JPH0597432A - Superconductor - Google Patents

Superconductor

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Publication number
JPH0597432A
JPH0597432A JP3256763A JP25676391A JPH0597432A JP H0597432 A JPH0597432 A JP H0597432A JP 3256763 A JP3256763 A JP 3256763A JP 25676391 A JP25676391 A JP 25676391A JP H0597432 A JPH0597432 A JP H0597432A
Authority
JP
Japan
Prior art keywords
superconductor
hours
temperature
mixed
partial pressure
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
Application number
JP3256763A
Other languages
Japanese (ja)
Inventor
Hitoshi Nobumasa
均 信正
Kazuharu Shimizu
一治 清水
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toray Industries Inc
Original Assignee
Toray Industries Inc
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Toray Industries Inc filed Critical Toray Industries Inc
Priority to JP3256763A priority Critical patent/JPH0597432A/en
Publication of JPH0597432A publication Critical patent/JPH0597432A/en
Pending legal-status Critical Current

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Classifications

    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

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  • Superconductor Devices And Manufacturing Methods Thereof (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)
  • Compositions Of Oxide Ceramics (AREA)
  • Inorganic Compounds Of Heavy Metals (AREA)

Abstract

(57)【要約】 【目的】高酸素分圧中におけるHIP処理温度が低くて
も、従来のものと同等の超電導特性をもつLa(212
6)系超電導体を提供する。 【構成】一般式、(La1−ηBaη2−θ(Ca
1−γMgγ1+θCuδ ただし、 0≦η<0.2 0≦θ<0.3 0<γ≦0.4 5.9<δ<6.1 か、 (La1−αSrα2−βCa1+βCu2−ξLi
ξζ ただし、 0≦α<0.3 0≦β<0.3 0<ξ≦0.3 5.9<ζ<6.1 で表わされる超電導体。
(57) [Abstract] [Purpose] La (212) has superconducting properties equivalent to those of conventional ones even when the HIP treatment temperature in high oxygen partial pressure is low.
6) Providing a system superconductor. [Structure] General formula, (La 1-η Ba η ) 2-θ (Ca
1-γ Mg γ ) 1 + θ Cu 2 O δ , where 0 ≦ η <0.2 0 ≦ θ <0.3 0 <γ ≦ 0.4 5.9 <δ <6.1 or (La 1-α Sr α ) 2- βCa1 + βCuCu2 -ξLi
ξ O ζ However, a superconductor represented by 0 ≦ α <0.3 0 ≦ β <0.3 0 <ξ ≦ 0.3 5.9 <ζ <6.1.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は、核融合炉、電磁流体
発電機、加速器、回転電気機器(電動機、発電機等)、
磁気分離機、磁気浮上列車、核磁気共鳴測定装置、磁気
推進船、電子線露光装置、各種実験装置等のマグネット
コイル材料として適し、また、送電線、電気エネルギー
貯蔵器、変圧器、整流器、調相器等の電力損失が問題に
なる用途に適し、さらに、ジョセフソン素子、SQUI
D素子、超電導トランジスタ等の素子として適し、さら
にまた、赤外線探知材料、磁気遮蔽材料等の機能材料と
して適した超電導体に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a nuclear fusion reactor, a magnetohydrodynamic generator, an accelerator, a rotating electric machine (motor, generator, etc.),
Suitable as a magnetic coil material for magnetic separators, magnetic levitation trains, nuclear magnetic resonance measurement equipment, magnetic propulsion vessels, electron beam exposure equipment, various experimental equipment, transmission lines, electric energy storage, transformers, rectifiers, regulators, etc. Suitable for applications where power loss is a problem such as phaser, Josephson device, SQUI
The present invention relates to a superconductor suitable as an element such as a D element and a superconducting transistor, and further as a functional material such as an infrared detection material and a magnetic shielding material.

