JPH0687696A - Method for manufacturing superconducting thin film - Google Patents

Method for manufacturing superconducting thin film

Info

Publication number
JPH0687696A
JPH0687696A JP4232515A JP23251592A JPH0687696A JP H0687696 A JPH0687696 A JP H0687696A JP 4232515 A JP4232515 A JP 4232515A JP 23251592 A JP23251592 A JP 23251592A JP H0687696 A JPH0687696 A JP H0687696A
Authority
JP
Japan
Prior art keywords
thin film
superconducting thin
substrate
oxide superconductor
thermal expansion
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
Application number
JP4232515A
Other languages
Japanese (ja)
Inventor
Kazuo Koe
和郎 向江
Toshiyuki Matsui
俊之 松井
Takeshi Suzuki
健 鈴木
Hiroshi Kimura
浩 木村
Takashi Ishii
孝志 石井
Koichi Tsuda
孝一 津田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric 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
Application filed by Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP4232515A priority Critical patent/JPH0687696A/en
Publication of JPH0687696A publication Critical patent/JPH0687696A/en
Pending legal-status Critical Current

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  • Inorganic Compounds Of Heavy Metals (AREA)
  • Crystals, And After-Treatments Of Crystals (AREA)
  • Superconductor Devices And Manufacturing Methods Thereof (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)

Abstract

(57)【要約】 【目的】成膜中の冷却過程で引っ張り熱応力に起因して
発生する超電導薄膜の亀裂をなくす。 【構成】(001)軸以外の結晶配向性を持つ酸化物超
電導体と、この酸化物超電導体より熱膨張係数が大きい
基板を用いて、この基板上に酸化物超電導体の薄膜を形
成することにより、その成膜中の高温から室温に冷却す
る過程で、基板の方が超電導薄膜より大きく収縮するの
で、超電導薄膜には圧縮応力が作用し、超電導薄膜内に
亀裂が生ずるのを防ぐことができる。
(57) [Abstract] [Purpose] To eliminate cracks in the superconducting thin film caused by tensile thermal stress during the cooling process during film formation. [Structure] An oxide superconductor having a crystal orientation other than the (001) axis and a substrate having a coefficient of thermal expansion larger than that of the oxide superconductor are used to form a thin film of the oxide superconductor on the substrate. Therefore, in the process of cooling from high temperature during the film formation to room temperature, the substrate shrinks more than the superconducting thin film, so that compressive stress acts on the superconducting thin film and it is possible to prevent cracks from occurring in the superconducting thin film. it can.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、酸化物超電導薄膜の製
造方法に関するる。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for producing an oxide superconducting thin film.

【0002】[0002]

【従来の技術】酸化物超電導体をジョセフソン素子など
の電子素子に利用するためには、この超電導体を薄膜化
する必要がある。とくに積層形のジョセフソン接合を作
製するとき、コヒーレンス長の短い(001)軸以外の
結晶配向性を持つ超電導薄膜としなければならない。酸
化物超電導体の薄膜を形成するには、通常、スパッタ
法,電子ビーム蒸着法またはレーザーアブレーション法
などの物理蒸着やMOCVDなどの化学蒸着法を用い
て、基板上に堆積する方法が行なわれている。これらの
成膜法において、超電導薄膜をエピタキシャル成長させ
るために、基板を数100℃以上の高温に加熱するの
で、高温成膜後に室温まで冷却する過程で、基板と超電
導薄膜の熱膨張係数が異なると、超電導薄膜内にストレ
スが発生し、これが原因で亀裂が生ずる。とくに、超電
導薄膜の結晶配向性が(001)以外の場合は、熱膨張
係数が酸化物超電導体より小さいMgOやSrTiO3
のような材料の基板を用いると、冷却過程で超電導薄膜
に引っ張り応力が発生し、微小な亀裂が入ってしまう。
詳細な調査によると、この亀裂は亀裂の入りやすい(0
01)面内で発生していることが判明した。この亀裂の
様子を図2の酸化物超電導素子の模式斜視図に示す。図
2は、例えば従来多用されており、熱膨張係数が9.4
×10-6/℃を有するSrTiO3 (110)の基板1
上に、c軸方向の熱膨張係数が18.46×10-6/℃
の酸化物超電導薄膜2を形成すると、基板1の方が超電
導薄膜2より熱膨張係数が小さいために、超電導薄膜2
に亀裂3が発生することを示すものである。
2. Description of the Related Art In order to use an oxide superconductor in electronic devices such as Josephson devices, it is necessary to make the superconductor thin. In particular, when manufacturing a laminated Josephson junction, a superconducting thin film having a crystal orientation other than the (001) axis with a short coherence length must be used. To form a thin film of oxide superconductor, a physical vapor deposition method such as a sputtering method, an electron beam vapor deposition method or a laser ablation method, or a chemical vapor deposition method such as MOCVD is usually used to deposit a film on a substrate. There is. In these film forming methods, the substrate is heated to a high temperature of several hundreds of degrees Celsius or more in order to epitaxially grow the superconducting thin film. , Stress is generated in the superconducting thin film, which causes cracks. In particular, when the crystal orientation of the superconducting thin film is other than (001), the coefficient of thermal expansion of MgO or SrTiO 3 is smaller than that of the oxide superconductor.
When a substrate made of such a material is used, a tensile stress is generated in the superconducting thin film during the cooling process, and minute cracks are formed.
Detailed examination shows that this crack is prone to cracking (0
01) It was found that it occurred in the plane. The state of this crack is shown in the schematic perspective view of the oxide superconducting element of FIG. FIG. 2 shows that, for example, the thermal expansion coefficient is 9.4, which is often used conventionally.
Substrate 1 of SrTiO 3 (110) having × 10 −6 / ° C.
The coefficient of thermal expansion along the c-axis is 18.46 × 10 -6 / ° C.
When the oxide superconducting thin film 2 of 1 is formed, the substrate 1 has a smaller thermal expansion coefficient than the superconducting thin film 2.
It shows that cracks 3 occur in the.

