JPH01166415A - Manufacture of superconductive film - Google Patents
Manufacture of superconductive filmInfo
- Publication number
- JPH01166415A JPH01166415A JP62323773A JP32377387A JPH01166415A JP H01166415 A JPH01166415 A JP H01166415A JP 62323773 A JP62323773 A JP 62323773A JP 32377387 A JP32377387 A JP 32377387A JP H01166415 A JPH01166415 A JP H01166415A
- Authority
- JP
- Japan
- Prior art keywords
- film
- ion beam
- high voltage
- target substrate
- voltage pulse
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 238000004519 manufacturing process Methods 0.000 title claims description 8
- 239000000758 substrate Substances 0.000 claims abstract description 34
- 238000010884 ion-beam technique Methods 0.000 claims abstract description 33
- 239000000463 material Substances 0.000 claims abstract description 14
- 238000004544 sputter deposition Methods 0.000 claims description 12
- 239000012528 membrane Substances 0.000 abstract 2
- 238000000034 method Methods 0.000 description 9
- 239000013078 crystal Substances 0.000 description 7
- 150000002500 ions Chemical class 0.000 description 7
- 238000007493 shaping process Methods 0.000 description 3
- 238000005245 sintering Methods 0.000 description 2
- MMOXZBCLCQITDF-UHFFFAOYSA-N N,N-diethyl-m-toluamide Chemical compound CCN(CC)C(=O)C1=CC=CC(C)=C1 MMOXZBCLCQITDF-UHFFFAOYSA-N 0.000 description 1
- 238000000975 co-precipitation Methods 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005307 ferromagnetism Effects 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 238000007750 plasma spraying Methods 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 239000002887 superconductor Substances 0.000 description 1
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
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は超電導膜の製造方法に係り、特に高圧パルスイ
オンビームを利用した超電導膜の製造方法に関するもの
である。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a method for manufacturing a superconducting film, and particularly to a method for manufacturing a superconducting film using a high-pressure pulsed ion beam.
[従来の技術]
近年超電導材料が注目されており、大きく分けて強磁性
の発生、大電流の輸送及び素子の三分野に利用されてい
る。そして、この超電導材料を膜として例えばCu’l
oO,5rTi03等の成膜基板表面に形成する超電導
膜の製造方法が開発されている。[Prior Art] Superconducting materials have attracted attention in recent years, and are used in three main fields: generation of ferromagnetism, transport of large currents, and devices. Then, this superconducting material is used as a film, for example, Cu'l
A method for manufacturing a superconducting film formed on the surface of a film-forming substrate such as oO, 5rTi03, etc. has been developed.
従来、超電導膜の製造方法には、(1) 成膜基板表
面に超電導材料の粉体を混合焼結、または共沈後焼結す
る方法、C) 数10にVの比較的低電圧の連続イオン
ビームを超電導材料からなるターゲット基板に照射して
スパッタガスを発生させて成膜基板表面に形成する方法
、(3)fl電導材料な成膜基板表面にプラズマ溶射す
る方法等があった。Conventionally, methods for producing superconducting films include (1) mixing and sintering superconducting material powder on the surface of a film-forming substrate, or sintering after coprecipitation, and C) continuously applying a relatively low voltage of several tens of volts. There have been methods such as irradiating an ion beam onto a target substrate made of a superconducting material to generate sputtering gas to form a film on the surface of the substrate, and (3) plasma spraying on the surface of a film forming substrate made of a fl conductive material.
[発明が解決しようとする問題点]
ところで、従来の超電導膜の製造方法にあっては、何れ
も単結晶若しくは単結晶に近い強記向性の超電導体を得
るには至っておらず、膜厚も薄いという問題があった。[Problems to be Solved by the Invention] By the way, none of the conventional methods for producing superconducting films have been able to obtain a superconductor having a single crystal or a strong writing tendency close to a single crystal, and the film thickness There was also the problem that it was thin.
そのため、超を導膜の飽和電流密度(Jc)^/32が
小さく、総電流量も大きくとれないという問題があった
。Therefore, there was a problem that the saturation current density (Jc)^/32 of the superconducting film was small and the total amount of current could not be large.
