JPH0264099A - Production of single crystal of tl-ca-ba-cu-o based high-temperature superconducting material - Google Patents
Production of single crystal of tl-ca-ba-cu-o based high-temperature superconducting materialInfo
- Publication number
- JPH0264099A JPH0264099A JP21777388A JP21777388A JPH0264099A JP H0264099 A JPH0264099 A JP H0264099A JP 21777388 A JP21777388 A JP 21777388A JP 21777388 A JP21777388 A JP 21777388A JP H0264099 A JPH0264099 A JP H0264099A
- Authority
- JP
- Japan
- Prior art keywords
- single crystal
- raw material
- temperature
- based high
- superconducting material
- 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.)
- Granted
Links
- 239000013078 crystal Substances 0.000 title claims abstract description 21
- 239000000463 material Substances 0.000 title claims abstract description 11
- 238000004519 manufacturing process Methods 0.000 title claims description 6
- 239000002994 raw material Substances 0.000 claims abstract description 15
- 239000000203 mixture Substances 0.000 claims abstract description 13
- 238000007716 flux method Methods 0.000 claims abstract description 4
- 229910002480 Cu-O Inorganic materials 0.000 claims abstract 3
- 229910052802 copper Inorganic materials 0.000 claims abstract 3
- 239000007858 starting material Substances 0.000 claims abstract 3
- 238000002844 melting Methods 0.000 claims description 2
- 230000008018 melting Effects 0.000 claims description 2
- 239000000470 constituent Substances 0.000 claims 1
- 239000010949 copper Substances 0.000 abstract 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 abstract 2
- 229910008649 Tl2O3 Inorganic materials 0.000 abstract 1
- 150000001875 compounds Chemical class 0.000 abstract 1
- 239000004020 conductor Substances 0.000 abstract 1
- QTQRFJQXXUPYDI-UHFFFAOYSA-N oxo(oxothallanyloxy)thallane Chemical compound O=[Tl]O[Tl]=O QTQRFJQXXUPYDI-UHFFFAOYSA-N 0.000 abstract 1
- 230000004907 flux Effects 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 238000002156 mixing Methods 0.000 description 2
- 239000002887 superconductor Substances 0.000 description 2
- 239000002253 acid Substances 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000001747 exhibiting effect Effects 0.000 description 1
- 230000004927 fusion Effects 0.000 description 1
- 239000008188 pellet Substances 0.000 description 1
- 230000035484 reaction time Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明はTl−Ca−Ba−Cu−0系高温超電導材料
の単結晶製造方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a method for producing a single crystal of a Tl-Ca-Ba-Cu-0 based high temperature superconducting material.
[従来技術]
T I −Ca−B a−Cu−0系では曲の酸1ヒ物
超電導材料と同様 CuOやCuO+(Ca、Ba)0
をフラックスとして使用した単結晶の成長が試みられた
が、安定して製造することが難しい状態にあった。[Prior art] In the T I -Ca-B a-Cu-0 system, CuO and CuO + (Ca, Ba) 0 are similar to the acid 1 arsenide superconducting material in the song.
Attempts have been made to grow single crystals using this as a flux, but it has been difficult to produce them stably.
〔発明が解決しようとする課題]
従来の原料組成ではいわゆる高温和と呼ばれるTcの高
いmmサイズの結晶が得られなかった。これは高温相の
晶出する組成や生成する構造が不明であったため製造条
件がずれていたことによるからであった。[Problems to be Solved by the Invention] With conventional raw material compositions, mm-sized crystals with a high Tc, which is called a high-temperature sum, cannot be obtained. This was because the manufacturing conditions were different because the composition in which the high-temperature phase crystallized and the structure formed were unknown.
[問題点を解決するための手段とその効果]そこで発明
者らはかかる課題を解決せんとして精力的に努力した結
果、特許請求の範囲に記載の製造方法を見い出したもの
であって、
■結晶成長に使用する原料中の(Ca+Cu)の原子比
が50〜80at%、TlとBaの原子比がl:1でか
つ10at%〜25at%となるよう配合比を調整する
こと
■原料融合f&910〜860℃の温度範囲内で1〜1
2時間温度を保持すること
を要件にしたものである。[Means for Solving the Problems and Their Effects] Therefore, the inventors made strenuous efforts to solve the problems, and as a result, they discovered the manufacturing method described in the claims, which is: ■Crystals. Adjust the blending ratio so that the atomic ratio of (Ca+Cu) in the raw materials used for growth is 50 to 80 at%, the atomic ratio of Tl and Ba is 1:1, and 10 at% to 25 at% ■ Raw material fusion f&910 ~ 1-1 within the temperature range of 860℃
The requirement is to maintain the temperature for 2 hours.
