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JPH0531492B2 - - Google Patents
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JPH0531492B2 - - Google Patents

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Publication number
JPH0531492B2
JPH0531492B2 JP62200928A JP20092887A JPH0531492B2 JP H0531492 B2 JPH0531492 B2 JP H0531492B2 JP 62200928 A JP62200928 A JP 62200928A JP 20092887 A JP20092887 A JP 20092887A JP H0531492 B2 JPH0531492 B2 JP H0531492B2
Authority
JP
Japan
Prior art keywords
film
superconducting
superconducting material
base material
spray nozzle
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.)
Expired - Lifetime
Application number
JP62200928A
Other languages
Japanese (ja)
Other versions
JPS6445015A (en
Inventor
Kyoji Tachikawa
Minoru Matsuda
Yukio Shinho
Teruo Suzuki
Makoto Kabasawa
Itaru Watanabe
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.)
Tokai University
JFE Engineering Corp
Original Assignee
Tokai University
Nippon Kokan 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 Tokai University, Nippon Kokan Ltd filed Critical Tokai University
Priority to JP62200928A priority Critical patent/JPS6445015A/en
Publication of JPS6445015A publication Critical patent/JPS6445015A/en
Publication of JPH0531492B2 publication Critical patent/JPH0531492B2/ja
Granted legal-status Critical Current

