JPH085672B2 - Method for producing oxide superconductor - Google Patents
Method for producing oxide superconductorInfo
- Publication number
- JPH085672B2 JPH085672B2 JP63026129A JP2612988A JPH085672B2 JP H085672 B2 JPH085672 B2 JP H085672B2 JP 63026129 A JP63026129 A JP 63026129A JP 2612988 A JP2612988 A JP 2612988A JP H085672 B2 JPH085672 B2 JP H085672B2
- Authority
- JP
- Japan
- Prior art keywords
- oxide superconductor
- temperature
- composition
- producing
- ratio
- 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
Links
- 238000004519 manufacturing process Methods 0.000 title claims description 7
- 239000002887 superconductor Substances 0.000 title claims description 6
- 239000013078 crystal Substances 0.000 claims description 9
- 238000004544 sputter deposition Methods 0.000 claims description 2
- 239000000203 mixture Substances 0.000 description 18
- 239000000463 material Substances 0.000 description 11
- 230000007704 transition Effects 0.000 description 8
- 239000002994 raw material Substances 0.000 description 5
- 239000012535 impurity Substances 0.000 description 3
- 229910052761 rare earth metal Inorganic materials 0.000 description 3
- 238000009792 diffusion process Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000002245 particle Substances 0.000 description 2
- 239000006104 solid solution Substances 0.000 description 2
- 229910004247 CaCu Inorganic materials 0.000 description 1
- 238000002441 X-ray diffraction Methods 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 238000009529 body temperature measurement Methods 0.000 description 1
- 238000001354 calcination Methods 0.000 description 1
- RKTYLMNFRDHKIL-UHFFFAOYSA-N copper;5,10,15,20-tetraphenylporphyrin-22,24-diide Chemical compound [Cu+2].C1=CC(C(=C2C=CC([N-]2)=C(C=2C=CC=CC=2)C=2C=CC(N=2)=C(C=2C=CC=CC=2)C2=CC=C3[N-]2)C=2C=CC=CC=2)=NC1=C3C1=CC=CC=C1 RKTYLMNFRDHKIL-UHFFFAOYSA-N 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 230000005292 diamagnetic effect Effects 0.000 description 1
- 230000003628 erosive effect Effects 0.000 description 1
- 238000013213 extrapolation Methods 0.000 description 1
- 238000010304 firing Methods 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 150000002500 ions Chemical class 0.000 description 1
- 238000005404 magnetometry Methods 0.000 description 1
- 238000001755 magnetron sputter deposition Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000000465 moulding Methods 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- 238000004627 transmission electron microscopy Methods 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 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
- Inorganic Compounds Of Heavy Metals (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
- Compositions Of Oxide Ceramics (AREA)
Description
【発明の詳細な説明】 産業上の利用分野 本発明は酸化物超超伝導材料に関する。TECHNICAL FIELD The present invention relates to an oxide superconducting material.
従来の技術 近年超伝導材としてYBaCuO系の材料が報告され、色々
な試験研究が行われている。その結果、この材料は非常
に不安定であり、又超伝導状態の開始温度と完了温度と
の差が大きいといった大きな欠点がある事が知られてき
た。さらに希土類元素を多量に使用する為に価格もたか
く市況変動に左右されやすいといった経済的にも不安定
な要素を抱えている。これらすべてについての改良がの
ぞまれている。2. Description of the Related Art In recent years, YBaCuO-based materials have been reported as superconducting materials, and various test studies have been conducted. As a result, it has been known that this material is very unstable and has a big defect that the difference between the starting temperature and the completion temperature of the superconducting state is large. In addition, since it uses a large amount of rare earth elements, it has an economically unstable element that the price is high and it is easily affected by market fluctuations. Improvements in all of these are desired.
さらに極く最近、SrBiCuO系の新材料が報告されてい
る。しかし、これらについては詳しいことは現在の所不
明である。Even more recently, new SrBiCuO-based materials have been reported. However, the details of these are currently unknown.
