JPH04202094A - Production of superconducting thin film - Google Patents
Production of superconducting thin filmInfo
- Publication number
- JPH04202094A JPH04202094A JP2335147A JP33514790A JPH04202094A JP H04202094 A JPH04202094 A JP H04202094A JP 2335147 A JP2335147 A JP 2335147A JP 33514790 A JP33514790 A JP 33514790A JP H04202094 A JPH04202094 A JP H04202094A
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- superconducting thin
- oxide superconducting
- oxide
- buffer layer
- 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.)
- Pending
Links
- 239000010409 thin film Substances 0.000 title claims description 46
- 238000004519 manufacturing process Methods 0.000 title claims description 10
- 239000000758 substrate Substances 0.000 claims description 16
- 238000000034 method Methods 0.000 claims description 11
- 239000000463 material Substances 0.000 description 17
- 235000012431 wafers Nutrition 0.000 description 17
- 239000002131 composite material Substances 0.000 description 7
- 239000013078 crystal Substances 0.000 description 7
- 239000002887 superconductor Substances 0.000 description 6
- 239000010408 film Substances 0.000 description 5
- 229910021521 yttrium barium copper oxide Inorganic materials 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- MCMNRKCIXSYSNV-UHFFFAOYSA-N Zirconium dioxide Chemical compound O=[Zr]=O MCMNRKCIXSYSNV-UHFFFAOYSA-N 0.000 description 2
- 238000001816 cooling Methods 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 229910002244 LaAlO3 Inorganic materials 0.000 description 1
- 238000009825 accumulation Methods 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000005336 cracking Methods 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 238000003746 solid phase reaction Methods 0.000 description 1
- 238000010671 solid-state reaction Methods 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
Landscapes
- Crystals, And After-Treatments Of Crystals (AREA)
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Oxygen, Ozone, And Oxides In General (AREA)
- Inorganic Compounds Of Heavy Metals (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、酸化物超電導薄膜の作製方法に関する。より
詳細には、本発明は、Y系等のCu複合酸化物による超
電導薄膜を、特にSiウェハを下地基板として作製する
ための新規な方法に関する。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a method for producing an oxide superconducting thin film. More specifically, the present invention relates to a novel method for producing a superconducting thin film using a Y-based Cu complex oxide, particularly using a Si wafer as a base substrate.
従来の技術
超電導現象は、液体ヘリウムによる冷却が必須な極低温
における固有の現象であるとかつては考えられていた。Conventional technology Superconductivity was once thought to be a unique phenomenon at extremely low temperatures that require cooling with liquid helium.
しかしながら、1986年にベドノーツ、ミューラー等
によって、30にで超電導状態を示す(La、 Ba)
2CU○、が発見されて以来、1987年には、チュ
ー等によって90に台の超電導臨界温度Tcを有するY
Ba2CU30y発見され、続いて、1988年には前
出等によって100に以上の臨界温度を示す所謂Bi系
の複合酸化物系超電導材料が発見された。However, in 1986, Bednotes, Muller et al. showed a superconducting state at 30°C (La, Ba).
Since the discovery of 2CU○, in 1987, Chu et al.
Ba2CU30y was discovered, and subsequently, in 1988, the so-called Bi-based composite oxide superconducting material having a critical temperature of 100 degrees or higher was discovered by the aforementioned et al.
これらの一連の複合酸化物系超電導材料は、廉価な液体
窒素による冷却で超電導現象を実現することができるの
で、超電導技術の実用的な応用の可能性が俄に取り沙汰
されるようになった。These series of composite oxide-based superconducting materials can achieve superconductivity by cooling with inexpensive liquid nitrogen, so the possibility of practical application of superconducting technology has suddenly begun to be discussed.
当初、これらの複合酸化物系超電導材料は、固相反応法
による焼結体として合成されていたが、その後の研究の
進捗により、今日では、薄膜として作製することにより
、極めて品質の高いものが得られるようになってきた。Initially, these composite oxide-based superconducting materials were synthesized as sintered bodies using a solid-state reaction method, but as a result of subsequent research progress, today it is possible to fabricate them as thin films of extremely high quality. I'm starting to get it.
但し、これらの複合酸化物は、それぞれに複雑な結晶構
造を有し、特定の基板上に特定の条件で成膜した場合に
のみ有効な超電導特性を発揮する相を形成する。即ち、
酸化物超電導薄膜の下地基板としては、MgO単結晶基
板、5rTiO+単結晶基板等が使用されている。However, each of these composite oxides has a complex crystal structure and forms a phase that exhibits effective superconducting properties only when it is formed on a specific substrate under specific conditions. That is,
As the underlying substrate for the oxide superconducting thin film, an MgO single crystal substrate, a 5rTiO+ single crystal substrate, etc. are used.
