JPH0471877B2 - - Google Patents
Info
- Publication number
- JPH0471877B2 JPH0471877B2 JP62109519A JP10951987A JPH0471877B2 JP H0471877 B2 JPH0471877 B2 JP H0471877B2 JP 62109519 A JP62109519 A JP 62109519A JP 10951987 A JP10951987 A JP 10951987A JP H0471877 B2 JPH0471877 B2 JP H0471877B2
- Authority
- JP
- Japan
- Prior art keywords
- raw material
- single crystal
- cuo
- material rod
- mol
- 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
Links
- QPLDLSVMHZLSFG-UHFFFAOYSA-N Copper oxide Chemical compound [Cu]=O QPLDLSVMHZLSFG-UHFFFAOYSA-N 0.000 claims description 65
- 239000013078 crystal Substances 0.000 claims description 55
- 239000002994 raw material Substances 0.000 claims description 25
- 239000002904 solvent Substances 0.000 claims description 16
- 238000004519 manufacturing process Methods 0.000 claims description 9
- 229910052746 lanthanum Inorganic materials 0.000 claims description 8
- 238000010438 heat treatment Methods 0.000 claims description 7
- MRELNEQAGSRDBK-UHFFFAOYSA-N lanthanum(3+);oxygen(2-) Chemical compound [O-2].[O-2].[O-2].[La+3].[La+3] MRELNEQAGSRDBK-UHFFFAOYSA-N 0.000 claims description 7
- FZLIPJUXYLNCLC-UHFFFAOYSA-N lanthanum atom Chemical compound [La] FZLIPJUXYLNCLC-UHFFFAOYSA-N 0.000 claims description 4
- NZPIUJUFIFZSPW-UHFFFAOYSA-H lanthanum carbonate Chemical compound [La+3].[La+3].[O-]C([O-])=O.[O-]C([O-])=O.[O-]C([O-])=O NZPIUJUFIFZSPW-UHFFFAOYSA-H 0.000 claims description 4
- 239000005751 Copper oxide Substances 0.000 claims description 3
- 229910017569 La2(CO3)3 Inorganic materials 0.000 claims description 3
- 229910000431 copper oxide Inorganic materials 0.000 claims description 3
- 229960001633 lanthanum carbonate Drugs 0.000 claims description 3
- 238000000034 method Methods 0.000 description 15
- 229910021193 La 2 O 3 Inorganic materials 0.000 description 12
- 239000000203 mixture Substances 0.000 description 11
- 238000010586 diagram Methods 0.000 description 8
- 239000012071 phase Substances 0.000 description 8
- 230000012010 growth Effects 0.000 description 6
- 239000000155 melt Substances 0.000 description 6
- 238000007716 flux method Methods 0.000 description 4
- 239000002244 precipitate Substances 0.000 description 4
- 239000006104 solid solution Substances 0.000 description 4
- 239000000243 solution Substances 0.000 description 4
- 238000001816 cooling Methods 0.000 description 3
- 229910052736 halogen Inorganic materials 0.000 description 3
- 150000002367 halogens Chemical class 0.000 description 3
- 238000002844 melting Methods 0.000 description 3
- 230000008018 melting Effects 0.000 description 3
- 239000000843 powder Substances 0.000 description 3
- 239000007858 starting material Substances 0.000 description 3
- 239000010949 copper Substances 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 238000012544 monitoring process Methods 0.000 description 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000004455 differential thermal analysis Methods 0.000 description 1
- 230000005496 eutectics Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 239000007791 liquid phase Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000011812 mixed powder Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 239000000047 product Substances 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 239000007790 solid phase Substances 0.000 description 1
- 239000002887 superconductor Substances 0.000 description 1
- 230000005068 transpiration Effects 0.000 description 1
- 238000005303 weighing Methods 0.000 description 1
Classifications
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B29/00—Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
- C30B29/10—Inorganic compounds or compositions
- C30B29/16—Oxides
- C30B29/22—Complex oxides
- C30B29/225—Complex oxides based on rare earth copper oxides, e.g. high T-superconductors
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B13/00—Single-crystal growth by zone-melting; Refining by zone-melting
- C30B13/16—Heating of the molten zone
- C30B13/22—Heating of the molten zone by irradiation or electric discharge
- C30B13/24—Heating of the molten zone by irradiation or electric discharge using electromagnetic waves
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B15/00—Single-crystal growth by pulling from a melt, e.g. Czochralski method
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B9/00—Single-crystal growth from melt solutions using molten solvents
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/80—Constructional details
- H10N60/85—Superconducting active materials
- H10N60/855—Ceramic superconductors
- H10N60/857—Ceramic superconductors comprising copper oxide
Landscapes
- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Organic Chemistry (AREA)
- Crystallography & Structural Chemistry (AREA)
- Materials Engineering (AREA)
- Metallurgy (AREA)
- Inorganic Chemistry (AREA)
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Ceramic Engineering (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明はLa2CuO4単結晶のフローテイングゾ
ーン法による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 La 2 CuO 4 single crystal using a floating zone method.
