JPH0764620B2 - Oxide superconductor composition and method for producing the same - Google Patents
Oxide superconductor composition and method for producing the sameInfo
- Publication number
- JPH0764620B2 JPH0764620B2 JP62331736A JP33173687A JPH0764620B2 JP H0764620 B2 JPH0764620 B2 JP H0764620B2 JP 62331736 A JP62331736 A JP 62331736A JP 33173687 A JP33173687 A JP 33173687A JP H0764620 B2 JPH0764620 B2 JP H0764620B2
- Authority
- JP
- Japan
- Prior art keywords
- composition
- oxide superconductor
- powder
- producing
- superconductor composition
- 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
- 239000000203 mixture Substances 0.000 title claims description 35
- 239000002887 superconductor Substances 0.000 title claims description 15
- 238000004519 manufacturing process Methods 0.000 title claims description 8
- 241000954177 Bangana ariza Species 0.000 claims description 7
- 229910052775 Thulium Inorganic materials 0.000 claims description 5
- 229910052761 rare earth metal Inorganic materials 0.000 claims description 5
- 229910052727 yttrium Inorganic materials 0.000 claims description 5
- VWQVUPCCIRVNHF-UHFFFAOYSA-N yttrium atom Chemical group [Y] VWQVUPCCIRVNHF-UHFFFAOYSA-N 0.000 claims description 5
- 229910052692 Dysprosium Inorganic materials 0.000 claims description 4
- 229910052691 Erbium Inorganic materials 0.000 claims description 4
- 229910052693 Europium Inorganic materials 0.000 claims description 4
- 229910052688 Gadolinium Inorganic materials 0.000 claims description 4
- 229910052779 Neodymium Inorganic materials 0.000 claims description 4
- 229910052772 Samarium Inorganic materials 0.000 claims description 4
- 229910052769 Ytterbium Inorganic materials 0.000 claims description 4
- KBQHZAAAGSGFKK-UHFFFAOYSA-N dysprosium atom Chemical compound [Dy] KBQHZAAAGSGFKK-UHFFFAOYSA-N 0.000 claims description 4
- UYAHIZSMUZPPFV-UHFFFAOYSA-N erbium Chemical compound [Er] UYAHIZSMUZPPFV-UHFFFAOYSA-N 0.000 claims description 4
- OGPBJKLSAFTDLK-UHFFFAOYSA-N europium atom Chemical compound [Eu] OGPBJKLSAFTDLK-UHFFFAOYSA-N 0.000 claims description 4
- UIWYJDYFSGRHKR-UHFFFAOYSA-N gadolinium atom Chemical compound [Gd] UIWYJDYFSGRHKR-UHFFFAOYSA-N 0.000 claims description 4
- 229910052746 lanthanum Inorganic materials 0.000 claims description 4
- FZLIPJUXYLNCLC-UHFFFAOYSA-N lanthanum atom Chemical compound [La] FZLIPJUXYLNCLC-UHFFFAOYSA-N 0.000 claims description 4
- QEFYFXOXNSNQGX-UHFFFAOYSA-N neodymium atom Chemical compound [Nd] QEFYFXOXNSNQGX-UHFFFAOYSA-N 0.000 claims description 4
- KZUNJOHGWZRPMI-UHFFFAOYSA-N samarium atom Chemical compound [Sm] KZUNJOHGWZRPMI-UHFFFAOYSA-N 0.000 claims description 4
- NAWDYIZEMPQZHO-UHFFFAOYSA-N ytterbium Chemical compound [Yb] NAWDYIZEMPQZHO-UHFFFAOYSA-N 0.000 claims description 4
- 229910052689 Holmium Inorganic materials 0.000 claims description 3
- 229910052765 Lutetium Inorganic materials 0.000 claims description 3
- KJZYNXUDTRRSPN-UHFFFAOYSA-N holmium atom Chemical compound [Ho] KJZYNXUDTRRSPN-UHFFFAOYSA-N 0.000 claims description 3
- OHSVLFRHMCKCQY-UHFFFAOYSA-N lutetium atom Chemical compound [Lu] OHSVLFRHMCKCQY-UHFFFAOYSA-N 0.000 claims description 3
- 238000000354 decomposition reaction Methods 0.000 claims description 2
- 238000002844 melting Methods 0.000 claims description 2
- 230000008018 melting Effects 0.000 claims description 2
- 238000010304 firing Methods 0.000 claims 1
- 238000010438 heat treatment Methods 0.000 claims 1
- 239000000843 powder Substances 0.000 description 14
- 239000000463 material Substances 0.000 description 10
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 8
