JPH03215319A - Manufacturing method of thin film superconductor - Google Patents
Manufacturing method of thin film superconductorInfo
- Publication number
- JPH03215319A JPH03215319A JP2007422A JP742290A JPH03215319A JP H03215319 A JPH03215319 A JP H03215319A JP 2007422 A JP2007422 A JP 2007422A JP 742290 A JP742290 A JP 742290A JP H03215319 A JPH03215319 A JP H03215319A
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- layer
- alkaline earth
- oxide
- substrate
- 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.)
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Links
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment
Landscapes
- Inorganic Compounds Of Heavy Metals (AREA)
- Chemical Vapour Deposition (AREA)
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
- Physical Vapour Deposition (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gL 超伝導薄膜の製造方法に関するものであ
も 特く 多元系の薄膜超伝導体の形成において、超伝
導薄膜の制御性が優れ より高性能な超伝導特性が得ら
れる製造方法に関するものである。[Detailed Description of the Invention] Industrial Field of Application The present invention relates to a method for producing a superconducting thin film. Especially in the formation of a multi-component thin film superconductor, the superconducting thin film has excellent controllability and higher performance. The present invention relates to a manufacturing method that provides excellent superconducting properties.
従来の技術
高温超伝導体として、A15型2元系化合物として窒化
ニオプ(NbN)やゲルマニウムニオブ(Nb*Ge)
等が知られていたが、 これらの超伝導材料の超伝導転
移温度はたかだか24Kであった
一X ペロブス力イト系3元化合物番よ さらに高い
転移温度が期待さ% Ba−La−Cu−0系の高温
超伝導体が提案された [ファイト シュリ7ト 7エ
ア7イシゝ−ク コンデづスビマター第64巻第189
頁(J,G.Bendorz and K.A.Mul
ler,Zetshrift Furphysik
B− Condensed Matter 6
4, 189−193(1986)) ]。Conventional technology As a high-temperature superconductor, niobium nitride (NbN) and germanium niobium (Nb*Ge) are used as A15 type binary compounds.
etc., but the superconducting transition temperature of these superconducting materials was at most 24 K. An even higher transition temperature is expected compared to the ternary compounds of the 1X perovskite system.Ba-La-Cu-0 A system of high-temperature superconductors was proposed.
Page (J, G. Bendorz and K. A. Mul
ler, Zetshrift Furphysik
B- Condensed Matter 6
4, 189-193 (1986)].
さら!Q Bi−Sr−Ca−Cu−0系の材料7K
IOOK以上の転移温度を示すことも発見された[
シ゛ヤ八゜ニース゛・シ゛↑−ナル・オ7゛・ア7゜ラ
イビ・7イシ”ツクス第27巻第209頁 (H.Ma
eda, Y,Tanaka, M,Fukuto
mi and T,Asano,Japanese
Journal of Applied P
hyscs 27. L209−L210(198
8)》 コ。Sara! Q Bi-Sr-Ca-Cu-0 material 7K
It was also discovered that it exhibits a transition temperature higher than IOOK [
27th volume, page 209 (H. Ma
eda, Y., Tanaka, M., Fukuto
mi and T, Asano, Japanese
Journal of Applied P
hyscs 27. L209-L210 (198
8)》 Ko.
さらにBi−Sr−Ca−Cu−0超伝導体と同様の結
晶構造を持板 超伝導転移温度が120Kを超えるTI
−Ba−Ca−Cu−0系が発見された [ネ4ft一
第332巻第138頁(Z, Z, Sheng an
d A.M.Hermann, Nature Vol
.332. 138−139(1988))]。Furthermore, it has a crystal structure similar to that of Bi-Sr-Ca-Cu-0 superconductor.TI has a superconducting transition temperature exceeding 120K.
-Ba-Ca-Cu-0 system was discovered.
dA. M. Hermann, Nature Vol.
.. 332. 138-139 (1988))].