Links

Classifications

    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Landscapes

  • Inorganic Compounds Of Heavy Metals (AREA)
  • Superconductor Devices And Manufacturing Methods Thereof (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔産業上の利用分野〕 この発明は、超電導材の製造方法に関するもの
である。 〔従来の技術およびその問題点〕 超電導材料は、既に高エネルギー粒子加速器、
医療診断用MRI−CT物性研究装置等において、
超電導マグネツトの形で実用化されている。ま
た、発電機、エネルギーの貯蔵や変換、リニアモ
ーターカー、資源回収用磁気分離装置、核融合
炉、送電ケーブル、磁気シールド材等への応用、
さらには、ジヨセフソン効果を用いた超電導素子
は、超高速コンピユーター、赤外線検出器、低雑
音の増幅器等への応用が期待されており、これら
が本格的に実用化された場合の産業的、社会的イ
ンパクトの大きさは、未だ測りがたい。 これまでに開発された超電導材料の代表的なも
のとして、Nb−Ti合金があり、現在9Tまでの磁
界発生用線材として広く使用されている。Nb−
Ti合金のTc(超電導状態が存在する臨界温度)
は、9Kである。また、Nb−Ti合金よりも格段に
高いTcを有する材料として化合物系超電導材料
が開発され、現在Nb3Sn(Tc:18K)とV3Ga
(Tc:15K)が線材化され実用に供せられてい
る。さらに、Nb3Geでは23KのTcが得られてい
る。 このように長年に亘つて高Tc超電導材料を得
るための努力がなされてきたが、従来の合金系お
よび化合物系超電導材料においては、Tc23Kが
大きな壁になつている。Tcが23K以下の超電導
材料の冷却には、高価な液体Heが必要であり、
このことが超電導材料の広範な応用を阻害してい
る。このTcの壁を打破する材料として、1986年
にIBMチユーリツヒのMu¨ller氏等が、Ba−La−
Cu−O系の酸化物で超電導の徴候が認められた
と発表して以来、酸化物系超電導材料の開発競争
に拍車がかかつた。1986年にはTc40Kであつた
ものが、1987年の初には、早くも77Kの液体窒素
温度を超えるY−Ba−Cu−O系超電導材料が開
発され、Tcは約93Kに達した。さらに、その後
も精力的な開発が続けられており、今のところ安
全性等に問題はあるものの室温で超電導現象を示
す超電導材料の開発も報告されている。液体窒素
温度で使用可能な高温超電導材料の発見は、前述
した応用分野への期待度を増々高めるものである
が、実際の応用化に当つては、線材化、皮膜化な
どの加工技術の開発が伴わなければならない。 〔発明が解決しようとする問題点〕 超電導物質を皮膜化するには、超電導物質を溶
射法や蒸着法によつて基材上に付与させることが
考えられるが、これらの方法によれば、安定して
形成できる皮膜の厚さはたかだか1μm程度であ
り、給電容量が制限されること、加えて皮膜形成
速度が小さく、所定の膜形成に多大の時間を要す
る等の問題が残されている。 この発明の目的は、厚被膜を安定に形成させ、
加えて大きな成膜速度で超電導物質からなる皮膜
を基材上に形成させることができる超電導材の製
造方法を提供することにある。 〔問題点を解決するための手段〕 この発明は、基材の表面上に、溶射法によつて
CuxOy基を含む複合酸化物超電導物質の皮膜を形
成させ、次いで、このようにして得られた、前記
基材と前記皮膜とからなる超電導素材を500から
980℃の温度に加熱しながら、前記超電導素材に
圧下を加え、これによつて、前記皮膜の緻密性を
向上させ、次いで、前記超電導素材を酸素含有雰
囲気中において、20℃/min以下の冷却速度で冷
却し、これによつて前記皮膜に所定の超電導特性
を付与することに特徴を有するものである。 次に、この発明の、超電導材の製造方法の一実
施態様を図面を参照しながら説明する。 第1図は、この発明の、超電導材の製造方法の
一実施態様を示す断面図である。 第1図に示すようなプラズマ溶射装置1を使用
して、銅製基材2の表面上に、Y−Ba−Cu−O
系等の酸化物からなる超電導物質の皮膜3を形成
する。なお、溶射装置1は、プラズマ溶射以外の
例えば、ガス溶射等であつてもよい。 プラズマ溶射装置1は、真空容器4と、真空容
器4内に設けられた溶射ノズル5と、溶射ノズル
5内に設けられたタングステン電極6と、溶射ノ
ズル5と電極6との間に接続されたプラズマ電源
7とからなつている。 真空容器4内に、溶射ノズル5と対向して板状
または棒状の基材2を設置し、真空容器4内を減
圧しながら、溶射ノズル5内にアルゴン、ヘリウ
ム等のプラズマガスおよびY−Ba−Cu−O系等
の酸化物からなる超電導物質の粉末(10から
100μm)をそれぞれ連続的に供給し、そして、プ
ラズマ電源7を作動させて、溶射ノズル5と電極
6との間にプラズマアークを発生させる。 上述した溶射装置によつて、基材2と皮膜3と
からなる超電導素材8を得たら、次に、第2図に
示すように、超電導素材8をヒーター9を有する
加熱炉10によつて、500から980℃の温度に加熱
しながら、プレス11によつて皮膜3に圧下を加
える。これによつて、基材2の表面上に溶射され
た超電導物質の粒子同士の密着度が高まるので、
皮膜3の空孔率が減少する。また、基材2と皮膜
3との密着度も高くなる。 このようにして、超電導素材8に、所謂ホツト
プレスを施したら、超電導素材8を大気または酸
素雰囲気中において、20℃/min以下の速度で冷
却する。これによつて、超電導物質からなる皮膜
3の結晶構造は、斜方晶になる。この結果、超電
皮膜3が得られる。 ここで、熱処理温度を500〜980℃としたのは、
500℃未満では、均質な斜方晶を得ることが難し
く、且つ、酸素欠損量が大きく、十分な超電導特
性を得ることが困難であり、一方、熱処理温度が
980℃を超えると、基材と皮膜とが反応し、皮膜
中に基材物質が侵入し、超電導特性を示さなくな
るためである。 また、冷却速度を20℃/min以下としたのは、
20℃/minを超える冷却速度においては、皮膜に
割れが生じる危険性が高まること、皮膜と基材が
ハクリし易いこと、および、結晶中の酸素欠損量
が大きくなるためである。 次に、この発明の実施例について説明する。 第1図に示すプラズマ溶射装置1の真空容器4
内に、銅製の板状基材2をセツトし、プラズマガ
スとして、アルゴンガスとヘリウムガスとの混合
ガス(Ar:20/min、He:40/min)を溶
射ノズル5内に連続的に供給し、プラズマ電源7
から溶射ノズル5と電極6との間に15Kwの電力
を供給し、Y0.3−Ba0.7−Cu1−O3-yからなる超電
導物質の粉末(粒径10から100μm)を溶射ノズル
5内に供給し、そして、真空容器4内の気圧を
80mbarに減圧して、基材2の表面上に150μmの
膜厚を有する、超電導物質からなる皮膜3を形成
した。 次いで、このようにして得た、基材2と皮膜3
とからなる超電導素材8を、真空容器4から取り
出して加熱炉10内に装入し、大気下で500℃の
温度に30分間、プレス11によつて5Kgf/mm2
圧下しながら加熱した。次いで、このように圧下
を加えながら加熱した超電導素材8を10℃/min
の速度で冷却し、板状超電導材を製造した。 次に、超電導素材8の加熱温度を800℃に変え
た以外は、上述した実施例と同一条件に従つて別
の板状超電導材を製造した。 そして、このようにして製造した各超電導材の
一部を垂直に切断し、切断面を研摩した後、光学
顕微鏡によつて切断面を観察し、空孔率を調べ
た。この結果を超電導素材8にホツトプレス処理
を施さなかつた場合、即ち、溶射ままの場合と合
わせて第1表に示す。
[Industrial Field of Application] The present invention relates to a method for manufacturing a superconducting material. [Conventional technology and its problems] Superconducting materials have already been used in high-energy particle accelerators,
In MRI-CT physical property research equipment for medical diagnosis, etc.
It has been put into practical use in the form of superconducting magnets. Applications include generators, energy storage and conversion, linear motor cars, magnetic separation devices for resource recovery, nuclear fusion reactors, power transmission cables, magnetic shielding materials, etc.
