JP2812915B2 - Grain-free manganese oxide-based crystal and magnetoresistive element using the same - Google Patents

Grain-free manganese oxide-based crystal and magnetoresistive element using the same

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Publication number
JP2812915B2
JP2812915B2 JP8074863A JP7486396A JP2812915B2 JP 2812915 B2 JP2812915 B2 JP 2812915B2 JP 8074863 A JP8074863 A JP 8074863A JP 7486396 A JP7486396 A JP 7486396A JP 2812915 B2 JP2812915 B2 JP 2812915B2
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Japan
Prior art keywords
grain
crystal
manganese oxide
oxide
based crystal
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Japanese (ja)
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JPH09263495A (en
Inventor
英樹 桑原
好紀 十倉
泰秀 富岡
敦 朝光
浩 守友
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Sanyo Electric Co Ltd
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Sanyo Electric Co Ltd
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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、ペロブスカイト型
構造をもつ新規な無粒界型マンガン酸化物系結晶体、そ
の製造方法及びそれから成る磁気抵抗素子に関するもの
である。
The present invention relates to a novel grain-free manganese oxide crystal having a perovskite structure, a method for producing the same, and a magnetoresistive element comprising the same.

【0002】[0002]

【従来の技術】最近、銅酸化物における高温超伝導の発
見以来、遷移金属酸化物のスピンチャージ結合動力学が
再度注目されるようになり、それに関連して負の巨大磁
気抵抗現象を示すペロブスカイト型マンガン酸化物系材
料に対する研究が行われるようになった。
BACKGROUND OF THE INVENTION Since the discovery of high-temperature superconductivity in copper oxides, the spin-charge coupling kinetics of transition metal oxides has regained attention, and perovskites exhibiting a negative giant magnetoresistance phenomenon in connection therewith. Research on manganese oxide-based materials has started.

【0003】そして、これまでにLaAlO3基板上に
La−Ca−Mn系酸化物、La−Pb−Mn系酸化
物、La−Ba−Mn系酸化物などをエピタキシャル成
長させた薄膜が提案されている[「サイエンス(Sci
ence)」,第264巻,第413ページ、「フィジ
カル・レビュー・レターズ(Physical Rev
iew Letters)」,第71巻,第2331ペ
ージ、「フィジカルレビュー・ビー(Physical
Review B)」,第63巻,1990ペー
ジ]。
[0003] Then, La-Ca-Mn-based oxide LaAlO 3 substrate so far, La-Pb-Mn-based oxide, a thin film such as La-Ba-Mn based oxide is epitaxially grown have been proposed ["Science (Sci
ence), Vol. 264, pp. 413, "Physical Rev Letters (Physical Rev)
view Letters ", Vol. 71, p. 2331," Physical Review Bee (Physical)
Review B) ", Vol. 63, p. 1990].

【0004】他方、ペロブスカイト型構造のマンガン酸
化物を主体とする結晶状セラミックスはいくつか知られ
ているが、これらはいずれも多数の粒界によって区画さ
れた多数の結晶の集合体として得られたものであり、単
結晶体のものは得られていなかった。
On the other hand, some crystalline ceramics mainly composed of a manganese oxide having a perovskite structure are known, and all of them are obtained as an aggregate of a large number of crystals partitioned by a large number of grain boundaries. And a single crystal was not obtained.

【0005】その後、本発明者らにより、磁気相転移温
度付近すなわち強磁性相と反強磁性相との転移温度付近
で大きな磁気抵抗を示す、ペロブスカイト型構造をもつ
Pr−Ca−Mn系酸化物やPr−Sr−Mn系酸化物
の無粒界型結晶体(特願平6−271566号)及びL
a−Sr−Mn系酸化物の無粒界型結晶体(特願平6−
271567号)などが見出された。しかしながら、こ
れらの材料を磁気抵抗素子として利用するためには、そ
の利用目的に応じ、さらに良好な磁気抵抗特性及びヒス
テリシス特性をもつ無粒界型結晶体が要求される。
[0005] Then, the present inventors have found that a Pr-Ca-Mn-based oxide having a perovskite structure and exhibiting a large magnetic resistance near the magnetic phase transition temperature, ie, near the transition temperature between the ferromagnetic phase and the antiferromagnetic phase. And Pr-Sr-Mn-based oxides without grain boundaries (Japanese Patent Application No. 6-271566).
A grain-boundary crystal of an a-Sr-Mn-based oxide (Japanese Patent Application No. Hei 6
271567) and the like. However, in order to use these materials as a magnetoresistive element, a grain-boundary crystal having better magnetoresistive characteristics and hysteresis characteristics is required according to the purpose of use.