【0002】[0002]

【従来の技術】超電導転移温度の高い超電導体として、
よく知られている一連の銅複合酸化物系超電導体があ
る。これらの銅複合酸化物系超電導体と構造が類似する
銅複合酸化物、すなわち、単位格子中に、主としてCa
からなる層を挟んで底面を対向させたCuとOとからな
る2つのピラミッド構造を含み、これらピラミッド構
造、主としてCa、ピラミッド構造からなる層がLa
を介して積み重なった構造の、いわゆるLa(21
26)系銅複合酸化物は、結晶構造の類似性から超電導
になることが予想され、多くの研究がなされている。そ
して、(La1−xSrCaCuなるもの
で、Tczeroが40〜50Kの超電導特性が確認されて
いる(“Nature”、第345巻、第602〜60
4頁、1990年)。しかしながら、この超電導体は、
難取り扱い性の原料を使用する必要があるうえにガラス
アンビル中に封じ込めて焼結せねばならず、製造がやっ
かいであるばかりか、大型のものや長尺のものの製造に
は適さない。その後、La2−xCa1+xCu
において、空気中や1気圧の酸素中で焼結したものを高
酸素分圧中でHIP(Hot Isostatic Press )処理する
と超電導化できることが判明したが、この組成のもの
は、HIP処理温度を1200℃前後まで上げなければ
ならず、しかも、この温度は融点に近いために微妙な温
度制御が必要で、工業的ではない。
2. Description of the Related Art As a superconductor having a high superconducting transition temperature,
There is a series of well known copper complex oxide based superconductors. A copper composite oxide having a structure similar to those of these copper composite oxide superconductors, that is, in the unit cell, mainly Ca
It includes two pyramid structures composed of Cu and O, the bottom surfaces of which are opposed to each other with a layer made of La, and a layer composed of these pyramid structures, mainly Ca and the pyramid structure is La 2
Of O 2 through the stacked structure, so-called La (21
The 26) -based copper composite oxide is expected to become superconducting due to the similarity in crystal structure, and many studies have been conducted. Then, superconducting properties of (La 1-x Sr x ) 2 CaCu 2 O y with Tc zero of 40 to 50 K have been confirmed (“Nature”, Volume 345, Volumes 602 to 60).
4 pages, 1990). However, this superconductor
Not only is it difficult to manufacture, but it is not suitable for the production of large or long products, because it requires the use of difficult-to-handle raw materials and must be contained in a glass anvil and sintered. Then, La 2-x Ca 1 + x Cu 2 O y
In the above, it was found that HIP (Hot Isostatic Press) treatment of a product sintered in air or oxygen of 1 atm in a high oxygen partial pressure makes it superconducting, but this composition has a HIP treatment temperature of 1200 ° C. It has to be raised to the front and back, and since this temperature is close to the melting point, delicate temperature control is required, which is not industrial.

【0003】[0003]

【発明が解決しようとする課題】この発明の目的は、従
来の、いわゆるLa(2126)系超電導体の上述した
問題点を解決し、高酸素分圧中におけるHIP処理温度
が低くても従来のものと同等の超電導特性を得ることが
できるLa(2126)系超電導体を提供するにある。
SUMMARY OF THE INVENTION An object of the present invention is to solve the above-mentioned problems of the conventional so-called La (2126) type superconductor, and to solve the conventional problems even when the HIP treatment temperature is high during high oxygen partial pressure. Another object of the present invention is to provide a La (2126) -based superconductor capable of obtaining superconducting properties equivalent to those of the above.

【0004】[0004]

【課題を解決するための手段】上記目的を達成するため
に、この発明は、下記一般式で表される超電導体を提供
する(以下、これを第1発明という。)。
In order to achieve the above object, the present invention provides a superconductor represented by the following general formula (hereinafter referred to as the first invention).

【0005】 (La1−ηBaη2−θ(Ca1−γMgγ1+θCuδ ただし、 0≦η<0.2 0≦θ<0.3 0<γ≦0.4 5.9<δ<6.1 また、この発明は、下記一般式で表される超電導体を提
供する(以下、これを第2発明という。)。
(La 1-η Ba η ) 2-θ (Ca 1-γ Mg γ ) 1 + θ Cu 2 O δ However, 0 ≦ η <0.2 0 ≦ θ <0.3 0 <γ ≦ 0.4 5.9 <δ <6.1 The present invention also provides a superconductor represented by the following general formula (hereinafter referred to as the second invention).

