JPH0362978A - Method of producing oxide superconductor circuit - Google Patents
Method of producing oxide superconductor circuitInfo
- Publication number
- JPH0362978A JPH0362978A JP1198399A JP19839989A JPH0362978A JP H0362978 A JPH0362978 A JP H0362978A JP 1198399 A JP1198399 A JP 1198399A JP 19839989 A JP19839989 A JP 19839989A JP H0362978 A JPH0362978 A JP H0362978A
- Authority
- JP
- Japan
- Prior art keywords
- phase
- superconducting
- laser
- oxide superconductor
- oxide
- 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.)
- Granted
Links
- 239000002887 superconductor Substances 0.000 title claims abstract description 12
- 238000000034 method Methods 0.000 title description 16
- 230000001678 irradiating effect Effects 0.000 claims abstract description 3
- 238000004519 manufacturing process Methods 0.000 claims description 6
- 230000002542 deteriorative effect Effects 0.000 abstract description 4
- 238000005979 thermal decomposition reaction Methods 0.000 abstract description 2
- 230000004927 fusion Effects 0.000 abstract 1
- 238000009792 diffusion process Methods 0.000 description 5
- 239000000463 material Substances 0.000 description 4
- 238000005530 etching Methods 0.000 description 3
- 239000000155 melt Substances 0.000 description 3
- 239000000843 powder Substances 0.000 description 3
- 239000002253 acid Substances 0.000 description 2
- 239000012670 alkaline solution Substances 0.000 description 2
- 239000004020 conductor Substances 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 230000000149 penetrating effect Effects 0.000 description 2
- 208000031872 Body Remains Diseases 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 229910000416 bismuth oxide Inorganic materials 0.000 description 1
- 239000007767 bonding agent Substances 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000006378 damage Effects 0.000 description 1
- 238000000354 decomposition reaction Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- TYIXMATWDRGMPF-UHFFFAOYSA-N dibismuth;oxygen(2-) Chemical compound [O-2].[O-2].[O-2].[Bi+3].[Bi+3] TYIXMATWDRGMPF-UHFFFAOYSA-N 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000010587 phase diagram Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 239000000243 solution Substances 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- 238000001039 wet etching Methods 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
Landscapes
- Manufacturing Of Electrical Connectors (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
(イ)技術分野
本発明は、レーザー照射により酸化物、Ifl電導電導
体型体路を作製する方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION (a) Technical Field The present invention relates to a method for producing oxide, Ifl electrically conductive conductive tracks by laser irradiation.
(ロ)従来技術
従来、いったん酸化物超電導成型体を作製し、その一部
を非超電導相にする方法としては各種あり、その代表的
なものに次の方法があるが、それぞれ多くの欠点があっ
た。即ち、
(a)酸化物超電導成型体の所定個所に所定形状の非a
電導相を作製するために、該超電導成型体を加工してそ
の接合に非超電導物質を接合剤として使用し、その接合
部分が非15電導相となるようにする方法。(B) Prior Art Conventionally, there are various methods for once producing an oxide superconducting molded body and converting a part of it into a non-superconducting phase. there were. That is, (a) a predetermined shape of a non-a
A method of processing the superconducting molded body and using a non-superconducting substance as a bonding agent to bond the bonded parts to form a non-conducting phase in order to produce a conductive phase.
例えば、各リングの一部に切込を形成し、該リングには
円電流が流れないように作製した超電導体のスリット入
りのリング数個を重ね合わせて全体としてコイル状とし
、超電導電流を流すために接合材としてa″Yf、4粉
を用いて接合形成せしめて超電導電流が流れるようにし
、−・方各リング相互間のその他の接触部分は非超電導
物質で接合して非、tfl電導相を形成せしめることに
よってa電場71!流が流れないようにする。かくして
、超電導′¥L流がコイルの一端から他端に向って流れ
る。For example, a notch is formed in a part of each ring, and several superconductor rings with slits made so that no circular current flows through the rings are stacked together to form a coil shape, and a superconducting current is passed through the ring. For this purpose, a''Yf, 4 powder is used as a bonding material to form a bond so that a superconducting current flows, and the other contact parts between each ring are bonded with a non-superconducting material to form a non-, TFL conducting phase. The a electric field 71! current is prevented from flowing by forming a superconducting current 71!.Thus, the superconducting '\L current flows from one end of the coil to the other end.