[従来の技術]
La2CuO4単結晶はLa原子の位置を少量BaやSr
原子で置き換えると30〜40Kの低温で超伝導体と
なり、極低温素子としてこれからの応用が期待さ
れている。そのため大型の良質な単結晶が望ま
れ、その製造方法の開発が望まれている。[Conventional technology] La 2 CuO 4 single crystal has a small amount of Ba or Sr at the position of the La atom.
When replaced with atoms, it becomes a superconductor at low temperatures of 30 to 40 K, and is expected to find future applications as cryogenic devices. Therefore, large-sized, high-quality single crystals are desired, and the development of methods for producing them is desired.
しかしLa2CuO4は高温にしてゆくと1050℃付近
で分解溶融するため、単結晶と同一組成の原料か
ら単結晶を製造することができない。そのためフ
ラツクス法や溶液ひきあげ法で結晶育成がされて
いる。フラツクス法においては育成時間が3日で
最大8×8×2mmの大きさの単結晶が、溶液ひき
あげ法では育成時間が9〜10時間で9×7×4mm
の大きさの単結晶が現在までに育成されている。 However, as La 2 CuO 4 decomposes and melts at around 1050°C when heated to high temperatures, single crystals cannot be produced from raw materials with the same composition as single crystals. Therefore, crystal growth is carried out using the flux method or the solution pulling method. With the flux method, a single crystal with a maximum size of 8 x 8 x 2 mm can be produced in 3 days, while with the solution pulling method, a single crystal with a maximum size of 9 x 7 x 4 mm can be produced with a growth time of 9 to 10 hours.
To date, single crystals of the size have been grown.
[発明が解決しようとする問題点]
このように、フラツクス法では結晶育成に長時
間を要し、育成結晶が小さく、融剤から育成結晶
を分離する操作が必要である。また溶液ひきあげ
法ではかなり高度の結晶成長技術が必要であり、
容器に充填した出発原料はごく少量が単結晶とな
り、大部分は容器に残り、数回の結晶成長で純度
の低下のため高価な原料を捨てなければならない
等の問題点があつた。[Problems to be Solved by the Invention] As described above, in the flux method, crystal growth takes a long time, the grown crystals are small, and an operation to separate the grown crystals from the flux is required. In addition, the solution pulling method requires fairly sophisticated crystal growth technology.
A very small amount of the starting material filled in the container becomes a single crystal, and most of it remains in the container, resulting in problems such as the need to throw away expensive raw materials because the purity decreases after several crystal growths.
[問題点を解決するための手段]
この発明は上記実情に鑑み、La2O3−Cu0系の
相平衡図に基づき実際のLa2CuO4単結晶製造に適
したフローテイングゾーン法を研究した結果開発
されたもので、銅酸ランタンの原料棒と種結晶の
間に酸化ランタンおよび炭酸ランタンのうちの少
なくとも一種が28.9〜7.1モル%、酸化銅が71.1〜
92.9モル%からなる溶媒を設け、溶媒を1040〜
1330℃に加熱して浮遊溶融帯を形成し、浮遊溶融
帯を原料棒方向に移動させることにより種結晶に
単結晶を析出成長させることを特徴とする。[Means for Solving the Problems] In view of the above-mentioned circumstances, the present invention is based on the phase equilibrium diagram of the La 2 O 3 -Cu0 system and researched a floating zone method suitable for actual production of La 2 CuO 4 single crystals. As a result, 28.9 to 7.1 mol% of at least one of lanthanum oxide and lanthanum carbonate and 71.1 to 71.1 mol% of copper oxide are contained between the lanthanum cuprate raw material rod and the seed crystal.