【0006】 (La1−αSrα2−βCa1+βCu2−ξLiξζ ただし、 0≦α<0.3 0≦β<0.3 0<ξ≦0.3 5.9<ζ<6.1 この発明の超電導体は、構造的には、単位格子中に、C
uまたはこれと置換したLiの周りにOが5配位したピ
ラミッド構造を2ユニット含んでいる。また、これらC
uまたはLiとOとからなるピラミッド型ユニットは、
主としてアルカリ土類元素であるCaやMgを挟んで底
面を対向させた配置になっている。さらに、各単位格子
は、c軸方向(ピラミッド型の底面に垂直な方向)に、
ピラミッド型の頂点に位置するOと、Laまたはこれと
置換したSrやBaとで岩塩構造を形成しながら積み重
なっている。また、この結晶構造の単一相は、Laまた
はこれと置換したSrやBaと、アルカリ土類元素であ
るCaやMgと、CuまたはLiの比がある範囲内にあ
るときにのみ得られる。すなわち、第1発明と第2発明
における一般式において、θやβが上述した範囲から外
れると、結晶構造が別の結晶系になったり、他の不純物
相(絶縁体)が多く混在するようになる。
(La 1-α Sr α ) 2-β Ca 1 + β Cu 2-ξ Li ξ O ζ where 0 ≦ α <0.3 0 ≦ β <0.3 0 <ξ ≦ 0.3 5.9 <Ζ <6.1 The structure of the superconductor of the present invention is C in the unit cell.
It contains two units of a pyramid structure in which O is five-coordinated around u or Li substituted with u. Also, these C
The pyramid type unit consisting of u or Li and O is
The arrangement is such that the bottom surfaces face each other with sandwiching mainly Ca or Mg which are alkaline earth elements. Furthermore, each unit cell is in the c-axis direction (direction perpendicular to the bottom surface of the pyramid type),
O located at the apex of the pyramid and La or Sr or Ba substituted with La are stacked while forming a rock salt structure. Further, the single phase of this crystal structure is obtained only when the ratio of La or Sr or Ba substituted with La to Ca or Mg that is an alkaline earth element and Cu or Li is within a certain range. That is, in the general formulas of the first invention and the second invention, if θ or β deviates from the above-mentioned range, the crystal structure may become a different crystal system, or other impurity phases (insulators) may be mixed. Become.

【0007】この発明の超電導体においては、超電導電
荷担体は正孔で与えられ、従来の正孔型銅複合酸化物系
超電導体と同じく、正孔濃度がCu1個あたり0.01
以上、0.25以下の時にのみ超電導体となる。そうし
て、正孔濃度は、第1発明の場合は−6+0.5θ+η
−0.5×η×θ+δ、第2発明の場合は(−12+β
+2α−α×β+ξ+2ζ)/(2−ξ)で与えられる
から、第1発明の場合は2.01<−4+0.5θ+η
−0.5×η×θ+δ<2.25でなければならず、第
2発明の場合は2.01<(−8+β+2α−α×β−
ξ+2ζ)/(2−ξ)<2.25でなければならない
ことになる。
In the superconductor of the present invention, the superconducting charge carrier is given by holes, and the hole concentration is 0.01 per Cu, as in the conventional hole-type copper complex oxide superconductor.
As described above, it becomes a superconductor only when it is 0.25 or less. Then, the hole concentration is −6 + 0.5θ + η in the case of the first invention.
−0.5 × η × θ + δ, in the case of the second invention (-12 + β
+ 2α−α × β + ξ + 2ζ) / (2-ξ), so in the case of the first invention, 2.01 <−4 + 0.5θ + η
−0.5 × η × θ + δ <2.25, and 2.01 <(− 8 + β + 2α−α × β− in the case of the second invention.
ξ + 2ζ) / (2-ξ) <2.25.