発明が解決しようとする課題
しかしながら、上述のような酸化物単結晶基板は、一般
に高価な上に供給が少なく、酸化物超電導体の実用化を
考えた場合に極めて不利な要件のひとつであると考えら
れている。また、酸化物基板は大径のものが人手し難く
、酸化物超電導薄膜が今後大面積化してい(ことを考え
た場合に適切な材料とは考え難い。Problems to be Solved by the Invention However, the above-mentioned oxide single crystal substrates are generally expensive and in short supply, which is one of the extremely disadvantageous requirements when considering the practical use of oxide superconductors. It is considered. In addition, it is difficult to handle large-diameter oxide substrates manually, and considering that oxide superconducting thin films will have larger areas in the future, it is difficult to consider this material to be an appropriate material.
そこで、廉価且つ高品質な基板材料として現在量も安定
に供給されているSiウェハを下地基板として酸化物超
電導薄膜を作製することが提案されている。ところが、
Siウェハと酸化物超電導体とは、熱膨張率差が非常に
大きい。即ち、S1単結晶の熱膨張率が2.4程度であ
るのに対して、代表的な酸化物超電導体であるY系複合
酸化物の熱膨張率は14以上もある。このため、Siウ
ェハ上に酸化物超電導薄膜を成膜した場合、熱的なミス
マツチのためにクラックを生じてしまう。Therefore, it has been proposed to fabricate an oxide superconducting thin film using a Si wafer, which is currently stably supplied as an inexpensive and high-quality substrate material, as a base substrate. However,
There is a very large difference in thermal expansion coefficient between a Si wafer and an oxide superconductor. That is, while the coefficient of thermal expansion of the S1 single crystal is about 2.4, the coefficient of thermal expansion of the Y-based composite oxide, which is a typical oxide superconductor, is 14 or more. For this reason, when an oxide superconducting thin film is formed on a Si wafer, cracks occur due to thermal mismatch.
そこで、本発明は、上記従来技術の問題点を解決し、S
Iウェハ上に、クラックを生じることなく酸化物超電導
薄膜を成膜することができる新規な超電導薄膜の作製方
法を提供することをその目的としている。Therefore, the present invention solves the problems of the prior art and
The purpose of the present invention is to provide a novel method for producing a superconducting thin film that can form an oxide superconducting thin film on an I-wafer without causing cracks.
課題を解決するための手段
即ち、本発明に従うと、Siウェハを下地基板として酸
化物超電導薄膜を作製する方法において、S]ウェハ上
に、目的とする酸化物超電導薄膜よりも格子定数の小さ
な酸化物によりバッファ層を形成する工程と、該バッフ
ァ層上に酸化物超電導薄膜を成膜する工程とを含むこと
を特徴とする超電導薄膜の作製方法が提供される。Means for Solving the Problems According to the present invention, in a method for producing an oxide superconducting thin film using a Si wafer as a base substrate, an oxide film having a smaller lattice constant than the target oxide superconducting thin film is formed on the S] wafer. A method for producing a superconducting thin film is provided, which includes the steps of forming a buffer layer using a material, and forming an oxide superconducting thin film on the buffer layer.
芥月
本発明に係る酸化物超電導薄膜の作製方法においては、
酸化物超電導薄膜の成膜に先立って、81基板上に、酸
化物超電導薄膜よりも格子定数の小さい材料により形成
したバッファ層を形成する工程を含んでいる。In the method for producing an oxide superconducting thin film according to the present invention,
Prior to forming the oxide superconducting thin film, the method includes a step of forming a buffer layer made of a material having a smaller lattice constant than the oxide superconducting thin film on the 81 substrate.
ここで、バッファ層とは、その直上に酸化物超電導薄膜
を成膜し得る特定の材料層を指している。Here, the buffer layer refers to a specific material layer on which an oxide superconducting thin film can be formed.
即ち、高品質な酸化物超電導薄膜を形成するために下地
材料に要求される特性は、
■酸化物超電導薄膜との格子定数のマツチングがよいこ
と、
■下地材料と酸化物超電導薄膜との間での元素の相互拡
散が小さいこと、
である。しかしながら、Slは、格子定数については酸
化物超電導体とのマツチングが良好であるが、通常の酸
化物超電導薄膜の成膜温度(700℃前後)では元素の
相互拡散が激しく、Siウェハを下地基板として酸化物
超電導薄膜を作製しても、超電導特性が著しく低いか、
または消失してしまうことが知られている。In other words, the properties required of the base material in order to form a high-quality oxide superconducting thin film are: 1. Good lattice constant matching with the oxide superconducting thin film; 2. Good lattice constant matching between the base material and oxide superconducting thin film. The interdiffusion of the elements is small. However, although Sl has good matching with oxide superconductors in terms of lattice constant, at the normal deposition temperature of oxide superconducting thin films (around 700°C), interdiffusion of elements is severe, and Si wafers are used as base substrates. Even if we create an oxide superconducting thin film, the superconducting properties are extremely low, or
Or it is known to disappear.