この種の材料の超伝導機構の詳細は明らかではないが、
転移温度が室温以上に高くなる可能性があり、高温超
伝導体として従来の2元系化合物より、より有望な特性
が期待されも
発明が解決しようとする課題
この種の材料{よ 現在の技術で(瓜 主として焼結と
いう過程で形成されており、セラミックの粉末あるいは
ブロックの形状で得られている場合が多b〜
一人 この種の材料をデバイス等で実用化する場合 薄
膜状に加工することが強く要望されていも
薄膜状にする手法として真空蒸着法 マグネトロンスパ
ッタ汰 プラズマCVD法などの様々な方法を用いて、
酸化物超伝導体の薄膜化が行われているバ 従来の技術
では良好な超伝導特性を有する薄膜作製には難しい点が
多かった
特E, Bi−Sr−Ca−Cu−Oi Tl−B
a−Ca−Cu−0系にζ友超伝導転移温度の異なるい
くつかの相が存在し100K以上の臨界温度を持つ相を
薄膜の形態で達成するの1友 非常に困難であり、,各
層を制御して結晶性にすぐれた単結晶を作製するのは大
変困難であるとされてい九
これは基体の形状の影響を受仇 結晶の島状構造ができ
やすく、電流密度が小さくなり易く、超伝導特性が低下
し易い等の問題を持っていることが主な原因であも
そのためへ 電子デバイス等に応用を考える場合に必要
とされている膜厚100A程度においては 高性能な超
伝導薄膜をえることは困難とされていた
本発明は上述したような従来の課題を克服するために提
案されたものであり、酸化物超伝導薄膜を、再現性及び
結晶性に優れ基体上に積層でき瓜薄膜超伝導体の製造方
法を提供することを目的とすa
課題を解決するための手段
本発明の薄膜超伝導体の製造方法は 基体上く銅および
アルカリ土類(IIa族)を含む物質から成る酸化物の
層を形成した丸 さらにビスマスを含む酸化物の層を形
成した上へ 銅を含む酸化物超伝導薄膜を形成させて作
製するというものであa作用
本発明者らは基体上K, 各種物質の形成を試み九
結晶系の一仇 層拡散の度合等を考虜し 検討した結果
まず銅およびアルカリ土類を含む物質よりなる酸化物
の層を形成した後1;; Bi−0層を形成すも さ
らにその上へ 銅を含む複合酸化物超伝導薄膜を積層さ
せると、グレインのほとんどない単結晶薄膜が形成され
も
これは基体上に最初形成した 銅及びアルカリ土類から
なる酸化物ζよ 加熱された基体上に基体の凹凸を埋め
るように広がり形成される。その後Bi−0膜を形成さ
せることによって、基体表面に平坦な面が形成できるも
のと考えられも
また複合酸化物超伝導薄膜の層をビスマスあるいはタリ
ウムを含む酸化物の層と、銅及びアルカリ土類を含む物
質からなる酸化物層とを周期的に積層させて得ることに
より、層間の拡散が抑えられ 結晶性が向上すも
実施例
一般に基体に用いられる物質はなんらかの凹凸を有し
その凹凸は薄膜の結晶性に大きく影響すも
従って薄膜を形成するとき、特に超薄膜デバイスを形成
する時に&よ その凹凸の小さいものを用いなけれ(戴
特性にすぐれた結晶性のよい薄膜が得られなl.%
Lかし 生産工程上その凹凸をなくすることは不可能
に近(〜 超伝導薄膜は特にその結晶性が特性に大きな
影響を及ぼしていると考えられ 電流密度の改善にはま
ず第一に結晶性の向上があげられも
また基板の凹凸は結晶の島状構造を作り易く、電流密度
の低下、また転移温度の低下につながも従って超薄膜の
形成に(よ この凹凸の影響をまず避ける必要があa
しかし本発明の製造方法によれ(戴 基板上に銅酸化物
及びアルカリ土類酸化物各々を主体とする層を形成する
たべ この層が基板の凹状の部分から優先的に付着し
基板を平坦化する効果があり、この上に形成される超伝
導薄膜の超伝導特性を良好に出来も
本発明に適応される酸化物超伝導薄膜(よ 少なくとも
銅を含有すa その中でもこの酸化物超伝導薄膜へ ビ
スマスとアルカリ土類(IIa族)、あるいはタリウム
(T1)とアルカリ土類(IIa族)、あるいはイット
リウム(Y)とアルカリ土類(IIa族)、あるいはネ
オジウム(Nd)とアルカリ土類(IIa族)、あるい
はランタン(La)とアルカリ土類(Ila族)の内何
れかを含む酸化物薄膜を用いると、特に超伝導特性が良
好になるため好まし(〜
また本発明の薄膜超伝導体の製造方法で法 銅酸化物を
主体とする層とアルカリ土類酸化物を主体とする層を基
体上に形成するとき、基体を加熱することが好まし一一
特に基体温度を550℃から900℃で形成すると、基
体表面の平坦化の効果がより高くなムまた 各種超伝導
体についても形成して膜の結晶構造について詳細に調べ
た
銅およびアルカリ土類を含む物質はそれのみでペロブス
カイト構造を有する薄膜が形成さh Bi−0層もし
くはTI−0層を基板に直接形成した場合に比べ その
結晶性は数段向上し グレインも観察されなくなりへ
特にBi系では650℃以下の基体温度″C% Tl系
では300℃で形成してL IOOK以上の臨界温度
が得られることが判明し また結晶性も良く、臨界温度
が80Kの超伝導相の結晶等とも区別制御し形成するこ
とができ、再現性もすぐれてい九
またBig Tl系以外の超伝導体で杖 結晶性と超
伝導特性との向上の効果が認められ九さらに本発明によ
り、良質で高性能な薄膜超伝導体を、再現性良く得るこ
とが可能となa本発明の製造方法ζよ 厚み数Aの薄層
を周期的に積層させることが必要であも 数Aの周期性
を持つ物質を積層させる方法としてC上 従来MBE
法 EB蒸着法やスパッタリング法等いくつか考えられ
ていも 特番ζ MBE法やEB蒸着法等法周期的積層
を達成するのに適していも
しかしこの種の非常に薄い層の積層に1よ 従来スパッ
タリング法は不向きとみられていた この理由(上 成
膜中のガス圧の高さに起因する不純物の混入 およびエ
ネルギーの高い粒子によるダメージによると考えられて
いも
しかしなが収 本発明者ら1友 スパッタリングにより
異なる薄い層の積層を行なったとこへ 意外にも良好な
積層膜の作製が可能なことを発見し九 この原因はスパ
ッタ中の高い酸素ガス圧およびスパッタ放電が、 ペロ
ブスカイト構造の形成に都合がよいためと考えられも
また 複数種の単一物質をターゲットとして順次スパッ
タを行う周期的形成法ではないCVDa高周波スパッタ
リング法等でk 充分に形成可能であa しかし周期的
形成法(友 制御性に優れていも
また 特にスパッタリング法は成分組成への依存性が大
きい超伝導薄膜において、制御性に優れた製法であも
まずビスマス系でスパッタリング法を用いた例について
述べも
すなわ板 BiターゲットとSr*CasCusターゲ
ットを、アルゴンと酸素混合ガス中で交互にスパッタリ
ングし 種々の温度のMgO基板上に周期的に積層させ
tも
このようにして得られた基板をX線回折により評価する
と、基板温度が400℃以下の場合には積層周期構造に
対応するピークが認められるが、400℃〜550℃と
高くすると周期構造が弱くなり、他の相の出現が認めら
れる。ところが、 さらに温度を高LA550℃〜90
0℃の範囲の基体温度でg;!, IOOK以上の臨
界温度を持つ相が作製し得ることを発見した。Although the details of the superconducting mechanism of this type of material are not clear,
The transition temperature of this type of material can be higher than room temperature, and it is expected that this type of material will have more promising properties as a high-temperature superconductor than conventional binary compounds. (Melon) It is mainly formed through the process of sintering, and is often obtained in the form of ceramic powder or blocksb~ One person When this type of material is to be put to practical use in devices, etc., it must be processed into a thin film. Although there is a strong demand for this, various methods such as vacuum evaporation, magnetron sputtering, and plasma CVD are used to form thin films.
