JPH0949059A - Material having magnetic resistance effect - Google Patents
Material having magnetic resistance effectInfo
- Publication number
- JPH0949059A JPH0949059A JP7203485A JP20348595A JPH0949059A JP H0949059 A JPH0949059 A JP H0949059A JP 7203485 A JP7203485 A JP 7203485A JP 20348595 A JP20348595 A JP 20348595A JP H0949059 A JPH0949059 A JP H0949059A
- Authority
- JP
- Japan
- Prior art keywords
- composition
- fine crystal
- crystal grains
- amorphous phase
- sample
- 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
Links
- 239000000463 material Substances 0.000 title claims abstract description 37
- 230000000694 effects Effects 0.000 title claims abstract description 30
- 230000005291 magnetic effect Effects 0.000 title abstract description 36
- 239000013078 crystal Substances 0.000 claims abstract description 39
- 229910052735 hafnium Inorganic materials 0.000 claims abstract description 9
- 229910052715 tantalum Inorganic materials 0.000 claims abstract description 9
- 229910052721 tungsten Inorganic materials 0.000 claims abstract description 8
- 229910052720 vanadium Inorganic materials 0.000 claims abstract description 8
- 229910052726 zirconium Inorganic materials 0.000 claims abstract description 8
- 229910052758 niobium Inorganic materials 0.000 claims abstract description 7
- 229910052719 titanium Inorganic materials 0.000 claims abstract description 7
- 150000001875 compounds Chemical class 0.000 claims abstract description 5
- 229910052761 rare earth metal Inorganic materials 0.000 claims abstract description 5
- 150000002910 rare earth metals Chemical class 0.000 claims abstract description 5
- 239000000203 mixture Substances 0.000 claims description 74
- 239000010408 film Substances 0.000 abstract description 31
- 239000010409 thin film Substances 0.000 abstract description 10
- 229910052757 nitrogen Inorganic materials 0.000 abstract description 4
- 229910000889 permalloy Inorganic materials 0.000 abstract description 4
- 239000002356 single layer Substances 0.000 abstract description 2
- 230000001105 regulatory effect Effects 0.000 abstract 3
- 229910052742 iron Inorganic materials 0.000 abstract 1
- XEEYBQQBJWHFJM-UHFFFAOYSA-N iron Substances [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 41
- 238000010586 diagram Methods 0.000 description 17
- 230000000052 comparative effect Effects 0.000 description 12
- 239000007789 gas Substances 0.000 description 12
- 238000004544 sputter deposition Methods 0.000 description 8
- 229910045601 alloy Inorganic materials 0.000 description 7
- 239000000956 alloy Substances 0.000 description 7
- 238000000034 method Methods 0.000 description 7
- 239000000758 substrate Substances 0.000 description 7
- 238000010438 heat treatment Methods 0.000 description 6
- 230000003068 static effect Effects 0.000 description 6
- 230000006837 decompression Effects 0.000 description 5
- 238000004458 analytical method Methods 0.000 description 4
- 238000002173 high-resolution transmission electron microscopy Methods 0.000 description 4
- 230000005415 magnetization Effects 0.000 description 4
- 229910017106 Fe—Hf—O Inorganic materials 0.000 description 3
- 239000002772 conduction electron Substances 0.000 description 3
- 238000010894 electron beam technology Methods 0.000 description 3
- 230000001747 exhibiting effect Effects 0.000 description 3
- 229910052760 oxygen Inorganic materials 0.000 description 3
- 230000005641 tunneling Effects 0.000 description 3
- 229910020630 Co Ni Inorganic materials 0.000 description 2
- 229910002440 Co–Ni Inorganic materials 0.000 description 2
- 229910003271 Ni-Fe Inorganic materials 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 2
- 239000002131 composite material Substances 0.000 description 2
- 230000001419 dependent effect Effects 0.000 description 2
- 238000002003 electron diffraction Methods 0.000 description 2
- 239000011261 inert gas Substances 0.000 description 2
- 238000001755 magnetron sputter deposition Methods 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 1
- MYMOFIZGZYHOMD-UHFFFAOYSA-N Dioxygen Chemical compound O=O MYMOFIZGZYHOMD-UHFFFAOYSA-N 0.000 description 1
- 229910005435 FeTaN Inorganic materials 0.000 description 1
- 238000002441 X-ray diffraction Methods 0.000 description 1
- 239000000654 additive Substances 0.000 description 1
- 230000000996 additive effect Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 229910001873 dinitrogen Inorganic materials 0.000 description 1
- 229910001882 dioxygen Inorganic materials 0.000 description 1
- 239000006185 dispersion Substances 0.000 description 1
- 238000004993 emission spectroscopy Methods 0.000 description 1
- 230000005294 ferromagnetic effect Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000009616 inductively coupled plasma Methods 0.000 description 1
- 238000001659 ion-beam spectroscopy Methods 0.000 description 1
- 229910001337 iron nitride Inorganic materials 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 239000011159 matrix material Substances 0.000 description 1
- 150000004767 nitrides Chemical class 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 239000008188 pellet Substances 0.000 description 1
- 239000002244 precipitate Substances 0.000 description 1
- 238000005546 reactive sputtering Methods 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Magnetic Heads (AREA)
- Hall/Mr Elements (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は磁気センサ、磁気ヘ
ッド等への応用がなされる磁気抵抗効果素子用の材料に
関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a material for a magnetoresistive effect element which is applied to a magnetic sensor, a magnetic head and the like.