そこで、酸化物超電導薄膜の下地となる結晶構造を有し
、且つ、Siの拡散に対して障壁となるような材料によ
ってバッファ層を形成することが既に提案されている。Therefore, it has already been proposed to form a buffer layer using a material that has a crystal structure that serves as a base for the oxide superconducting thin film and that acts as a barrier to Si diffusion.
但し、このような従来のバッファ層は、Siウェハとの
熱的なミスマツチによる酸化物超電導薄膜の特性劣化に
ついては充分に配慮されていなかった。即ち、−船釣な
方法として、Slの熱膨張係数と酸化物超電導体の熱膨
張係数との中間の熱膨張係数を有するバッファ層を形成
することにより、酸化物超電導薄膜の熱歪を緩和する方
法がある。しかしながら、このような方法では、Siウ
ェハの厚さに対してバッファ層の厚さが非常に薄いので
、クラックの発生を有効に解決することはできなかった
。However, in such a conventional buffer layer, sufficient consideration has not been given to deterioration of the characteristics of the oxide superconducting thin film due to thermal mismatch with the Si wafer. That is, as a simple method, the thermal strain of the oxide superconductor thin film is alleviated by forming a buffer layer having a thermal expansion coefficient intermediate between that of Sl and that of the oxide superconductor. There is a way. However, in this method, since the thickness of the buffer layer is very thin compared to the thickness of the Si wafer, it has not been possible to effectively solve the problem of cracking.
これに対して、本発明に係る方法においては、酸化物超
電導薄膜よりも格子定数の小さい材料によりバッファ層
を形成することにより、その熱歪を格子歪により相殺す
ることが可能である。On the other hand, in the method according to the present invention, by forming the buffer layer from a material having a smaller lattice constant than that of the oxide superconducting thin film, it is possible to offset the thermal strain by the lattice strain.
即ち、一般に、格子定数の異なる材料をエピタキシャル
成長させた場合、その格子不整合によって歪が導入され
る。即ち、例えば、基板の格子定数をa5、薄膜の格子
定数をafとしたとき、a5<afのときには薄膜に圧
縮歪が、as>afのときには薄膜に引張歪が作用する
。That is, in general, when materials with different lattice constants are epitaxially grown, strain is introduced due to the lattice mismatch. That is, for example, when the lattice constant of the substrate is a5 and the lattice constant of the thin film is af, compressive strain acts on the thin film when a5<af, and tensile strain acts on the thin film when as>af.
一方、Siウェハ上に酸化物超電導薄膜を成膜する場合
、熱膨張係数差により酸化物超電導薄膜に作用する熱歪
は引張力向である。従って、酸化物超電導薄膜よりも格
子定数の小さい材料でバッファ層を形成することにより
、酸化物超電導薄膜に格子不整合による圧縮歪を印加さ
せ、薄膜に作用する引張力向の歪を緩和させるこができ
る。On the other hand, when forming an oxide superconducting thin film on a Si wafer, the thermal strain acting on the oxide superconducting thin film due to the difference in thermal expansion coefficient is in the direction of tensile force. Therefore, by forming the buffer layer with a material whose lattice constant is smaller than that of the oxide superconducting thin film, compressive strain due to lattice mismatch can be applied to the oxide superconducting thin film, and strain in the direction of the tensile force acting on the thin film can be alleviated. I can do it.
尚、上述のような本発明に係る方法においてバッファ層
として使用し得る材料としては、Y2O3、ZrO2、
YへI○3、LaAlO3及びその積層構造等を例示す
ることができる。In addition, materials that can be used as the buffer layer in the method according to the present invention as described above include Y2O3, ZrO2,
Examples of Y include I○3, LaAlO3, and a stacked structure thereof.
以下、実施例を挙げて本発明をより具体的に説明するが
、以下の開示はあくまでも本発明の一実施例に過ぎず、
本発明の技術的範囲を何ら限定するものではない。Hereinafter, the present invention will be described in more detail with reference to Examples, but the following disclosure is merely an example of the present invention.
This is not intended to limit the technical scope of the present invention in any way.
実施例
直径2インチの81単結晶ウエハを複数用意し、Y−B
a−Cuの複合酸化物超電導薄膜く以下、”YBCO”
と記載する)を成膜した。Example A plurality of 81 single crystal wafers with a diameter of 2 inches were prepared, and Y-B
a-Cu composite oxide superconducting thin film, hereinafter referred to as “YBCO”
) was formed into a film.
