JPH03197320A - Manufacturing method of thin film superconductor - Google Patents
Manufacturing method of thin film superconductorInfo
- Publication number
- JPH03197320A JPH03197320A JP1339012A JP33901289A JPH03197320A JP H03197320 A JPH03197320 A JP H03197320A JP 1339012 A JP1339012 A JP 1339012A JP 33901289 A JP33901289 A JP 33901289A JP H03197320 A JPH03197320 A JP H03197320A
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- oxygen
- manufacturing
- substrate
- film superconductor
- Prior art date
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Classifications
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- 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
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- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Superconductors And Manufacturing Methods Therefor (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、高臨界温度を持つ酸化物超電導体の薄膜超電
導導体製造方法、特にN d2CuOa型結晶構造の酸
化物超電導体薄膜の製造方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a method for producing a thin film superconductor of an oxide superconductor having a high critical temperature, and particularly to a method for producing a thin film of an oxide superconductor having a N d2CuOa type crystal structure. be.
従来の技術
高い超電導転移温度を持つ酸化物超電導体として、Ba
−La−Cu−0系の超電導体が発見された[シーエイ
、シー、ヘードノルフ ?シトー ケイ、■−、ミュラ
ー(J 、G、Bedno−rz and に、A
、Muller)wブフイトシ1リフト フ1? フイ
シー−り(ZeitshriFtfur Physi
k B)−Condensed Matter、v
ol、64゜189−193(+986)]。これ以来
数々の新しい酸化物超電導体が発見されるに至った。Conventional technology Ba is an oxide superconductor with a high superconducting transition temperature.
-La-Cu-0 system superconductor discovered [C, C, Hednorf? Sito, K., Müller, J., G., Bedno-Rz and A.
, Muller) w Buhuitoshi 1 lift fu 1? ZeitshriFtfur Physi
k B)-Condensed Matter, v
ol, 64°189-193 (+986)]. Since then, many new oxide superconductors have been discovered.
ところで最近、これら従来の酸化物超電導体とは常電導
状態における電荷輸送担体が異なる、N d−Ce−C
u−0に代表されるN d2 C110A型結晶構造の
新しい酸化物超電導体が発見された[ワ仁トクラ、エイ
J、りh4−7ント″ ニス、つ子ター(Y、Toku
ra、H,Takagi andS、Uchida)
、2イf+−(Nature)vol 、337,34
5−347(1989)]。この種の材料の超電導機構
の詳細は明らかではないが、転移温度がさらに高くなる
可能性があり、また新しいデバイスの実現等の有望な応
用が期待される。By the way, recently, N d-Ce-C, which has a different charge transport carrier in the normal conduction state from these conventional oxide superconductors, has been developed.
A new oxide superconductor with the N d2 C110A type crystal structure represented by u-0 has been discovered.
ra, H, Takagi and S, Uchida)
, 2i f + - (Nature) vol, 337, 34
5-347 (1989)]. Although the details of the superconducting mechanism of this type of material are not clear, the transition temperature may be even higher, and promising applications such as the realization of new devices are expected.
発明が解決しようとする課題
しかしながら、N d−Ce−Cu−0系の材料は、現
在の技術では主として焼結という過程でしか形成できな
いため、セラミックの粉末あるいはブロックの形状でし
か得られない。一方、この種の材料を実用化する場合、
薄膜状に加工することが強く要望されているが、従来の
技術では、良好な超電導特性を有する薄膜作製は非常に
困難とされてい本発明は、このような従来技術の課題を
解決することを目的とするものである。Problems to be Solved by the Invention However, with current technology, Nd-Ce-Cu-0 based materials can only be formed mainly through the process of sintering, and therefore can only be obtained in the form of ceramic powder or blocks. On the other hand, when putting this type of material into practical use,
Although there is a strong demand for processing into a thin film, it is considered extremely difficult to fabricate a thin film with good superconducting properties using conventional techniques.The present invention aims to solve the problems of the conventional techniques. This is the purpose.