この(a)法の場合は、超電導成型体どうしの接合部分
に非超電導相を形成せしめる方法であるが、該方法は一
体成型ができないので手数がかかり、高情度の回路の作
製は極めて難しい。In the case of method (a), a non-superconducting phase is formed at the joint between superconducting molded bodies, but this method is time-consuming because it cannot be integrally molded, and it is extremely difficult to create a high-performance circuit. .
(b)酸化物超電導I&型体の所望部分に所定形状の非
超電導相を形成せしめる場合、非15電導相としたい部
分にFeやCoの薄膜を形成させ、熱拡散により該部分
の超電導相を破壊して非、tfl電導相を形成させる方
法。(b) When forming a non-superconducting phase of a predetermined shape in a desired part of an oxide superconducting I&type body, a thin film of Fe or Co is formed in the part where the non-15 conducting phase is desired, and the superconducting phase in the part is formed by thermal diffusion. Method of destruction to form a non-tfl conductive phase.
この(b)法は、FeやCoの拡散によって非超電導相
を形成させる訳であるが、その作製過程においてその拡
散状態を断面観察する必要があるので、完全な非超電導
相を形成するには長時間を必要とし、しかも高精度の作
製が難しい。In this method (b), a non-superconducting phase is formed by diffusion of Fe or Co, but since it is necessary to observe the diffusion state in a cross section during the fabrication process, it is difficult to form a complete non-superconducting phase. It requires a long time and is difficult to manufacture with high precision.
(c)酸化物の超電導成型体に非超電導相を形成させる
に際して、該成型体の表面にレジストを塗布した後、所
定部分のみのレジストを剥離して酸又はアルカリ液でエ
ツチングして溶解させることによりa ’、y導電流を
遮断する方法。(c) When forming a non-superconducting phase in a superconducting oxide molded body, after applying a resist to the surface of the molded body, peeling off the resist only in a predetermined portion and etching it with an acid or alkaline solution to dissolve it. A method of interrupting the conductive current by a' and y.
この(c)法は、上記の通り酸又はアルカリ液でエツチ
ングするので、該溶液が成型体内に浸透して超電導特性
を劣化させる等の欠点がある。As described above, this method (c) involves etching with an acid or alkaline solution, and therefore has drawbacks such as the solution penetrating into the molded body and deteriorating the superconducting properties.
(ハ)発明の開示
本発明は、上記のような従来の諸欠点を解消するために
開発された全く新規な酸化物a電導体の回路作製法であ
って、酸化物超電導成型体にレーザーを照射することに
より被照射部分を分解又は溶融させ超電導相を破壊して
非a電導相に変質させ、レーザーが照射されない部分を
もって回路を形成するものである。(C) Disclosure of the Invention The present invention is a completely new method for manufacturing a circuit using an oxide a conductor, which was developed in order to eliminate the conventional drawbacks as described above. By irradiating the irradiated portion, the irradiated portion is decomposed or melted, the superconducting phase is destroyed, and the superconducting phase is transformed into a non-a conductive phase, and a circuit is formed with the portion that is not irradiated with the laser.
即ち、本発明法では酸化物a電導成型体の所定部分に所
定形状の非8電導相を形成させる場合、該部分にCO2
ガスレーザーやYAGレーザー等を使用し、レーザー光
のビームスポット径とバク−を調侑して照射することに
より、該部分を加熱分解又は溶融させて所望形状の非m
’rrt、導相を形成させて、超電導電流を遮断するの
である。That is, in the method of the present invention, when a non-8 conductive phase of a predetermined shape is formed in a predetermined portion of an oxide a conductive molded body, CO2 is added to that portion.
By using a gas laser, YAG laser, etc., and adjusting the beam spot diameter and backlight of the laser beam, the part is thermally decomposed or melted to form a non-molecular shape in the desired shape.
'rrt, a conductive phase is formed and the superconducting current is interrupted.
木5i!!明は酸化物超電導体にレーデ−を照射して非
iB電導相を形成させるに際して、成型体を完全に切断
するのではなく、部分的に変質させるのみであるので、
該部分の接合力は全く失われないのである。Tree 5i! ! When light irradiates an oxide superconductor with radar to form a non-iB conductive phase, it does not completely cut the molded body, but only partially alters its quality.
The bonding strength of this part is not lost at all.
第3図にレーザー照射により、tll’i’lt導相が
変質する状況例を示したが、図中見はレーザービームを
受けて溶融変質した溶融部であり、Sはレーザービーム
を受けて加熱分解し変質した部分を示す固体部であって
、レーザー光を完全に貫通させないで所定部分のみの超
電導相を破壊して非超電導相を形成させるのである。Figure 3 shows an example of a situation in which the tll'i'lt conductive phase changes in quality due to laser irradiation. The middle part of the figure is the molten part that has been melted and altered by the laser beam, and S is the molten part that has been heated by the laser beam. It is a solid part that shows decomposed and altered parts, and the superconducting phase in only a predetermined part is destroyed and a non-superconducting phase is formed without the laser beam completely penetrating it.