- 238000000034 method Methods 0.000 description 8
- 239000001301 oxygen Substances 0.000 description 8
- 229910052760 oxygen Inorganic materials 0.000 description 8
- QPLDLSVMHZLSFG-UHFFFAOYSA-N Copper oxide Chemical compound [Cu]=O QPLDLSVMHZLSFG-UHFFFAOYSA-N 0.000 description 6
- AYJRCSIUFZENHW-UHFFFAOYSA-L barium carbonate Chemical compound [Ba+2].[O-]C([O-])=O AYJRCSIUFZENHW-UHFFFAOYSA-L 0.000 description 6
- 239000007791 liquid phase Substances 0.000 description 6
- 229910052573 porcelain Inorganic materials 0.000 description 6
- 238000001354 calcination Methods 0.000 description 4
- 239000013078 crystal Substances 0.000 description 4
- 239000012071 phase Substances 0.000 description 4
- 238000000634 powder X-ray diffraction Methods 0.000 description 4
- 238000005245 sintering Methods 0.000 description 4
- 229960004643 cupric oxide Drugs 0.000 description 3
- 238000003825 pressing Methods 0.000 description 3
- 239000007858 starting material Substances 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- CURLTUGMZLYLDI-UHFFFAOYSA-N Carbon dioxide Chemical compound O=C=O CURLTUGMZLYLDI-UHFFFAOYSA-N 0.000 description 2
- -1 Carbon ions Chemical class 0.000 description 2
- 229910009203 Y-Ba-Cu-O Inorganic materials 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 230000002950 deficient Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 229910052758 niobium Inorganic materials 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- 230000005668 Josephson effect Effects 0.000 description 1
- 238000002441 X-ray diffraction Methods 0.000 description 1
- 241000981595 Zoysia japonica Species 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910001422 barium ion Inorganic materials 0.000 description 1
- 159000000009 barium salts Chemical class 0.000 description 1
- 238000009835 boiling Methods 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 229910002092 carbon dioxide Inorganic materials 0.000 description 1
- 239000001569 carbon dioxide Substances 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 239000007795 chemical reaction product Substances 0.000 description 1
- 238000000975 co-precipitation Methods 0.000 description 1
- 238000013329 compounding Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000004455 differential thermal analysis Methods 0.000 description 1
- 238000004108 freeze drying Methods 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 239000011261 inert gas Substances 0.000 description 1
- 229910000765 intermetallic Inorganic materials 0.000 description 1
- 229910052745 lead Inorganic materials 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 239000011812 mixed powder Substances 0.000 description 1
- 239000004570 mortar (masonry) Substances 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- SIWVEOZUMHYXCS-UHFFFAOYSA-N oxo(oxoyttriooxy)yttrium Chemical compound O=[Y]O[Y]=O SIWVEOZUMHYXCS-UHFFFAOYSA-N 0.000 description 1
- 125000004430 oxygen atom Chemical group O* 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 238000007493 shaping process Methods 0.000 description 1
- 238000003746 solid phase reaction Methods 0.000 description 1
- 230000007704 transition Effects 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
- Compositions Of Oxide Ceramics (AREA)
- Inorganic Compounds Of Heavy Metals (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は、各種の超伝導応用装置や超伝導素子に使用さ
れる酸化物超伝導材料に関するものである。Description: TECHNICAL FIELD The present invention relates to an oxide superconducting material used in various superconducting application devices and superconducting elements.