課題を解決するための手段
本発明は、主成分が、Nd2CuOn型結晶構造の(A
1− * B x ) 2 Cu O4で表わされる
複合酸化物の超電導薄膜を作製するため、基本的にスパ
ッタ蒸着法を用いて、適当な基体上に結晶性の高い薄膜
を形成すると共に、酸素欠損の導入を行うことにより酸
素の含有量を化学量論比より少ない最適値にするという
ものである。ここで、AはNd、 Ss。Means for Solving the Problems The present invention provides a method in which the main component is (A
1- *B By introducing this, the oxygen content is brought to an optimum value lower than the stoichiometric ratio. Here, A is Nd, Ss.
P「のうちの少なくとも一種、BはCe、Thのうちの
少なくとも一種の元素を示す。また、Xは、0.06≦
X≦0.08の範囲の数値である。B represents at least one element of Ce and Th. X represents 0.06≦
It is a numerical value in the range of X≦0.08.
作用
本発明は、上記のような構成によって、良質で高性能な
Nd2CLIOa型結晶構造の薄膜超電導体を再現性良
く得ることが可能となった。Effects The present invention, with the above-described configuration, has made it possible to obtain a high-quality, high-performance thin film superconductor having an Nd2CLIOa type crystal structure with good reproducibility.
実施例
本発明者らはこのN d2Cuo a型結晶構造の酸化
物超電導体に対して、スパッタ蒸着法による薄膜作製を
行ない、作製条件と薄膜の超電導性の関係について詳細
に調べた。スパッタリングターゲットとしては、A元素
、B元素、Cuを含む酸化物を大気中において高温で熱
処理して得た焼結体を用いた。ただしAはNd、 S
m、 Prのうちの少なくとも一種、BはCe、Th
のうちの少なくとも一種の元素を示す。その結果400
℃〜1000℃に加熱した単結晶基体上に、例えばNd
+、5sCe@、+5Cubaの薄膜を、NdとCeと
Cuを含むターゲットをスパッタして成膜させ、結晶化
r4膜を得ることが出来た。そして単結晶基板の使用は
、アルミナのような非結晶材料を基板として用いた場合
に比べてNd+、5sCeu、+5CIJOJ薄膜の結
晶性を改善するという作用があることを確認した。M8
0単結晶を基板として用いた場合には、 (001)、
あるいは(110)の結晶軸方向に配向する。特に
5rTi03.BaTio3.LaAlO3,LaGa
O3等のペロブスカイト型の結晶構造を有する単結晶を
基板として使用した場合には、その結晶軸にそフて N
IL、5sCee、+5CuOaの結晶軸が配向し、良
好な結晶性を持つ薄膜が得られることを発明者らは見い
だした。EXAMPLE The present inventors fabricated a thin film of this oxide superconductor having the N d2Cuo a-type crystal structure by sputter deposition, and investigated in detail the relationship between the fabrication conditions and the superconductivity of the thin film. As a sputtering target, a sintered body obtained by heat-treating an oxide containing element A, element B, and Cu at high temperature in the atmosphere was used. However, A is Nd, S
m, at least one of Pr, B is Ce, Th
Indicates at least one element of The result was 400
For example, Nd
+, 5sCe@, and +5Cuba thin films were formed by sputtering a target containing Nd, Ce, and Cu, and crystallized r4 films were successfully obtained. It was also confirmed that the use of a single crystal substrate has the effect of improving the crystallinity of the Nd+, 5sCeu, +5CIJOJ thin film compared to the case where an amorphous material such as alumina is used as the substrate. M8
When a 0 single crystal is used as a substrate, (001),
Alternatively, it is oriented in the (110) crystal axis direction. Especially 5rTi03. BaTio3. LaAlO3, LaGa
When a single crystal with a perovskite crystal structure such as O3 is used as a substrate, N
The inventors have discovered that the crystal axes of IL, 5sCee, and +5CuOa are oriented, and a thin film with good crystallinity can be obtained.