Thin films of oxide superconductors are being made.Special E, Bi-Sr-Ca-Cu-Oi Tl-B, which had many difficulties in producing thin films with good superconducting properties using conventional techniques.
In the a-Ca-Cu-0 system, there are several phases with different zeta superconducting transition temperatures, and it is extremely difficult to achieve a phase with a critical temperature of 100 K or more in the form of a thin film. It is said that it is very difficult to control the crystallinity and produce a single crystal with excellent crystallinity.9 This is influenced by the shape of the substrate, which tends to form an island-like crystal structure, which tends to reduce the current density. The main reason is that the superconducting properties tend to deteriorate easily, but for this reason, it is a high-performance superconducting thin film at a film thickness of about 100A, which is required when considering application to electronic devices, etc. The present invention was proposed to overcome the above-mentioned conventional problems, and it is possible to stack oxide superconducting thin films on a substrate with excellent reproducibility and crystallinity. It is an object of the present invention to provide a method for manufacturing a thin film superconductor of the present invention.A method for manufacturing a thin film superconductor of the present invention includes the following steps: A method for manufacturing a thin film superconductor of the present invention includes: A superconducting thin film of an oxide containing copper is formed on top of a layer of oxide containing bismuth. After trying to form various substances and considering the degree of layer diffusion, etc., we found that after first forming an oxide layer consisting of a substance containing copper and alkaline earth, 1;;Bi- 0 layer is formed, but when a composite oxide superconducting thin film containing copper is laminated on top of it, a single crystal thin film with almost no grains is formed, but this consists of the copper and alkaline earth that were initially formed on the substrate. Oxide ζ is formed on the heated substrate by spreading to fill the irregularities of the substrate. By subsequently forming a Bi-0 film, it is thought that a flat surface can be formed on the substrate surface. By periodically laminating oxide layers made of a substance containing the above-mentioned substances, diffusion between the layers can be suppressed and crystallinity can be improved.
The unevenness greatly affects the crystallinity of the thin film, so when forming a thin film, especially when forming an ultra-thin film device, it is necessary to use a material with small unevenness (to obtain a thin film with excellent properties and good crystallinity). Rare l.%
However, it is almost impossible to eliminate the unevenness due to the production process (~ It is believed that the crystallinity of superconducting thin films in particular has a large influence on the characteristics, and the first thing to do to improve current density is crystallinity. Although the surface roughness of the substrate can be improved, it is also easy to form crystal island structures, leading to a decrease in current density and transition temperature. However, according to the manufacturing method of the present invention, the layer which forms a layer mainly composed of copper oxide and alkaline earth oxide on the substrate preferentially adheres from the concave portion of the substrate.