即ち、Tl系超超電導体高温相の原子比はTl:Ca:
Ba:Cu=2:2:2:3であるが、フラックス法に
よる単結晶育成には原料として2223組成比にさらに
フラックス材を添加する必要がある0発明者らはフラッ
クス材として。That is, the atomic ratio of the high temperature phase of the Tl-based superconductor is Tl:Ca:
Ba:Cu=2:2:2:3, but in order to grow a single crystal by the flux method, it is necessary to further add a flux material to the composition ratio of 2223 as a raw material.The inventors used this as a flux material.
(CaO+Cu0)を使用し、その添加量の最適化を図
った。(CaO+Cu0) was used, and the amount added was optimized.
その結果は第1図に示す通りで、原料としてTl:Ca
:Ba:Cu=2:6:2:6の時に最も高いTcを有
する結晶が得られることが判明した。The results are shown in Figure 1, with Tl:Ca as the raw material.
It has been found that a crystal having the highest Tc can be obtained when :Ba:Cu=2:6:2:6.
これはこの組成比が丁度高温相結晶が晶出する組成範囲
にあるためである。また、(Ca+Cu)が50〜80
at%内のその他の組成でも原料溶融後910〜860
℃の温度内で1〜12時間保持することにより高温相の
生成が進行することが判明した。これは高温相が上記温
度内で包晶反応により生成するためである。保持時間は
組成比や温度によって異なるが900℃では1時間程度
、860℃付近では12時間程度の反応時間が必要であ
る。This is because this composition ratio is exactly within the composition range in which high-temperature phase crystals crystallize. In addition, (Ca+Cu) is 50 to 80
Even with other compositions within the at% range, after melting the raw materials, the
It has been found that the formation of a high temperature phase progresses by holding the sample at a temperature of 1 to 12 hours. This is because the high temperature phase is generated by a peritectic reaction within the above temperature range. Although the holding time varies depending on the composition ratio and temperature, a reaction time of about 1 hour is required at 900°C, and about 12 hours at around 860°C.
[実施例]
各原料組成比におけるTc (K)は次の通りであった
。すなわち。[Example] Tc (K) at each raw material composition ratio was as follows. Namely.
原料組成比 Tc (K)Tl:Ca
:Ba:Cu
2 3 2 3.75 114−1152 4
2 4.5 115
2 5 2 5.25 118
2 7 2 6.75 115
2 8 2 7゜5 94
上記組成比でT 1203 、CaO、BaO2,Cu
Oを混合、約1〜2t o n / c m・でペレッ
ト成形したものを原料とした。原料は内径10〜12m
mφのAuパイプ中に封入し、さらにこの、A uパイ
プをpするつぼ内に挿入し、炉内に入れ、結晶を成長さ
せた。成長条件は第2図に示すとおりである。炉内は流
量200〜500m1/分のo2ガスフローとし、原料
チャージ量は2〜5gとした。冷却tIiI料を扮砕
フラックスより結晶を取り出したところ、結晶は0.5
〜2.5mm口のサイズのものが得られた。これらの結
晶をDC帯磁4!測定によりTcを測定したところ10
8〜120にの種々のTcを持つ結晶が得られた。この
うち118〜120にのTcを示す結晶は0.5〜1.
5mm口程度であった9
[本発明の効果]
これまでTl−Ca−Ba−Cu−0系超電導体の低T
c相単結晶しか得られながったが、本発明によりmmサ
イズの大型の高温和(Tc=118〜120K>の単結
晶が安定して得られるようになり、産業上における実施
範囲が格段に広がる効果は極めて大きい。Raw material composition ratio Tc (K)Tl:Ca
:Ba:Cu 2 3 2 3.75 114-1152 4
2 4.5 115 2 5 2 5.25 118 2 7 2 6.75 115 2 8 2 7゜5 94 At the above composition ratio, T 1203, CaO, BaO2, Cu
The raw material was prepared by mixing O and forming pellets at about 1 to 2 tons/cm. The raw material has an inner diameter of 10 to 12 m.