さらに、通常酸化物薄膜の作製の場合、スパッタガスと
して、アルゴンなどの不活性ガスと酸素または酸化ガス
をほぼ等量混合して用いる。ところがN To CuO
a型結晶構造の酸化物超電導体においては、スパッタガ
ス中の酸素あるいは酸化ガスの分圧を極端に低くして成
膜すると、意外にも良好な超電導性が、すなわち、セラ
ミックス材料とほぼ等しい20にのものが、再現性良く
得られることを得られることを本発明者らは発見した。Furthermore, in the case of producing an oxide thin film, a mixture of approximately equal amounts of an inert gas such as argon and oxygen or an oxidizing gas is used as a sputtering gas. However, N To CuO
In an oxide superconductor with an a-type crystal structure, when the film is formed with an extremely low partial pressure of oxygen or oxidizing gas in the sputtering gas, surprisingly good superconductivity can be obtained, that is, almost the same as that of ceramic materials. The present inventors have discovered that the following can be obtained with good reproducibility.
この原因は現在のところ明らかではないが、この種の材
料のセラミックスの焼結においては還元雰囲気がよいと
も言われており、スパッタ蒸着中の酸素分圧を低くする
ことにより不必要な酸素が薄膜の結晶構造中に入らない
、あるいは、薄膜の組成が、Nd+、5sCes、+5
CuOa−uと適当な量yの酸素欠損が導入されている
ため、良い結果が得られているのではないかと思われる
。さらに、酸素あるいは酸化ガスを全く含まない不活性
ガスのみの場合にも良好な超電導特性が得られることを
見いだした。不活性ガスとしてはアルゴンが比較的利用
し易く、また結果も良いことを確認した。これらの理由
は、Nd2CuOn型の結晶構造を作るにはある程度の
酸素が必要ではあるが、その酸素はターゲットから十分
供給することが可能であると思われる。The cause of this is not clear at present, but it is said that a reducing atmosphere is good for sintering ceramics made of this type of material, and by lowering the oxygen partial pressure during sputter deposition, unnecessary oxygen is removed from the thin film. or the composition of the thin film is Nd+, 5sCes, +5
It seems that good results are obtained because CuOa-u and an appropriate amount of oxygen vacancies are introduced. Furthermore, it has been found that good superconducting properties can be obtained even when using only an inert gas that does not contain any oxygen or oxidizing gas. It was confirmed that argon is relatively easy to use as an inert gas and gives good results. The reason for these is that although a certain amount of oxygen is required to create the Nd2CuOn type crystal structure, it is thought that the oxygen can be sufficiently supplied from the target.
スパッタ蒸着した膜、特に、基体温度を750℃〜10
00℃とした膜の結晶性は、超電導特性を得るには十分
であるが、さらに大気中もしくは10−3気圧以上の酸
素を含んだ雰囲気で、900℃〜1100℃の温度範囲
で一定時間加熱することによって結晶性を高めることが
でき、さらに優れた超電導特性を得ることができること
を確認した。あわせて、熱処理後、室温以下に急冷する
ことが、酸素含有量を少なくして後の還元処理を容易に
することを見いだした。Sputter-deposited films, especially when the substrate temperature is 750°C to 10°C.
Although the crystallinity of the film at 00°C is sufficient to obtain superconducting properties, it is necessary to heat it for a certain period of time in the temperature range of 900°C to 1100°C in the air or in an atmosphere containing oxygen at 10-3 atmospheres or more. It was confirmed that by doing so, it was possible to improve crystallinity and obtain even better superconducting properties. Additionally, it has been found that rapid cooling to room temperature or lower after heat treatment reduces the oxygen content and facilitates subsequent reduction treatment.
また、本発明者らは、適当な還元処理を行い、酸素欠損
の導入により酸素の含有量を化学量論比より少ない最適
値にすることによって、最適の超電導特性を得ることが
できることを見いだした。In addition, the present inventors have discovered that optimal superconducting properties can be obtained by performing appropriate reduction treatment and reducing the oxygen content to an optimal value lower than the stoichiometric ratio by introducing oxygen vacancies. .
