JPH025582A - Manufacture of superconducting thin film - Google Patents
Manufacture of superconducting thin filmInfo
- Publication number
- JPH025582A JPH025582A JP63157114A JP15711488A JPH025582A JP H025582 A JPH025582 A JP H025582A JP 63157114 A JP63157114 A JP 63157114A JP 15711488 A JP15711488 A JP 15711488A JP H025582 A JPH025582 A JP H025582A
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- substrate
- orientation
- temperature
- superconducting thin
- 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
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
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
- Physical Vapour Deposition (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 本発明は超伝導薄膜の製造方法に関する。[Detailed description of the invention] Industrial applications The present invention relates to a method for manufacturing a superconducting thin film.
超電導体は、その電気抵抗が零になる性質を利用して1
強力磁場発生装置や半導体素子の配線に。Superconductors utilize the property of having zero electrical resistance to
For wiring of strong magnetic field generators and semiconductor devices.
また、ジョセフソン効果を利用した高速スイッチ素子や
微小磁場、電場センサとして使用される。It is also used as a high-speed switching element that utilizes the Josephson effect, and as a micromagnetic field or electric field sensor.
従来の技術
超電導体は、薄膜としての利用価値が大きい、薄膜の基
板には、セラミックス、単結晶、アモルファス物質、金
属等が用いられるが、酸化物の薄膜を作成した場合、基
板の種類と作成条件によって。Conventional technologySuperconductors have great utility as thin films.Ceramics, single crystals, amorphous materials, metals, etc. are used for thin film substrates, but when creating oxide thin films, the type and creation of the substrate Depending on the conditions.
結晶の方位が変わりやすい。TI、 Ba、 Ca
、 Cuの酸化物超伝導体は、斜方晶系で、(RE)
BaaCusO□21系(REは希土類元素)超電導体
と類似の結晶構造をもち、(100)と(010)方向
に電流が流れ易いことが推定される[ヨウイチ ェノモ
ト(YoulchI Enomoto)イ也:ジャパニ
ーズ・ジャーナル・オブ・アプライド・フィジックス(
J、 Appl、 Phys、) 28巻、ページL1
248〜L1250. 1987年6月19日受付]。Crystal orientation is easily changed. TI, Ba, Ca
, Cu oxide superconductor is orthorhombic, (RE)
It has a crystal structure similar to that of BaaCusO□21-based superconductors (RE is a rare earth element), and it is estimated that current flows easily in the (100) and (010) directions. Journal of Applied Physics (
J, Appl, Phys,) Volume 28, Page L1
248~L1250. Received June 19, 1987].
応用の観点からは、基板面に垂直に(001)軸を並べ
ることが望ましい。(001)配向、即ち、C軸配向に
適した基板を選び、高度にC軸配向した薄膜超電導体を
作成する必要がある。From an application standpoint, it is desirable to align the (001) axes perpendicular to the substrate surface. It is necessary to select a substrate suitable for (001) orientation, that is, C-axis orientation, and create a thin film superconductor with highly C-axis orientation.
発明が解決しようとする課題
本発明の目的は、基板面に平行に、 (100)ある
いは(010)軸を配向させる。即ち、基板面に垂直に
(OOi)方向が配向するようにすることである。Problems to be Solved by the Invention An object of the present invention is to orient the (100) or (010) axis parallel to the substrate surface. That is, the (OOi) direction is oriented perpendicular to the substrate surface.
課題を解決するための手段
基板として(001)面にへき閲させたMgO中結晶を
用い、アルゴン(Ar)/酸素(02)が体重比で95
15〜60/40. ガス圧力が80〜200mT、
基板の温度が400〜600°Cの条件下で9スパツタ
法によりTL(Bat−ncall)ecuc022−
x酸化物〔但し、 A=0.3〜0.7. B=5
〜9.C=3〜7]を成膜させる。Means for Solving the Problem Using a (001) crystal in MgO as a substrate, the argon (Ar)/oxygen (02) ratio was 95 by weight.