発明が解決しようとする課題 本発明は上述のような温度差、安定性、さらには経済
性の問題のない材料を提供することを目的とする。DISCLOSURE OF THE INVENTION Problems to be Solved by the Invention An object of the present invention is to provide a material that does not have the above-mentioned temperature difference, stability, and economical problems.
課題を解決するための手段 ABiCuO(Aはアルカリ土族よりなる元素の少なくとも
一種以上を含む)を主とした酸化物超伝導体の製造方法
であって、A/Bi/Cuの比が3/2/2よりなる第1の結晶相成
分と、ACuOを主とした第2の結晶相成分とを別々に用意
し、その後これらをスパッタにより多層に積層すること
を特徴とする酸化物超伝導体の製造方法である。Means for Solving the Problem A method for producing an oxide superconductor mainly containing ABiCuO (A includes at least one element of alkaline earth group), wherein an A / Bi / Cu ratio is 3/2. A first crystal phase component consisting of / 2 and a second crystal phase component mainly composed of ACuO are separately prepared, and then these are laminated in multiple layers by sputtering. It is a manufacturing method.
また、Aのイオン半径が1オングストロームより大き
い元素とそれ以下の元素が混在していることを特徴とす
る酸化物超伝導体の製造方法である。Further, it is a method for producing an oxide superconductor characterized in that an element having an ionic radius of A larger than 1 angstrom and an element having a smaller ionic radius are mixed.
作用 不安定性の原因となる希土類元素やアルカリ土族元素
を多量に含まず、安定している為に水による浸食等が生
じない。また上述の2結晶相の各々の固溶範囲はかなり
広いと推定され、その為と思われるが不純物相を殆ど含
有せず、これも安定性に役立っていると思われる。さら
にこの事が上述の温度差を小さくするのに役立っている
と思われる。現在の所理由は良く分からないが上記2結
晶相の界面に於いて特異な事が生じているの2点が超伝
導転移温度の向上の原因と推定される。Since it does not contain a large amount of rare earth elements and alkaline earth elements that cause instability, it is stable and does not cause erosion by water. Further, the solid solution range of each of the above-mentioned two crystal phases is presumed to be quite wide, and this is considered to be the reason, but it contains almost no impurity phase, and this also seems to be useful for stability. Furthermore, this seems to be useful for reducing the above-mentioned temperature difference. Although the reason for this is not clear at present, it is presumed that the two points that a peculiar thing occurs at the interface of the above-mentioned two crystal phases are the causes of the improvement of the superconducting transition temperature.
さらに明白なように高価な供給の不安定な希土類元素
を全く含まない事からも分かるように経済性にも優れて
いる。Furthermore, as is apparent, it does not contain expensive rare earth elements, which are unstable, and it has excellent economic efficiency.
実施例 一般的な最近のYBaCuO系の材料について追試を行った
所、所謂123(Y/Ba/Cuの比)の最適な組成でも本発明者
らの検討によれば、転移温度は約90度Kであったが、上
述の温度差は10度近く有り非常に大きい事が示され、又
少し組成を変動させれば不純物相が生成し特性が変動す
る事が示された。Example When a general recent YBaCuO-based material was additionally tested, the transition temperature was about 90 ° C. according to the study by the present inventors even with the optimum composition of so-called 123 (Y / Ba / Cu ratio). Although it was K, it was shown that the above-mentioned temperature difference was close to 10 degrees and was extremely large, and that the impurity phase was generated and the characteristics fluctuated if the composition was slightly changed.
これに対して本発明者らの検討によれば新材料は以下
に示したように安定した優れた特性を有している。On the other hand, according to the study by the present inventors, the new material has stable and excellent characteristics as shown below.