【0003】[0003]

【発明が解決しようとする課題】問題は、図2に示すよ
うな亀裂3は、超電導薄膜2を電子素子として利用する
ためには不都合であり、したがって、成膜過程で亀裂3
の入らない超電導薄膜2を形成しなければならないこと
である。本発明の目的は、成膜中の冷却過程で、引っ張
り熱応力に起因する亀裂が発生することのない超電導薄
膜を製造する方法を提供することにある。
The problem is that the crack 3 as shown in FIG. 2 is inconvenient for using the superconducting thin film 2 as an electronic device, and therefore, the crack 3 during the film formation process.
That is, it is necessary to form a superconducting thin film 2 which does not enter. An object of the present invention is to provide a method for producing a superconducting thin film in which cracks due to tensile thermal stress do not occur in the cooling process during film formation.

【0004】[0004]

【課題を解決するための手段】上記の課題を解決するた
めに、本発明の方法は、酸化物超電導体として(00
1)軸以外の結晶配向性を持つLnBa2 Cu3 O7-X
(LnはY,La,Sm,Eu,Gd,Dy,Ho,E
r,Tm,Yb,Lnのうちのいずれか一つの元素,x
は酸素欠損量)を用い、これら酸化物超電導体より熱膨
張係数が大きく、熱膨張係数が18.5×10-6/℃以
上のLaSrGaO4 ,VO2 ,GaCO 3 などの基板
を用いて、この基板上に酸化物超電導体の薄膜を形成す
るものである。
[Means for Solving the Problems]
For this reason, the method of the present invention uses (00
1) LnBa having crystal orientation other than the axis2Cu3O7-X
(Ln is Y, La, Sm, Eu, Gd, Dy, Ho, E
Any one element of r, Tm, Yb, and Ln, x
Is the oxygen deficiency) and the thermal expansion from these oxide superconductors
Large expansion coefficient, thermal expansion coefficient 18.5 × 10-6/ ° C or less
On LaSrGaOFour, VO2, GaCO 3Substrate such as
To form a thin film of oxide superconductor on this substrate.
It is something.

【0005】[0005]

【作用】以上のようにして基板上に超電導薄膜を形成す
ることにより、その成膜中の数100℃以上から室温に
冷却する過程で、基板が超電導薄膜より多く収縮するの
で、超電導薄膜には圧縮応力が作用し、超電導薄膜内に
亀裂が生ずるのを防ぐことができる。
By forming the superconducting thin film on the substrate as described above, the substrate shrinks more than the superconducting thin film in the process of cooling from several 100 ° C. or higher during the film formation to room temperature. It is possible to prevent the generation of cracks in the superconducting thin film due to the action of compressive stress.

【0006】[0006]

【実施例】以下、本発明を実施例に基づき説明する。本
発明は、酸化物超電導体より熱膨張係数の大きい基板を
用いることにあり、得られた酸化物超電導素子の模式斜
視図を図1に示す。図1の素子は、図2に示したような
亀裂3の発生は認められない。
EXAMPLES The present invention will be described below based on examples. The present invention resides in using a substrate having a coefficient of thermal expansion larger than that of the oxide superconductor. A schematic perspective view of the obtained oxide superconducting element is shown in FIG. In the device shown in FIG. 1, the generation of the crack 3 as shown in FIG. 2 is not recognized.