15-60/40. Gas pressure is 80~200mT,
TL (Bat-ncall) ecuc022- by 9 sputtering method under the condition that the substrate temperature is 400 to 600°C.
x oxide [However, A=0.3-0.7. B=5
~9. C=3 to 7] is formed into a film.
作用
基板の温度が低ずぎるか、Ar102が大きすぎるか、
あるいは、ガス圧力が低ずぎると9作成した薄膜は多結
晶体あるいはアモルファス体である。Is the temperature of the working substrate too low, or is Ar102 too large?
Alternatively, if the gas pressure is too low, the thin film produced will be polycrystalline or amorphous.
しかし、適当なAr102.ガス圧力および基板温度で
は、薄膜の<001)軸が基板面に垂直に揃って。However, suitable Ar102. At gas pressure and substrate temperature, the <001) axis of the thin film is aligned perpendicular to the substrate plane.
エビタギシアル的に配向成長する。Ebitagistically oriented growth.
実施例
i膜it RF−マグネトロンスパッタ法により作成し
た。ターゲットの組成はTL(Bat−oca向)、I
Cuc02.−x +:但し、 A:0,2へ−0
,8,R==J〜10. C=2〜・8コである。原
料のTl2O3,BaCO3,CaC0a、CuOを所
定量、配合9 混合し9 ターゲットとした。ターゲッ
ト粉末は、銅皿に入れ、200kg/cm2の圧力でプ
レスした。Example I Film It was prepared by RF-magnetron sputtering. The composition of the target is TL (for Bat-oca), I
Cuc02. -x +: However, A: -0 to 0,2
,8,R==J~10. C=2 to 8. Predetermined amounts of raw materials Tl2O3, BaCO3, CaC0a, and CuO were mixed to form a target. The target powder was placed in a copper pan and pressed at a pressure of 200 kg/cm2.
スパッタガスはI Ar102が体積比で97/3〜
50150の範囲の混合ガスである。ガス圧力は606
0−25Oの範囲で変化させた。基板の温度は350−
650℃である。基板とターゲットの距離は8ernで
ある。The sputtering gas is IAr102 with a volume ratio of 97/3~
50150 range. Gas pressure is 606
It was varied in the range of 0-25O. The temperature of the board is 350-
The temperature is 650°C. The distance between the substrate and the target is 8ern.
基板には、(100)面でへき関したMgO単結晶を用
いた。成膜は6時間行った。For the substrate, an MgO single crystal cleaved along the (100) plane was used. Film formation was carried out for 6 hours.
類似の結晶構造の(RE )B a2 Cus Op?
−x単結晶の場合、斜方晶系の(010)、(100)
方向の電気抵抗が、(001)方向に比べて、かなり低
いことが報告占れている(−に記の文献)。従って、臨
界電流密度も(010)、(100)方向で大きいこと
が容易に推定できる。成膜は+ 5mmX15mmの
形状で行い、X線回折パターンを観測してのち。Similar crystal structure (RE)B a2 Cus Op?
-x In the case of single crystal, (010), (100) of orthorhombic system
It has been reported that the electrical resistance in the (001) direction is considerably lower than that in the (001) direction (references listed in -). Therefore, it can be easily estimated that the critical current density is also large in the (010) and (100) directions. The film was formed in a shape of +5 mm x 15 mm, and the X-ray diffraction pattern was observed.
RFマグネトロンスパッタ法でPt電極を付けた。Pt electrodes were attached using RF magnetron sputtering.