It has the effect of flattening the substrate and improves the superconducting properties of the superconducting thin film formed thereon. To superconducting thin films Bismuth and alkaline earth (group IIa), or thallium (T1) and alkaline earth (group IIa), or yttrium (Y) and alkaline earth (group IIa), or neodymium (Nd) and alkali It is preferable to use an oxide thin film containing either an earth element (Group IIa) or lanthanum (La) or an alkaline earth element (Group Ila) because the superconducting properties are particularly good. Method for producing a thin film superconductor When forming a layer mainly composed of copper oxide and a layer mainly composed of alkaline earth oxide on a substrate, it is preferable to heat the substrate. When formed at temperatures between 550°C and 900°C, the effect of flattening the substrate surface is even greater.Also, materials containing copper and alkaline earth metals, which have been formed on various superconductors and whose crystal structures were investigated in detail, are A thin film with a perovskite structure is formed when the Bi-0 layer or TI-0 layer is directly formed on the substrate.The crystallinity is improved by several steps and grains are no longer observed.Especially for Bi-based materials, the temperature is below 650°C. In the Tl system, it was found that a critical temperature higher than LIOOK can be obtained by forming at 300°C.It also has good crystallinity, and can be formed by controlling and controlling it to distinguish it from superconducting phase crystals, etc., which have a critical temperature of 80K. Furthermore, the present invention has been shown to improve the crystallinity and superconducting properties of superconductors other than Big Tl-based superconductors. According to the manufacturing method of the present invention, it is possible to obtain a material with good reproducibility, even if it is necessary to periodically stack thin layers with a thickness of several A.A method of stacking materials with periodicity of several A As C on Conventional MBE
Although several methods have been considered, such as EB evaporation and sputtering, MBE and EB evaporation are suitable for achieving periodic stacking. This method was thought to be unsuitable for this reason (1) It is believed that this is due to the contamination of impurities caused by the high gas pressure during film formation and the damage caused by high-energy particles. They discovered that it was possible to produce a surprisingly good laminated film by laminating different thin layers.9 The reason for this was that the high oxygen gas pressure during sputtering and the sputtering discharge were favorable for the formation of a perovskite structure. This is thought to be due to the fact that it can be formed sufficiently by CVDa high-frequency sputtering method, which is not a periodic formation method in which sputtering is performed sequentially using multiple types of single materials as targets. In particular, the sputtering method is highly dependent on the composition of superconducting thin films, and although it is a manufacturing method with excellent controllability, we will also discuss an example in which the sputtering method was used for a bismuth-based film. *A CasCus target was sputtered alternately in a mixed gas of argon and oxygen, and periodically stacked on MgO substrates at various temperatures. When the substrates thus obtained were evaluated by X-ray diffraction, it was found that the substrate temperature was When the temperature is below 400°C, a peak corresponding to the laminated periodic structure is observed, but when the temperature is increased to 400°C to 550°C, the periodic structure becomes weaker and other phases appear.However, when the temperature is further increased to 550°C, the periodic structure becomes weaker. ~90
g at a substrate temperature in the range of 0°C;! , discovered that it is possible to create phases with critical temperatures higher than IOOK.
さらニBiターゲットをスパツタし基体上にBi酸化物
を形成した場合と、Sr*Ca*Cusターゲ・ソトを
スパッタし基体上にSr−Ca−Cu酸化物を形成した
場合とを比較すると、後者の酸化物形成した場合の方が
薄膜の結晶性が格段に向上し グレインが見られなくな
り、電流密度が倍増することを発見し九
そこでまずはじめのSr−Ca−Cuの酸化物の膜厚を
調節し 膜の結晶性を調べると、基体の凹凸のサイズに
顕著な依存を示し 基体の凹凸の厚さをある程度超える
程度Sr−Ca−Cu酸化物の厚さを形成するとその効
果は顕著になも このSr−Ca−Cu酸化物により、
基体の平坦化が行なえたためと考えられも
また この効果は膜厚の薄い方が顕著であるた八 薄膜
超伝導のデバイス化に有用な製造法であるといえも
第1図に本発明の超伝導薄膜の製造方法により形成した
超伝導薄膜の基体付近の模式図を示す。Furthermore, when comparing the case where Bi oxide is formed on the substrate by sputtering a Bi target and the case where Sr-Ca-Cu oxide is formed on the substrate by sputtering a Sr*Ca*Cu target, the latter They discovered that when an oxide of Sr-Ca-Cu was formed, the crystallinity of the thin film was much improved, no grains were seen, and the current density doubled. When the crystallinity of the film was examined, it was found that it depended markedly on the size of the irregularities on the substrate, and when the thickness of the Sr-Ca-Cu oxide was formed to a degree that exceeded the thickness of the irregularities on the substrate, the effect became remarkable. Also, due to this Sr-Ca-Cu oxide,
Although this effect is thought to be due to the flattening of the substrate, this effect is more pronounced as the film thickness becomes thinner. A schematic diagram of the vicinity of a base of a superconducting thin film formed by a method for manufacturing a conductive thin film is shown.