上述の如き問題点に鑑みて本発明は、飽和電流密度(J
c)を増大させるべく単結晶構造もしくは、これに近い
強記向性を有すると共に、膜厚の厚い超電導膜の製造方
法を提供することを目的とするものである。In view of the above-mentioned problems, the present invention provides a saturation current density (J
c) It is an object of the present invention to provide a method for manufacturing a superconducting film having a single crystal structure or a strong write orientation close to this structure and having a thick film thickness in order to increase the value of c).
[問題点を解決するための手段]
従来技術における問題点を解決すべく本発明は、波形整
形した高電圧パルスをイオンビーム発生装置に印加し、
この発生装置から高圧のパルスイオンビームを瞬間的に
発生させ真空雰囲気中で超電導材料からなるターゲット
基板に照射してスパッタガスを発生させて成膜基板表面
に超電導膜を形成するようにしたものである。[Means for Solving the Problems] In order to solve the problems in the prior art, the present invention applies a waveform-shaped high voltage pulse to an ion beam generator,
This generator instantaneously generates a high-pressure pulsed ion beam and irradiates it onto a target substrate made of superconducting material in a vacuum atmosphere to generate sputtering gas and form a superconducting film on the surface of the film-forming substrate. be.
[作 用]
上述の如く構成され、上記イオンビーム発生装置に波形
整形した高電圧パルスを印加することにより、この発生
装置から高圧のパルスイオンビームが瞬間的に発生する
。この高圧パルスイオンビームを真空雰囲気中で超電導
材料からなるターゲット基板に照射する。パルスイオン
ビームはターゲット基板の表面を瞬間的に非熱平衡的に
プラズマ化し、活性度の高いスパッタガスを発生させる
。[Function] By applying a waveform-shaped high voltage pulse to the ion beam generator configured as described above, a high voltage pulsed ion beam is instantaneously generated from the generator. A target substrate made of a superconducting material is irradiated with this high-pressure pulsed ion beam in a vacuum atmosphere. The pulsed ion beam instantaneously turns the surface of the target substrate into plasma in a non-thermal equilibrium manner, generating highly active sputtering gas.
ここのスパッタガスはパルス的に成膜基板表面に打ち込
まれ、極めて配向性の強い超電導膜が生成されるもので
ある。The sputtering gas here is pulsed onto the surface of the film-forming substrate, producing a superconducting film with extremely strong orientation.
[実施例]
以下に本発明の超電導膜の製造方法を添付図面に基づい
て詳述する。[Example] The method for manufacturing a superconducting film of the present invention will be described in detail below with reference to the accompanying drawings.
まず、本発明方法を実施するために採用する装置の例に
ついて述べる。第1図に示す如く、密閉容器1内に臨ん
でイオンビーム発生装置2が取り付けられている。これ
ら密閉容器1とイオンビーム発生装置2とは排気系(図
示せず)に接続され、夫々の内部は真空雰囲気に維持さ
れるようになっている。上記イオンビーム発生器r!1
2は例えば高電圧により固体表面をフラッシュオーバさ
せ、プラズマを供給し、瞬時に大量のイオンを発生させ
るイオン源及び静電加速装置からなっている。First, an example of an apparatus employed to carry out the method of the present invention will be described. As shown in FIG. 1, an ion beam generator 2 is installed facing inside a closed container 1. These closed container 1 and ion beam generator 2 are connected to an exhaust system (not shown), and the insides of each are maintained in a vacuum atmosphere. The above ion beam generator r! 1
2 consists of an ion source and an electrostatic accelerator that flashover the solid surface using high voltage, supply plasma, and instantaneously generate a large amount of ions.
