the present inventors can increase the contrast with the multilayer film in order to improve the defect inspection performance by DUV exposure, and at the time of electron beam drawing. The present inventors have found a material and a film structure of an absorption film having low electrical insulation so as not to cause displacement. The present invention is based on such knowledge.
即ち、本発明の第1の態様は、基板上に形成された多層膜からなる高反射層と、前記多層膜上に形成された吸収膜からなる低反射層とを備える極端紫外線露光用マスクブランクにおいて、前記吸収膜は、2層以上の薄膜からなり、その最上層の薄膜は、波長150nmから300nmの紫外線に対する消衰係数が0から1.2の範囲にあり、シート抵抗が50MΩ/□以下であることを特徴とする極端紫外線露光用マスクブランクを提供する。 That is, the first aspect of the present invention is an extreme ultraviolet exposure mask blank comprising a high reflection layer comprising a multilayer film formed on a substrate and a low reflection layer comprising an absorption film formed on the multilayer film. The absorption film is composed of two or more thin films, and the uppermost thin film has an extinction coefficient in the range of 0 to 1.2 with respect to ultraviolet light having a wavelength of 150 nm to 300 nm, and a sheet resistance of 50 MΩ / □ or less. An extreme ultraviolet exposure mask blank is provided.
以上のように構成される極端紫外線露光用マスクブランクにおいて、吸収膜の最上層の薄膜は、波長150nmから300nmの紫外線に対する消衰係数が0.1から1.0の範囲にあるものとすることが出来る。また、吸収膜の最上層の薄膜は、波長150nmから300nmの紫外線に対する屈折率が1.5から2.5の範囲にあるものとすることが出来る。 In the extreme ultraviolet exposure mask blank configured as described above, the uppermost thin film of the absorption film has an extinction coefficient in the range of 0.1 to 1.0 for ultraviolet light having a wavelength of 150 nm to 300 nm. I can do it. In addition, the uppermost thin film of the absorption film may have a refractive index in the range of 1.5 to 2.5 with respect to ultraviolet rays having a wavelength of 150 nm to 300 nm.
更に、吸収膜の最上層の薄膜は、金属、珪素、及び酸素を主たる構成元素として含むものとすることが出来る。また、吸収膜の最上層の薄膜は、金属、珪素、酸素、及び窒素を主たる構成元素として含むものとすることが出来る。 Further, the uppermost thin film of the absorption film can contain metal, silicon, and oxygen as main constituent elements. In addition, the uppermost thin film of the absorption film can contain metal, silicon, oxygen, and nitrogen as main constituent elements.
本発明の第2の態様は、上述した極端紫外線露光用マスクブランクの前記吸収層を吸収層パターンに形成してなることを特徴とする極端紫外線露光用マスクを提供する。 According to a second aspect of the present invention, there is provided an extreme ultraviolet exposure mask, wherein the absorption layer of the above-described extreme ultraviolet exposure mask blank is formed into an absorption layer pattern.
また、本発明の第3の態様は、上述した極端紫外線露光用マスクに極端紫外線を照射し、その反射光を被露光体に照射することを特徴とする露光方法を提供する。 According to a third aspect of the present invention, there is provided an exposure method characterized by irradiating the above-mentioned extreme ultraviolet exposure mask with extreme ultraviolet light and irradiating the object with the reflected light.
本発明によると、吸収膜を2層以上の薄膜により構成し、その最上層の薄膜を、波長150nmから300nmの紫外線に対する消衰係数が0から1.2の範囲にあり、シート抵抗が50MΩ/□以下であるものとすることにより、DUV露光による欠陥検査性能を向上させるとともに、電子線描画の際に位置ずれが生ずることのない極端紫外線露光用マスクのためのマスクブランクを得ることが出来る。 According to the present invention, the absorption film is composed of two or more thin films, and the uppermost thin film has an extinction coefficient in the range of 0 to 1.2 with respect to ultraviolet light having a wavelength of 150 nm to 300 nm, and a sheet resistance of 50 MΩ / By making the following, it is possible to improve the defect inspection performance by DUV exposure and to obtain a mask blank for an extreme ultraviolet exposure mask that does not cause misalignment during electron beam drawing.