イオン半径1オングストローム以下のMg,Caの一群
と、それよりも大きなイオン半径のSr,Baの一群から少
なくとも一種以上と、Bi,Cuを含む酸化物を三者の比が
ほぼ3/2/2なるように秤量し、次に均一に混合した。こ
れを甲原料とする。次に同様に三者の比が1/0/2に配合
し乙原料とする。甲乙の原料を混合して各種の組成の物
を作成した。良く混合した後に800から850度で仮焼、さ
らに粉砕、成型した後に焼成を850度6時間行った後に8
20度に保持し、50度/時間で除冷した。得られた結果を
第一表に示す。A group of Mg, Ca with an ionic radius of 1 angstrom or less and at least one group of Sr, Ba with an ionic radius larger than that, and an oxide containing Bi, Cu have a ratio of about 3/2/2. Were weighed and then mixed evenly. This is used as a raw material. Next, similarly, the ratio of the three is mixed to 1/0/2 and used as the second raw material. Raw materials of Kotsu were mixed to prepare various compositions. After mixing well, calcination at 800 to 850 degrees, crushing and molding, then firing at 850 degrees for 6 hours, then 8
The temperature was maintained at 20 ° C and the mixture was cooled at 50 ° C / hour. The obtained results are shown in Table 1.
第1表に於いて、転移温度は超伝導の開始点を示す抵
抗温度曲線での屈曲点(外挿点)の温度と零抵抗になる
終了点の温度の中間の値を示す。また、温度差はこれら
開始点と終了点の温度差を示す。また、同表の割合は試
料の帯磁率・温度測定より算出したものである。具体的
には、試料の完全反磁性(マイスナー効果)を示す遷移
温度(転移温度にほぼ等しい)が80K付近と105から115K
の2種類存在するため、両者の中間点の95Kでの完全反
磁性量(体積分相当)を求めてV1とし、60K以下のそれ
を求めてV2とし、V1/V2×100(%)を「割合」と定め
た。同表に於いて、組成9の試料以外は全てアルカリ土
族元素のイオン半径が1オングストローム以下の元素と
それより大きい元素を混在させたものを示す。また、同
表の組成1から8より明らかな様に上述の温度差は全て
5度以下と小さく、転移温度も80Kのもの(組成5)と1
05から115K(組成1〜4、組成6〜8)との2種が混在
しているものの安定している事が示された。表には高温
のものを記載してある。100度K以上の物の割合は同表
より明らかに上記組成比が2/1/2の時に最大になってい
る事が確認された。さらに同表の組成3、7〜9の試料
の結果を比較すると判るように、上記二群の元素を混在
せしめる事によって、単独の群に属する元素の組合せの
場合には転移温度が20から30K(同表組成9ではSrの
み)のものが105K以上(組成3ではSrとCaの組合せ、組
成7では(Sr,Ba)とCaの組合せ、組成8では(Sr,Ba)
と(Ca,Mg)の組合せ)となっている事が示されてい
る。さらに高温高湿下(60度60%)に1ケ月放置する耐
湿テストでは所謂YBaCu系材料では全体が白色に変化し
かなり崩壊したのに対して、本材料は同表の組成9を除
き、表面が僅かに白色化したのみであり非常に安定して
いる事が示された。 In Table 1, the transition temperature is an intermediate value between the temperature at the inflection point (extrapolation point) on the resistance temperature curve indicating the start point of superconductivity and the end point temperature at which the resistance becomes zero. The temperature difference indicates the temperature difference between the starting point and the ending point. The ratios in the table are calculated from the magnetic susceptibility and temperature measurements of the sample. Specifically, the transition temperature (almost equal to the transition temperature) showing the complete diamagnetism (Meissner effect) of the sample is around 80K and from 105 to 115K.
Since there are two types, V1 is obtained by finding the perfect diamagnetic amount (corresponding to the volume) at 95K at the midpoint between them, and V2 is obtained by finding it below 60K, and V1 / V2 x 100 (%) is Ratio ”. In the table, all of the samples other than the sample of composition 9 show the mixture of an element having an ionic radius of an alkaline earth element of 1 angstrom or less and an element having a larger ion radius. Also, as is clear from compositions 1 to 8 in the table, the above temperature differences are all 5 degrees or less, and the transition temperature is 80K (composition 5).