【0006】[0006]

【発明が解決しようとする課題】本発明は、これまで知
られている無粒界型結晶体よりも磁気抵抗特性及びヒス
テリシス特性が向上した無粒界型結晶体を提供すること
を目的としてなされたものである。
SUMMARY OF THE INVENTION An object of the present invention is to provide a grain-boundary crystal having improved magnetoresistance and hysteresis characteristics as compared with the grain-bound crystal known so far. It is a thing.

【0007】[0007]

【課題を解決するための手段】本発明者らは、従来の無
粒界型結晶体とは異なった磁気相転移温度を有する新規
な無粒界型結晶体を開発するために、鋭意研究を重ねた
結果、先に提案したPr−Sr−Mn系酸化物又はLa
−Sr−Mn系酸化物のPr又はLaの一部をNdで置
き換えることによりその磁気抵抗特性及びヒステリシス
特性を向上させうることを見出し、この知見に基づいて
本発明をなすに至った。
Means for Solving the Problems The present inventors have made intensive studies to develop a novel grain-boundary crystal having a magnetic phase transition temperature different from that of a conventional grain-boundary crystal. As a result of the superposition, the previously proposed Pr—Sr—Mn-based oxide or La
The present inventors have found that substituting a part of Pr or La of the -Sr-Mn-based oxide with Nd can improve the magnetoresistance and hysteresis characteristics thereof, and have accomplished the present invention based on this finding.

【0008】すなわち、本発明は、一般式 (Nd1-xx1-ySryMnO3 …(I) (式中のMはLa又はPrであり、x及びyは次の範囲
の数である。0.2≦x≦0.8、0.4≦y≦0.
6)で表わされる組成のペロブスカイト型構造をもつ無
粒界型マンガン酸化物系結晶体を提供するものである。
Namely, the present invention has the general formula (Nd 1-x M x) 1-y Sr y MnO 3 ... (I) ( where M in the formula is La or Pr, x and y are in the following ranges 0.2 ≦ x ≦ 0.8, 0.4 ≦ y ≦ 0.
An object of the present invention is to provide a grain-free manganese oxide-based crystal having a perovskite structure having a composition represented by 6).

【0009】また、本発明に従えば、Nd、Sr及びM
nとLa又はPrとを、酸化物又は加熱により酸化物に
変換しうる化合物の形で、原子比Sr/Mnが0.4〜
0.6、原子比(Nd+M)/Mn(ただしMは前記と
同じ)が0.6〜0.4、原子比(Nd+M+Sr)/
Mnが1、原子比Nd/Mが、1/4〜4/1になる割
合で混合して焼結し、次いでこの焼結体を融解状態から
フローティングゾーン法により結晶成長させることによ
り、前記一般式で表わされる組成のペロブスカイト型構
造をもつ無粒界型マンガン酸化物系結晶体を製造するこ
とができる。
According to the present invention, Nd, Sr and M
n and La or Pr in the form of an oxide or a compound capable of being converted to an oxide by heating, and having an atomic ratio Sr / Mn of 0.4 to
0.6, atomic ratio (Nd + M) / Mn (where M is the same as above) 0.6 to 0.4, atomic ratio (Nd + M + Sr) /
By mixing and sintering at a ratio of Mn of 1 and an atomic ratio of Nd / M of 1 / to 4/1, the crystal of the sintered body is grown from a molten state by a floating zone method. A grain-free manganese oxide-based crystal having a perovskite structure having a composition represented by the formula can be produced.