還元処理の方法としては、真空中もしくは酸素分圧10
−3気圧以下のアルゴン等の不活性ガス雰囲気で、加熱
することが有効であることを見いだした。その際の、酸
素の脱離量あるいは欠損量は、酸素の拡散過程に強く依
存する。すなわち、加熱する際の処理温度!!囲として
は、500℃〜900℃が適当であるが、必要な処理時
閏は、超電導体の膜厚及び表面状態によっても影響を受
けるが、処理温度が高いほど短い時間で済むことを見い
だした。しかしながら、処理時閏が長すぎると、かえっ
て超電導性を損なわせる結果となり、各処理温度には最
適な処理時間が存在することを見いだした。The method of reduction treatment is in a vacuum or at an oxygen partial pressure of 10
It has been found that heating in an inert gas atmosphere such as argon at a pressure of -3 atmospheres or less is effective. At this time, the amount of oxygen desorbed or the amount of defects strongly depends on the oxygen diffusion process. In other words, the processing temperature when heating! ! The appropriate temperature range is 500°C to 900°C, but the required processing time is also affected by the film thickness and surface condition of the superconductor, but it has been found that the higher the processing temperature, the shorter the processing time. . However, if the processing time is too long, the superconductivity will be impaired, and it has been found that there is an optimum processing time for each processing temperature.
もう一つの還元処理の方法として、少なくともフッ素ガ
スを含んだ雰囲気下で加熱することによって酸素をフッ
素と置換すれば、超電導特性を得ることができることを
見いだした。As another reduction treatment method, we have discovered that superconducting properties can be obtained by replacing oxygen with fluorine by heating in an atmosphere containing at least fluorine gas.
以下に、更に具体的な実施例を示す。More specific examples are shown below.
NdとCeとCuを含む酸化物セラミックス焼結体をタ
ーゲットとして用い、チタン酸ストロンチウム(100
)面の基体上に、高周波プレナーマグネトロンスバッタ
により薄膜作製を行なった。このターゲットは、Nd2
O3、CeO2、CuOを大気中1050℃で8時閉熱
処理し得た焼結体を用いた。スパッタガスは純アルゴン
ガスとしたが、良好な結晶性の薄膜が形成可能であった
。この理由は、N d2Cuo a型の結晶構造を作る
にはある程度の酸素が必要で、その酸素はターゲットか
ら供給されるのが一番適していることによると思われる
。Using an oxide ceramic sintered body containing Nd, Ce, and Cu as a target, strontium titanate (100
) A thin film was fabricated on the surface of the substrate by high-frequency planar magnetron scattering. This target is Nd2
A sintered body obtained by subjecting O3, CeO2, and CuO to heat treatment in the air at 1050° C. for 8 hours was used. Although pure argon gas was used as the sputtering gas, a thin film with good crystallinity could be formed. The reason for this seems to be that a certain amount of oxygen is required to create the N d2Cuo a type crystal structure, and that oxygen is most suitably supplied from the target.
蒸着中の基体の温度としては400℃〜1000℃とし
た場合に、低温で薄膜の電気抵抗に超伝導の兆候が認め
られたが、特に750℃〜1000℃で形成した薄膜に
おいては、ゼロ抵抗が20に程度で確認され、また結晶
性も良く再現性もすぐれていた。When the temperature of the substrate during vapor deposition was 400°C to 1000°C, signs of superconductivity were observed in the electrical resistance of the thin film at low temperatures, but especially in thin films formed at 750°C to 1000°C, zero resistance was observed. was confirmed to be about 20%, and the crystallinity was also good and the reproducibility was excellent.
以下本発明の内容を深く理解されるために、さらに具体
的な実施例を示す。More specific examples will be shown below in order to better understand the content of the present invention.