このように、 Mi71導成型体を切断することなくそ
の部分をf質させるのみであるから、酸化物超電導戊型
体口体の保有する強度等は全く変らないのである。また
、レーザー光波照射部以外の超電導相の特性を劣化させ
る心配も全くないのである。In this way, the Mi71 conductive molded body is not cut, but only the f-quality is made in that part, so the strength etc. of the oxide superconducting hollow body remains unchanged. Furthermore, there is no fear that the characteristics of the superconducting phase other than the laser beam irradiation portion will deteriorate.
例えば、YBa、Cu3 o、+ X(7)酸化物超電
導材料で成型した厚さが3IIIIで内径がLoom−
φで長さが100mmの円筒形成型体を所定速度で回転
させながらかつその軸方向に上昇又は下降移動するよう
にセットし、これに固定型CO2ガスレーザ−30wに
よりスポット径3IIIIφで照射すると、上記円筒の
スポット照射部分が溶融又は分解してYB azCu3
0.− x超電導相が変質し、Y、、BalCu、0.
、やBaCuO2あるいはCuO等の非超電導相が形成
されるのである。For example, a material with a thickness of 3III and an inner diameter of Loom-
A cylindrical mold body with a length of 100 mm in φ is rotated at a predetermined speed and set to move upward or downward in the axial direction, and when it is irradiated with a fixed CO2 gas laser 30w with a spot diameter of 3IIIφ, the above-mentioned result is obtained. The spot irradiated part of the cylinder melts or decomposes and YB azCu3
0. - x superconducting phase is altered, Y, , BalCu, 0.
, BaCuO2, CuO, and other non-superconducting phases are formed.
かくして、上記円筒形成型体に所定ピッチの螺線状の非
超電導相が形成されるため、超電導コイルが形成された
ことになる。In this way, a spiral non-superconducting phase with a predetermined pitch is formed in the cylindrical mold body, so that a superconducting coil is formed.
上記の場合は固定型CO2ガスレーザーを使用したので
、被照射r&型体を所定の速度で回転させながら北昇移
動させなければならないが、走査型レーザーを使用すれ
ば成型体を固定しておいてレーザーを走査させてもよい
ことは勿論である。In the above case, a fixed type CO2 gas laser was used, so the irradiated r & mold body had to be moved northward while rotating at a predetermined speed, but if a scanning laser was used, the molded body could be fixed and moved. Of course, it is also possible to use a laser for scanning.
また、被明射酸化物超電導体ごとに溶融又は分解して変
質する温度が異なるので、予め相図を参煕して加ニジス
テムにおけるレーザー光のビームスポット径、パワー、
熱吸収、移動速度、冷却速度等の設計条件を設定すれば
、目的とする非超電導相が形成できる。In addition, since the temperature at which the irradiated oxide superconductor melts or decomposes and changes its quality is different, refer to the phase diagram in advance to determine the beam spot diameter and power of the laser beam in the Canadian system.
By setting design conditions such as heat absorption, movement speed, cooling rate, etc., the desired non-superconducting phase can be formed.
次に、本発明法を実施例により説明する。Next, the method of the present invention will be explained using examples.
(ニ)実施例
実施例I
YBa、、Cu3o7− x酸化物a−ri7導材料で
成型したHさ4 mm 、内径50mmφ、長さ100
1I11の円筒形成型体を周速度2 ays1分で回転
させながらゆっくりと上昇移動するようにセットし、固
定型CO,ガスレーザー30wを用いて2■スポツトに
点点を合わせ、円筒形成型体の外周面にレーチー光を貝
通させないようにしながらピッチ4II11の螺線状非
超電導相を形成すべく照射し、所定部分の超電導相を溶
融・分解して変質させてから急冷した。(D) Examples Example I Molded with YBa, Cu3o7-x oxide a-ri7 conductive material, height 4 mm, inner diameter 50 mmφ, length 100
Set the cylindrical mold body of 1I11 so that it moves slowly upward while rotating at a circumferential speed of 2 ays 1 minute, and use a fixed CO and gas laser 30w to align the dots at 2 ■ spots to measure the outer periphery of the cylindrical mold body. It was irradiated to form a spiral non-superconducting phase with a pitch of 4II11 while preventing the Lechie light from passing through the surface, and the superconducting phase in a predetermined portion was melted and decomposed to change its quality, and then it was rapidly cooled.