From 05 to 115K (composition 1 to 4, composition 6 to 8), two kinds were mixed, but it was shown to be stable. The table shows high temperature. From the same table, it was clearly confirmed that the ratio of the products having a temperature of 100 degrees K or more was the maximum when the composition ratio was 2/1/2. Further, as can be seen by comparing the results of the samples of compositions 3 and 7 to 9 in the same table, by mixing the elements of the above two groups, the transition temperature is 20 to 30 K in the case of the combination of the elements belonging to the single group. (Sr in Table 9 only Sr) is 105K or more (composition 3 is a combination of Sr and Ca, composition 7 is a combination of (Sr, Ba) and Ca, composition 8 is (Sr, Ba)
And (Ca, Mg) combination). In a moisture resistance test in which the material was left under high temperature and high humidity (60 degrees 60%) for 1 month, the so-called YBaCu-based material turned white and collapsed considerably. Was only slightly whitened, indicating that it was very stable.
又、X線による解析の結果ではかなり広い範囲で単一
の3/2/2の組成比からなる結晶相(現在検討中であるが
格子定数がa=15.3オングストローム,b=c=22.9オン
グストロームの正方晶と表面上記述され、透過電子顕微
鏡の結果と合わせれば単位胞5.4オングストロームの疑
似立方晶よりなると推定される。)と1/0/2の組成より
なる所謂CaCu2O3の結晶相を形成しており、これらが焼
結体を構成する粒子内に互いに重なり微細な薄い析出層
を構成している事が確認された。上述の様に組成比2/1/
2で最適に成るのはこれらの結晶相が1/1になる事に対応
しており、これら二結晶相の界面で特異な事が生じてい
ると推定される。In addition, the result of the X-ray analysis shows that a crystal phase consisting of a single 3/2/2 composition ratio in a fairly wide range (currently under study, the lattice constants are a = 15.3 angstrom and b = c = 22.9 angstrom). The surface is described as tetragonal, and when combined with the results of transmission electron microscopy, it is estimated that it is composed of a pseudocubic unit cell of 5.4 angstroms.) And a so-called CaCu 2 O 3 crystal phase with a composition of 1/0/2. It was confirmed that they were formed and these particles overlap each other in the particles constituting the sintered body to form a fine thin deposition layer. As mentioned above, composition ratio 2/1 /
The optimum value of 2 corresponds to the fact that these crystal phases become 1/1, and it is presumed that a peculiar thing occurs at the interface between these two crystal phases.
次にマグネトロンスパッタリング法を用い人為的に多
層の積層を行った。ターゲットとしては上記の甲乙両原
料単独で製造した物を用い、酸素を4%含むArガス中
で、基板温度を550度に保ち各々の薄膜を交互に積層し
た。1層の厚さを200から1000オングストロームに変え
て種々のものを形成した所、一部には転移温度80度をも
つ不純物相が認められたがいずれも100度K以上を示し
た。低温に保持している事から積層間の拡散は小さいと
推定される。又電子顕微鏡による断面の観察結果でも拡
散は小さい事が示されている。又上述の様に厚さの比が
ほぼ1/1の時に、同様に最適に成る事も確認された。Next, the magnetron sputtering method was used to artificially stack multiple layers. As a target, the above-mentioned raw materials prepared from both raw materials were used, and the thin films were alternately laminated while maintaining the substrate temperature at 550 ° C. in Ar gas containing 4% oxygen. When various layers were formed by changing the thickness of one layer from 200 to 1000 angstroms, an impurity phase having a transition temperature of 80 degrees was observed in some of them, but all showed 100 degrees K or more. Since it is kept at a low temperature, it is estimated that the diffusion between the layers is small. Further, the observation of the cross section by an electron microscope shows that the diffusion is small. It was also confirmed that, as described above, when the thickness ratio was about 1/1, the optimum value was obtained.