Furthermore, superconducting elements using the Josephson effect are expected to be applied to ultra-high-speed computers, infrared detectors, low-noise amplifiers, etc., and if these are put into full-scale practical use, they will have significant industrial and social impact. The magnitude of the impact is still difficult to measure. Nb-Ti alloy is a typical superconducting material developed so far, and is currently widely used as a wire for generating magnetic fields up to 9T. Nb−
Tc of Ti alloy (critical temperature at which superconducting state exists)
is 9K. In addition, compound superconducting materials have been developed as materials with Tc much higher than Nb-Ti alloys, and currently Nb 3 Sn (Tc: 18K) and V 3 Ga
(Tc: 15K) has been made into wire and put into practical use. Furthermore, a Tc of 23K has been obtained with Nb 3 Ge. Although efforts have been made to obtain high Tc superconducting materials for many years, Tc23K has become a major barrier to conventional alloy-based and compound-based superconducting materials. Expensive liquid He is required to cool superconducting materials with Tc below 23K.
This hinders the widespread application of superconducting materials. In 1986, Mr. Mu¨ller of IBM Zurich and others proposed Ba-La-
Since the announcement that signs of superconductivity were observed in Cu-O-based oxides, the race to develop oxide-based superconducting materials has accelerated. In 1986, Tc was 40K, but in early 1987, a Y-Ba-Cu-O based superconducting material was developed that exceeded the liquid nitrogen temperature of 77K, and Tc reached approximately 93K. Furthermore, vigorous development has continued since then, and there have been reports of the development of superconducting materials that exhibit superconductivity at room temperature, although there are currently safety issues. The discovery of high-temperature superconducting materials that can be used at liquid nitrogen temperatures has raised expectations for the aforementioned application fields, but for actual application, it is necessary to develop processing techniques such as wire rods and coatings. must be accompanied by [Problems to be solved by the invention] In order to form a film with a superconducting material, it is possible to apply the superconducting material onto a base material by a thermal spraying method or a vapor deposition method. The thickness of the film that can be formed using this method is approximately 1 μm at most, which limits the power supply capacity, and in addition, the film formation rate is slow and it takes a long time to form the desired film. The purpose of this invention is to form a thick film stably,
In addition, it is an object of the present invention to provide a method for producing a superconducting material that can form a film made of a superconducting material on a base material at a high film formation rate. [Means for Solving the Problems] This invention provides a method of spraying onto the surface of a base material by a thermal spraying method.
A film of a composite oxide superconducting material containing a Cu x O y group is formed, and then the thus obtained superconducting material consisting of the base material and the film is
Pressure is applied to the superconducting material while heating it to a temperature of 980°C, thereby improving the denseness of the film, and then cooling the superconducting material at a rate of 20°C/min or less in an oxygen-containing atmosphere. It is characterized in that it is cooled at a rapid rate, thereby imparting predetermined superconducting properties to the film. Next, one embodiment of the method for manufacturing a superconducting material according to the present invention will be described with reference to the drawings. FIG. 1 is a sectional view showing one embodiment of the method for manufacturing a superconducting material according to the present invention. Using a plasma spraying apparatus 1 as shown in FIG. 1, Y-Ba-Cu-O