電気抵抗は4端子法で測定した。種々の条件で作成した
薄膜試料について、電気抵抗と帯磁率の温度変化の測定
により、超伝導現象を示すかどうかをしらべた。(00
1)、(002)、(003)・・・・方向が、基板に
垂直に配向している度合を表わすために配向率をI(0
01)/[I(001)→−I(010)コと定義した
。完全に(001)方向に配向しているならば、即ち、
基板に垂直に(001)方向が完全に揃っているならば
、配向率は1になる。この配向率が太き(なるスパッタ
リング条件を求めた。組成TL(Baa、6Casr、
)acos022−xについて種々のスパッタリング条
件で作成した薄膜の配向率を第1表に示す。この組成の
薄膜は試みたスパッタリング条件の範囲で、超伝導特性
を示し、臨界温度は95〜125にであった。Electrical resistance was measured using a four-terminal method. For thin film samples prepared under various conditions, we investigated whether they exhibit superconductivity by measuring temperature changes in electrical resistance and magnetic susceptibility. (00
1), (002), (003)... To express the degree to which the directions are oriented perpendicular to the substrate, the orientation rate is expressed as I(0
01)/[I(001)→-I(010). If it is completely oriented in the (001) direction, that is,
If the (001) direction is perfectly aligned perpendicular to the substrate, the orientation ratio will be 1. The sputtering conditions were determined such that this orientation ratio was thick.Composition TL (Baa, 6Casr,
) Table 1 shows the orientation ratios of thin films produced under various sputtering conditions for acos022-x. A thin film with this composition exhibited superconducting properties within the range of sputtering conditions tested, with a critical temperature of 95-125°C.
配向率I(001)/[I(001)+I(010)]
は+ Ar102が9515〜60/40. ガス
圧力が8080−2O0,基板温度が400〜800℃
の範囲では、非常に大きく0.5以上になっている。Orientation rate I(001)/[I(001)+I(010)]
+Ar102 is 9515~60/40. Gas pressure is 8080-2O0, substrate temperature is 400-800℃
In the range of , it is very large and exceeds 0.5.
第1表 T L(Ba@、5Cal11.5)scuG
o22−xの作成条件と配向率の関係[1コ
第1表
T la (B aa、s Cae、s )* Cua
O22−Xの作成条件と配向率の関係[2コ
第1表
T 1a(Baa、5Caa、5)scueo2a−x
の作成条件と配向率の関係[3コ
第1表
T l4(Bas、5Cae、5)scuso22−x
の作成条件と配向率の関係[4]
CをA= 0.2〜0.8. B=4〜10. C
=2〜8の範囲で変えたときの超伝導臨界温度Tcと配
向率の関係を第2表に示す。×は少なくとも液体窒素温
度以上では超伝導を示さなかった試料である。Table 1 T L (Ba@, 5Cal11.5) scuG
Relationship between production conditions and orientation rate of o22-x [1 piece Table 1 T la (B aa, s Cae, s ) * Cua
Relationship between production conditions and orientation rate of O22-X [2 pieces Table 1 T 1a(Baa, 5Caa, 5)scueo2a-x
Relationship between production conditions and orientation rate [3 pieces Table 1
Relationship between production conditions and orientation rate [4] C and A=0.2 to 0.8. B=4-10. C
Table 2 shows the relationship between the superconducting critical temperature Tc and the orientation rate when the superconducting critical temperature Tc is varied within the range of =2 to 8. × indicates a sample that did not exhibit superconductivity at least above the liquid nitrogen temperature.
第2表の結果から+ T14(Ba+−acall)
scucOaa−i+ [:但し、 A=0.3〜0
.7. B=5〜9. C=3〜7]の組成の試料
が77に以上の臨界温度と高い配向率をもつことがわか
る。From the results in Table 2 + T14 (Ba+-acall)
scucOaa-i+ [: However, A=0.3~0
.. 7. B=5-9. It can be seen that the sample with a composition of C=3 to 7] has a critical temperature of 77 or higher and a high orientation rate.
配向率の高い0.5以上の試料の室温における比抵抗は
、かなり低かった。例えば、配向率が0.76の試料の
比抵抗は、配向率が0.17の試料の比抵抗の約60分
の1であった。The specific resistance at room temperature of samples with a high orientation ratio of 0.5 or more was quite low. For example, the specific resistance of a sample with an orientation rate of 0.76 was about 1/60 of the specific resistance of a sample with an orientation rate of 0.17.
(以下余白)
次に、スパッタリング条件を一定にして、すなわちAr
10a:90/10. ガス圧力=200mT。(Left below) Next, the sputtering conditions were kept constant, that is, Ar
10a:90/10. Gas pressure = 200mT.