【0008】構造が理想的に実現されたとき、第1発明
の超電導体は(La1−ηBaη(Ca1−γMg
γCuとなり、第2発明の超電導体は(La
1− αSrαCaCu2−ξLiξとなる
が、通常は酸素の過不足があるため、第1発明の場合は
(La1−ηBaη)2−θ(Ca1−γMgγ1+
θCuδ、第2発明の場合は(La1−αSrα
2−βCa1+βCu −ξLiξζという、一般式
において5.9<δ<6.1や5.9<ζ<6.1とい
う組成範囲が許される。また、上述した岩塩構造におけ
る、Laまたはこれと置換したSrやBaの位置の元素
と、CuまたはLiとOとからなるピラミッド型ユニッ
トの対向する底面間に挟まれたCaやMgの位置の元素
とは若干の入れ代わりがあり、特に、CaやMgの位置
に入るべき元素の一部がLaまたはこれと置換したSr
やBaの位置に入ったほうが構造が安定になる。そのた
め、第1発明においては0≦θ<0.3、第2発明にお
いては0≦β<0.3という制限が加わる。さらに、第
1発明においては、BaやMgの固溶限界から0≦η<
0.2や0<γ≦0.4という制限が加わり、第2発明
においては、SrやLiの固溶限界から0≦α<0.3
や0<ξ≦0.3という制限が加わる。
When the structure is ideally realized, the superconductor of the first invention is (La 1-η Ba η ) 2 (Ca 1-γ Mg
γ ) 1 Cu 2 O 6 , and the superconductor of the second invention is (La
1- α Sr α ) 2 Ca 1 Cu 2-ξ Li ξ O 6 , but normally there is an excess or deficiency of oxygen, so in the case of the first invention, (La 1-η Ba η) 2-θ (Ca 1-γ Mg γ ) 1+
θ Cu 2 O δ , in the case of the second invention (La 1-α Sr α )
A composition range of 5.9 <δ <6.1 or 5.9 <ζ <6.1 in the general formula of 2-β Ca 1 + β Cu 2 −ξ Li ξ O ζ is allowed. Further, in the rock salt structure described above, the element at the position of La or Sr or Ba substituted with La and the element at the position of Ca or Mg sandwiched between the opposed bottom surfaces of the pyramid-shaped unit made of Cu or Li and O. There is a slight replacement with, and in particular, some of the elements that should enter the positions of Ca and Mg are La or Sr in which it is substituted.
The structure becomes more stable when entering the position of or Ba. Therefore, 0 ≦ θ <0.3 is imposed in the first invention, and 0 ≦ β <0.3 is imposed in the second invention. Further, in the first invention, 0 ≦ η <from the solid solution limit of Ba or Mg.
0.2 and 0 <γ ≦ 0.4 are added, and in the second invention, 0 ≦ α <0.3 from the solid solution limit of Sr and Li.
And the restriction of 0 <ξ ≦ 0.3 is added.

【0009】さて、この発明の超電導体においては、O
の量を制御して注入する正孔濃度を調整するために、高
酸素分圧中でHIP処理を施す。通常のLa2−xCa
1+ Cuでは、その融点ぎりぎりの温度、すな
わち、1200℃前後の高温で熱処理しなければ酸素が
取り込まれにくく、超電導電荷担体が注入できないため
に十分な超電導転移温度が得られないが、第1、第2発
明では、3価のLaを2価のBaで置換したり、3価の
Laを2価のSrで置換したり、2価のCuを1価のL
iで置換し、また、これらの置換とさらにMgによるC
aの置換によって原子のパッキング状態を変え、Oを取
り込みやすくしてあるために、1100℃以下でのHI
P処理によっても、La2−xCa1+xCu
1200℃前後の温度でのHIP処理による場合と同程
度の超電導転移温度が得られ、HIP処理のサイクルを
早めることができ、また、HIP処理に要するエネルギ
ーを低減できる。
Now, in the superconductor of the present invention, O
HIP treatment is performed in a high oxygen partial pressure in order to control the amount of H 2 and adjust the concentration of holes to be injected. Normal La2 - xCa
In 1+ x Cu 2 O y , oxygen is not easily taken in unless heat treatment is performed at a temperature close to its melting point, that is, at a high temperature of about 1200 ° C., and a superconducting charge carrier cannot be injected, so that a sufficient superconducting transition temperature cannot be obtained. In the first and second inventions, trivalent La is substituted with divalent Ba, trivalent La is substituted with divalent Sr, and divalent Cu is monovalent L.
i, and these substitutions and additionally C by Mg
By substituting a, the packing state of atoms is changed to facilitate the incorporation of O.
Even with P treatment, a superconducting transition temperature of the same level as in the case of HIP treatment at a temperature of about 1200 ° C. of La 2−x Ca 1 + x Cu 2 O y can be obtained, and the cycle of HIP treatment can be accelerated, and The energy required for HIP processing can be reduced.