A film 3 of a superconducting material made of an oxide such as a superconductor is formed. In addition, the thermal spraying apparatus 1 may be a gas thermal spraying method other than plasma thermal spraying. The plasma spraying apparatus 1 includes a vacuum vessel 4, a thermal spray nozzle 5 provided in the vacuum vessel 4, a tungsten electrode 6 provided in the thermal spray nozzle 5, and connected between the thermal spray nozzle 5 and the electrode 6. It consists of a plasma power supply 7. A plate-shaped or rod-shaped base material 2 is installed in a vacuum vessel 4 facing a thermal spray nozzle 5, and while the pressure inside the vacuum vessel 4 is reduced, a plasma gas such as argon or helium and Y-Ba are injected into the thermal spray nozzle 5. - Powder of superconducting material made of oxides such as Cu-O (from 10 to
100 μm), and then the plasma power source 7 is activated to generate a plasma arc between the thermal spray nozzle 5 and the electrode 6. Once the superconducting material 8 consisting of the base material 2 and the coating 3 is obtained by the above-described thermal spraying apparatus, the superconducting material 8 is then heated in a heating furnace 10 having a heater 9, as shown in FIG. While heating to a temperature of 500 to 980°C, pressure is applied to the film 3 using a press 11. This increases the degree of adhesion between the particles of the superconducting material sprayed onto the surface of the base material 2.
The porosity of the coating 3 is reduced. Furthermore, the degree of adhesion between the base material 2 and the film 3 also increases. After so-called hot pressing is applied to the superconducting material 8 in this manner, the superconducting material 8 is cooled at a rate of 20° C./min or less in the air or an oxygen atmosphere. As a result, the crystal structure of the film 3 made of the superconducting material becomes orthorhombic. As a result, a superelectric coating 3 is obtained. Here, the heat treatment temperature was set at 500 to 980℃ because
At temperatures below 500℃, it is difficult to obtain homogeneous orthorhombic crystals, and the amount of oxygen vacancies is large, making it difficult to obtain sufficient superconducting properties.
This is because if the temperature exceeds 980°C, the base material and the film will react, the base material will penetrate into the film, and the superconducting property will no longer be exhibited. In addition, the cooling rate was set to 20℃/min or less because
This is because, at a cooling rate exceeding 20°C/min, the risk of cracking in the film increases, the film and the base material are likely to peel off, and the amount of oxygen vacancies in the crystal increases. Next, embodiments of the invention will be described. Vacuum vessel 4 of plasma spraying apparatus 1 shown in FIG.
A copper plate-shaped substrate 2 is set inside the spray nozzle 5, and a mixed gas of argon gas and helium gas (Ar: 20/min, He: 40/min) is continuously supplied as plasma gas into the thermal spray nozzle 5. and plasma power supply 7
A power of 15 Kw is supplied between the thermal spray nozzle 5 and the electrode 6 from Then, the atmospheric pressure inside the vacuum container 4 is
The pressure was reduced to 80 mbar, and a film 3 made of a superconducting material having a film thickness of 150 μm was formed on the surface of the base material 2. Next, the base material 2 and the film 3 obtained in this way
The superconducting material 8 consisting of was taken out from the vacuum container 4, placed in the heating furnace 10, and heated in the atmosphere at a temperature of 500° C. for 30 minutes while being reduced by the press 11 at 5 kgf/mm 2 . Next, the superconducting material 8 heated while applying pressure in this manner is heated at 10°C/min.
A plate-shaped superconducting material was produced by cooling at a rate of . Next, another plate-shaped superconducting material was manufactured under the same conditions as in the above-mentioned example except that the heating temperature of the superconducting material 8 was changed to 800°C. A portion of each of the superconducting materials thus produced was vertically cut, the cut surfaces were polished, and the cut surfaces were observed with an optical microscope to examine the porosity. The results are shown in Table 1 together with the case where the superconducting material 8 was not subjected to hot press treatment, that is, the case where it was left as thermally sprayed.