以下、発明を実施するための最良の形態について説明する。 The best mode for carrying out the invention will be described below.
図1は、本発明の一実施形態に係る極端紫外線露光用マスクを示す断面図である。図1に示すように、極端紫外線露光用マスク1は、低熱膨張ガラス基板2と、この低熱膨張ガラス基板2上に形成された高反射部3と、この高反射部3上に形成されたキャップ層4と、このキャップ層4の一部の上に形成された低反射部5とを備える。
FIG. 1 is a sectional view showing an extreme ultraviolet exposure mask according to an embodiment of the present invention. As shown in FIG. 1, an extreme
高反射部3としては、例えば、モリブデン層とシリコン層を交互に、例えば40対成膜してなる積層体を用いることが出来る。この積層体の合計の厚さは、例えば2.5〜3.0μmである。
As the highly
キャップ層4としては、例えば厚さ11nmのシリコン膜を用いることが出来る。
As the
低反射部5は、2層以上の薄膜からなる吸収膜であり、図1では、上層吸収膜5aと下層吸収膜5bからなる2層の場合を示している。なお、キャップ層4と下層吸収膜5bとの間には緩衝膜6が設けられているが、これは必ずしも設けなくてもよい。
The
下層吸収膜5bは、主としてEUV光を吸収する膜であり、例えば、吸収能の大きいTa成分を多く含むTaSi膜が採用され、十分なEUV光の吸収を担うために、700A前後の厚めの膜厚が採用される。また、TaSi膜は、同時に、欠陥検査に用いるDUV光に対する吸収性も大きい。
The
下層吸収膜5bは、膜厚の厚い膜でもあることから、下層吸収膜5b内に入射したDUV光はほとんど下層吸収膜5b内で吸収されてしまう。このため、以下の検討結果は、下層吸収膜5bより下にある緩衝膜にはほとんど影響されない。
Since the
一方、上層吸収膜5aは、主としてDUV光に対する反射率(R2)を、薄膜干渉効果により低減するための反射防止効果を担う膜である。従って、上層吸収膜5aは、DUV光に対してもある程度透明な膜である必要があり、膜厚は50〜300A、例えば、せいぜい200A程度が反射防止効果上好適である。 On the other hand, the upper-layer absorption film 5a is a film mainly responsible for an antireflection effect for reducing the reflectivity (R2) with respect to DUV light by the thin film interference effect. Therefore, the upper-layer absorption film 5a needs to be a film that is transparent to some extent with respect to DUV light, and a film thickness of 50 to 300A, for example, about 200A at most is suitable for the antireflection effect.
本発明者らは、高反射部と低反射部との高いコントラスが得られ、かつ低反射部の表面のシート抵抗が低い、最適な上層吸収膜5aを求めるために、上層吸収膜5aの光学定数と反射率コントラストとの関係について各種の計算を行った。 In order to obtain an optimum upper-layer absorption film 5a in which the high contrast between the high-reflection portion and the low-reflection portion is obtained and the sheet resistance of the surface of the low-reflection portion is low, the present inventors Various calculations were performed on the relationship between the constant and the reflectance contrast.
なお、吸収膜上層膜のコントラストCは、下記の式により定義した。 Note that the contrast C of the upper film of the absorbing film was defined by the following equation.