【0010】本発明によれば、また前記一般式(I)で
表わされる組成のペロブスカイト型構造をもつ無粒界型
マンガン酸化物系結晶体から成るメモリースイッチング
型磁気抵抗素子が提供される。
According to the present invention, there is also provided a memory switching type magnetoresistive element comprising a grain-free manganese oxide-based crystal having a perovskite structure having a composition represented by the general formula (I).

【0011】[0011]

【発明の実施の形態】前記一般式(I)において、Mは
La又はPrであるが、MがLaの場合、xは0.6以
下が特に好ましい。また、MがPrの場合、xは0.2
〜0.8の全域にわたって、良好な磁気物性を示す。本
発明方法に従い、一般式(I)で表わされる組成のペロ
ブスカイト型構造をもつ無粒界型マンガン酸化物系結晶
体を製造するには、NdとSrとMnとLa又はPrの
酸化物あるいは加熱により酸化物に変換可能な化合物を
所定の割合で混合し、原料混合物を調製する。この際用
いられる酸化物としては、例えばNd23,Pr23
La23,SrO,Mn34などが挙げられ、また加熱
により酸化物に変換可能な化合物としては、例えばNd
2(CO33,Pr2(CO33,La2(CO33,M
nCO3,SrCO3のような炭酸塩や、Nd(HCO3
3,Pr(HCO33,La(HCO33,Sr(HC
32,Mn(HCO32のような重炭酸塩などが挙げ
られる。これらの原料は、それぞれ粉末状で用いられ、
Mnに対するSrの原子比が0.4〜0.6、Mnに対
するNdとMの合計の原子比が0.6〜0.4、Mnに
対するNdとMとSrの合計の原子比が1になる割合で
混合される。この混合には、メタノール、エタノール、
アセトンのような揮発性有機溶剤を加えた湿式混合を用
いるのが好適である。
BEST MODE FOR CARRYING OUT THE INVENTION In the general formula (I), M is La or Pr. When M is La, x is particularly preferably 0.6 or less. When M is Pr, x is 0.2
Good magnetic properties are exhibited over the entire range of 0.80.8. In order to produce a grain-boundary manganese oxide-based crystal having a perovskite structure having a composition represented by the general formula (I) according to the method of the present invention, an oxide of Nd, Sr, Mn, La, or Pr or heat Are mixed in a predetermined ratio to prepare a raw material mixture. The oxide used at this time is, for example, Nd 2 O 3 , Pr 2 O 3 ,
La 2 O 3 , SrO, Mn 3 O 4 and the like. Examples of the compound which can be converted to an oxide by heating include Nd.
2 (CO 3 ) 3 , Pr 2 (CO 3 ) 3 , La 2 (CO 3 ) 3 , M
carbonates such as nCO 3 and SrCO 3 , and Nd (HCO 3 )
3 , Pr (HCO 3 ) 3 , La (HCO 3 ) 3 , Sr (HC
Bicarbonates such as O 3 ) 2 and Mn (HCO 3 ) 2 . Each of these raw materials is used in powder form,
The atomic ratio of Sr to Mn is 0.4 to 0.6, the total atomic ratio of Nd and M to Mn is 0.6 to 0.4, and the total atomic ratio of Nd, M and Sr to Mn is 1. Mixed in proportions. This mixture includes methanol, ethanol,
It is preferred to use wet mixing with a volatile organic solvent such as acetone.