(従来の技術) 従来より超伝導材料としては例えばPb,Nb,Nb3Ge等の単
体金属、合金、金属間化合物が知られていた。超伝導材
料はジョセフソン素子などのエレクトロニクスデバイス
や超伝導磁石用のコイルなどを作るのに用いられ、特に
ジョセフソン接合の高感度性、高精度性、低雑音性を利
用したSQUIDや精密計測への応用ならびに交流ジョセフ
ソン効果の他、ジョセフソン接合の応答高速性と低消費
電力性に着目した電子計算機への応用が期待されてい
る。(Prior Art) Conventionally, as superconducting materials, for example, simple metals such as Pb, Nb, Nb 3 Ge, alloys, and intermetallic compounds have been known. Superconducting materials are used to make electronic devices such as Josephson devices and coils for superconducting magnets. In addition to the application of AC and the Josephson effect, it is expected to be applied to electronic computers that focus on the high-speed response and low power consumption of Josephson junctions.
ところで超伝導材料の超伝導転移温度Tcは、できるだけ
高いことが望まれる。従来からTcの高い材料としてはTc
が23.2KのNb3Geが知られていたが、最近ではLa−Ba−Cu
−O系のうち(La1-xBax)2CuO4で0.075≦x≦0.1の組
成のものがTcが30Kに、Y−Ba−Cu−O系のうちYBa2Cu3
Oyの組成のもののTcが90K前後をもつと相次いで報告さ
れている。さらにこのYBa2Cu3OyのYの位置を他の希土
類元素のうちランテン、ネオジミウム、サマリウム、ユ
ーロピウム、ガドリニウム、ジスプロシウム、ホロミウ
ム、エルビウム、ツリウム、イッテルビウム、ツリウム
に置き換えても、またこれらの元素が2種類以上混合さ
れていても、ほぼ同じ90K程度のTcをもつことも報告さ
れている。Y−Ba−Cu−O系を始めとするこれらの超伝
導体のTcは液体窒素の沸点(77K)よりも高くなったこ
とにより、実用材料としての期待が大きくなってきてい
る。By the way, it is desired that the superconducting transition temperature Tc of the superconducting material is as high as possible. As a material with a high Tc, Tc
Was known to be 23.2K Nb 3 Ge, but recently La-Ba-Cu
Among the --O system, (La 1-x Ba x ) 2 CuO 4 having a composition of 0.075 ≦ x ≦ 0.1 has a Tc of 30 K, and Y--Ba--Cu--O system YBa 2 Cu 3
It has been successively reported that the Tc of the composition of Oy has around 90K. Furthermore, even if the Y position of this YBa 2 Cu 3 O y is replaced with lanthanum, neodymium, samarium, europium, gadolinium, dysprosium, holmium, erbium, thulium, ytterbium, and thulium among other rare earth elements, these elements are also replaced. It is also reported that even if two or more kinds are mixed, they have almost the same Tc of about 90K. Since the Tc of these superconductors including the Y-Ba-Cu-O system has become higher than the boiling point (77K) of liquid nitrogen, expectations as a practical material are increasing.
Y−Ba−Cu−O系を始めとする酸素欠損型3層ペロブス
カイト構造をもつ超伝導体のTcは90Kと高い値を示す材
料であるが、通常の磁器製造方法では相対密度が高々90
%のものしか得られにくく、機械的にもろく、重要な特
性である臨界電流密度Jcも一般に低い。これは出発原料
として用いられる炭酸バリウム(BaCO3)の分解が不十
分のまま1000℃前後の温度で焼結を完了さざるを得ない
ことによる。すなわちBaCO3の分解を十分なほど温度を
上げると反応物である酸素欠損型3層ペロブスカイト構
造が分解し、異相が生成するためである。最近では、出
発原料として炭酸バリウム以外のバリウム塩を用いる試
みや通常の磁器製造方法以外の共沈法、凍結乾燥法を適
用する試みがなされているが、いずれの場合も反応途中
で空気中の炭酸ガス(CO2)や混合粉中に含まれる炭素
分とむすびついてBaイオンが炭酸バリウム(BaCO3)と
なり前述したと同じ結果となる。さらにREBa2Cu3Oyなる
組成式で表される超伝導体組成物の焼結体の臨界電流密
度Jcは一般に低い。これはREBa2Cu3Oyなる組成物の結晶
構造が斜方晶であるため超伝導特性が異方性をもってい
ることに起因する。即ち、焼結体を構成する一つ一つの
結晶粒は単結晶に近いものであっても、焼結体は多結晶
体であるため全体として超伝導特性は平均化されてしま
うことによる。ところが従来の組成物や従来の製造方法
では、超伝導電流を流しやすい方向に配向した粉体を作
成することや配向した粉体の方向をそろえて焼結させる
ことは困難であった。The Tc of superconductors having an oxygen-deficient three-layer perovskite structure such as the Y-Ba-Cu-O system is a material showing a high value of 90K, but the relative density is 90 at most in the ordinary porcelain manufacturing method.