その結果、レーザービームを照射した部分には完全に非
超電導相が形成され、目的とするa電導コイルの成型体
を作製することができた。As a result, a non-superconducting phase was completely formed in the portion irradiated with the laser beam, and the desired molded body of the a-conducting coil could be produced.
このコイルで流せる電流f直は400A/cmzであり
、バルクで流せる電流値と同等であった。The current f direct that could be passed through this coil was 400 A/cmz, which was equivalent to the current value that could be passed in bulk.
比較例
り記実施例1で供試したのと同じYB a2Cu30.
−x酸化物a電導材料で成型したHさ4 mm 、内径
50鵬厘φ9幅5讃會のリング状成型体を各リングの一
部を切断して円M、流が流れなくしたものを数個作製し
、1[いにコイル状になるように切込み口をずらせて固
定し、切断部分にはa″Ff、導電流を流すためにL記
すング戊型体と同質の酸化物#flTL導粉のペースト
を塗布し、その他の部分(非mW導相とする部分)には
酸化ビスマス粉のベートストを塗布し、920℃で10
時間加熱処理して拡散接合させコイルを作製した。Comparative Example The same YB a2Cu30. as used in Example 1 was used.
-x Oxide a A ring-shaped molded body with a height of 4 mm, an inner diameter of 50 mm, a width of 5 mm, and a diameter of 5 mm is cut out to form a circle M, and the flow is stopped. A piece of oxide was prepared, and fixed by shifting the incision so that it would form a coil shape. Powder paste was applied, and the other parts (parts to be non-mW conductive) were coated with Batest, which is made of bismuth oxide powder, and heated at 920°C for 10
A coil was fabricated by heat treatment for a period of time and diffusion bonding.
その結果、拡散接合させたコイルでも一応は電流は流れ
るが、その接合部分で流せる電ti値は10A/ctm
zと極めて小さく、従ってコイルとして流せる電流値も
小さくてこのリングのみで流せる電流値も20A/am
”と著しく低下した。As a result, current flows through the diffusion bonded coil, but the current ti value that can flow through the bond is 10A/ctm.
z is extremely small, so the current that can be passed as a coil is also small, and the current that can be passed only with this ring is 20A/am.
” has decreased significantly.
(ホ)発明の結果
)述したように、本発明法によればレーザーのビームス
ポット径を調節し、酸化物超電導体の所定部分に照射し
、溶融又は分解によりMi電導相を変質させる温度まで
加熱することにより照射部分の超電導相を破壊して半導
体もしくは絶縁体等の非超電導相に変質させ、任意な回
路を特性を低下させることなく容易に作製することがで
きるのである。(E) Results of the invention) As described above, according to the method of the present invention, the beam spot diameter of the laser is adjusted and irradiated onto a predetermined portion of the oxide superconductor until the temperature reaches a temperature that changes the Mi conductive phase by melting or decomposition. By heating, the superconducting phase in the irradiated area is destroyed and transformed into a non-superconducting phase such as a semiconductor or an insulator, making it possible to easily create any circuit without deteriorating its characteristics.
しかも、本発明は従来法のようなガスエツチングやウェ
ットエツチング等を全く必要とせず、容易かつ短時間で
高精度に処理ができ、更にレーザー照射によって形成さ
れた非超電導相が構造材として作用する利点もある。Moreover, the present invention does not require any gas etching or wet etching as required in conventional methods, and can be processed easily, quickly and with high precision.Furthermore, the non-superconducting phase formed by laser irradiation acts as a structural material. There are also advantages.
なお、上記実施例ではY−Ba−Cu−0系の酸化物超
電導体の回路作製について説明したが、本発明法が他の
酸化物超電導体にも適用できることは勿論である。In addition, although the above-mentioned example explained circuit production of Y-Ba-Cu-0 type oxide superconductor, it goes without saying that the method of the present invention can be applied to other oxide superconductors.
4、図面簡単な説明
第1図は、本発明法により円筒形酸化物超電導成型体か
ら作製したコイル状回路を示す斜視図、第2図は同様に
平板型成型体から作製した回路を示す平面図、第3図は
レーザー照射によりkfi電導相が溶融又は分解して変
質する状況例を示す断面説明図である。4. Brief description of the drawings Fig. 1 is a perspective view showing a coiled circuit produced from a cylindrical oxide superconducting molded body by the method of the present invention, and Fig. 2 is a plan view showing a circuit similarly produced from a flat plate-shaped molded body. 3 are cross-sectional explanatory diagrams showing an example of a situation where the KFI conductive phase melts or decomposes and changes in quality due to laser irradiation.