【0007】このような素子を得るために、本発明で
は、酸化物超電導体にYBa2 Cu3O7-X (xは酸素
欠損量)[以下YBCOと略称する]を用い、基板1と
してLaSrGaO4 (110)を用いる。YBCOの
c軸方向の線膨張係数は18.46×10-6/℃であ
り、LaSrGaO4 の(001)方向の線膨張係数は
18.9×10-6/℃である。成膜法は、RFマグネト
ロンスパッタ法を用い、基板温度650℃で300nm
の膜厚にYBCO薄膜2aを形成した。成膜後、室温に
冷却して得られたYBCO薄膜2aは(110)配向と
なり、図1に示すように、亀裂が発生することはない。
In order to obtain such a device, in the present invention, YBa 2 Cu 3 O 7-X (x is an oxygen deficiency amount) [hereinafter abbreviated as YBCO] is used as the oxide superconductor, and LaSrGaO is used as the substrate 1. 4 (110) is used. The linear expansion coefficient of YBCO in the c-axis direction is 18.46 × 10 −6 / ° C., and the linear expansion coefficient of LaSrGaO 4 in the (001) direction is 18.9 × 10 −6 / ° C. RF magnetron sputtering is used as the film forming method, and the substrate temperature is 650 ° C. and the thickness is 300 nm.
The YBCO thin film 2a was formed to a film thickness of. After the film formation, the YBCO thin film 2a obtained by cooling to room temperature has a (110) orientation, and as shown in FIG. 1, no cracks occur.

【0008】次に、酸化物超電導体にYBCOを用い、
基板1にVO2 (110)を用いた。VO2 の(00
1)方向の線膨張係数は21.4×10-6/℃である。
成膜法と膜厚は上記の場合と同様にし、成膜後室温に冷
却して得られたYBCO薄膜2aは(013)配向をし
ており、このときも、図1に示したのと同じく、亀裂の
発生は全くなかった。
Next, using YBCO for the oxide superconductor,
VO 2 (110) was used for the substrate 1. VO 2 (00
The coefficient of linear expansion in the 1) direction is 21.4 × 10 -6 / ° C.
The film forming method and the film thickness were the same as in the above case, and the YBCO thin film 2a obtained by cooling to room temperature after the film formation had a (013) orientation, and at this time, as in the case shown in FIG. There were no cracks at all.

【0009】さらに、酸化物超電導体にYBCOを用
い、基板1にGaCO3 (110)を用いてYBCO薄
膜2aを作製した。GaCO3 の(001)方向の線膨
張係数は26.3×10-6/℃である。上記二つの場合
と同様の成膜法と膜厚により、成膜後室温に冷却して得
られたYBCO薄膜2aは(013)配向をしており、
この場合も前記二例と同じく亀裂の発生は認められなか
った。
Further, YBCO was used for the oxide superconductor, and GaCO 3 (110) was used for the substrate 1 to form a YBCO thin film 2a. The linear expansion coefficient of GaCO 3 in the (001) direction is 26.3 × 10 -6 / ° C. The YBCO thin film 2a obtained by cooling to room temperature after the film formation has the (013) orientation by the film formation method and the film thickness similar to the above two cases,
In this case as well, the occurrence of cracks was not recognized as in the above two cases.

【0010】以上3種類の異なる基板1を用いた場合に
ついて述べたが、これらの例から、基板の熱膨張係数は
少なくとも18.5×10-6/℃であればよく、また、
酸化物超電導体は上記の他に、LnBa2 Cu3 O7-X
(LnはLa,Sm,Eu,Gd,Dy,Ho,Er,
Tm,Yb,Lnのうちのいずれか一つの元素,xは酸
素欠損量)を用いても、同様の効果を得ることができ
る。
The case where three different kinds of substrates 1 are used has been described above. From these examples, the coefficient of thermal expansion of the substrate should be at least 18.5 × 10 −6 / ° C., and
In addition to the above, oxide superconductors include LnBa 2 Cu 3 O 7-X
(Ln is La, Sm, Eu, Gd, Dy, Ho, Er,
The same effect can be obtained by using any one element of Tm, Yb, and Ln and x is an oxygen deficiency amount.

【0011】以上のように、本発明では(001)軸以
外の結晶配向性を持つ(c軸に傾きを持つ)酸化物超電
導体と、この酸化物超電導体より熱膨張係数の大きい基
板を用いることにより、成膜中の高温から室温に冷却す
る過程で、基板の方が超電導薄膜より収縮が大きく、超
電導薄膜に圧縮応力が働くので、亀裂が発生するのを防
ぐことができる。
As described above, according to the present invention, an oxide superconductor having a crystal orientation other than the (001) axis (having an inclination in the c axis) and a substrate having a thermal expansion coefficient larger than that of the oxide superconductor are used. As a result, in the process of cooling from a high temperature during film formation to room temperature, the substrate shrinks more than the superconducting thin film, and compressive stress acts on the superconducting thin film, so that cracking can be prevented.