【0010】この発明の超電導体は、いろいろな方法に
よって製造することができる。たとえば、いわゆる粉末
混合法によることができる。この方法は、成分元素の酸
化物やその前駆体(炭酸塩、硝酸塩等)の粉末を所望の
割合で混合し、焼結温度以下の温度で焼成し、さらに粉
砕、混合し、所望の形状に成形し、酸素分圧が5気圧以
下の雰囲気中で焼結し、さらに酸素分圧10気圧以上の
雰囲気中でHIP処理して超電導体とする方法である。
The superconductor of the present invention can be manufactured by various methods. For example, a so-called powder mixing method can be used. In this method, powders of oxides of component elements and precursors thereof (carbonates, nitrates, etc.) are mixed at a desired ratio, fired at a temperature equal to or lower than the sintering temperature, further pulverized and mixed to obtain a desired shape. This is a method of forming, sintering in an atmosphere having an oxygen partial pressure of 5 atm or less, and further HIPing it in an atmosphere having an oxygen partial pressure of 10 atm or more to obtain a superconductor.

【0011】また、薄膜を形成する場合は、よく知られ
た、電子ビーム蒸着法、レーザー蒸着法等の各種蒸着法
によったり、マグネトロンスパッタ法等の各種スパッタ
法、ハロゲン化物や有機金属等を用いる化学的気相成長
法、硝酸塩や有機酸塩等を用いた霧化法、アルコキシド
等を用いた塗布法によることができる。
Further, when forming a thin film, well-known various vapor deposition methods such as electron beam vapor deposition method and laser vapor deposition method, various sputtering methods such as magnetron sputtering method, halides and organic metals are used. The chemical vapor deposition method used, the atomization method using a nitrate or an organic acid salt, or the coating method using an alkoxide or the like can be used.

【0012】そして、この発明の超電導体は、テープ
状、線状、繊維状、シート状等、いろいろな形態にして
用いることができる。また、炭素繊維や、セラミックス
や、銀等の金属からなる補強線材上に形成して用いるこ
ともできる。さらに、銀シース等の補強用中空材料に詰
め込んで使用することもできる。さらにまた、銅等のマ
トリクスを用いて多芯線構造の超電導線材とすることも
できる。また、Si、MgO、SrTiO、LaGa
、NdGaO等の基板上に薄膜として形成し、い
ろいろな素子や、LSIの配線用として用いることがで
きる。
The superconductor of the present invention can be used in various forms such as a tape form, a linear form, a fibrous form and a sheet form. It can also be used by forming it on a reinforcing wire made of carbon fiber, ceramics, or metal such as silver. Further, it can be used by being packed in a hollow reinforcing material such as a silver sheath. Furthermore, a superconducting wire having a multi-core wire structure can be formed by using a matrix of copper or the like. In addition, Si, MgO, SrTiO 3 , LaGa
It can be formed as a thin film on a substrate such as O 3 or NdGaO 3 and can be used for wiring various elements and LSI.

【0013】[0013]

【実施例1】La、BaCO、CaCO、M
gO、CuOの各粉末を、La:Ba:Ca:Mg:C
uが1.6:0.2:1.0:0.2:2.0になるよ
うに計りとり、メノウ乳鉢で混合した後、Al
容器に入れ、空気中にて950℃で12時間焼成した。
さらに、再びメノウ乳鉢で粉砕し、ペレット状に成形
し、空気中にて1000℃で24時間焼成した後、徐冷
した。
Example 1 La 2 O 3 , BaCO 3 , CaCO 3 , M
Each powder of gO and CuO was added to La: Ba: Ca: Mg: C.
u was measured to be 1.6: 0.2: 1.0: 0.2: 2.0, mixed in an agate mortar, put in an Al 2 O 3 container, and heated in air at 950 ° C. It was baked for 12 hours.
Further, it was ground again in an agate mortar, molded into pellets, baked in air at 1000 ° C. for 24 hours, and then gradually cooled.