%, It is mechanically brittle, and the critical current density Jc, which is an important characteristic, is generally low. This is because the sintering of barium carbonate (BaCO 3 ) used as a starting material has to be completed at a temperature of around 1000 ° C while the decomposition of barium carbonate (BaCO 3 ) is insufficient. That is, when the temperature of BaCO 3 is sufficiently raised to decompose, the oxygen deficient three-layer perovskite structure, which is a reaction product, is decomposed and a different phase is generated. Recently, attempts have been made to use a barium salt other than barium carbonate as a starting material, a coprecipitation method other than the usual porcelain manufacturing method, and an attempt to apply a freeze-drying method. Carbon ions contained in carbon dioxide (CO 2 ) and mixed powder are bound together, and Ba ions become barium carbonate (BaCO 3 ) with the same result as described above. Furthermore, the critical current density Jc of the sintered body of the superconductor composition represented by the composition formula REBa 2 Cu 3 O y is generally low. This is because the composition of REBa 2 Cu 3 O y has an orthorhombic crystal structure and therefore has an anisotropic superconducting property. That is, even if each of the crystal grains forming the sintered body is close to a single crystal, since the sintered body is a polycrystalline body, the superconducting properties are averaged as a whole. However, with the conventional composition and the conventional manufacturing method, it has been difficult to prepare a powder oriented in a direction in which a superconducting current easily flows or to sinter the oriented powder in the same direction.
(発明が解決しようとする問題点) REBa2Cu3Oyなる組成式で表される超伝導体組成物の焼結
体において未反応物が残る問題、低温で焼結できない問
題、配向した粉体を作成できない問題、配向した粉体の
方向をそろえて焼結できない問題があった。(Problems to be solved by the invention) REBa 2 Cu 3 O y The problem that unreacted substances remain in the sintered body of the superconductor composition represented by the composition formula, the problem that it cannot be sintered at low temperature, the oriented powder There was a problem that a body could not be created and a problem that the oriented powder could not be aligned and sintered.
本発明は従来の組成物や従来の磁器組成物の製造方法で
は解決できなかった未反応物が残る問題、低温で焼結で
きない問題、配向した粉体を作成できない問題、配向し
た粉体の方向をそろえて焼結できない問題を解決する超
伝導体組成物とその製造方法を提供することにある。INDUSTRIAL APPLICABILITY The present invention is a problem that unreacted substances remain that cannot be solved by the conventional composition or the conventional method for producing a porcelain composition, a problem that sintering at low temperature is not possible, a problem that oriented powder cannot be produced, and a direction of oriented powder An object of the present invention is to provide a superconductor composition and a method for producing the same, which solves the problem that sintering is not possible.
(問題点を解決するための手段) 本発明は酸化物超伝導体組成物、特に従来のREBa2Cu3Oy
なる組成物とは異なるREBa2Cu3+xOyなる組成式で0.03≦
x≦0.3の範囲にCuの化学量論比からのずれがある酸化
物超伝導体組成物において、未反応物が残らず、低温で
焼結ができ、配向した粉体が得られ、配向した粉体の方
向をそろえた焼結体の製造方法を見いだしたものであ
る。(Means for Solving the Problems) The present invention relates to an oxide superconductor composition, particularly a conventional REBa 2 Cu 3 O y.
REBa 2 Cu 3 + x O y with a composition formula of 0.03 ≦
In the oxide superconductor composition where there is a deviation from the stoichiometric ratio of Cu in the range of x ≦ 0.3, there is no unreacted material, sintering is possible at low temperature, and an oriented powder is obtained and oriented. The inventors have found a method for producing a sintered body in which the directions of the powder are aligned.