The material was sealed in an Au pipe of mφ, and the Au pipe was further inserted into a p-type crucible and placed in a furnace to grow crystals. The growth conditions are as shown in FIG. The inside of the furnace had an O2 gas flow of 200 to 500 m1/min, and the raw material charge amount was 2 to 5 g. Crush the cooled tIiI material
When the crystal was taken out from the flux, the crystal was 0.5
A sample with a mouth size of ~2.5 mm was obtained. These crystals are DC magnetized 4! When Tc was measured, it was 10
Crystals with various Tc's from 8 to 120 were obtained. Among these, crystals exhibiting a Tc of 118 to 120 are 0.5 to 1.
9 [Effects of the present invention] Until now, the low T of Tl-Ca-Ba-Cu-0 based superconductors
Previously, only c-phase single crystals could be obtained, but with the present invention, it is now possible to stably obtain mm-sized large single crystals with a high temperature sum (Tc = 118 to 120 K>), which greatly expands the scope of industrial implementation. The effects that spread over the world are extremely large.
Claims (2)
酸化物超電導材料の単結晶をフラックス法により製造す
る際に、出発原料中の(Ca+Cu)の組成が50at
%〜80at%、TlとBaの原子比が1:1でかつ1
0at%〜25at%であることを特徴とするTl−C
a−Ba−Cu−O系高温超電導材料の単結晶製造方法
。(1) When producing a single crystal of an oxide superconducting material containing Tl, Ca, Ba, and Cu as constituent elements by a flux method, the composition of (Ca+Cu) in the starting material is 50 at.
% to 80 at%, the atomic ratio of Tl and Ba is 1:1, and 1
Tl-C characterized by being 0 at% to 25 at%
A method for producing a single crystal of a-Ba-Cu-O based high temperature superconducting material.
〜12時間原料の温度を保持する請求第1項のTl−C
a−Ba−Cu−O系高温超電導材料の単結晶製造方法
。(2), 1 within the temperature range of 910-860℃ after melting the raw material.
Tl-C according to claim 1, which maintains the temperature of the raw material for ~12 hours.
A method for producing a single crystal of a-Ba-Cu-O based high temperature superconducting material.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63217773A JPH0818911B2 (en) | 1988-08-30 | 1988-08-30 | Method for producing single crystal of T1-Ca-Ba-Cu-O high temperature superconducting material |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63217773A JPH0818911B2 (en) | 1988-08-30 | 1988-08-30 | Method for producing single crystal of T1-Ca-Ba-Cu-O high temperature superconducting material |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0264099A true JPH0264099A (en) | 1990-03-05 |
JPH0818911B2 JPH0818911B2 (en) | 1996-02-28 |
Family
ID=16709505
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63217773A Expired - Lifetime JPH0818911B2 (en) | 1988-08-30 | 1988-08-30 | Method for producing single crystal of T1-Ca-Ba-Cu-O high temperature superconducting material |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0818911B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH026330A (en) * | 1988-03-07 | 1990-01-10 | Sanyo Electric Co Ltd | Production of superconducting material and superconducting single crystal |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6353043A (en) * | 1986-08-22 | 1988-03-07 | Tokyo Electric Co Ltd | Laser diode driving control circuit of laser printer |
JPH026330A (en) * | 1988-03-07 | 1990-01-10 | Sanyo Electric Co Ltd | Production of superconducting material and superconducting single crystal |
-
1988
- 1988-08-30 JP JP63217773A patent/JPH0818911B2/en not_active Expired - Lifetime
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6353043A (en) * | 1986-08-22 | 1988-03-07 | Tokyo Electric Co Ltd | Laser diode driving control circuit of laser printer |
JPH026330A (en) * | 1988-03-07 | 1990-01-10 | Sanyo Electric Co Ltd | Production of superconducting material and superconducting single crystal |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH026330A (en) * | 1988-03-07 | 1990-01-10 | Sanyo Electric Co Ltd | Production of superconducting material and superconducting single crystal |
Also Published As
Publication number | Publication date |
---|---|
JPH0818911B2 (en) | 1996-02-28 |
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