【0014】次に、ペレット状の焼結体を、酸素とアル
ゴンとの混合比が1:4の混合ガスを使用し、1020
℃で、総圧力1800気圧(酸素分圧:360気圧)中
にて3時間HIP処理し、その後、1.5時間で室温ま
で冷却した。
Next, the pellet-shaped sintered body was mixed with a mixed gas of oxygen and argon at a mixing ratio of 1: 4 and 1020
HIP treatment was carried out at a temperature of ℃ at a total pressure of 1800 atm (oxygen partial pressure: 360 atm) for 3 hours, and then cooled to room temperature in 1.5 hours.

【0015】得られた超電導体は、組成が(La
0.89Ba0.111.8(Ca0. 83Mg
0.171.2Cu6.03で、通常の四端子法
によって電気抵抗の温度依存性を測定したところ、58
Kで超電導転移にともなう抵抗の急激な低下が始まり
(Tconset )、32Kで抵抗が零になった(T
zero)。粉末にして交流帯磁率の温度依存性を測定し
たところ、51Kでマイスナー効果の始まり(Tc
(χ)onset )を確認できた。
The composition of the obtained superconductor is (La
0.89 Ba 0.11) 1.8 (Ca 0. 83 Mg
0.17 ) 1.2 Cu 2 O 6.03 , the temperature dependence of the electrical resistance was measured by the ordinary four-terminal method.
At K, the resistance began to drop sharply due to the superconducting transition (Tc onset ), and at 32K, the resistance became zero (T
c zero ). When the temperature dependence of the AC susceptibility was measured in powder form, the onset of the Meissner effect (Tc
(Χ) onset ) was confirmed.

【0016】[0016]

【実施例2】La、SrCO、CaCO、C
uO、LiCOの各粉末を、La:Sr:Ca:C
u:Liが1.8:0.2:1.0:1.8:0.2に
なるように計りとり、メノウ乳鉢で混合した後、Al
の容器に入れ、空気中にて950℃で12時間焼成
した。さらに、再びメノウ乳鉢で粉砕し、ペレット状に
成形し、空気中にて1050℃で12時間焼成した後、
室温下に取り出した。次に、ペレット状の焼結体を、酸
素とアルゴンとの混合比が1:4の混合ガスを使用し、
1075℃で、総圧力2000気圧(酸素分圧:400
気圧)中にて8時間HIP処理し、その後、2時間で室
温まで冷却した。
Example 2 La 2 O 3 , SrCO 3 , CaCO 3 , C
uO and Li 2 CO 3 powders were mixed with La: Sr: Ca: C.
u: Li was measured to be 1.8: 0.2: 1.0: 1.8: 0.2, mixed in an agate mortar, and then Al 2
It was put in a container of O 3 and baked in air at 950 ° C. for 12 hours. Furthermore, after crushing again in an agate mortar, forming into pellets, and baking in air at 1050 ° C. for 12 hours,
It was taken out at room temperature. Next, the pellet-shaped sintered body was mixed with a mixed gas of oxygen and argon at a ratio of 1: 4,
At 1075 ° C, total pressure 2000 atm (oxygen partial pressure: 400
HIP treatment for 8 hours in the atmospheric pressure), and then cooled to room temperature in 2 hours.

【0017】得られた超電導体は、組成が(La0.9
Sr0.1CaCu1.8Li0.26.02
であり、Tconset は60K、Tczeroは43K、Tc
(χ)onset は53Kであった。
The composition of the obtained superconductor is (La 0.9
Sr 0.1 ) 2 Ca 1 Cu 1.8 Li 0.2 O 6.02
, Tc onset is 60K, Tc zero is 43K, Tc
(Χ) onset was 53K.

【0018】[0018]

【実施例3】La、CaCO、MgO、CuO
の各粉末を、La:Ca:Mg:Cuが1.8:0.
9:0.3:2.0になるように計りとり、メノウ乳鉢
で混合した後、Alの容器に入れ、空気中にて9
50℃で12時間焼成した。さらに、再びメノウ乳鉢で
粉砕し、ペレット状に成形した。
Example 3 La 2 O 3 , CaCO 3 , MgO, CuO
Each powder of La: Ca: Mg: Cu was 1.8: 0.
Weigh it out to 9: 0.3: 2.0, mix it in an agate mortar, put it in a container of Al 2 O 3 , and put it in air for 9
It was baked at 50 ° C. for 12 hours. Further, it was crushed again in an agate mortar and molded into pellets.