例えばYBa2Cu3+xOyなる組成式でx=0,0.015,0.03,0.0
9,0.30,0.35である組成物を通常の磁器製造方法にて合
成した。このとき、空気中900℃で12時間仮焼を行い、
さらに酸素1気圧中980℃で4時間仮焼を行ったところ
xの大きい0.03以上のものについては一部溶融が起こっ
た。これらを再粉砕し、加圧成形を行ったところxが0.
03以上の組成物について加圧方向に対して平行に結晶構
造でいうところのC軸がそろい、粉末X線回折法により
配向した粉末が得られていることが確認された。For example, in the composition formula YBa 2 Cu 3 + x O y , x = 0,0.015,0.03,0.0
Compositions of 9,0.30 and 0.35 were synthesized by a usual porcelain manufacturing method. At this time, calcining in air at 900 ° C for 12 hours,
Furthermore, when calcination was performed at 980 ° C. for 4 hours in one atmosphere of oxygen, some of 0.03 or more having large x melted. When these were re-ground and pressure-molded, x was 0.
It was confirmed that powders having the C-axis, which is the crystal structure, were aligned in parallel with the pressing direction for the compositions of 03 and above, and the powder was oriented by the powder X-ray diffraction method.
以下、本発明を実施例によりさらに詳細に説明する。Hereinafter, the present invention will be described in more detail with reference to Examples.
(実施例) 出発原料として純度99.9%以上の酸化イットリウム(Y2
O3)、炭酸バリウム(BaCO3)、酸化第二銅(CuO)を使
用し配合比がモル比で1:2:3+xとなるように各々秤量
する。ここでxは0,0.015,0.03,0.09,0.30,0.35とし
た。つぎに秤量した各材料をボールミルにて湿式混合し
た後、空気中900℃で12時間仮焼しライカイを行い、引
続き酸素中980℃で4時間再び仮焼を行った。このとき
xが0.03以上の組成物において一部液相が現れた。この
ことを確かめるためにこれらの組成物について酸素中に
て室温から1100℃まで示差熱分析を行ったところxが0.
03以上の組成物で特に明瞭に980℃付近に吸熱反応があ
ることが確認された。この液相が介在することにより固
相反応が促進され密度が向上し機械的強度が増加するこ
とが期待される。2回仮焼を行った粉末を乳鉢にて粉砕
し、さらにボールミルにて再粉砕を行い、整粒後、1ton
/cm2の圧力で加圧整形を行った。この成形体の加圧方向
に対して垂直な面を粉末X線回折法を用いて調べたとこ
ろ、xが0.03以上の組成物で粉体が加圧方向に対して平
行にC軸がそろっていることが確認された。このC軸配
向の程度を定量化するために粉末X線回折図において
(006)と(200)の2本の回折線のX線強度比を比較し
た。これらの結果は第1図に示すように、x=0の組成
物では(006)回折線と(200)回折線の強度比が2程度
であったものがx=0.09の組成物で最大となり強度比は
約32倍となった。さらに、これらの組成物粉体の成形体
を酸素中980℃にて焼結を行ったところX線回折線の強
度比は変わらず配向した焼結体を得ることができた。第
1表にこれらの組成物の焼結体の寸法密度と回折X線の
強度比から求めた不純物相の割合と交流帯磁率から求め
た4.2Kにおける超伝導体相の体積割合を示す。寸法密度
もxの増加に従い若干増加していることになる。このよ
うにCuの増加分xが0.03以上で一部分解した液相が介在
する温度以上で熱処理を行うことにより密度の向上とC
軸配向する粉体と焼結体が得られることになる。逆にx
が0.30をこえれば実効的な超伝導体相が減少することは
明白であり配向の程度もxが0.35になるまで単調に減少
していることから実用的ではない。(Example) As a starting material, yttrium oxide (Y 2
O 3 ), barium carbonate (BaCO 3 ), and cupric oxide (CuO) are used and weighed so that the compounding ratio is 1: 2: 3 + x in molar ratio. Here, x was set to 0,0.015,0.03,0.09,0.30,0.35. Next, the weighed materials were wet-mixed by a ball mill, calcined in air at 900 ° C. for 12 hours to perform re-calcination, and subsequently, calcined again in oxygen at 980 ° C. for 4 hours. At this time, a liquid phase partially appeared in the composition in which x was 0.03 or more. To confirm this, differential thermal analysis was performed on these compositions in oxygen from room temperature to 1100 ° C., where x was 0.