このイオンビーム発生装置2にはイオン源用高圧パルス
電源3が接続されている。このイオン源用高圧パルス電
源3は例えば高電圧パルスを発生するマルクス高電圧発
生器と、この高電圧パルスの波形整形を行うブルームラ
イン波形整形回路とからなっている。上記密閉容器1内
にはイオンビーム発生装置2の照射口に臨んで傾斜して
超電導材料からなるターゲット基板4が設けられている
。A high-voltage pulse power source 3 for an ion source is connected to this ion beam generator 2 . The high-voltage pulse power supply 3 for the ion source includes, for example, a Marx high-voltage generator that generates high-voltage pulses, and a Blumlein waveform shaping circuit that shapes the waveform of this high-voltage pulse. A target substrate 4 made of a superconducting material is provided in the sealed container 1 and inclined so as to face the irradiation port of the ion beam generator 2 .
超電導材料には例えばY−Ba−Cu、 Y−Ba−C
u−0,La−Ba−Cu、 La−Ba−Cu−0,
Eu−Ba−Cu或いはEu−Ba−Cu−0等の平板
状の材料を採用する。このターゲット基板4の上方には
、これから発生するスパッタガス5に臨んで成膜基板6
が設けられている。成膜基板6には例えばCuやHgO
,SrT io+等の平板状の材料を採用する。Superconducting materials include, for example, Y-Ba-Cu, Y-Ba-C
u-0, La-Ba-Cu, La-Ba-Cu-0,
A flat material such as Eu-Ba-Cu or Eu-Ba-Cu-0 is used. Above this target substrate 4 is a film forming substrate 6 facing the sputtering gas 5 that will be generated.
is provided. The film-forming substrate 6 is made of, for example, Cu or HgO.
, SrT io+ or the like is used.
次に上述の如き装置を用いて本発明方法を説明する。Next, the method of the present invention will be explained using the apparatus as described above.
まず、密閉容器1及びイオンビーム発生装置2内を排気
系により排気して真空雰囲気にした後、イオン源用高圧
パルス電源3のマルクス高圧発生器により高電圧パルス
を発生させる0次に、この高圧電圧パルスの波形を上記
イオン源用高圧パルス電源3のブルームライン波形整形
回路で整形する。そして、この波形整形した高電圧パル
スをイオンビーム発生装置2に印加する。すると、イオ
ンビーム発生装置2は高圧のパルスイオンビーム7を瞬
間的に発生し、上記超電導材料からなるターゲット基板
4に向けて照射する。この高圧のパルスイオンビーム7
はターゲット基板4の表面を瞬間的に非熱平衡的にプラ
ズマ化し、活性度の高いスパッタガス5を発生させる。First, the inside of the closed container 1 and the ion beam generator 2 are evacuated by the exhaust system to create a vacuum atmosphere, and then a high voltage pulse is generated by the Marx high voltage generator of the high voltage pulse power supply 3 for the ion source. The waveform of the voltage pulse is shaped by the Blumlein waveform shaping circuit of the high-voltage pulse power supply 3 for the ion source. Then, this waveform-shaped high voltage pulse is applied to the ion beam generator 2. Then, the ion beam generator 2 instantaneously generates a high-pressure pulsed ion beam 7 and irradiates it toward the target substrate 4 made of the superconducting material. This high-pressure pulsed ion beam 7
The surface of the target substrate 4 is instantaneously turned into plasma in a non-thermal equilibrium manner, and a highly active sputtering gas 5 is generated.
このスパッタガス5はパルス的に上記成膜基板6の表面
に打ち込まれる。これにより、成膜基板6の表面に単結
晶構造に近く、極めて配向性の高い超電導膜を形成する
ものである。This sputtering gas 5 is pulsed onto the surface of the film forming substrate 6. This forms a superconducting film on the surface of the film-forming substrate 6 that has a nearly single-crystal structure and has extremely high orientation.
これは消!!電力を同一とした場合、連続イオンビーム
をターゲット基板4に連続照射すると低電圧にしなけれ
ばならないが、瞬間的に照射すれば高電圧にすることが
可能となる。そして、この高電圧パルスの波形を整形す
ることにより急峻な短パルスにして、これをイオンビー
ム発生装置2に印加するとイオンビームは高圧のパルス
イオンビーム7としてターゲット基板4に照射されるか
らである。This is off! ! When the power is the same, if the target substrate 4 is continuously irradiated with a continuous ion beam, a low voltage must be applied, but if the ion beam is irradiated instantaneously, a high voltage can be applied. Then, by shaping the waveform of this high-voltage pulse, it becomes a steep short pulse, and when this is applied to the ion beam generator 2, the ion beam is irradiated onto the target substrate 4 as a high-voltage pulsed ion beam 7. .