A solvent consisting of 92.9 mol% is provided, and the solvent is 1040 ~
It is characterized by heating to 1330°C to form a floating molten zone, and by moving the floating molten zone in the direction of the raw material rod, a single crystal is precipitated and grown on the seed crystal.
なおLa2CuO4のLa原子およびCu原子の位置に
何らかの異種元素が少量混入しても、その相平衡
図が定性的にLa2O3−Cu0系の相平衡図と本質的
に変らない場合には、原料棒中に少量の異種元素
を混入することにより、全く同じ方法によつて異
種元素を混入したLa2CuO4固溶体単結晶を製造す
ることも可能である。 Note that even if a small amount of some kind of foreign element is mixed in at the positions of the La and Cu atoms in La 2 CuO 4 , the phase equilibrium diagram is qualitatively the same as the phase equilibrium diagram of the La 2 O 3 −Cu0 system. In addition, by mixing a small amount of a different element into the raw material rod, it is also possible to produce a La 2 CuO 4 solid solution single crystal mixed with a different element by the same method.
[作用]
まず、この発明の原理について述べる。第1図
は示差熱分析と急冷加熱法の結果から作図した
La2O3−Cu0系の相平衡図である。図中、黒点で
示すのは測定結果である。例えばLa2O3が50モル
%、Cu0が50モル%の組成からなるLa2CuO4を加
熱上昇させると1050℃付近で分解溶融してしま
う。[Operation] First, the principle of this invention will be described. Figure 1 was drawn from the results of differential thermal analysis and rapid cooling/heating method.
It is a phase equilibrium diagram of the La 2 O 3 −Cu0 system. In the figure, the black dots indicate the measurement results. For example, when La 2 CuO 4 having a composition of 50 mol % La 2 O 3 and 50 mol % Cu0 is heated, it decomposes and melts at around 1050°C.
次に、液相線A−B間の組成比、すなわちLa2
O3の28.9〜7.1モル%、Cu0の71.1〜92.9モル%の
範囲に混合した原料を約1330〜1040℃において加
熱融解したのち、融液を徐々に降温させると、融
液の組成は液相線A−Bに沿つて図のCu0側へず
れてゆき、La2CuO4が固相となつて析出してく
る。融液の組成が共晶点BよりCu0側であれば、
冷却時にまずCu0が析出し、融液の組成がA点よ
りLa2O3側であれば、冷却時にまずLa2O3の側の
結晶が析出し、いずれもLa2CuO4が析出成長する
ことができない。 Next, the composition ratio between liquidus line A-B, that is, La 2
After heating and melting a raw material containing 28.9 to 7.1 mol% of O3 and 71.1 to 92.9 mol% of Cu0 at approximately 1330 to 1040°C, when the temperature of the melt is gradually lowered, the composition of the melt changes to a liquid phase. It shifts toward the Cu0 side of the figure along the line A-B, and La 2 CuO 4 becomes a solid phase and precipitates. If the composition of the melt is closer to Cu0 than the eutectic point B,
Cu0 precipitates first during cooling, and if the composition of the melt is on the La 2 O 3 side from point A, crystals on the La 2 O 3 side precipitate first during cooling, and in both cases La 2 CuO 4 precipitates and grows. I can't.
この発明においてはフローテイングゾーン法に
おいてLa2CuO4原料棒と種結晶の間に設けられた
溶媒の成分組成を酸化ランタンおよび炭酸ランタ
ンのうちの少なくとも一種が28.9〜7.1モル%、
酸化銅が71.1〜92.9モル%にし、溶媒を1050〜
1350℃に加熱溶融し、上記溶融組成を安定に保ち
ながら原料棒の方向に移動させ、種結晶にLa2
CuO4単結晶を成長させるものである。 In this invention, in the floating zone method, the composition of the solvent provided between the La 2 CuO 4 raw material rod and the seed crystal is such that at least one of lanthanum oxide and lanthanum carbonate is 28.9 to 7.1 mol%;
Copper oxide is 71.1~92.9 mol%, solvent is 1050~
Melt by heating to 1350°C, move in the direction of the raw material rod while keeping the above melt composition stable, and add La 2 to the seed crystal.