It was confirmed that the compositions of 03 and above had an endothermic reaction at around 980 ° C particularly clearly. It is expected that the presence of this liquid phase promotes the solid phase reaction to improve the density and increase the mechanical strength. The powder that has been calcined twice is crushed in a mortar and then re-crushed in a ball mill to adjust the particle size to 1 ton.
Pressure shaping was performed at a pressure of / cm 2 . The surface of this molded body which was perpendicular to the pressing direction was examined by powder X-ray diffractometry. As a result, x was 0.03 or more and the powder was C-axis parallel to the pressing direction. Was confirmed. In order to quantify the degree of this C-axis orientation, the X-ray intensity ratios of the two diffraction lines (006) and (200) were compared in the powder X-ray diffraction diagram. As shown in FIG. 1, these results show that the intensity ratio of the (006) diffraction line and the (200) diffraction line was about 2 in the composition of x = 0, but became maximum in the composition of x = 0.09. The intensity ratio was about 32 times. Furthermore, when a molded body of these composition powders was sintered in oxygen at 980 ° C., an oriented sintered body could be obtained without changing the intensity ratio of X-ray diffraction lines. Table 1 shows the proportion of the impurity phase obtained from the dimensional density of the sintered bodies of these compositions and the intensity ratio of the diffracted X-rays, and the volume proportion of the superconductor phase at 4.2K obtained from the AC susceptibility. The dimensional density also slightly increases as x increases. In this way, by increasing the density x and the C
An axially oriented powder and a sintered body will be obtained. Conversely x
Is more than 0.30, the effective superconductor phase is obviously decreased, and the degree of orientation is monotonically decreased until x becomes 0.35, which is not practical.
この液相が出現する温度は仮焼を行う際の雰囲気酸素分
圧により変化する。たとえば酸素分圧が0.21気圧、即ち
空気中であれば約960℃となるため、この液相が出現す
る温度は熱力学的に決められる。さらに希土類元素がイ
ットリウム以外の元素についてはこの液相が出現する温
度は変化するため一義的には定めることはできない。し
かしなから、液相を一部介在させれば前述の結果は得ら
れることは明白である。 The temperature at which this liquid phase appears varies depending on the atmospheric oxygen partial pressure during calcination. For example, the oxygen partial pressure is 0.21 atm, that is, about 960 ° C. in air, so the temperature at which this liquid phase appears is thermodynamically determined. Further, for the rare earth elements other than yttrium, the temperature at which this liquid phase appears changes and cannot be uniquely determined. However, it is clear that the above result can be obtained by interposing a part of the liquid phase.
実施例ではイットリウムの例を示したが、他の希土類元
素であるランタン、ネオジミウム、サマリウム、ユーロ
ピウム、ガドリニウム、ジスプロシウム、ホロシウム、
エルビウム、ツリウム、イッテルビウム、ルテチウムな
どでも、イットリウムと同等の効果を示した。またこれ
らを2種類以上を含んでもよい。組成式あたりの酸素原
子数は7.1から6.3までの範囲、さらに好適には6.95から
6.3までの範囲である。Although the example of yttrium is shown in the examples, other rare earth elements such as lanthanum, neodymium, samarium, europium, gadolinium, dysprosium, holosium,
Erbium, thulium, ytterbium, and lutetium also showed the same effect as yttrium. Moreover, you may include 2 or more types of these. The number of oxygen atoms per composition formula is in the range of 7.1 to 6.3, more preferably 6.95.
The range is up to 6.3.
これは不活性ガス融解法やヨードメトリー法で測定し
た。This was measured by an inert gas melting method or an iodometry method.
(発明の効果) 実施例からも明らかなように、本発明によれば従来材料
にくらべ高度に配向した磁器を比較的低温で得ることが
でき、印刷法による厚膜配線やグリーンシート法を適用
した超伝導デバイスに応用が期待されるものである。(Effects of the Invention) As is clear from the examples, according to the present invention, highly oriented porcelain can be obtained at a relatively low temperature as compared with the conventional material, and thick film wiring by the printing method or the green sheet method is applied. It is expected to be applied to the superconducting devices mentioned above.