従って、ターゲット基板4から発生するスパッタガス5
も瞬間的に成膜基板6に打ち込まれ、超電導膜の形成は
高速で断続的なものとなり、その結晶は単結晶構造に近
くなり、強い配向性を有するようになるものである。こ
れにより超電導膜の飽和を流密度(Jc)を著しく大き
くすることができる。Therefore, the sputtering gas 5 generated from the target substrate 4
The superconducting film is instantaneously implanted into the film-forming substrate 6, and the superconducting film is formed intermittently at high speed, and its crystal becomes close to a single crystal structure and has strong orientation. This makes it possible to significantly increase the flow density (Jc) for saturation of the superconducting film.
[発明の効果]
以上要するに本発明によれば超電導材料からなるターゲ
ット基板に高圧のパルスイオンビームを瞬間的に照射し
てスパッタガスを発生させて成膜基板表面に超電導膜を
形成するようにしたので、スパッタガスはパルス的に成
膜基板表面に打ち込まれ、単結晶構造に近く極めて配向
性の強く、且つ膜厚の厚い超電導膜を製造することがで
きる。これにより、超電導膜に大きな飽和電流密度(J
c)を持たせることができる。[Effects of the Invention] In summary, according to the present invention, a target substrate made of a superconducting material is instantaneously irradiated with a high-pressure pulsed ion beam to generate sputtering gas, thereby forming a superconducting film on the surface of the film-forming substrate. Therefore, the sputtering gas is pulsed onto the surface of the film-forming substrate, making it possible to produce a superconducting film that is close to a single crystal structure, has extremely strong orientation, and is thick. This results in a large saturation current density (J
c).
第1図は本発明の超電導膜の製造方法を説明するための
概略図である。
図中、1は密閉容器、2はイオンビーム発生装置、3は
イオン源用高圧パルス電源、4はターゲット基板、5は
スパッタガス、6は成膜基板、7は高圧のパルスイオン
ビームである。FIG. 1 is a schematic diagram for explaining the method of manufacturing a superconducting film of the present invention. In the figure, 1 is a sealed container, 2 is an ion beam generator, 3 is a high-voltage pulsed power source for an ion source, 4 is a target substrate, 5 is a sputtering gas, 6 is a film forming substrate, and 7 is a high-pressure pulsed ion beam.
Claims (1)
印加し、該発生装置から高圧のパルスイオンビームを瞬
間的に発生させ真空雰囲気中で超電導材料からなるター
ゲット基板に照射してスパッタガスを発生させて成膜基
板表面に超電導膜を形成するようにしたことを特徴とす
る超電導膜の製造方法。A waveform-shaped high voltage pulse is applied to an ion beam generator, and a high-pressure pulsed ion beam is instantaneously generated from the generator and irradiated onto a target substrate made of a superconducting material in a vacuum atmosphere to generate sputtering gas. A method for producing a superconducting film, characterized in that the superconducting film is formed on the surface of a film-forming substrate.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62323773A JPH01166415A (en) | 1987-12-23 | 1987-12-23 | Manufacture of superconductive film |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62323773A JPH01166415A (en) | 1987-12-23 | 1987-12-23 | Manufacture of superconductive film |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01166415A true JPH01166415A (en) | 1989-06-30 |
Family
ID=18158460
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62323773A Pending JPH01166415A (en) | 1987-12-23 | 1987-12-23 | Manufacture of superconductive film |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01166415A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5709249A (en) * | 1994-06-27 | 1998-01-20 | Yazaki Corporation | Locking structure |
-
1987
- 1987-12-23 JP JP62323773A patent/JPH01166415A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5709249A (en) * | 1994-06-27 | 1998-01-20 | Yazaki Corporation | Locking structure |
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