It grows CuO 4 single crystals.
[実施例]
以下に実施例によつて本発明を詳細に説明す
る。[Examples] The present invention will be explained in detail below using Examples.
実施例 1
La2CuO4単結晶をフローテイングゾーン法によ
つて製造した。Example 1 A La 2 CuO 4 single crystal was produced by the floating zone method.
第2図に使用したフローテイングゾーン単結晶
製造装置を示す。図において、1は原料棒、2は
種結晶、3は溶融帯域(溶媒)、4および5はそ
れぞれ回転軸、6は石英管、7はハロゲンラン
プ、8は回転楕円鏡、9は監視窓、10はレン
ズ、11は監視用のスクリーンである。 Figure 2 shows the floating zone single crystal manufacturing apparatus used. In the figure, 1 is a raw material rod, 2 is a seed crystal, 3 is a melting zone (solvent), 4 and 5 are rotating shafts, 6 is a quartz tube, 7 is a halogen lamp, 8 is a spheroidal mirror, 9 is a monitoring window, 10 is a lens, and 11 is a monitoring screen.
La2O3とCu0をモル比にして1:1に混合した
粉末を900℃で2時間焼成し、その粉末を加圧成
形器で直径6mm、長さ7cmの丸棒状にして950℃
で2時間均質に焼成してLa2CuO4原料棒1とす
る。 A powder made by mixing La 2 O 3 and Cu0 in a molar ratio of 1:1 was fired at 900℃ for 2 hours, and the powder was molded into a round bar with a diameter of 6 mm and a length of 7 cm using a pressure molder at 950℃.
The mixture was fired homogeneously for 2 hours to obtain La 2 CuO 4 raw material rod 1.
同様に、La2O3を15モル%、Cu0を85モル%の
組成に混合した粉末を900℃で2時間焼成した後、
直径6mmの丸棒状に加圧成形し、950℃で2時間
均質に焼成して溶媒とする。しかるのち、この円
柱棒状の溶媒を径方向に切断し0.5〜0.9gの円板
にしてLa2CuO4原料棒に融着する。 Similarly, after baking a powder of 15 mol% La 2 O 3 and 85 mol% Cu0 at 900°C for 2 hours,
The product was pressure-molded into a round bar shape with a diameter of 6 mm, and baked homogeneously at 950°C for 2 hours to use as a solvent. Thereafter, this cylindrical rod-shaped solvent is cut in the radial direction to form a disk weighing 0.5 to 0.9 g and fused to the La 2 CuO 4 raw material rod.
このようにLa2CuO4原料棒の先端に溶媒を融着
した円柱棒状試料を、赤外線加熱方式を採用した
フローテイングゾーン法単結晶製造装置の上部試
料回転軸4に固定し、同様に下部回転軸5に種結
晶2を固定する。なお、この場合種結晶2と溶媒
をつけたLa2CuO4原料棒1が回転軸に対して偏心
しないように設定する。そして、ハロゲンランプ
7を用い赤外線を使用して上記溶媒を加熱融解し
たのちに種結晶を溶媒に接触させ、液体の表面張
力により原料棒と種結晶の間に溶媒を保持させ
る。 In this way, the cylindrical rod-shaped sample with the solvent fused to the tip of the La 2 CuO 4 raw material rod was fixed to the upper sample rotation shaft 4 of the floating zone method single crystal manufacturing apparatus that adopted the infrared heating method, and the lower rotation shaft was similarly fixed. Seed crystal 2 is fixed on shaft 5. In this case, the seed crystal 2 and the La 2 CuO 4 raw material rod 1 coated with the solvent are set so as not to be eccentric with respect to the rotation axis. After the solvent is heated and melted using infrared rays using a halogen lamp 7, the seed crystal is brought into contact with the solvent, and the solvent is held between the raw material rod and the seed crystal by the surface tension of the liquid.
しかる後に原料棒と種結晶とを互いに反対方向
に30rpmで回転させる。 Thereafter, the raw material rod and the seed crystal are rotated at 30 rpm in opposite directions.