【0012】次に、この原料混合物を、空気中、100
0〜1400℃の範囲の温度で焼結したのち、得られた
焼結体を微細に粉砕する。この焼結と粉砕の処理を2回
以上繰り返して組成の均質化を行ったのち、得られた粉
末を慣用の成形法例えばプレス成形により、ブロック状
例えば円柱状に成形し、さらに空気中1100〜150
0℃の範囲の温度で焼結する。この成形に際してはポリ
ビニルアルコールのようなバインダーを用いることもで
きる。次いで、得られた焼結体を酸素雰囲気下で、フロ
ーティングゾーン法を用いて、融解状態から結晶成長さ
せる。このフローティングゾーン法における雰囲気とし
ては、純粋な酸素を用いてもよいし、酸素と不活性ガス
例えばアルゴンの混合ガス又は空気でもよい。この際の
成長速度としては5〜15mm/h程度が適当である。
Next, this raw material mixture is placed in air at 100
After sintering at a temperature in the range of 0 to 1400 ° C., the obtained sintered body is finely pulverized. After the sintering and pulverization processes are repeated twice or more to homogenize the composition, the obtained powder is formed into a block shape, for example, a column shape by a conventional forming method, for example, press forming, and further formed into a 1100 to 1100 in air. 150
Sinter at a temperature in the range of 0 ° C. In this molding, a binder such as polyvinyl alcohol can be used. Next, the obtained sintered body is grown from a molten state in an oxygen atmosphere using a floating zone method. As the atmosphere in the floating zone method, pure oxygen may be used, or a mixed gas of oxygen and an inert gas such as argon or air may be used. An appropriate growth rate at this time is about 5 to 15 mm / h.

【0013】このようにして得られた無粒界型マンガン
酸化物系結晶体については、X線回折、電子線マイクロ
アナリシス、ICP質量分析および滴定分析により分析
し、x、yの値を確認することができる。
The thus obtained non-grain-bound manganese oxide-based crystal is analyzed by X-ray diffraction, electron beam microanalysis, ICP mass spectrometry and titration analysis to confirm the values of x and y. be able to.

【0014】本発明の無粒界型マンガン酸化物系結晶体
は電気抵抗及び磁化が温度変化で急峻に変化するととも
に、電気抵抗の磁場依存性いいかえると磁気抵抗値が非
常に大きな巨大磁気抵抗効果を示す。例えば液体窒素温
度(77K)付近で6桁以上の抵抗変化を起こす優れた
磁場特性を有する。
In the grain-boundary manganese oxide-based crystal of the present invention, the electric resistance and the magnetization change sharply with a change in temperature, and the magnetic resistance depends on the magnetic field. Is shown. For example, it has an excellent magnetic field characteristic that causes a resistance change of 6 digits or more around the temperature of liquid nitrogen (77 K).

【0015】また、その抵抗の変化は温度誘起又は磁場
誘起磁化の大きさを関数としてヒステリシスを示すの
で、この変化を構造メモリー及びそれに伴う抵抗スイッ
チメモリーあるいは磁気メモリーとして利用することが
できる。本発明の新規無粒界型マンガン酸化物系結晶体
は従来よりも大きなヒステリシスを示すので、利用上有
利である。
Further, since the change in resistance shows hysteresis as a function of the magnitude of temperature-induced or magnetic field-induced magnetization, this change can be used as a structure memory and a resistance switch memory or a magnetic memory associated therewith. The novel grain-free manganese oxide-based crystal of the present invention exhibits a larger hysteresis than conventional ones, and is therefore advantageous in use.

【0016】[0016]

【実施例】次に実施例により本発明をさらに詳細に説明
する。
Next, the present invention will be described in more detail by way of examples.

【0017】実施例1 Mn34粉末100重量部に、Nd23 88.9重量
部、Pr23 29.0重量部及びSrCO3 104重
量部をそれぞれ粉末状で混合し、エタノール50重量部
を加え、めのう乳鉢で30分間かきまぜた。次にこの混
合物を、空気中、1050℃において24時間焼成した
のち、焼成物を微粉末に粉砕し、エタノール50重量部
を加えて再び混合し、24時間焼成後、さらに粉砕混合
した。
[0017] Example 1 Mn 3 O 4 powder 100 parts by weight, Nd 2 O 3 88.9 parts by weight, were mixed Pr 2 O 3 29.0 parts by weight SrCO 3 104 parts by weight of each powder, ethanol 50 parts by weight were added, and the mixture was stirred in an agate mortar for 30 minutes. Next, this mixture was calcined in air at 1050 ° C. for 24 hours, and then the calcined product was pulverized into fine powder, and 50 parts by weight of ethanol was added and mixed again.