C=(R1−R2)/(R1+R2)×100%
R1:高反射部の反射率
R2:低反射部の反射率
上層吸収膜5aの光学定数と反射率コントラストとの関係についての計算結果を、図2〜図5に示す。なお、下層吸収膜5bを700Aの膜厚のTaSi膜とし、図では、上層吸収膜5aの光学定数(屈折率:n、消衰係数:k)をそれぞれ横軸、縦軸として、コントラストCを等高線で表している。
C = (R1-R2) / (R1 + R2) × 100%
R1: Reflectivity of the high reflection portion R2: Reflectance of the low reflection portion The calculation results regarding the relationship between the optical constant of the upper-layer absorption film 5a and the reflectance contrast are shown in FIGS. Note that the
上層吸収膜5bの膜厚を150A、200A、250Aの3種とし、検査波長(DUV光)は257nm、193nmの2種で代表させている。
The film thickness of the
即ち、図2は、上層吸収膜5bの膜厚が200A、検査波長が257nmの場合、図3は、上層吸収膜5bの膜厚が200A、検査波長が193nmの場合、図4は、上層吸収膜5bの膜厚が150A、検査波長が193nmの場合、図5は、上層吸収膜5bの膜厚が250A、検査波長が193nmの場合をそれぞれ示す。
That is, FIG. 2 shows the case where the film thickness of the
図2〜図5から、次のことが分る。 The following can be seen from FIGS.
即ち、検査波長が短くなると、n、kの最適範囲(コントラストCが高い範囲)は、nは小さくなる方向へ、kは大きくなる方向へ移動する。同様に、上層吸収膜5bの膜厚が厚くなると、nが小さくなる方向へ、最適範囲は移動する。
That is, when the inspection wavelength is shortened, the optimum range of n and k (the range where the contrast C is high) moves in a direction where n becomes smaller and k becomes larger. Similarly, when the thickness of the
しかし、どの場合においても、上層吸収膜5aのkの好適な範囲は0〜1.2付近であることがわかる。kの最適な値は、0.3付近である。同様に、nの好適な範囲は1.5〜2.5付近である。 However, in any case, it can be seen that the preferable range of k of the upper absorption film 5a is around 0 to 1.2. The optimum value of k is around 0.3. Similarly, a preferred range for n is around 1.5 to 2.5.
上述したように、上層吸収膜5aは、0<k<1.2の比較的透明な膜である必要がある。従って、上層吸収膜5aの材質としては、単なる金属膜を用いることは出来ず、酸素や窒素を含む化合物膜の方がよい。これらの酸化物膜や窒化物膜は、例えば、通常の不活性ガスに酸素や窒素などの反応性ガスを混合した反応性スパッタリングにより作製することができる。 As described above, the upper absorption film 5a needs to be a relatively transparent film with 0 <k <1.2. Accordingly, a simple metal film cannot be used as the material of the upper absorption film 5a, and a compound film containing oxygen or nitrogen is better. These oxide films and nitride films can be produced, for example, by reactive sputtering in which a reactive gas such as oxygen or nitrogen is mixed with a normal inert gas.
ところで、透明な膜ほど電気的な絶縁性が大きく、このような膜上で電子線描画すると、チャージアップして、パターンの位置ずれが生じてしまうので、透明な膜は電子線描画に不適である。そのため、絶縁性の大きい膜を電子線描画する場合、チャージアップを防止するために、電子線レジスト上に、シート抵抗が通常50MΩ/□程度の導電性ポリマーを塗布している。しかし、導電ポリマーの使用は、工程数や欠陥増加の要因となるので望ましくない。 By the way, a transparent film has a higher electrical insulating property, and if electron beam drawing is performed on such a film, the pattern is displaced and the position of the pattern is shifted. Therefore, the transparent film is not suitable for electron beam drawing. is there. Therefore, when an electron beam is drawn on a highly insulating film, a conductive polymer having a sheet resistance of usually about 50 MΩ / □ is applied on the electron beam resist in order to prevent charge-up. However, the use of a conductive polymer is undesirable because it increases the number of processes and defects.
そこで、上層吸収膜5aに必要な特性として、光学的な透明性と電気的な導電性という、相反する2つの特性を両立するよう、最適な上層吸収膜5aを得ることが必要となる。
ところで、金属ターゲットを用いて反応性スパッタリングを行っていくとき、不活性ガスに対する反応性ガスの混合比が小さいうちは、金属性の遮光性膜が得られ、ある混合比以上で急激に非金属製の透明膜となる。従って上記のような、透明性と導電性の両立する膜をこの方法で得ることは困難である。
Therefore, it is necessary to obtain the optimum upper-layer absorption film 5a so as to satisfy two contradictory characteristics such as optical transparency and electrical conductivity as necessary characteristics for the upper-layer absorption film 5a.