基体11上i;; Sr−Ca−Cu酸化物12のA
層を形成し このA層上にBi酸化物13のB層を形成
しさらにこのB層上にBi−Sr−Ca−Cu酸化物1
4の複合酸化物超伝導薄膜が積層されていも
上記温度範囲でBiとSr2CaeCusのスパッタリ
ングレートを適宜に調節すると、積層周期に対応してL
OOK以上の相が出現し 結晶性が向上し九特に550
℃〜900℃の場合にはIOOK以上の臨界温度の相の
結晶性が非常に良好なものが作製し得ることも合わせて
発見し九
基体温度IJt 900℃以上の際{友 薄膜が蒸発
して堆積しなかっ九
基体温度を550℃〜900℃で作製した薄膜はそのま
まの状態でも超伝導転移を示すが、 酸素中で基体温度
を850℃程度で熱処理を行なうと、より確実に100
K以上の臨界温度を示し島
また550℃〜900℃で積層した薄膜ζ友 特に再現
性に優れていることも発見し九
以下具体的実施例を挙げて、本発明をより詳細に説明す
る。i on the substrate 11;; A of the Sr-Ca-Cu oxide 12;
A B layer of Bi oxide 13 is formed on this A layer, and a Bi-Sr-Ca-Cu oxide 1 is further formed on this B layer.
Even if the composite oxide superconducting thin films of No. 4 are laminated, if the sputtering rate of Bi and Sr2CaeCus is appropriately adjusted in the above temperature range, L will change depending on the lamination period.
A phase of OOK or higher appears and the crystallinity improves, especially at 550.
It was also discovered that when the temperature is between 900°C and 900°C, it is possible to produce a phase with very good crystallinity at a critical temperature of IOOK or higher. Thin films produced at substrate temperatures of 550°C to 900°C that are not deposited exhibit superconducting transition even in their original state, but heat treatment in oxygen at a substrate temperature of about 850°C more reliably transforms the superconducting transition to 100°C.
It has also been discovered that thin films having a critical temperature of K or higher and laminated at temperatures of 550 to 900 DEG C. are particularly excellent in reproducibility.
実施例l
第2図のようへBi−0ターゲット21、Sr−Ca−
Cu−0ターゲット22、 Bi−Sr−Ca−Cu−
0ターゲット23の3種類が、 基体24に焦点を結ぶ
ように配した
酸化マグネシウム単結晶(100)面を基体24として
、プレーナーマグネトロンスパツタ法により、スパッタ
リング蒸着して、上記基体24上に結晶性の被膜として
付着させた
この時基体24をヒータ25で約700℃に加熱しAr
と02の混合ガス雰囲気(ガス混合比は5:1で圧力は
3Pa)中玄 各ターゲットのスパッタリングを行なっ
た
各ターゲットのスパッタ電流i;J.. Bi−0を
100m&Sr−Ca−Cu−0を100m& Bi
−Sr−Ca−Cu−0を150mAとしt4本実施例
で用いた基体24の表面の凹凸は約10Aと見積られた
たべ まずSr−Ca−Cu−0ターゲット22上でシ
ャッター26を開き約3OA形成し 次いでBi−0タ
ーゲット21上でシャッター12を開き約1分形成LA
Bi−Sr−Ca−Cu−0ターゲット23上でシャッ
ター26を開き必要とする膜厚になるまでスパッタリン
グを行った なおこれら工程の間中基板加熱は引続き行
一入 周期的積層を行なり九本発明の製造方法により形
成した薄膜超伝導体&友 直接Bi系超伝導体を基体上
に形成した場合に比べ ゼロ抵抗温度は数十K上昇し九
基体の凹凸のIOAはSr−Ca−Cu酸化物層で平坦
化され 基体表面にこのSr−Ca−Cu酸化物と同様
のべロブス力イト構造を持つ複合酸化物超伝導薄膜の結
晶層力丈 安定に形成されているものと考えられもさら
にJcが約2倍となった
またこの薄膜超伝導体を表面観察等での観察によると、
グレインのサイズが大きくなっていもこのJcの増加の
理由ははっきりとは解明されていない力丈 電気伝導は
Cu−0面内で行なわれると考えられている力交 平坦
化によりCu−0面のつながりがよくなったためと、グ
レインのサイズが大きくなり電流の障壁が減ったためと
が考えられもこのようにして形成された薄膜超伝導体1
戴 膜厚を変化させてL IOOK以上の臨界温度を
持つ相を作製することができ九
この膜厚を変えた薄膜超伝導体のr looo人程度
の薄膜を作製した場合について分析を行った結果 組成
はBi:Sr:Ca:Cu=2:2:2:3となってい
たこのままの状態でもこの薄膜超伝導体はIOOK以上
の超伝導転移を示した力丈 さらに850℃で1時間の
熱処理を酸素中で行なうと、非常に再現性良く100K
以上の臨界温度を達成することができ九本発明の製造に