【表】 第1表から明らかなように、本発明法によれ
ば、超電導素材にホツトプレス処理を施すことに
よつて、皮膜の空孔率が溶射ままの場合に比べて
小さくなることがわかつた。 次に、各超電導材から試験片(基材厚:2mm、
皮膜厚:0.15mm、幅:5mm、長さ:50mm)を切り
出し、これを液体窒素(77K)中に浸漬し、四端
子法によつて、臨界電流密度(Jc)について調べ
た。この結果を溶射ままの場合と合わせて第2表
に示す。
[Table] As is clear from Table 1, according to the method of the present invention, by hot-pressing the superconducting material, the porosity of the film was found to be smaller than when it was sprayed as is. . Next, a test piece (base material thickness: 2 mm,
A piece (film thickness: 0.15 mm, width: 5 mm, length: 50 mm) was cut out, immersed in liquid nitrogen (77K), and examined for critical current density (Jc) using the four-terminal method. The results are shown in Table 2 together with the as-sprayed case.

【表】 第1表から明らかなように、本発明法によれ
ば、ホツトプレス処理によつて、皮膜の空孔率が
減少し且つ超電導物質の粒子同士の密着度が高く
なるので(Js)の値が、溶射ままの場合に比べて
大きくなることがわかつた。 次に、上記試験片と同一寸法の試験片を
ASTMC633−79に従つて、基材2と皮膜3との
密着強度試験に供した。この結果を溶射ままの場
合と合わせて第3表に示す。
[Table] As is clear from Table 1, according to the method of the present invention, the porosity of the film is reduced and the adhesion between the particles of the superconducting material is increased by the hot press treatment, so that (Js) It was found that the value was larger than that of the as-sprayed case. Next, take a test piece with the same dimensions as the above test piece.
An adhesion strength test between the base material 2 and the film 3 was conducted in accordance with ASTMC633-79. The results are shown in Table 3 together with the as-sprayed case.