【0018】得られた粉末混合物を2ton/cm2
水圧プレスにより直径5mm、長さ約80mmの円柱状
ロッドに成形し、空気中、1350℃において48時間
加熱焼成した。次に、このようにして得たロッドを2個
のハロゲン白熱灯と半長円形状焦点鏡を備えたフローテ
ィングゾーン炉を用い融解し、結晶成長させた。この
際、原材料ロッドと種ロッドは逆方向に相対速度30r
pmで回転させ、100%酸素気流中、約5mm/hの
速度で結晶成長させた。
The resulting powder mixture was formed into a cylindrical rod having a diameter of 5 mm and a length of about 80 mm by a 2 ton / cm 2 hydraulic press, and was fired and heated at 1350 ° C. for 48 hours in air. Next, the rod thus obtained was melted using a floating zone furnace equipped with two halogen incandescent lamps and a semi-ellipsoidal focusing mirror to grow crystals. At this time, the raw material rod and the seed rod move in opposite directions at a relative speed of 30r.
The crystal was grown at a speed of about 5 mm / h in a 100% oxygen flow while rotating at pm.

【0019】次に、このようにして得た結晶の中央部を
切断し、粉砕して粉末状にし、粉末X線回折分析及びI
CP質量分析を行ったところ、(Nd0.75 Pr0.25
0.5Sr0.5MnO3の組成をもつ無粒界型マンガン酸化
物系結晶体が得られ、それ以外の不純物相は存在しない
ことが確認された。
Next, the central part of the crystal thus obtained was cut, crushed to a powder, and subjected to powder X-ray diffraction analysis and
When CP mass spectrometry was performed, (Nd 0.75 Pr 0.25 )
A grain-free manganese oxide-based crystal having a composition of 0.5 Sr 0.5 MnO 3 was obtained, and it was confirmed that there was no other impurity phase.

【0020】この結晶体はa0=5.4375Å、b0
7.6357Å、c0=5.4802Åをもつ斜方晶系
(空間群Pnma)であった。図1はこのものの磁化の
温度依存性を示すグラフである。
This crystal has a 0 = 5.4375 ° and b 0 =
It was an orthorhombic system (space group Pnma) having 7.6357 ° and c 0 = 5.4802 °. FIG. 1 is a graph showing the temperature dependence of the magnetization of this.

【0021】実施例2 Mn34粉末100重量部に、Nd23 59.9重量
部、Pr53 58.1重量部及びSrCO3 104重
量部をそれぞれ粉末状で混合して調製した原料混合物を
用い、実施例1と同様にして、(Nd0.5 Pr0.50.5
Sr0.5MnO3の組成をもつ無粒界型マンガン酸化物系
結晶体を製造した。
[0021] Example 2 Mn 3 O 4 powder 100 parts by weight, Nd 2 O 3 59.9 parts by weight, were mixed Pr 5 O 3 58.1 parts by weight SrCO 3 104 parts by weight of each powder preparation (Nd 0.5 Pr 0.5 ) 0.5 in the same manner as in Example 1 using the raw material mixture thus obtained.
A grain-free manganese oxide-based crystal having a composition of Sr 0.5 MnO 3 was produced.

【0022】この結晶体は、a0=5.4386Å、b0
=7.6405Å、c0=5.4809Åをもつ斜方晶
系(空間群Pnma)であった。図2は、このものの磁
化の温度依存性を示すグラフ、図3は異なった磁場下に
おける電気抵抗の温度依存性を示すグラフである。
This crystal has a 0 = 5.4386Å, b 0
= 7.6405 ° and c 0 = 5.4809 ° (having an orthorhombic system (space group Pnma)). FIG. 2 is a graph showing the temperature dependence of the magnetization of the sample, and FIG. 3 is a graph showing the temperature dependence of the electric resistance under different magnetic fields.

【0023】実施例3 Mn34粉末100重量部に、Nd23 94.8重量
部、La23 23.0重量部及びSrCO3 104.
0重量部をそれぞれ粉末状で混合して調製した原料混合
物を用い、実施例1と同様にして、(Nd0.8La0.2
0.5Sr0.5MnO3の組成をもつ無粒界型マンガン酸化
物系結晶体を製造した。
[0023] EXAMPLE 3 Mn 3 O 4 powder 100 parts by weight, Nd 2 O 3 94.8 parts by weight, La 2 O 3 23.0 parts by weight SrCO 3 104.
In the same manner as in Example 1, (Nd 0.8 La 0.2 )
A grain-boundary manganese oxide-based crystal having a composition of 0.5 Sr 0.5 MnO 3 was produced.