この酸素中の熱処理を加えたことより、各金属元素の酸
化が促進され この構造を作るのに各層の安定を図るの
に効果があり、結晶性の向上が図られたものと考えられ
も実施例2
Bi, CaCq 2個のSr*Cuの計4個のタ
ーゲットを用t\ スパッタ蒸着が行っ九
MgO(100)基体に焦点を結ぶように各ターゲット
を約30゜傾けて設置しtら
ターゲットの前方には回転するシャッターがあり、その
中に設けられたスリットの回転により、まずSr*Cu
→CaCu→Srs Cロのサイクルで約5凰 その後
Bi+ Srs Cu−b CaCu−+ Srt C
u−* CaCu−* Srs Cu−+ Biのサイ
クルでスパッタ蒸着を行なっ九
基体をヒーターで約300℃に加熱し アルゴン対酸素
の比率を5対1の混合雰囲気でガス圧を3Paのガス中
で、各ターゲットのスパッタリングを行なった 各ター
ゲットのスパッタ電流ハBiを30m入SreCuを5
0m入 CaCuを250mAとし シャッタの回転周
期をlO分間として間歇を設けて周期的積層を行なった
とこへ 基体温度300℃で105K以上の臨界温度を
持つ相を作製することができた
約1時間の蒸着により100A程度の薄膜が作製され九
この時の組成はBi:Sr:Ca:Cu=2:2:2:
3となっていた このままの状態でもこの薄膜は105
K以上の超伝導転移を示し島
このように層状構造ごとにターゲットを設け薄膜超伝導
体を作製する事により、より結晶性の高い薄膜がえら札
基体の凹凸の影響のな(\ 平坦式 ダレインのない
単結晶薄膜が形成されt4実施例2のように間隙を設け
た製造方法によると、間歇のない場合に比べ 結晶化が
低温で進へまたX線等の評価によってもシャープなピー
クがみら札 結晶性の向上が図られ九
本発明の製造方法バ 構成金属の構造のつながりがよく
、結晶性の優れた薄膜を作るのに非常に役だっているた
めと考えられも
本発明は基体の表面を安定なベロブス力イト構造を持板
構成組成の一部で形成すると言う基本思想であるた八
結品性のよい高性能な超伝導薄膜が得られも
スバッタ蒸着で異なる物質を積層させる方法として!よ
組成の異なる複数個のターゲットのスパッタリングす
る方法がある力丈 組成分布を設けた1ヶのターゲット
の放電位置を制御して、侵食領域を周期的に制御すると
いう方法を用いると比較的簡単に達成することができも
また スパッタ蒸着を用いない場合は特く 成膜東 成
膜後あるいは間歇時の少なくとも何れかの時点に0象の
導入を行なうと良(〜
さらにO■あるいはNeoのイオンビームを基体上に照
射する力\ またはOtあるいはNeoのプラズマに曝
すと、より結晶性の向上が図られ 臨界電流密度が向上
する効果があ翫
またスパッタリング法k 例えばレーザービームスパッ
タあるいはイオンビームスバッタを用いた場合も形成で
き、複数個のターゲットを周期運動させて、ビームの照
射するターゲットを周期的に変えれば 周期的積層膜が
実現されもなお本実施例及び上記はスパッタを例として
あげた戟 MBE, 多元のEB装置等でも本発明の
薄膜超伝導体の形成は可能である力丈 その場合(上形
成隊 形成中あるいは間歇時の内少なくともいずれかの
過程く 酸素イオンビームプラズマ照射などにより、酸
素の供給を行なう方が望ましt〜また 上記実施例では
Bi系の薄膜超伝導体について例を述べたバ 類似の構
造を持つ超伝導薄風少なくともタリウム(Tl)および
アルカリ土類(Ila族)および銅を含む酸化物薄風
あるいは少なくともイットリウム(Y)およびアルカリ
土類(Ila族)および銅を含む酸化物薄風 あるいは
少なくともネオジウム(Nd)およびアルカリ土類(I
Ia族)および銅を含む酸化物薄風 あるいは少なくと
もランタン(La)およびアルカリ土類(Ila族)お
よび銅を含む酸化物薄膜の層でも同様の結果が得られた
発明の効果
以上のようく 本発明の薄膜超伝導体の製造方法(よ
酸化物超伝導薄膜の再現性のよい結晶性のよい作製方法
を提供するものであり、工業上極めて大きな価値を有す
るものであもExample 1 Bi-0 target 21, Sr-Ca-
Cu-0 target 22, Bi-Sr-Ca-Cu-
Three types of 0 targets 23 are sputter-deposited using a planar magnetron sputtering method using a magnesium oxide single crystal (100) plane arranged so as to be focused on the base body 24, so that a crystalline layer is formed on the base body 24. At this time, the substrate 24, which has been deposited as a film, is heated to about 700°C with a heater 25 and exposed to Ar.
and 02 mixed gas atmosphere (gas mixture ratio: 5:1, pressure: 3 Pa) Sputtering current i for each target; J. .. 100m of Bi-0 & 100m of Sr-Ca-Cu-0 & Bi
- Sr-Ca-Cu-0 was set at 150 mA, and the unevenness on the surface of the substrate 24 used in this example was estimated to be about 10 A. First, the shutter 26 was opened on the Sr-Ca-Cu-0 target 22 to give an electric current of about 3 OA. Next, open the shutter 12 on the Bi-0 target 21 and form LA for about 1 minute.
