JPH0333003A - Superconducting thin film production equipment - Google Patents
Superconducting thin film production equipmentInfo
- Publication number
- JPH0333003A JPH0333003A JP1163950A JP16395089A JPH0333003A JP H0333003 A JPH0333003 A JP H0333003A JP 1163950 A JP1163950 A JP 1163950A JP 16395089 A JP16395089 A JP 16395089A JP H0333003 A JPH0333003 A JP H0333003A
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- electrode
- discharge
- superconducting thin
- compd
- 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
Landscapes
- Oxygen, Ozone, And Oxides In General (AREA)
- Inorganic Compounds Of Heavy Metals (AREA)
- Chemical Vapour Deposition (AREA)
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Abstract
Description
本発明は酸化物超電導体の薄膜作成装置に係り。
とくに、酸化物超電導体のMOCVDによる薄膜作成装
置に関する。The present invention relates to an apparatus for forming a thin film of an oxide superconductor. In particular, it relates to an apparatus for forming thin films of oxide superconductors by MOCVD.
有機金属を原料に用いる化学気相成長法、いわゆるMO
CVDは、装置の大型化が容易であり、複雑形状の基板
、大面積基板への成膜が可能であるという優れた特徴を
有し、酸化物超電導体の薄膜作成方法としても有望な方
法となるものと考えられてている(たとえば、新技術開
発事業団監修「高温超電導データブック」第59頁、丸
首株式%式%))
しかしながら、従来技術では、薄膜作成時の基板温度は
約800℃にすることが必要であり、このため、酸化物
薄膜と基板との相互作用がおこり、超電導薄膜の性能低
下、基板の変性、剥離の発生などの問題が発生している
。Chemical vapor deposition method using organic metals as raw materials, so-called MO
CVD has excellent features such as easy upscaling of equipment and the ability to form films on complex-shaped substrates and large-area substrates, making it a promising method for producing thin films of oxide superconductors. (For example, "High Temperature Superconductivity Data Book" supervised by New Technology Development Corporation, p. 59, round neck stock % formula %)) However, with conventional technology, the substrate temperature during thin film production is approximately 800°C. Therefore, the interaction between the oxide thin film and the substrate occurs, causing problems such as deterioration of the performance of the superconducting thin film, deterioration of the substrate, and occurrence of peeling.
本発明の目的は、酸化物高温超電導体薄膜形成のための
MOCVD装置において、基板近傍に直流放電を発生せ
る機構を設けること、望ましくは排気系側の電極の温度
を200〜400℃に保つ機構を設けること、さらに望
ましくは電極に金属の硼素化物、とくに望ましくはイツ
トリウム、バリウム、ランタン、ストロンチウムの硼素
化物の少なくとも一者を用いることにより達成される。An object of the present invention is to provide a mechanism for generating DC discharge near a substrate in an MOCVD apparatus for forming an oxide high temperature superconductor thin film, and preferably a mechanism for maintaining the temperature of the electrode on the exhaust system side at 200 to 400°C. This can be achieved by providing the electrode, and more preferably by using a metal boride, particularly preferably at least one of yttrium, barium, lanthanum, and strontium boride.
本発明において、直流放電は有機金属化合物と酸素を高
速の電子や紫外線により励起して、有機金属化合物の酸
化反応を促進する作用をもつ。
また、排気側の電極を200〜400℃に保つ機構は、
副生成物や未反応物の電極への付着を防止する作用をも
つ。
また、電極に電極に金属の硼素化物、とくにY。
Ba、Sr、Laの硼素化物を用いることは、放電電圧
の低下、電極の酸化による放電の不安定化の防止という
作用がある。In the present invention, the DC discharge has the effect of exciting the organometallic compound and oxygen with high-speed electrons and ultraviolet rays, thereby promoting the oxidation reaction of the organometallic compound. In addition, the mechanism that maintains the exhaust side electrode at 200 to 400°C is
It has the effect of preventing by-products and unreacted substances from adhering to the electrode. Also, metal borides, especially Y, can be used as electrodes. The use of borides of Ba, Sr, and La has the effect of lowering the discharge voltage and preventing destabilization of the discharge due to oxidation of the electrode.