【表】 第3表から明らかなように、本発明法によれ
ば、ホツトプレス処理によつて皮膜と基材との密
着強度が、溶射ままの場合に比べて高いことがわ
かる。 次に、上記試験片と同一寸法の試験片を三点曲
げ試験に供して、皮膜の割れ発生時の試験片の曲
げ角度を測定し、これによつて、皮膜の強度につ
いて調べた。この結果を溶射ままの場合と合わせ
て第4表に示す。
[Table] As is clear from Table 3, according to the method of the present invention, the adhesion strength between the coating and the base material is higher due to the hot press treatment than when the coating is as-sprayed. Next, a test piece having the same dimensions as the above test piece was subjected to a three-point bending test, and the bending angle of the test piece at the time of cracking of the film was measured, thereby examining the strength of the film. The results are shown in Table 4 together with the as-sprayed case.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、この発明によれば、皮膜
を溶射法によつて形成することによつて、皮膜の
膜厚を厚くすることができ、しかも、皮膜を短時
間で形成することができる。さらに、皮膜をホツ
トプレス処理することによつて、超電導物質の粒
子同士が互いに強固に接着するので、皮膜の空孔
率が減少して(Jc)の値が大きくなると共に、皮
膜の強度および基材と皮膜との密着強度が高くな
るといつたきわめて有用な効果をもたらされる。
As explained above, according to the present invention, by forming the coating by thermal spraying, the thickness of the coating can be increased, and moreover, the coating can be formed in a short time. Furthermore, by hot-pressing the film, the particles of the superconducting material firmly adhere to each other, which reduces the porosity of the film and increases the value of (Jc). When the adhesion strength between the film and the film increases, extremely useful effects are brought about.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、この発明の方法によつて、基材の表
面上に超電導物質からなる皮膜を形成している状
態様を示す断面図、第2図は、この発明の方法に
よつて、超電導素材にホツトプレス処理を施して
いる状態を示す断面図、第3図は、三点曲げ試験
法を示す正面図である。 図面において、1……プラズマアーク溶射装
置、2……基材、3……皮膜、4……真空容器、
5……溶射ノズル、6……電極、7……プラズマ
電源、8……超電導素材、9……ヒーター、10
……加熱炉、11……プレス。
FIG. 1 is a sectional view showing how a film made of a superconducting substance is formed on the surface of a substrate by the method of the present invention, and FIG. FIG. 3 is a cross-sectional view showing a state in which the material is hot-pressed, and FIG. 3 is a front view showing a three-point bending test method. In the drawings, 1... plasma arc thermal spraying device, 2... base material, 3... film, 4... vacuum vessel,
5... Thermal spray nozzle, 6... Electrode, 7... Plasma power source, 8... Superconducting material, 9... Heater, 10
...Heating furnace, 11...Press.

Claims (1)

【特許請求の範囲】[Claims] 1 基材の表面上に、溶射法によつてCuxOy基を
含む複合酸化物超電導物質の皮膜を形成させ、次
いで、このようにして得られた、前記基材と前記
皮膜とからなる超電導素材を500から980℃の温度
に加熱しながら、前記超電導素材に圧下を加え、
これによつて、前記皮膜の緻密性を向上させ、次
いで、前記超電導素材を酸素含有雰囲気中におい
て、20℃/min以下の冷却速度で冷却し、これに
よつて前記皮膜に所定の超電導性を付与すること
を特徴とする、超電導材の製造方法。
1. A film of a composite oxide superconducting material containing a Cu x O y group is formed on the surface of a base material by a thermal spraying method, and then a film consisting of the base material and the film obtained in this way is formed. While heating the superconducting material to a temperature of 500 to 980°C, applying pressure to the superconducting material,
This improves the density of the film, and then cools the superconducting material in an oxygen-containing atmosphere at a cooling rate of 20°C/min or less, thereby giving the film a predetermined superconductivity. A method for producing a superconducting material, the method comprising:
JP62200928A 1987-08-13 1987-08-13 Manufacture of superconductive material Granted JPS6445015A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62200928A JPS6445015A (en) 1987-08-13 1987-08-13 Manufacture of superconductive material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62200928A JPS6445015A (en) 1987-08-13 1987-08-13 Manufacture of superconductive material

Publications (2)

Publication Number Publication Date
JPS6445015A JPS6445015A (en) 1989-02-17
JPH0531492B2 true JPH0531492B2 (en) 1993-05-12

Family

ID=16432615

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62200928A Granted JPS6445015A (en) 1987-08-13 1987-08-13 Manufacture of superconductive material

Country Status (1)

Country Link
JP (1) JPS6445015A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH035306A (en) * 1989-05-30 1991-01-11 Nec Corp Production and heat treatment of superconducting thin film

Also Published As

Publication number Publication date
JPS6445015A (en) 1989-02-17

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