【0019】次に、ペレット状成形体を、酸素とアルゴ
ンとの混合比が1:4の混合ガスを使用し、1050℃
で、総圧力1500気圧(酸素分圧:300気圧)中に
て5時間HIP処理し、その後、1時間で室温まで冷却
した。
Next, the pellet-shaped molded body was heated at 1050 ° C. using a mixed gas of oxygen and argon at a mixing ratio of 1: 4.
Then, HIP treatment was carried out for 5 hours at a total pressure of 1500 atm (oxygen partial pressure: 300 atm), and then cooled to room temperature for 1 hour.

【0020】得られた超電導体は、組成が(La1.8
(Ca0.75Mg0.251. Cu6.07
で、Tconset は52K、Tczeroは31K、Tc
(χ)on set は45Kであった。
The composition of the obtained superconductor is (La 1.8
(Ca 0.75 Mg 0.25 ) 1. 2 Cu 2 O 6.07
So, Tc onset is 52K, Tc zero is 31K, Tc
(Χ) on set was 45K.

【0021】[0021]

【比較例1】La、CaCO、CuOの各粉末
を、La:Ca:Cuが1.8:1.2:2.0になる
ように計りとり、メノウ乳鉢で混合した後、Al
の容器に入れ、空気中にて950℃で12時間焼成し
た。さらに、再びメノウ乳鉢で粉砕し、ペレット状に成
形し、空気中にて1050℃で12時間焼成した後、室
温下に取り出した。
Comparative Example 1 La 2 O 3 , CaCO 3 , and CuO powders were weighed so that La: Ca: Cu was 1.8: 1.2: 2.0, and mixed in an agate mortar. Al 2 O 3
It was put in a container of and heated at 950 ° C. in air for 12 hours. Further, it was ground again in an agate mortar, formed into pellets, baked in air at 1050 ° C. for 12 hours, and then taken out at room temperature.

【0022】次に、ペレット状の焼結体を、酸素とアル
ゴンとの混合比が1:4の混合ガスを使用し、1050
℃で、総圧力2000気圧(酸素分圧:400気圧)中
にて5時間HIP処理し、その後、2時間で室温まで冷
却した。
Next, the pellet-shaped sintered body was mixed with a mixed gas of oxygen and argon at a mixing ratio of 1: 4, and 1050
HIP treatment was performed at a temperature of ℃ for 5 hours at a total pressure of 2000 atm (oxygen partial pressure: 400 atm), and then cooled to room temperature for 2 hours.

【0023】得られた超電導体は、組成がLa1.8
1.2Cuであり、Tcon set は40K、Tc
zeroは15K、Tc(χ)onset は32Kであった。
The composition of the obtained superconductor is La 1.8 C.
a 1.2 Cu 2 O 5 , Tc on set 40K, Tc
Zero was 15K and Tc (χ) onset was 32K.

【0024】[0024]

【比較例2】La、CaCO、CuOの各粉末
を、La:Ca:Cuが1.8:1.2:2.0になる
ように計りとり、メノウ乳鉢で混合した後、Al
の容器に入れ、空気中にて950℃で12時間焼成し
た。さらに、再びメノウ乳鉢で粉砕し、ペレット状に成
形し、空気中にて1050℃で12時間焼成した後、室
温下に取り出した。
Comparative Example 2 La 2 O 3 , CaCO 3 , and CuO powders were weighed so that La: Ca: Cu was 1.8: 1.2: 2.0, and mixed in an agate mortar. Al 2 O 3
It was put in a container of and heated at 950 ° C. in air for 12 hours. Further, it was ground again in an agate mortar, formed into pellets, baked in air at 1050 ° C. for 12 hours, and then taken out at room temperature.