The shutter 26 was opened on the Bi-Sr-Ca-Cu-0 target 23 and sputtering was performed until the required film thickness was achieved.During these steps, the substrate was continued to be heated one row at a time, and periodic lamination was performed to form nine films. Thin film superconductor & friend formed by the manufacturing method of the invention Compared to the case where Bi-based superconductor is directly formed on the substrate, the zero resistance temperature rises by several tens of K, and the IOA of the irregularities of the substrate is Sr-Ca-Cu oxidized. It is thought that the crystalline layer of a composite oxide superconducting thin film having a belobedite structure similar to this Sr-Ca-Cu oxide is formed stably on the surface of the substrate after being flattened by the Sr-Ca-Cu oxide layer. According to surface observation of this thin film superconductor, which has approximately doubled Jc,
Even though the grain size increases, the reason for this increase in Jc is not clearly elucidated. Electrical conduction is thought to occur within the Cu-0 plane. This is thought to be due to improved connectivity and a reduction in the current barrier due to the increased grain size.
It is possible to create a phase with a critical temperature higher than LIOOK by changing the film thickness.The results of an analysis of the case where a thin film of about the same size as a superconductor was created by changing the film thickness. The composition was Bi:Sr:Ca:Cu=2:2:2:3.Even in this state, this thin film superconductor showed a superconducting transition of IOOK or better.Furthermore, it was heat-treated at 850℃ for 1 hour. When carried out in oxygen, the temperature at 100K is very reproducible.
By adding this heat treatment in oxygen to the production of the present invention, the oxidation of each metal element is promoted, and it is effective in stabilizing each layer to create this structure. However, in Example 2, sputter deposition was performed using a total of four targets of Bi, CaCq, and two Sr*Cu, focusing on the MgO (100) substrate. Each target was set up at an angle of about 30 degrees so that it would connect. There is a rotating shutter in front of the target, and by rotating the slit in it, the Sr*Cu
→CaCu→Srs Approximately 5 凰 in C cycle then Bi+ Srs Cu-b CaCu-+ Srt C
Sputter deposition was performed using a cycle of u-*CaCu-*Srs Cu-+Bi, and the nine substrates were heated to approximately 300°C with a heater, and the gas pressure was 3 Pa in a mixed atmosphere with an argon to oxygen ratio of 5:1. Sputtering was carried out on each target.
When periodic lamination was carried out with 0m input CaCu at 250mA and a shutter rotation period of 10 minutes with intervals, it was possible to create a phase with a critical temperature of 105K or more at a substrate temperature of 300℃. A thin film of about 100A was produced by vapor deposition, and the composition at this time was Bi:Sr:Ca:Cu=2:2:2:
3 Even in this state, this thin film is 105
By creating a thin film superconductor by setting a target for each layered structure, a thin film with higher crystallinity can be produced without being affected by the irregularities of the substrate. When a monocrystalline thin film is formed without gaps, and a manufacturing method with gaps as in t4 Example 2, crystallization progresses at lower temperatures compared to the case without gaps, and sharp peaks are observed when evaluated using X-rays, etc. This is thought to be because the structure of the constituent metals is well connected and is very useful for producing thin films with excellent crystallinity. The basic idea is to form a stable belobed structure on the surface with a part of the constituent composition of the holding plate.Although a high-performance superconducting thin film with good cohesiveness can be obtained, it is also a method of laminating different materials by sputter deposition. There is a method of sputtering multiple targets with different compositions.It is relatively easy to use a method of periodically controlling the erosion area by controlling the discharge position of one target with a composition distribution. Although this can be easily achieved, especially when sputter deposition is not used, it is recommended to introduce the 0 phase at least at some point after the film formation or during the intermittent period (~ In addition, it is recommended to introduce the 0 By irradiating the substrate with an ion beam or exposing it to Ot or Neo plasma, the crystallinity can be further improved and the critical current density can be increased.Also, sputtering methods such as laser beam sputtering or ion beam sputtering can be used. It can also be formed using sputtering, and by periodically moving multiple targets and periodically changing the targets irradiated with the beam, a periodic laminated film can be realized. It is possible to form the thin film superconductor of the present invention using MBE, multi-dimensional EB equipment, etc. In that case, it is possible to form the thin film superconductor of the present invention by oxygen ion beam plasma irradiation, etc., during at least one of the steps during formation or intermittently. , it is preferable to supply oxygen. In addition, in the above embodiment, an example was given for a Bi-based thin film superconductor. ) and copper-containing oxide thin air
or an oxide thin film containing at least yttrium (Y) and alkaline earths (Ila group) and copper; or at least neodymium (Nd) and alkaline earths (I
Similar results were obtained with an oxide thin film layer containing at least lanthanum (La) and alkaline earth (Ila group) and copper. Method for manufacturing the thin film superconductor of the invention
It provides a method for producing oxide superconducting thin films with good crystallinity and good reproducibility, and is of great industrial value.