基板温度550°Cで作成した薄膜の超伝導特性と配向
率について組成の依存性をしらべた。組成式%式%
第2表 組成式Tla (Bat−ncan) Bcu
c022−。We investigated the composition dependence of the superconducting properties and orientation ratio of thin films prepared at a substrate temperature of 550°C. Composition formula % Formula % Table 2 Composition formula Tla (Bat-ncan) Bcu
c022-.
の薄膜の超伝導臨界m度TO2配同率の組成依存性[1
]
第2表
組成式TIA(Bat−ncaa) ecueo22−
xの薄膜の超伝導臨界温度Tc+ 配向率の組成依存
性[2コ
第2表
組成式Tlz (Bat−ocall) 1lCucO
22−の薄膜の超伝導臨界温度Tc+ 配向率の組成
依存性[3コ
発明の効果
本発明によれば、スパッタ法で、アルゴン/酸素。Composition dependence of superconducting critical m degree TO2 coordination ratio of thin film [1
] Table 2 Composition formula TIA (Bat-ncaa) ecueo22-
Superconducting critical temperature Tc+ of the thin film of
22- Superconducting Critical Temperature Tc+ of Thin Film Composition Dependency of Orientation Rate [3 Effects of the Invention According to the present invention, argon/oxygen is used by the sputtering method.
ガス圧力、基板温度を制御するだけで、MgO単結晶上
に9面に平行に比抵抗の低い、即ち、X板面に垂直に高
度に(001)軸が配向した超電導薄膜を形成できる。By simply controlling the gas pressure and substrate temperature, it is possible to form a superconducting thin film on an MgO single crystal with low resistivity parallel to the nine planes, that is, with the (001) axis highly oriented perpendicular to the X-plate plane.
Claims (1)
晶基板上に、アルゴン/酸素が体積比で95/5〜60
/40、ガス圧力が80〜200mT、基板の温度が4
00〜600℃で、スパッタ法により、Tl_4(Ba
_1_−_ACa_A)_BCu_CO_2_2_−_
X酸化物[但し、A=0.3〜0.7、B=5〜9、C
=3〜7]薄膜を形成させることにより、基板面に平行
に電気抵抗の低い結晶方位(100)および(010)
軸を配向させることを特徴とする超電導薄膜の製造方法
。On a MgO (magnesia) single crystal substrate cleaved in the (100) plane, argon/oxygen was applied at a volume ratio of 95/5 to 60.
/40, gas pressure is 80-200mT, substrate temperature is 4
Tl_4(Ba
_1_-_ACa_A)_BCu_CO_2_2_-_
X oxide [However, A = 0.3 to 0.7, B = 5 to 9, C
=3~7] By forming a thin film, crystal orientations (100) and (010) with low electrical resistance parallel to the substrate surface
A method for producing a superconducting thin film characterized by orienting its axes.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63157114A JPH025582A (en) | 1988-06-24 | 1988-06-24 | Manufacture of superconducting thin film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63157114A JPH025582A (en) | 1988-06-24 | 1988-06-24 | Manufacture of superconducting thin film |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH025582A true JPH025582A (en) | 1990-01-10 |
Family
ID=15642528
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63157114A Pending JPH025582A (en) | 1988-06-24 | 1988-06-24 | Manufacture of superconducting thin film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH025582A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9045643B2 (en) | 2006-04-21 | 2015-06-02 | Nippon Sheet Glass Company Limited | Bright pigment, method for producing the pigment, and waterborne resin composition containing the pigment |
| US9107834B2 (en) | 2007-04-18 | 2015-08-18 | Nippon Sheet Glass Company, Limited | Bright pigment and cosmetic composition using the same |
-
1988
- 1988-06-24 JP JP63157114A patent/JPH025582A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9045643B2 (en) | 2006-04-21 | 2015-06-02 | Nippon Sheet Glass Company Limited | Bright pigment, method for producing the pigment, and waterborne resin composition containing the pigment |
| US9107834B2 (en) | 2007-04-18 | 2015-08-18 | Nippon Sheet Glass Company, Limited | Bright pigment and cosmetic composition using the same |
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