By the way, when performing reactive sputtering using a metal target, a metallic light-shielding film can be obtained while the mixing ratio of the reactive gas to the inert gas is small. It becomes a transparent film. Accordingly, it is difficult to obtain a film having both transparency and conductivity as described above by this method.
遮光性から透明性への急激な変化を緩和するには、金属ターゲットではなく、金属と、半導体である珪素(Si)を含む化合物ターゲットを用いて、反応性スパッタリングを行えばよい。 In order to mitigate a rapid change from light shielding properties to transparency, reactive sputtering may be performed using a compound target including a metal and silicon (Si), which is a semiconductor, instead of a metal target.
この場合、金属に対しSiの組成比が大きすぎると、透明な膜にはなりやすいが、シート抵抗<50MΩ/□を満たすことが困難となり、結局、透明性と導電性の両立する膜を得ることが困難となる。 In this case, if the composition ratio of Si with respect to the metal is too large, a transparent film tends to be formed, but it becomes difficult to satisfy the sheet resistance <50 MΩ / □, and eventually a film having both transparency and conductivity is obtained. It becomes difficult.
下記表1に、TaSi2をターゲットとし、ArとO2の混合ガスをスパッタガスとして用いて、反応性スパッタリングで作製したTaSixOy膜について、光学定数(n、k)とシート抵抗を測定した結果を示す。
下記表2に、TaSi2をターゲットとし、ArとN2及びO2の混合ガスをスパッタガスとして用いて、反応性スパッタリングで作製したTaSixOyNz膜について、光学定数(n、k)とシート抵抗を測定した結果を示す。
下記表3に、ZrSi2をターゲットとし、ArとO2の混合ガスをスパッタガスとして用いて、反応性スパッタリングで作製したZrSixOy膜について、光学定数(n、k)とシート抵抗を測定した結果を示す。ArとO2の総流量は、40SCCMで一定である。
下記表4に、ZrSi2をターゲットとし、ArとN2Oの混合ガスをスパッタガスとして用いて、反応性スパッタリングで作製したZrSixOyNz膜について、光学定数(n、k)とシート抵抗を測定した結果を示す。ArとN2Oの総流量は、40SCCMで一定である。
上記表1〜表4から明らかなように、ターゲット材料とガス流量などの成膜条件を適切に選択することにより、所望の透明性(光学定数)と導電性(シート抵抗)を両立させた上層吸収膜を得ることが出来る。 As is apparent from Tables 1 to 4, an upper layer that achieves both desired transparency (optical constant) and conductivity (sheet resistance) by appropriately selecting the target material and film formation conditions such as gas flow rate. An absorption film can be obtained.
即ち、消衰係数が0から1.2の範囲、シート抵抗が50MΩ/□以下となるようなガス流量を選択することにより、極端紫外線露光用マスクに好適な上層吸収膜を形成することが可能である。 That is, by selecting a gas flow rate such that the extinction coefficient is in the range of 0 to 1.2 and the sheet resistance is 50 MΩ / □ or less, an upper-layer absorption film suitable for an extreme ultraviolet exposure mask can be formed. It is.
本発明に係る極端紫外線露光用マスクは、半導体集積回路の製造のためのフォトリソグラフィ技術等に好適に使用することが可能であり、半導体の分野において非常に有用である。 The extreme ultraviolet exposure mask according to the present invention can be suitably used in a photolithography technique or the like for manufacturing a semiconductor integrated circuit, and is very useful in the field of semiconductors.
1…極端紫外線露光用マスク、2…低熱膨張ガラス基板、3…高反射部、4…キャップ層、5…低反射部、5a…上層吸収膜、5b…下層吸収膜、6…緩衝膜。
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