【0012】[0012]

【発明の効果】本発明の方法によれば、(001)軸以
外の結晶配向性を持つ酸化物超電導体と、この酸化物超
電導体より熱膨張係数の大きい基板を使用して、この基
板上に超電導薄膜を形成したために、その成膜工程にお
ける数100℃以上の高温から室温に冷却する過程で、
基板が超電導薄膜より多く収縮し、超電導薄膜には圧縮
応力が作用するので、超電導薄膜内に亀裂の発生が起き
ることがなくなり、その結果、亀裂のない超電導薄膜に
リソグラフィなどを用いて微細加工を施すことにより、
良好な特性を持つジョセフソン素子を作製することが可
能となる。
According to the method of the present invention, an oxide superconductor having a crystal orientation other than the (001) axis and a substrate having a thermal expansion coefficient larger than that of the oxide superconductor are used. Since the superconducting thin film was formed on the surface of
Since the substrate shrinks more than the superconducting thin film, and the compressive stress acts on the superconducting thin film, cracks do not occur in the superconducting thin film. By applying
It is possible to manufacture a Josephson device having good characteristics.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明により得られる酸化物超電導素子の模式
斜視図
FIG. 1 is a schematic perspective view of an oxide superconducting element obtained by the present invention.

【図2】酸化物超電導素子に生じた亀裂の様子を示す模
式斜視図
FIG. 2 is a schematic perspective view showing a state of cracks generated in an oxide superconducting element.

【符号の説明】[Explanation of symbols]

1 基板 2 超電導薄膜 2a YBCO薄膜 3 亀裂 1 substrate 2 superconducting thin film 2a YBCO thin film 3 crack

───────────────────────────────────────────────────── フロントページの続き (72)発明者 木村 浩 神奈川県川崎市川崎区田辺新田1番1号 富士電機株式会社内 (72)発明者 石井 孝志 神奈川県川崎市川崎区田辺新田1番1号 富士電機株式会社内 (72)発明者 津田 孝一 神奈川県川崎市川崎区田辺新田1番1号 富士電機株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Hiroshi Kimura 1-1 Tanabe Nitta, Kawasaki-ku, Kawasaki-shi, Kanagawa Fuji Electric Co., Ltd. No. 1 in Fuji Electric Co., Ltd. (72) Inventor Koichi Tsuda 1-1 No. 1 Tanabe Nitta, Kawasaki-ku, Kawasaki City, Kanagawa Prefecture Fuji Electric Co., Ltd.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】酸化物超電導体に(001)軸以外の結晶
配向性を持つLnBa2 Cu3 O7-X (LnはY,L
a,Sm,Eu,Gd,Dy,Ho,Er,Tm,Y
b,Lnのうちのいずれか一つの元素,xは酸素欠損
量)を用い、これら酸化物超電導体より熱膨張係数の大
きい材料の基板を用いて、この基板上に前記酸化物超電
導体の薄膜を形成することを特徴とする超電導薄膜の製
造方法。
1. An oxide superconductor having LnBa 2 Cu 3 O 7-X (Ln is Y, L having crystal orientation other than the (001) axis.
a, Sm, Eu, Gd, Dy, Ho, Er, Tm, Y
Any one element of b and Ln, x is an oxygen deficiency amount), a substrate of a material having a larger thermal expansion coefficient than these oxide superconductors is used, and a thin film of the oxide superconductor is formed on the substrate. Forming a superconducting thin film.
【請求項2】請求項1記載の方法において、基板の熱膨
張係数は18.5×10-6/℃以上であることを特徴と
する超電導薄膜の製造方法。
2. The method for producing a superconducting thin film according to claim 1, wherein the substrate has a thermal expansion coefficient of 18.5 × 10 −6 / ° C. or more.
【請求項3】請求項1または2記載の方法において、基
板はLaSrGaO 4 ,VO2 ,GaCO3 のうちのい
ずれかを用いることを特徴とする超電導薄膜の製造方
法。
3. The method according to claim 1 or 2, wherein
The plate is LaSrGaO Four, VO2, GaCO3Out of
Manufacturing method of superconducting thin film characterized by using a gap
Law.
JP4232515A 1992-09-01 1992-09-01 Method for manufacturing superconducting thin film Pending JPH0687696A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4232515A JPH0687696A (en) 1992-09-01 1992-09-01 Method for manufacturing superconducting thin film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4232515A JPH0687696A (en) 1992-09-01 1992-09-01 Method for manufacturing superconducting thin film

Publications (1)

Publication Number Publication Date
JPH0687696A true JPH0687696A (en) 1994-03-29

Family

ID=16940542

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4232515A Pending JPH0687696A (en) 1992-09-01 1992-09-01 Method for manufacturing superconducting thin film

Country Status (1)

Country Link
JP (1) JPH0687696A (en)

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