第1図(友 本発明の一実施例により形成した超伝導薄
膜の模式医 第2図(友 本発明の一実施例の薄膜超伝
導体製造用のマグネトロンスパツタ装置の基本構成図で
あも
11.24−−−基恢1 2 ・・・Sr−Ca−Cu
酸化IX 13・・・Bi酸化私1 4 ・・・Bi−
Sr−Ca−Cu酸化物、 2l・ ・ ・Bi−0タ
ーゲット、 22・ ・・Sr−Ca−Cu−0ターゲ
ット、 2 3 ・・拳Bi−Sr−Ca−Cu−0タ
ーゲット、 25・ ・・ヒーター、 26・ ・・シ
ャッター0Figure 1 (Friend) A schematic diagram of a superconducting thin film formed according to an embodiment of the present invention Figure 2 (Friend) A basic configuration diagram of a magnetron sputtering apparatus for producing a thin film superconductor according to an embodiment of the present invention. 11.24---Basic 1 2...Sr-Ca-Cu
Oxidation IX 13...Bi oxidation I 1 4...Bi-
Sr-Ca-Cu oxide, 2l...Bi-0 target, 22...Sr-Ca-Cu-0 target, 23...Fist Bi-Sr-Ca-Cu-0 target, 25... Heater, 26...Shutter 0
Claims (5)
体上に配し、前記A層上にビスマス(Bi)を含む酸化
物のB層を配し、前記B層上に銅を含む複合酸化物超伝
導薄膜を積層することを特徴とする、薄膜超伝導体の製
造方法。 ここにアルカリ土類は、 IIa族元素のうち少なくと
も一種あるいは二種以上の元素を示す。(1) A layer A of an oxide containing copper and an alkaline earth is disposed on a substrate, a B layer of an oxide containing bismuth (Bi) is disposed on the A layer, and a layer B containing copper is disposed on the B layer. A method for producing a thin film superconductor, characterized by laminating composite oxide superconducting thin films. Here, alkaline earth refers to at least one or two or more elements of Group IIa elements.
Bi)とアルカリ土類、あるいはタリウム(Tl)とア
ルカリ土類、あるいはイットリウム(Y)とアルカリ土
類、あるいはネオジウム(Nd)とアルカリ土類、ある
いはランタン(La)とアルカリ土類の内何れかを含む
層を積層した層であることを特徴とする、請求項1記載
の薄膜超伝導体の製造方法。 ここにアルカリ土類は、 IIa族元素のうち少なくと
も一種あるいは二種以上の元素を示す。(2) A complex oxide superconducting thin film containing copper is made of bismuth (
Bi) and alkaline earth, thallium (Tl) and alkaline earth, yttrium (Y) and alkaline earth, neodymium (Nd) and alkaline earth, or lanthanum (La) and alkaline earth. 2. The method for producing a thin film superconductor according to claim 1, wherein the layer is a laminated layer containing layers. Here, alkaline earth refers to at least one or two or more elements of Group IIa elements.
を含む酸化物の層と、銅酸化物を主体とする層と、アル
カリ土類酸化物を主体とする層とを、周期的に積層させ
て得ることを特徴とする、請求項1もしくは2何れかに
記載の薄膜超伝導体の製造方法。(3) A composite oxide superconducting thin film layer containing copper is formed by periodically layering an oxide layer containing bismuth, a layer mainly consisting of copper oxide, and a layer mainly consisting of alkaline earth oxide. 3. The method for producing a thin film superconductor according to claim 1, wherein the thin film superconductor is obtained by laminating layers.
グで行うことを特徴とする、請求項1記載の薄膜超伝導
体の製造方法。(4) The method for producing a thin film superconductor according to claim 1, wherein the evaporation of the composite oxide superconducting thin film is performed by sputtering.
℃から900℃の範囲に加熱することを特徴とする、請
求項1記載の薄膜超伝導体の製造方法。(5) When forming layer A on the substrate, the substrate is
The method for producing a thin film superconductor according to claim 1, characterized in that heating is performed to a temperature in the range of 900°C to 900°C.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2007422A JPH03215319A (en) | 1990-01-17 | 1990-01-17 | Manufacturing method of thin film superconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2007422A JPH03215319A (en) | 1990-01-17 | 1990-01-17 | Manufacturing method of thin film superconductor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03215319A true JPH03215319A (en) | 1991-09-20 |
Family
ID=11665434
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2007422A Pending JPH03215319A (en) | 1990-01-17 | 1990-01-17 | Manufacturing method of thin film superconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03215319A (en) |
-
1990
- 1990-01-17 JP JP2007422A patent/JPH03215319A/en active Pending
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