Nd+、5sCei、+sCu’50x の酸化物セラ
ミックス焼結体をターゲットとして用い、Mgo、
あるいは、SrT 1o3の (100) −あるいは
(110)面の単結晶基体上に、薄膜形成を行なフた。Using an oxide ceramic sintered body of Nd+, 5sCei, +sCu'50x as a target, Mgo,
Alternatively, a thin film was formed on a (100)- or (110)-plane single crystal substrate of SrT 1o3.
スパッタ電力160W、スパッタガス圧力3X10−3
T orrの条件のもとで、約1時閏スパッタ蒸着する
ことにより、約0. 5〜0. 8μm厚の薄膜が得ら
れた。スパッタガスは純アルゴンガスとし、この際の基
体温度を変化させて、結晶性および出現する超伝導特性
との関係を調べた。上記過程の後、薄膜の組成を調べた
ところ、金属元素の比率はNd: Ce: Cu=1.
85: 0.15: 1.Oとほぼ化学量論比にな
っていた。また薄膜の結晶構造は、X線回折法により調
べられた。Sputtering power 160W, sputtering gas pressure 3X10-3
By performing sputter deposition in about 1 hour under the condition of Torr, about 0. 5-0. A thin film with a thickness of 8 μm was obtained. The sputtering gas was pure argon gas, and the substrate temperature was varied to investigate the relationship between crystallinity and superconducting properties. After the above process, we investigated the composition of the thin film and found that the ratio of metal elements was Nd:Ce:Cu=1.
85: 0.15: 1. It was in a nearly stoichiometric ratio with O. The crystal structure of the thin film was also investigated by X-ray diffraction.
この結果、基板として5rTiO3(100)基板を用
いた場合、形成されたtilllH,tc軸が基板に垂
直に配向したN d2CuOa型の結晶構造であること
が判った。 5rT1C)3(110)基板を用いた
場合には、 (103)面の薄膜が成長し、Mg0(1
00)面には、 (110)ii、 (110)面に
は、(100)面が、それぞれ成長した。基体温度を7
50℃〜1000℃とした膜の結晶性は、超電導特性を
得るには十分であるが、さらに大気中もしくはlo−3
気圧以上の酸素を含んだ雰囲気で、900℃〜1100
℃の温度範囲で1時間〜2時閘加熱することによって結
晶性を高めることができ、さらに優れた超電導特性を得
ることができることを確認した。優れた超電導特性を与
える薄膜の結晶構造は、C軸が基板に垂直に配向したも
のが適していることが分かった。その意味で基体として
は、5rTio3(100)基板のほか、BaTio3
.LaAlO3,LaGaO3等のペロブスカイト型の
結晶構造を有する単結晶の(100)基板が優れている
ことを確認した。As a result, it was found that when a 5rTiO3 (100) substrate was used as the substrate, the formed tilllH,tc axis was oriented perpendicularly to the substrate to have an N d2CuOa type crystal structure. When a 5rT1C)3(110) substrate is used, a thin film of the (103) plane grows, and Mg0(1
The (110)ii and (100) planes grew on the 00) plane and the (110) plane, respectively. Substrate temperature to 7
The crystallinity of the film at 50°C to 1000°C is sufficient to obtain superconducting properties, but even in the atmosphere or lo-3
900°C to 1100°C in an atmosphere containing oxygen above atmospheric pressure
It was confirmed that crystallinity could be improved by heating in the temperature range of 1 to 2 hours, and even better superconducting properties could be obtained. It has been found that a thin film crystal structure in which the C-axis is oriented perpendicular to the substrate is suitable for providing excellent superconducting properties. In that sense, as a substrate, in addition to 5rTio3 (100) substrate, BaTio3
.. It was confirmed that single crystal (100) substrates having a perovskite crystal structure such as LaAlO3 and LaGaO3 are excellent.