発明の効果 本発明によれば、耐湿性に優れた、且つ、固溶範囲の
広く上述の温度差の小さな安定性再現性の優れた材料を
提供することができ、広く超伝導機器に適用され得る。Advantageous Effects of the Invention According to the present invention, it is possible to provide a material having excellent moisture resistance, a wide solid solution range, and a small temperature difference and excellent stability reproducibility, and is widely applied to superconducting equipment. obtain.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 河島 俊一郎 大阪府門真市大字門真1006番地 松下電器 産業株式会社内 (56)参考文献 特開 昭63−10084(JP,A) JAPANESE JOURNAL O F APPLIED PHYSICS,26 (12)1987 L2080−2081 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Shunichiro Kawashima 1006 Kadoma, Kadoma City, Osaka Prefecture Matsushita Electric Industrial Co., Ltd. (56) , 26 (12) 1987 L2080-2081
Claims (2)
少なくとも一種以上を含む)を主とした酸化物超伝導体
の製造方法であって、A/Bi/Cuの比が3/2/2よりなる第1
の結晶相成分と、ACuOを主とした第2の結晶相成分とを
別々に用意し、その後これらをスパッタにより多層に積
層することを特徴とする酸化物超伝導体の製造方法。1. A method for producing an oxide superconductor mainly comprising ABiCuO (A includes at least one element of alkaline earth group), wherein A / Bi / Cu ratio is 3/2/2. Consisting of the first
And a second crystal phase component mainly composed of ACuO are separately prepared, and then these are laminated in multiple layers by sputtering, and a method for producing an oxide superconductor.
大きい元素とそれ以下の元素が混在していることを特徴
とする特許請求の範囲第1項に記載の酸化物超伝導体の
製造方法。2. The method for producing an oxide superconductor according to claim 1, wherein elements having an ionic radius of A larger than 1 angstrom and elements having a smaller ionic radius are mixed.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63026129A JPH085672B2 (en) | 1988-02-05 | 1988-02-05 | Method for producing oxide superconductor |
| EP93201456A EP0560464B1 (en) | 1988-02-05 | 1989-02-03 | Superconductive oxide materials |
| DE68925294T DE68925294T2 (en) | 1988-02-05 | 1989-02-03 | Superconducting oxide materials |
| EP89301057A EP0331292B2 (en) | 1988-02-05 | 1989-02-03 | Oxyde superconductive material |
| DE68915578T DE68915578T3 (en) | 1988-02-05 | 1989-02-03 | Oxide superconducting material. |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63026129A JPH085672B2 (en) | 1988-02-05 | 1988-02-05 | Method for producing oxide superconductor |
Related Child Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7168314A Division JP2747438B2 (en) | 1995-06-09 | 1995-06-09 | Oxide superconducting material |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01201026A JPH01201026A (en) | 1989-08-14 |
| JPH085672B2 true JPH085672B2 (en) | 1996-01-24 |
Family
ID=12184953
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63026129A Expired - Lifetime JPH085672B2 (en) | 1988-02-05 | 1988-02-05 | Method for producing oxide superconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH085672B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01242459A (en) * | 1988-03-23 | 1989-09-27 | Semiconductor Energy Lab Co Ltd | Superconducting ceramics |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0643268B2 (en) * | 1988-01-20 | 1994-06-08 | 科学技術庁金属材料技術研究所長 | Oxide high temperature superconductor |
-
1988
- 1988-02-05 JP JP63026129A patent/JPH085672B2/en not_active Expired - Lifetime
Non-Patent Citations (1)
| Title |
|---|
| JAPANESEJOURNALOFAPPLIEDPHYSICS,26(12)1987L2080−2081 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01201026A (en) | 1989-08-14 |
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