まず、YBCOの格子定数よりも小さな格子定数を有す
るバッファ層として、下記の第1表に示す材料を使用し
てバッファ層を形成した。バッファ層の成膜はスパッタ
リング法により行った。成膜条件は、第1表に併せて示
す通りである。First, a buffer layer having a lattice constant smaller than that of YBCO was formed using the materials shown in Table 1 below. The buffer layer was formed by sputtering. The film forming conditions are also shown in Table 1.
第1表
上述のようにしてバッファ層を形成した各Siウヱハ上
に、Y −Ba−Cuの複合酸化物薄膜を成膜した。ま
た、比較のために、YBCOよりも格子定数が大きいM
g O、SrT+ 03を材料とするバッファ層を成膜
したSiウェハと、バッファ層のないSiウェハとを用
意し、各比較試料にも同じ酸化物超電導薄膜を成膜した
。成膜方法はスパンクリング法とした。成膜条件は下記
の第2表に示す通りである。Table 1 A Y--Ba--Cu composite oxide thin film was formed on each Si wafer on which a buffer layer was formed as described above. Also, for comparison, M, which has a larger lattice constant than YBCO,
A Si wafer on which a buffer layer made of g O, SrT+ 03 was formed and a Si wafer without a buffer layer were prepared, and the same oxide superconducting thin film was formed on each comparative sample. The film formation method was the spankling method. The film forming conditions are as shown in Table 2 below.
第2表
以上のようにして作製した各試料について、酸化物超電
導薄膜の表面性状を観察した。観察結果は、下記の第3
表に示す通りである。The surface properties of the oxide superconducting thin films were observed for each sample prepared as shown in Table 2. The observation results are shown in Section 3 below.
As shown in the table.
第3表
第3表に示すように、本発明に従って酸化物超電導薄膜
を作製することにより、クラックの発生は有効に防止さ
れる。Table 3 As shown in Table 3, the generation of cracks is effectively prevented by producing the oxide superconducting thin film according to the present invention.
発明の詳細
な説明したように、本発明に係る方法によれば、Siウ
ェハを基板として、クラックを発生ずることなく酸化物
超電導薄膜を成膜することができる。As described in detail, according to the method of the present invention, an oxide superconducting thin film can be formed using a Si wafer as a substrate without generating cracks.
Siウェハの使用は、基板が廉価で供給が安定している
ことだけではなく、微細加工技術等についての膨大な技
術的蓄積により、種々のデバイスの作製にも有利に作用
する。また、Siウェハは、相当大径のものが供給され
ており、酸化物超電導薄膜の大面積化にも充分対応でき
る。The use of Si wafers is advantageous not only because the substrates are inexpensive and stable in supply, but also because of the vast technological accumulation of microfabrication techniques and the like in the production of various devices. In addition, Si wafers are supplied with considerably large diameters, and can sufficiently accommodate large-area oxide superconducting thin films.
特許出願人 住友電気工業株式会社Patent applicant: Sumitomo Electric Industries, Ltd.
Claims (1)
る方法において、 Siウェハ上に、目的とする酸化物超電導薄膜よりも格
子定数の小さな酸化物によりバッファ層を形成する工程
と、該バッファ層上に酸化物超電導薄膜を成膜する工程
とを含むことを特徴とする超電導薄膜の作製方法。[Claims] A method for producing an oxide superconducting thin film using a Si wafer as a base substrate, comprising: forming a buffer layer on the Si wafer using an oxide having a smaller lattice constant than the target oxide superconducting thin film; A method for producing a superconducting thin film, the method comprising: forming an oxide superconducting thin film on the buffer layer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2335147A JPH04202094A (en) | 1990-11-30 | 1990-11-30 | Production of superconducting thin film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2335147A JPH04202094A (en) | 1990-11-30 | 1990-11-30 | Production of superconducting thin film |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH04202094A true JPH04202094A (en) | 1992-07-22 |
Family
ID=18285290
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2335147A Pending JPH04202094A (en) | 1990-11-30 | 1990-11-30 | Production of superconducting thin film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH04202094A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06196760A (en) * | 1992-12-25 | 1994-07-15 | Nec Corp | Superconductive lamination thin film |
| JP2008221088A (en) * | 2007-03-09 | 2008-09-25 | Yokohama National Univ | Oxide catalyst and method for decomposing organic components in gas using the same |
-
1990
- 1990-11-30 JP JP2335147A patent/JPH04202094A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06196760A (en) * | 1992-12-25 | 1994-07-15 | Nec Corp | Superconductive lamination thin film |
| JP2008221088A (en) * | 2007-03-09 | 2008-09-25 | Yokohama National Univ | Oxide catalyst and method for decomposing organic components in gas using the same |
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