さらに、この融けた溶媒を1〜2mm/hrの速度
で原料棒方向、すなわち上方に移動させて種結晶
にLa2CuO4単結晶を育成させる。なおこの育成は
大気圧下および酸素1気圧中で行つてもCu0等の
蒸散は微量であり、問題はなかつた。 Further, this melted solvent is moved toward the raw material rod, that is, upward, at a rate of 1 to 2 mm/hr, to grow a La 2 CuO 4 single crystal as a seed crystal. It should be noted that even if this growth was carried out under atmospheric pressure and 1 atm of oxygen, the transpiration of Cu0 etc. was very small and there was no problem.
原料棒がほぼ消費された時に育成した単結晶と
原料棒とを切り離して室温まで冷却した。この結
果、直径5mm、長さ5mmの円柱棒状のLa2CuO4単
結晶が得られた。 When the raw material rod was almost consumed, the grown single crystal and the raw material rod were separated and cooled to room temperature. As a result, a cylindrical rod-shaped La 2 CuO 4 single crystal with a diameter of 5 mm and a length of 5 mm was obtained.
実施例 2
(La0.9Ba0.1)2Cu04なる組成についてフローテ
イングゾーン法により固溶体単結晶を製造した。Example 2 A solid solution single crystal having the composition (La 0.9 Ba 0.1 ) 2 Cu0 4 was produced by the floating zone method.
90モル%La2O3+10モル%2BaCO3なる組成の
混合物とCu0をモル比にして1:1および15:85
に混合した粉末をそれぞれ原料棒および溶媒と
し、実施例1と同様の操作により同様の経過を経
て、直径5mm、長さ8mmの(La0.9Ba0.1)2Cu04固
溶体単結晶を得た。 The molar ratio of a mixture of 90 mol% La 2 O 3 + 10 mol% 2BaCO 3 and Cu0 is 1:1 and 15:85.
Using the mixed powder as a raw material rod and a solvent, the same procedure as in Example 1 was carried out to obtain a (La 0.9 Ba 0.1 ) 2 Cu0 4 solid solution single crystal with a diameter of 5 mm and a length of 8 mm.
この発明の製造方法では結晶中のLa原子の位
置をBaで置き換えても第1図のLa2O3−Cu0系の
相平衡図が本質的に変らないため(La0.9Ba0.1)2
Cu04単結晶が製造できた。 In the production method of this invention, even if the position of the La atom in the crystal is replaced with Ba, the phase equilibrium diagram of the La 2 O 3 -Cu0 system shown in Figure 1 remains essentially unchanged (La 0.9 Ba 0.1 ) 2
A Cu0 4 single crystal was produced.
Cuの位置に少量の異種元素を混入しても、定
性的に上記の相平衡図が本質的に変らない場合に
は同様に異種元素を混入したLa2CuO4固溶体単結
晶を得ることができる。 Even if a small amount of a different element is mixed at the Cu position, if the above phase equilibrium diagram does not essentially change qualitatively, a La 2 CuO 4 solid solution single crystal mixed with a different element can be obtained in the same way. .
La2CuO4単結晶の作製に際し、酸化ランタン
(La2O3)でなく、炭酸ランタン(La2(CO3)3)
を出発物質として用いることもできる。La2
(CO3)3は加熱中に
La2(CO3)3→La2O3+3CO2↑
なる反応を起し、La2O3に変化する。従つて出発
物質としてLa2(CO3)3とCu0を用いても、結果と
して第1図と全く同様の相平衡図が得られ、前述
した各実施例と同様の操作によつてLa2CuO4単結
晶およびLaの一部をBaまたはSrで置換した単結
晶を得ることができた。 When producing a La 2 CuO 4 single crystal, lanthanum carbonate (La 2 (CO 3 ) 3 ) was used instead of lanthanum oxide (La 2 O 3 ).
can also be used as a starting material. La 2
(CO 3 ) 3 undergoes the following reaction during heating: La 2 (CO 3 ) 3 →La 2 O 3 +3CO 2 ↑ and changes to La 2 O 3 . Therefore, even if La 2 (CO 3 ) 3 and Cu0 are used as starting materials, a phase equilibrium diagram completely similar to that shown in FIG. 1 is obtained as a result, and La 2 CuO 4 single crystals and single crystals in which part of La was replaced with Ba or Sr were obtained.