符号説明
1−円筒形酸化物超電導成型体 2−非超電導相3−超
電導相 4−平板状酸化物超電導成型体5−Go、、ガ
スレーザー 6−レーザービーム文−溶融変質部 S−
加熱分解変質部
特 許 出 願 人 同和鉱業株式会社第1
図
第2
図
ム
第3図Symbol explanation 1-Cylindrical oxide superconducting molded body 2-Non-superconducting phase 3-Superconducting phase 4-Tabular oxide superconducting molded body 5-Go, gas laser 6-Laser beam pattern-Melted altered part S-
Thermal decomposition altered part patent Applicant Dowa Mining Co., Ltd. Figure 1 Figure 2 Figure 3
Claims (1)
部を非超電導相に変質させて回路を形成することを特徴
とする酸化物超電導体の回路作製方法。1. A method for producing a circuit of an oxide superconductor, which comprises forming a circuit by irradiating the oxide superconductor with a laser to transform the irradiated portion into a non-superconducting phase.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1198399A JP2896579B2 (en) | 1989-07-31 | 1989-07-31 | Circuit fabrication method for oxide superconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1198399A JP2896579B2 (en) | 1989-07-31 | 1989-07-31 | Circuit fabrication method for oxide superconductor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0362978A true JPH0362978A (en) | 1991-03-19 |
| JP2896579B2 JP2896579B2 (en) | 1999-05-31 |
Family
ID=16390484
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1198399A Expired - Fee Related JP2896579B2 (en) | 1989-07-31 | 1989-07-31 | Circuit fabrication method for oxide superconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2896579B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH08120798A (en) * | 1994-10-27 | 1996-05-14 | Atsudo:Kk | Environment maintenance equipment for warehouses and factories |
| US6336252B1 (en) | 1998-12-07 | 2002-01-08 | Sugatsune Kogyo Co., Ltd. | Rotary damper |
-
1989
- 1989-07-31 JP JP1198399A patent/JP2896579B2/en not_active Expired - Fee Related
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH08120798A (en) * | 1994-10-27 | 1996-05-14 | Atsudo:Kk | Environment maintenance equipment for warehouses and factories |
| US6336252B1 (en) | 1998-12-07 | 2002-01-08 | Sugatsune Kogyo Co., Ltd. | Rotary damper |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2896579B2 (en) | 1999-05-31 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP2855614B2 (en) | Method of forming superconducting circuit | |
| EP0304807A2 (en) | Method for producing superconducting circuit | |
| JP2896579B2 (en) | Circuit fabrication method for oxide superconductor | |
| WO1989001053A1 (en) | A method for fabricating ceramic superconductors | |
| JPH0355889A (en) | Manufacture of superconducting multilayered circuit | |
| JPH01212407A (en) | Superconducting ceramic circuit device | |
| JP2904998B2 (en) | Solid object made of ceramic high-temperature superconducting material connected to metal conductor and method of manufacturing the same | |
| JP2637080B2 (en) | Method for manufacturing compound superconductor | |
| JP2870967B2 (en) | Heating device used for joining superconducting wires | |
| JP2564600B2 (en) | Processing method of oxide superconductor | |
| JPH02239102A (en) | Production of oxide superconductor | |
| JP2767454B2 (en) | Manufacturing method of oxide superconductor | |
| JPH02257529A (en) | Manufacture of oxide superconductor | |
| JPH02257528A (en) | Manufacture of oxide superconductor | |
| JPH04188682A (en) | Manufacturing method of point contact type Josephson junction element | |
| Chen et al. | CO/sub 2/laser welding of BiSrCaCu/sub 2/O/sub y/superconductors | |
| JP2925571B2 (en) | How to make a superconducting circuit | |
| JPH01243485A (en) | Manufacturing method for superconducting elements | |
| JPH0281405A (en) | Manufacture of coil-like superconductor material and manufacture of superconducting coil using the material | |
| JPH01244676A (en) | Manufacture of superconductive element | |
| JPS63310517A (en) | Manufacture of superconductor wire material | |
| JPH02257526A (en) | Manufacture of oxide superconductor | |
| JPH02258699A (en) | Production of oxide superconductor | |
| JPH02177216A (en) | Manufacturing method of superconducting wire | |
| JPH02187003A (en) | Superconducting coil manufacturing method |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| LAPS | Cancellation because of no payment of annual fees |