【0024】この結晶体は、a0=5.432Å、b0
7.642Å、c0=5.478Åをもつ斜方晶系(空
間群Pnma)であった。図4は、このものの磁化の温
度依存性を示すグラフ、図5はこのものの異なった磁場
下における電気抵抗の温度依存性を示すグラフ、図6は
このものの電子状態を示す相図である。
This crystal has a 0 = 5.432Å and b 0 =
It was an orthorhombic system (space group Pnma) with 7.642 ° and c 0 = 5.478 °. FIG. 4 is a graph showing the temperature dependence of the magnetization of this substance, FIG. 5 is a graph showing the temperature dependence of the electric resistance of the substance under different magnetic fields, and FIG. 6 is a phase diagram showing the electronic state of the substance.

【0025】[0025]

【発明の効果】本発明の新規な無粒界型マンガン酸化物
系結晶体は、優れた磁気抵抗特性及びヒステリシス特性
を有し、メモリースイッチング素子や磁気記録ヘッド素
子などとして好適である。
The novel grain-free manganese oxide-based crystal of the present invention has excellent magnetoresistance and hysteresis characteristics and is suitable as a memory switching element or a magnetic recording head element.

【図面の簡単な説明】[Brief description of the drawings]

【図1】 実施例1で得た結晶体の温度と磁化の関係を
示すグラフ。
FIG. 1 is a graph showing the relationship between temperature and magnetization of a crystal obtained in Example 1.

【図2】 実施例2で得た結晶体の温度と磁化の関係を
示すグラフ。
FIG. 2 is a graph showing a relationship between temperature and magnetization of a crystal obtained in Example 2.

【図3】 実施例2で得た結晶体の異なった磁場におけ
る温度と電気抵抗の関係を示すグラフ。
FIG. 3 is a graph showing the relationship between temperature and electric resistance of the crystal obtained in Example 2 under different magnetic fields.

【図4】 実施例3で得た結晶体の温度と磁化の関係を
示すグラフ。
FIG. 4 is a graph showing the relationship between the temperature and the magnetization of the crystal obtained in Example 3.

【図5】 実施例3で得た結晶体の異なった磁場におけ
る温度と電気抵抗の関係を示すグラフ。
FIG. 5 is a graph showing the relationship between temperature and electric resistance of the crystal obtained in Example 3 under different magnetic fields.

【図6】 実施例3で得た結晶体の電子状態を示す相
図。
FIG. 6 is a phase diagram showing the electronic state of the crystal obtained in Example 3.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 桑原 英樹 茨城県つくば市東1−1−4 産業技術 融合領域研究所内 アトムテクノロジー 研究体 (72)発明者 十倉 好紀 茨城県つくば市東1−1−4 産業技術 融合領域研究所内 アトムテクノロジー 研究体 (72)発明者 富岡 泰秀 茨城県つくば市東1−1−4 産業技術 融合領域研究所内 アトムテクノロジー 研究体 (72)発明者 朝光 敦 茨城県つくば市東1−1−4 産業技術 融合領域研究所内 アトムテクノロジー 研究体 (72)発明者 守友 浩 茨城県つくば市東1−1−4 産業技術 融合領域研究所内 アトムテクノロジー 研究体 (58)調査した分野(Int.Cl.6,DB名) C30B 1/00 - 35/00 C01G 1/00 - 57/00 H01L 43/08 - 43/10──────────────────────────────────────────────────続 き Continuing from the front page (72) Inventor Hideki Kuwahara 1-1-4 Higashi, Tsukuba, Ibaraki Pref. Atom Technology Research Center within the Research Institute for Industrial Technology (72) Yoshiki Tokura 1-1-4 Higashi, Tsukuba, Ibaraki Atom technology research body in the Research Institute for Industrial Technology (72) Inventor Yasuhide Tomioka 1-1-4 Higashi Tsukuba, Ibaraki Prefecture Atom technology research body in the Research Institute for Industrial Technology (72) Inventor Atsushi Asamitsu 1 1-4 Atom technology research institute for industrial technology fusion research institute (72) Inventor Hiroshi Moritomo 1-1-4 Higashi Tsukuba, Ibaraki Pref. Atom technology research institute for industrial technology fusion research institute (58) Field surveyed (Int.Cl . 6, DB name) C30B 1/00 - 35/00 C01G 1/00 - 57/00 H01L 43/08 - 43/10