【0025】次に、ペレット状の焼結体を、酸素とアル
ゴンとの混合比が1:4の混合ガスを使用し、1225
℃で、総圧力2000気圧(酸素分圧:400気圧)中
にて5時間HIPし、その後、2時間で室温まで冷却し
た。
Next, the pellet-shaped sintered body was mixed with 1225 using a mixed gas of oxygen and argon at a mixing ratio of 1: 4.
HIP was carried out at a temperature of ℃ at a total pressure of 2000 atm (oxygen partial pressure: 400 atm) for 5 hours and then cooled to room temperature for 2 hours.

【0026】得られた超電導体は、組成がLa
1.8(Ca0.75Mg0.251.2Cu
6.07であり、Tconset は58K、Tczeroは41
K、Tc(χ)onset は50Kであった。
The composition of the obtained superconductor is La.
1.8 (Ca 0.75 Mg 0.25 ) 1.2 Cu 2 O
It is 6.07 , Tc onset is 58K, Tc zero is 41.
The K and Tc (χ) onset were 50K.

【0027】[0027]

【発明の効果】この発明の超電導体は、一般式、 (La1−ηBaη2−θ(Ca1−γMgγ1+θCuδ ただし、 0≦η<0.2 0≦θ<0.3 0<γ≦0.4 5.9<δ<6.1 で表されるか、 (La1−αSrα2−βCa1+βCu2−ξLiξζ ただし、 0≦α<0.3 0≦β<0.3 0<ξ≦0.3 5.9<ζ<6.1 で表わされるもので、実施例にも示したように、高酸素
分圧中でのHIP処理温度が低くても、この系で知られ
ている従来のものと同等の超電導特性をもっている。
The superconductor of the present invention has the general formula: (La 1-η Ba η ) 2-θ (Ca 1-γ Mg γ ) 1 + θ Cu 2 O δ , where 0 ≦ η <0.20 ≦ It is represented by θ <0.3 0 <γ ≦ 0.4 5.9 <δ <6.1, or (La 1-α Sr α ) 2-β Ca 1 + β Cu 2-ξ Li ξ O ζ , It is expressed by 0 ≦ α <0.3 0 ≦ β <0.3 0 <ξ ≦ 0.3 5.9 <ζ <6.1, and as shown in the examples, in high oxygen partial pressure. Even if the HIP treatment temperature is low, it has superconducting properties equivalent to the conventional one known in this system.

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.5 識別記号 庁内整理番号 FI 技術表示箇所 H01L 39/24 ZAA Z 8728−4M ─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 5 Identification code Office reference number FI technical display location H01L 39/24 ZAA Z 8728-4M

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】下記一般式で表される超電導体。 (La1−ηBaη2−θ(Ca1−γMgγ1+θCuδ ただし、 0≦η<0.2 0≦θ<0.3 0<γ≦0.4 5.9<δ<6.11. A superconductor represented by the following general formula. (La 1-η Ba η ) 2-θ (Ca 1-γ Mg γ ) 1 + θ Cu 2 O δ However, 0 ≦ η <0.2 0 ≦ θ <0.3 0 <γ ≦ 0.4 5.9 <Δ <6.1 【請求項2】下記一般式で表される超電導体。 (La1−αSrα2−βCa1+βCu2−ξLiξζ ただし、 0≦α<0.3 0≦β<0.3 0<ξ≦0.3 5.9<ζ<6.12. A superconductor represented by the following general formula. (La 1-α Sr α ) 2-β Ca 1 + β Cu Cu 2-ξ Li ξ O ζ , where 0 ≦ α <0.3 0 ≦ β <0.3 0 <ξ ≦ 0.3 5.9 <ζ < 6.1
JP3256763A 1991-10-03 1991-10-03 Superconductor Pending JPH0597432A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3256763A JPH0597432A (en) 1991-10-03 1991-10-03 Superconductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3256763A JPH0597432A (en) 1991-10-03 1991-10-03 Superconductor

Publications (1)

Publication Number Publication Date
JPH0597432A true JPH0597432A (en) 1993-04-20

Family

ID=17297110

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3256763A Pending JPH0597432A (en) 1991-10-03 1991-10-03 Superconductor

Country Status (1)

Country Link
JP (1) JPH0597432A (en)

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