[発明の効果]
以上説明したように、この発明によれば比較的
短時間に任意の結晶軸方向に良質なLa2CuO4単結
晶を製造することができる。しかも製造に使用す
る原料の大部分を単結晶化できるので、フラツク
ス法および溶液ひきあげ法に比較し、原料コスト
の節約が可能である。[Effects of the Invention] As explained above, according to the present invention, a high-quality La 2 CuO 4 single crystal can be produced in any crystal axis direction in a relatively short time. Moreover, since most of the raw materials used for production can be made into single crystals, raw material costs can be saved compared to the flux method and the solution pulling method.
第1図はこの発明の原理を説明するためのLa2
O3−Cu0系の相平衡図、第2図はフローテイング
ゾーン単結晶製造装置の断面図である。
1……原料棒、2……種結晶、3……溶融帯
域、7……ハロゲンランプ。
Figure 1 is La 2 for explaining the principle of this invention.
The phase equilibrium diagram of the O 3 -Cu0 system, and FIG. 2 is a cross-sectional view of the floating zone single crystal manufacturing apparatus. 1... Raw material rod, 2... Seed crystal, 3... Melting zone, 7... Halogen lamp.
Claims (1)
ンタンおよび炭酸ランタンのうちの少なくとも一
種が28.9〜7.1モル%、酸化銅が71.1〜92.9モル%
からなる溶媒を設け、該溶媒を1040〜1330℃に加
熱して浮遊溶融帯を形成し、該浮遊溶融帯を前記
原料棒方向に移動させることにより前記種結晶に
単結晶を析出成長させることを特徴とする銅酸ラ
ンタン単結晶の製造方法。 2 前記原料棒が少量の異種元素を含むことを特
徴とする特許請求の範囲第1項記載の銅酸ランタ
ン単結晶の製造方法。[Claims] 1 Between the lanthanum cuprate raw material rod and the seed crystal, at least one of lanthanum oxide and lanthanum carbonate is present in an amount of 28.9 to 7.1 mol%, and copper oxide is present in an amount of 71.1 to 92.9 mol%.
A single crystal is precipitated and grown on the seed crystal by providing a solvent consisting of, heating the solvent to 1040 to 1330°C to form a floating molten zone, and moving the floating molten zone in the direction of the raw material rod. Characteristic manufacturing method of lanthanum cuprate single crystal. 2. The method for producing a lanthanum cuprate single crystal according to claim 1, wherein the raw material rod contains a small amount of a different element.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62109519A JPS63274697A (en) | 1987-05-01 | 1987-05-01 | Production of cupric acid-lanthanum single crystal |
| US07/168,021 US4956334A (en) | 1987-05-01 | 1988-03-14 | Method for preparing a single crystal of lanthanum cuprate |
| DE8888104090T DE3872922T2 (en) | 1987-05-01 | 1988-03-15 | METHOD FOR THE PRODUCTION OF LANTHANE SUPER SINGLE CRYSTAL. |
| EP88104090A EP0288709B1 (en) | 1987-05-01 | 1988-03-15 | method for preparing a single crystal of lanthanum cuprate |
| US07/521,624 US5057492A (en) | 1987-05-01 | 1990-05-10 | Method for preparing a single crystal of lanthanum cuprate |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62109519A JPS63274697A (en) | 1987-05-01 | 1987-05-01 | Production of cupric acid-lanthanum single crystal |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63274697A JPS63274697A (en) | 1988-11-11 |
| JPH0471877B2 true JPH0471877B2 (en) | 1992-11-16 |
Family
ID=14512318
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62109519A Granted JPS63274697A (en) | 1987-05-01 | 1987-05-01 | Production of cupric acid-lanthanum single crystal |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS63274697A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5157017A (en) * | 1987-06-12 | 1992-10-20 | At&T Bell Laboratories | Method of fabricating a superconductive body |
| JP2684432B2 (en) * | 1988-12-29 | 1997-12-03 | 弘直 兒嶋 | Superconducting oxide single crystal and method for producing the same |
-
1987
- 1987-05-01 JP JP62109519A patent/JPS63274697A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63274697A (en) | 1988-11-11 |
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