得られた薄膜の中には、成膜後あるいは上述の結晶化を
促進させるための加熱処理後に、超電導特性を示すもの
もあったが、その超電導特性は、適当な還元処理をによ
フて、さらに高めることができ、また、超電導特性を示
さなかったものについても、最適の超電導特性を得るこ
とができることを見いだした。また、熱処理後、室温以
下に急冷することが、酸素含有量を少なくして後の還元
処理を容易にすることを見いだした。還元処理の方法と
しては、真空中もしくは酸素分圧1o−a気圧以下のア
ルゴン等の不活性ガス雰囲気で、加熱することが有効で
あることを見いだした。膜厚5000Aの代表的な薄膜
について、処理温度および処理時間を変化させて、真空
中で加熱した際の電気抵抗の温度依存性を図に示す。曲
線11は還元処理前、曲線12.13.14は、600
’Cでツレぞれ2.16.52時間処理したもの、曲線
15は、800℃で2時間処理したものである。Some of the obtained thin films exhibited superconducting properties after being deposited or after the heat treatment described above to promote crystallization; It has been found that it is possible to further improve the superconducting properties, and even for those that did not exhibit superconducting properties, it is possible to obtain optimal superconducting properties. It has also been found that rapid cooling to room temperature or lower after heat treatment reduces the oxygen content and facilitates subsequent reduction treatment. It has been found that heating in a vacuum or in an inert gas atmosphere such as argon with an oxygen partial pressure of 1 o-a atmosphere or less is effective for the reduction treatment. The figure shows the temperature dependence of electrical resistance of a typical thin film with a thickness of 5000 A when heated in vacuum while varying the processing temperature and processing time. Curve 11 is before reduction treatment, curves 12, 13, and 14 are 600
Curve 15 was treated at 800°C for 2 hours.
転移温度22に以上の優れた超電導特性を得るのに必要
な処理時間は、600℃で8〜30時間、800℃で1
〜3時間処理であった。これより、酸素の脱離量あるい
は欠損量は、酸素の拡散過程に強く依存し、加熱する際
の処理温度範囲としては、500℃〜900℃が適当で
あるが、最適な処理時間は、超電導体の膜厚及び表面状
態によっても影響を受けるが、処理温度が高いほど短い
時間で済むが、最適時間範囲は狭いことを見いだしさら
に、本発明者らは、蒸着膜を還元し酸素含有量を少なく
する方法として、フッ素との置換効果を利用することが
有効であることを確認した。The treatment time required to obtain excellent superconducting properties with a transition temperature of 22 or higher is 8 to 30 hours at 600°C and 1 hour at 800°C.
The treatment was for ~3 hours. From this, the amount of oxygen desorption or loss strongly depends on the oxygen diffusion process, and the appropriate temperature range for heating is 500°C to 900°C, but the optimal processing time is Although it is influenced by the film thickness and surface condition of the body, the higher the processing temperature, the shorter the processing time, but the optimum time range is narrow. It was confirmed that utilizing the substitution effect with fluorine is an effective way to reduce the amount.
例えば、フッ素を含んだフロンガス等の雰囲気で放電を
起こし、活性なフッ素に薄膜を曝せば、フッ素との置換
効果によって酸素量を減らすことができ良好な超電導薄
膜を形成することが出来ることを確認した。For example, it was confirmed that if a thin film is exposed to active fluorine by causing a discharge in an atmosphere of fluorine-containing CFC gas, the amount of oxygen can be reduced due to the substitution effect with fluorine, and a good superconducting thin film can be formed. did.
なおこの結果は、Ndの代わりにS+w、Prあるいは
この少なくとも一種を含む組合せ、またCeの代わりに
Thあるいはこの少なくとも一種を含む組合せでも、同
様であることが確認された。It was confirmed that this result was the same for combinations containing S+w, Pr, or at least one of these instead of Nd, and for combinations containing Th or at least one of these instead of Ce.
発明の効果
本発明により、良質で高性能なN d2Cuo a型結
晶構造の薄膜超電導体を再現性良く得ることが可能とな
った0本発明の製造方法は、この種の物質を用いたデバ
イス等の応用には必須であり、本発明の工業的価値は大
きい。Effects of the Invention The present invention has made it possible to obtain a high-quality, high-performance thin film superconductor with an N d2Cuo a-type crystal structure with good reproducibility. It is essential for the application of this invention, and the industrial value of the present invention is great.