第1図は、本発明の実施例による磁器組成物の粉末X線
回折法による配向の程度を示す図。FIG. 1 is a diagram showing the degree of orientation of a porcelain composition according to an example of the present invention by a powder X-ray diffraction method.
フロントページの続き (72)発明者 内海 和明 東京都港区芝5丁目33番1号 日本電気株 式会社内 (56)参考文献 特開 昭64−9856(JP,A) 特開 昭64−45020(JP,A)Front page continued (72) Inventor Kazuaki Utsumi 5-33-1 Shiba, Minato-ku, Tokyo Inside NEC Corporation (56) References JP 64-9856 (JP, A) JP 64-64 45020 (JP, A)
Claims (2)
導体組成物において、希土類元素REがイットリウム、ラ
ンタン、ネオジミウム、サマリウム、ユーロピウム、ガ
ドリニウム、ジスプロシウム、ホロミウム、エルビウ
ム、ツリウム、イッテルビウム、ルテチウムの1種類ま
たは2種以上であり、Cuの化学量論比からのずれxが0.
03≦x≦0.3、yが6.3≦y≦7.1の範囲にあることを特
徴とする酸化物超伝導体組成物。1. An oxide superconductor composition represented by the composition formula REBa 2 Cu 3 + x O y , wherein the rare earth element RE is yttrium, lanthanum, neodymium, samarium, europium, gadolinium, dysprosium, holmium, erbium, One or more of thulium, ytterbium, and lutetium, and the deviation x from the stoichiometric ratio of Cu is 0.
An oxide superconductor composition, wherein 03 ≦ x ≦ 0.3 and y are in the range of 6.3 ≦ y ≦ 7.1.
導体組成物において、希土類元素REがイットリウム、ラ
ンタン、ネオジミウム、サマリウム、ユーロピウム、ガ
ドリニウム、ジスプロシウム、ホロミウム、エルビウ
ム、ツリウム、イッテルビウム、ルテチウムの1種類ま
たは2種以上であり、Cuの化学量論比からのずれxが0.
03≦x≦0.3、yが6.3≦y≦7.1の範囲にある酸化物超
伝導体組成物の一部溶融分解温度以上の熱処理を少なく
とも1回以上行なったのち該組成物を粉砕、加圧成形、
焼成することを特徴とする酸化物超伝導体組成物の製造
方法。2. In an oxide superconductor composition represented by the composition formula REBa 2 Cu 3 + x O y , the rare earth element RE is yttrium, lanthanum, neodymium, samarium, europium, gadolinium, dysprosium, holmium, erbium, One or more of thulium, ytterbium, and lutetium, and the deviation x from the stoichiometric ratio of Cu is 0.
03 ≦ x ≦ 0.3 and y is in the range of 6.3 ≦ y ≦ 7.1 After at least one heat treatment at a partial melting decomposition temperature or higher of the oxide superconductor composition, the composition is crushed and pressure-molded. ,
A method for producing an oxide superconductor composition, which comprises firing.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62331736A JPH0764620B2 (en) | 1987-12-25 | 1987-12-25 | Oxide superconductor composition and method for producing the same |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62331736A JPH0764620B2 (en) | 1987-12-25 | 1987-12-25 | Oxide superconductor composition and method for producing the same |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01172261A JPH01172261A (en) | 1989-07-07 |
| JPH0764620B2 true JPH0764620B2 (en) | 1995-07-12 |
Family
ID=18247032
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62331736A Expired - Lifetime JPH0764620B2 (en) | 1987-12-25 | 1987-12-25 | Oxide superconductor composition and method for producing the same |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0764620B2 (en) |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62200933A (en) * | 1986-02-28 | 1987-09-04 | Fujitsu Ltd | Pcm multiplex block |
| JPS649856A (en) * | 1987-07-03 | 1989-01-13 | Fumihiko Takei | Oxide superconductor crystals and their production |
| JPS6445020A (en) * | 1987-08-13 | 1989-02-17 | Univ Tokai | Manufacture of superconductive material |
-
1987
- 1987-12-25 JP JP62331736A patent/JPH0764620B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01172261A (en) | 1989-07-07 |
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