以下、代表的な酸化物超電導体である、Y B a、C
u307−x
の薄膜を作成する装置を実施例として本発明を説明する
。
用いた薄膜作成装置を第1図に示す。
反応管11は石英製で、電気炉10により加熱される。
電気炉10の外部に原料側電極1と排気系側電極2が封
入されている。電極1.2は両者とも表面をLaB、で
被覆したNi線である。直流放電は原料側電極1を接地
電位とし、排気側電極2に正の直流電位を印加して発生
させ、放電電流の大きさは回路に直列に抵抗4を入れて
制御する。
金属の原料には、Y、Ba、Cuのジピバロイルメタナ
ト錯体、(一般にY (DPM)、、Ba(DPM)2
、Cu(DPM)2と略記される)を用いた。これらの
原料6.7.8はそれぞれ110℃、240℃、120
℃の温度に保たれた容器に入れられており、キャリヤー
ガス(Ar)に輸送されて反応管に導入される。また、
酸化ガスにはボンベ9から供給される酸素を用いた。
この装置を用い、放電電流10mA、基板温度600℃
の条件で酸化マグネシウム基板上に作成した薄膜の抵抗
の温度依存性を第2図に示す。また、比較例として放電
を発生させないで作成した薄膜の抵抗の温度依存性も第
2図に示した。なお、第2図の縦軸は250にでの抵抗
に対する測定温度での抵抗である。
図のように、放電を発生させて作成した薄膜の抵抗は温
度の低下とともに減少し、さらに、超電導転移により零
抵抗となった(曲線21)。抵抗値が零となる臨界温度
は90にであった。一方。
放電を発生させずに作成した薄膜の抵抗は 温度の低下
とともに増加し、4.2Kにおいても超電導転移を示さ
なかった(曲線22)。すなわち、この結果から、直流
放電により低温においても超電導薄膜が作成できること
がわかる。
ところで、上記の実施例では表面をL a B、で被覆
したNi線を電極に用いたが、これらのかわりにNi線
をそのまま用いても同様の効果は得られる。 ただし、
Ni線の場合には放電を発生させるのに必要な電圧は約
100V上昇する。
また、鉄や銅などの金属では電極表面が酸化し。
放電が不安定となる。すなわち、電極としてはLaB&
で被覆したNi線の方が望ましい。
なお、上記LaB、の換わりにYB、、SrB、、Ba
BいCeB、などの硼素化合物を用いても良好な結果が
得られる。さらに、当然ながらこれらの硼素化合物その
ものを用いても同様の効果が得られる。
放電の効果は放電電流の増加とともに大きくなり、一定
の放電電流で効果は飽和し、その後はむしろ悪影響を及
ぼす。そして、飽和する放電電流値は装置の形状に依存
して変化するが、放電により超電導薄膜が作成可能とな
ることは本発明の効果そのものである。
上記の実施例では、Y B a 2 Cu 307−
X薄膜の作成装置について示したが、他の酸化物超電導
体のMOCVDについてもその膜成長機構は同一であり
1本発明により低温で超電導薄膜を作成することが可能
である。Below, representative oxide superconductors, Y B a, C
The present invention will be explained using an apparatus for forming a thin film of u307-x as an example. The thin film forming apparatus used is shown in Figure 1. The reaction tube 11 is made of quartz and is heated by the electric furnace 10. A raw material side electrode 1 and an exhaust system side electrode 2 are enclosed outside the electric furnace 10. Both electrodes 1.2 are Ni wires whose surfaces are coated with LaB. DC discharge is generated by setting the raw material side electrode 1 at ground potential and applying a positive DC potential to the exhaust side electrode 2, and the magnitude of the discharge current is controlled by inserting a resistor 4 in series in the circuit. Metal raw materials include dipivaloyl methanato complexes of Y, Ba, and Cu (generally Y (DPM), Ba (DPM)2
, Cu(DPM)2) was used. These raw materials 6.7.8 are 110℃, 240℃, and 120℃, respectively.
It is placed in a container maintained at a temperature of 0.degree. C., and is transported by a carrier gas (Ar) and introduced into a reaction tube. Also,
Oxygen supplied from a cylinder 9 was used as the oxidizing gas. Using this device, the discharge current was 10 mA, and the substrate temperature was 600°C.
Figure 2 shows the temperature dependence of the resistance of a thin film formed on a magnesium oxide substrate under these conditions. Furthermore, as a comparative example, FIG. 2 also shows the temperature dependence of the resistance of a thin film prepared without generating discharge. Note that the vertical axis in FIG. 2 is the resistance at the measured temperature with respect to the resistance at 250°C. As shown in the figure, the resistance of the thin film created by generating electric discharge decreased as the temperature decreased, and further became zero resistance due to superconducting transition (curve 21). The critical temperature at which the resistance value became zero was 90°C. on the other hand. The resistance of the thin film created without generating an electric discharge increased as the temperature decreased, and did not exhibit superconducting transition even at 4.2 K (curve 22). In other words, this result shows that a superconducting thin film can be created even at low temperatures by direct current discharge. Incidentally, in the above embodiment, Ni wires whose surfaces were coated with L a B were used as electrodes, but the same effect can be obtained by using Ni wires as they are instead. however,
In the case of Ni wire, the voltage required to generate a discharge increases by about 100V. Also, metals such as iron and copper oxidize the electrode surface. Discharge becomes unstable. That is, as an electrode, LaB&
A Ni wire coated with is more desirable. In addition, instead of the above LaB, YB, , SrB, , Ba
Good results can also be obtained using boron compounds such as CeB. Furthermore, as a matter of course, similar effects can be obtained by using these boron compounds themselves. The effect of discharge increases as the discharge current increases, and the effect saturates at a constant discharge current, after which it has a rather negative effect. Although the saturated discharge current value changes depending on the shape of the device, the fact that a superconducting thin film can be created by discharge is an advantage of the present invention. In the above example, Y Ba 2 Cu 307-
Although the apparatus for producing an X thin film has been described, the film growth mechanism is the same for MOCVD of other oxide superconductors, and it is possible to produce superconducting thin films at low temperatures using the present invention.