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 一般式 (Nd1-xx1-ySryMnO3 (式中のMはLa又はPrであり、x及びyは次の範囲
の数である。0.2≦x≦0.8、0.4≦y≦0.
6)で表わされる組成のペロブスカイト型構造をもつ無
粒界型マンガン酸化物系結晶体。
M according to claim 1 of the general formula (Nd 1-x M x) 1-y Sr y MnO 3 ( in the formula is La or Pr, x and y are numbers in the following range .0.2 ≦ x ≦ 0.8, 0.4 ≦ y ≦ 0.
A grain-boundary manganese oxide-based crystal having a perovskite structure having a composition represented by 6).
【請求項2】 Nd、Sr及びMnとLa又はPrと
を、酸化物又は加熱により酸化物に変換しうる化合物の
形で、原子比Sr/Mnが0.4〜0.6、原子比(N
d+M)/Mn(ただしMはLa又はPr)が0.6〜
0.4、原子比(Nd+M+Sr)/Mnが1、原子比
Nd/Mが0.25〜4になる割合で混合して焼結し、
次いでこの焼結体を融解状態からフローティングゾーン
法により結晶成長させることを特徴とする一般式 (Nd1-xx1-ySryMnO3 (式中のMは前記と同じ意味をもち、x及びyは次の範
囲の数である。0.25≦x≦0.6、0.4≦y≦
0.6)で表わされる組成のペロブスカイト型構造をも
つ無粒界型マンガン酸化物系結晶体の製造方法。
2. Nd, Sr and Mn and La or Pr in the form of an oxide or a compound capable of being converted to an oxide by heating, in the form of an atomic ratio Sr / Mn of 0.4 to 0.6 and an atomic ratio ( N
d + M) / Mn (M is La or Pr) 0.6 to
0.4, the atomic ratio (Nd + M + Sr) / Mn is 1, and the atomic ratio Nd / M is mixed at a ratio of 0.25 to 4 and sintered.
Then the general formula (Nd 1-x M x) 1-y Sr y MnO 3 ( having the same meaning as the M in the formula above, wherein the crystal is grown by a floating zone method of this sintered body from the molten state , X and y are numbers in the following range: 0.25 ≦ x ≦ 0.6, 0.4 ≦ y ≦
A method for producing a grain-free manganese oxide-based crystal having a perovskite structure having a composition represented by 0.6).
【請求項3】 一般式 (Nd1-xx1-ySryMnO3 (式中のMはLa又はPrであり、x及びyは次の範囲
の数である。0.2≦x≦0.6、0.4≦y≦0.
6)で表わされる組成のペロブスカイト型構造をもつ無
粒界型マンガン酸化物系結晶体から成るメモリースイッ
チング型磁気抵抗素子。
M of 3. A general formula (Nd 1-x M x) 1-y Sr y MnO 3 ( in the formula is La or Pr, x and y are numbers in the following range .0.2 ≦ x ≦ 0.6, 0.4 ≦ y ≦ 0.
A memory switching type magnetoresistive element comprising a grain-boundary manganese oxide-based crystal having a perovskite structure having a composition represented by 6).
JP8074863A 1996-03-28 1996-03-28 Grain-free manganese oxide-based crystal and magnetoresistive element using the same Expired - Lifetime JP2812915B2 (en)

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JP4496320B2 (en) 1999-03-25 2010-07-07 独立行政法人産業技術総合研究所 Magnetoresistive thin film
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