図は本発明の一実施例において製造された薄膜超電導体
の、電気抵抗の温度依存性を示す図である。
1・l・・・還元処理前、12.13.14・・・60
0℃で2.16.52時間処理、15・・・800℃で
2時閏処理。The figure is a diagram showing the temperature dependence of electrical resistance of a thin film superconductor manufactured in an example of the present invention. 1.l...Before reduction processing, 12.13.14...60
Treatment at 0°C for 2, 16, and 52 hours, 2 hours at 15...800°C.
Claims (5)
造の(A_1_−_xB_x)_2CuO_4で表され
る複合酸化物のスパッタ蒸着膜に対し、還元処理を施す
(ここで、AはNd,Sm,Prのうちの少なくとも一
種、BはCe,Thのうちの少なくとも一種の元素を示
す。 また、xは、0.06≦x≦0.08の範囲の数値であ
る)ことを特徴とする薄膜超電導体の製造方法。(1) A reduction treatment is performed on a sputter-deposited film of a composite oxide whose main component is (A_1_-_xB_x)_2CuO_4 having an Nd_2CuO_4 type crystal structure (here, A is Nd, Sm, Pr B represents at least one element of Ce and Th; x is a numerical value in the range of 0.06≦x≦0.08). manufacturing method.
る単結晶基板を用いることを特徴とする請求項1記載の
薄膜超電導体の製造方法。(2) The method for manufacturing a thin film superconductor according to claim 1, characterized in that a single crystal substrate having a perovskite crystal structure is used as the substrate.
−^3気圧以上の酸素を含んだ雰囲気で、900℃〜1
100℃の温度範囲で一定時間加熱して得た蒸着膜を用
いることを特徴とする請求項1記載の薄膜超電導体の製
造方法。(3) After sputter deposition, further in the atmosphere or 10^
-^ In an atmosphere containing oxygen of 3 atmospheres or more, 900℃~1
2. The method for producing a thin film superconductor according to claim 1, wherein a vapor deposited film obtained by heating in a temperature range of 100° C. for a certain period of time is used.
10^−^3気圧以下の不活性ガス雰囲気で、500℃
〜900℃の温度範囲で一定時間加熱することを特徴と
する請求項1記載の薄膜超電導体の製造方法。(4) As a method of reduction treatment, in a vacuum or in an inert gas atmosphere with an oxygen partial pressure of 10^-^3 atm or less at 500°C.
2. The method for producing a thin film superconductor according to claim 1, wherein the heating is performed at a temperature range of -900[deg.] C. for a certain period of time.
含んだ雰囲気下にさらすことを特徴とする請求項1記載
の薄膜超電導体の製造方法。(5) The method for manufacturing a thin film superconductor according to claim 1, wherein the reduction treatment includes exposing the thin film superconductor to an atmosphere containing at least fluorine gas.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1339012A JPH07106904B2 (en) | 1989-12-26 | 1989-12-26 | Method of manufacturing thin film superconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1339012A JPH07106904B2 (en) | 1989-12-26 | 1989-12-26 | Method of manufacturing thin film superconductor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03197320A true JPH03197320A (en) | 1991-08-28 |
| JPH07106904B2 JPH07106904B2 (en) | 1995-11-15 |
Family
ID=18323437
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1339012A Expired - Fee Related JPH07106904B2 (en) | 1989-12-26 | 1989-12-26 | Method of manufacturing thin film superconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH07106904B2 (en) |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02211678A (en) * | 1989-02-10 | 1990-08-22 | Sony Corp | Manufacture of superconducting metallic oxide material |
-
1989
- 1989-12-26 JP JP1339012A patent/JPH07106904B2/en not_active Expired - Fee Related
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02211678A (en) * | 1989-02-10 | 1990-08-22 | Sony Corp | Manufacture of superconducting metallic oxide material |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH07106904B2 (en) | 1995-11-15 |
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