本発明により、酸化物超電導体の薄膜が低温において作
成可能となる。これにより、高性能の超電導エレクトロ
ニクス素子、超電導導線、超電導シールド材の生産が可
能となる。According to the present invention, thin films of oxide superconductors can be formed at low temperatures. This will enable the production of high-performance superconducting electronic devices, superconducting wires, and superconducting shielding materials.
第1図は本発明の実施例における薄膜の作成に用いた薄
膜作成装置の模式図、第2図は本発明による電気特性改
善の効果を示すiasの抵抗−温度特性図である。
符号の説明
1・・・原料供給側電極、2・・・排気系側電極、3・
・・直流電源、4・・・放電電流制御用抵抗、5・・・
基板、6・Y (DPM) 3.7 ”・B a (D
P M ) z、8−Cu (D P M) 2.9
・・・酸素ボンベ、10・・・電気炉曲線21・・・放
電を発生させて作成した薄膜の抵抗の温度変化を示す曲
線、
曲線22・・・放電を発生させないで作成した薄膜の抵
抗の温度変化を示す曲線
第1IIIFIG. 1 is a schematic diagram of a thin film forming apparatus used for forming a thin film in an example of the present invention, and FIG. 2 is a resistance-temperature characteristic diagram of IAS showing the effect of improving electrical characteristics according to the present invention. Explanation of symbols 1... Raw material supply side electrode, 2... Exhaust system side electrode, 3...
...DC power supply, 4...Resistance for controlling discharge current, 5...
Board, 6・Y (DPM) 3.7”・B a (D
P M ) z, 8-Cu (D P M ) 2.9
...Oxygen cylinder, 10...Electric furnace curve 21...Curve showing the temperature change in the resistance of a thin film created by generating an electric discharge, Curve 22...Curve showing the change in resistance of a thin film created without generating an electric discharge Curve 1III showing temperature change
Claims (3)
、基板近傍に直流放電を発生せる機構を有することを特
徴とする超電導薄膜作成装置。1. A superconducting thin film forming apparatus characterized in that the MOCVD apparatus for producing an oxide high-temperature superconducting thin film includes a mechanism for generating a direct current discharge near a substrate.
構を有することを特徴とする請求項第1項記載の超電導
薄膜作成装置。2. 2. The superconducting thin film forming apparatus according to claim 1, further comprising a mechanism for controlling the temperature of the electrode on the exhaust system side to 200 to 400°C.
バリウム、ランタンストロンチウムの硼素化物の群から
選ばれる少なくとも一者を用いることを特徴とする請求
項第1項もしくは第2項記載の超電導薄膜作成装置。3. Metal boride, preferably yttrium, for the electrode.
3. The superconducting thin film forming apparatus according to claim 1, wherein at least one member selected from the group consisting of barium and lanthanum strontium borides is used.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1163950A JPH0333003A (en) | 1989-06-28 | 1989-06-28 | Superconducting thin film production equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1163950A JPH0333003A (en) | 1989-06-28 | 1989-06-28 | Superconducting thin film production equipment |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0333003A true JPH0333003A (en) | 1991-02-13 |
Family
ID=15783905
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1163950A Pending JPH0333003A (en) | 1989-06-28 | 1989-06-28 | Superconducting thin film production equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0333003A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7950280B2 (en) | 2004-07-27 | 2011-05-31 | Franz Haimer Maschinenbau Kg | Balance ring and method for balancing a rotating component |
-
1989
- 1989-06-28 JP JP1163950A patent/JPH0333003A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7950280B2 (en) | 2004-07-27 | 2011-05-31 | Franz Haimer Maschinenbau Kg | Balance ring and method for balancing a rotating component |
| JP4754564B2 (en) * | 2004-07-27 | 2011-08-24 | フランツ・ハイマー・マシーネンバウ・カーゲー | Balance ring and method for maintaining balance of rotating member |
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