【0002】[0002]
【従来の技術】従来、導電性物質に磁界を印加すると電
流方向の抵抗が変化する材料を磁気抵抗効果材料と総称
しており、この種の材料で実用化がなされてるものに、
Ni−Fe合金薄膜(パーマロイ薄膜)とCo−Ni合
金薄膜がある。また、これらの合金薄膜で得られる磁気
抵抗変化量(Δρ)は、0.007μΩcmが一般的で
あり、位置センサ、回転センサなどの磁気センサーとし
て、また、磁気ヘッドの再生ヘッド等として応用開発が
進められている。従って今後、磁気センサの高分解能化
あるいは磁気ヘッドの狭トラック化などに対応してより
大きな磁気抵抗効果を示す材料の開発が要求されてい
る。2. Description of the Related Art Conventionally, materials whose resistance changes in the direction of current when a magnetic field is applied to a conductive material are generally called magnetoresistive materials, and materials of this kind have been put into practical use.
There are Ni-Fe alloy thin films (permalloy thin films) and Co-Ni alloy thin films. In addition, the amount of change in magnetic resistance (Δρ) obtained with these alloy thin films is generally 0.007 μΩcm, and it can be applied and developed as a magnetic sensor such as a position sensor or a rotation sensor, or as a reproducing head of a magnetic head. It is being advanced. Therefore, in the future, it is required to develop a material exhibiting a larger magnetoresistive effect in response to the higher resolution of the magnetic sensor or the narrower track of the magnetic head.
【0003】[0003]
【発明が解決しようとする課題】しかしながら、前記し
たようなNi-Fe合金薄膜や、Co-Ni合金薄膜で得
られているような磁気抵抗変化量では、将来考えられる
磁気センサの高分解能化あるいは磁気ヘッドに応用した
場合の磁気記録の高密度化には十分に対応できない問題
があり、更に高い磁気抵抗変化量を示す材料の開発が望
まれている。これらの技術背景を基に本発明者らは、他
の組成系の磁性材料において優れた磁気抵抗効果を示す
材料について研究した結果、本願発明に到達した。However, with the amount of change in magnetoresistance obtained by the Ni-Fe alloy thin film or the Co-Ni alloy thin film as described above, it is expected that the resolution of the magnetic sensor will be improved in the future. When applied to a magnetic head, there is a problem that the high density of magnetic recording cannot be sufficiently dealt with, and development of a material exhibiting a higher magnetoresistance change amount is desired. Based on these technical backgrounds, the inventors of the present invention have arrived at the present invention as a result of research on a material exhibiting an excellent magnetoresistive effect among magnetic materials of other compositions.
【0004】本発明は前記事情に鑑みてなされたもので
あり、単層膜でパーマロイ薄膜と同程度あるいはそれ以
上の優れた磁気抵抗効果を得ることができる磁気抵抗効
果材料の提供を目的とする。The present invention has been made in view of the above circumstances, and an object of the present invention is to provide a magnetoresistive effect material capable of obtaining an excellent magnetoresistive effect equivalent to or higher than that of a permalloy thin film in a single layer film. .
【0005】[0005]
【課題を解決するための手段】請求項1記載の発明は前
記課題を解決するために、体心立方構造のFeを主成分
とする平均結晶粒径5nm以下の微細結晶粒が希土類金
属元素およびTi、Zr、Hf、V、Nb、Ta、Wの
群から選択される少なくとも1種または2種以上の元素
MとNまたはOとの化合物を含む非晶質相中に分散され
てなり、前記非晶質相が体積比率で組織の少なくとも2
0%以上を占める割合とされ、かつ、非晶質相の比抵抗
が、102μΩm以上であり、前記微細結晶粒の粒子相
互間の距離が、平均3〜10nmとされてなるものであ
る。In order to solve the above-mentioned problems, in order to solve the above-mentioned problems, fine crystal grains having a body-centered cubic structure containing Fe as a main component and having an average crystal grain size of 5 nm or less are rare earth metal elements and A dispersion in an amorphous phase containing a compound of at least one or two or more elements M and N or O selected from the group of Ti, Zr, Hf, V, Nb, Ta and W, and Amorphous phase has a volume ratio of at least 2 of texture
The specific resistance of the amorphous phase is 10 2 μΩm or more, and the distance between the fine crystal grains is 3 to 10 nm on average. .
【0006】前記課題を解決するために請求項2記載の
発明は、請求項1に記載の組成を以下の組成式で表され
るものとしたものである。Fe a M b N c、ただしこ
の組成式における組成比a,b,cは、原子%で、60≦a≦
70、10≦b≦15、19≦c≦25なる関係を満足す
るものとする。前記課題を解決するために請求項3記載
の発明は、請求項1に記載の組成を以下の組成式で表さ
れるものとしたものである。Fe d M e O f、ただ
し、組成比d,e,fは、原子%で、40≦d≦50、10≦
e≦30、20≦f≦40なる関係を満足するものとす
る。In order to solve the above-mentioned problems, the invention according to claim 2 is such that the composition according to claim 1 is represented by the following composition formula. Fe a M b N c , where the composition ratio a, b, c in this composition formula is 60% a ≦ 60%
70, 10 ≦ b ≦ 15, and 19 ≦ c ≦ 25 are satisfied. In order to solve the above-mentioned problems, the invention according to claim 3 is such that the composition according to claim 1 is represented by the following composition formula. Fe d M e O f, however, the composition ratio d, e, f is the atomic%, 40 ≦ d ≦ 50,10 ≦
It is assumed that the relationship of e ≦ 30 and 20 ≦ f ≦ 40 is satisfied.
【0007】[0007]
【発明の実施の形態】以下に本発明を更に詳細に説明す
る。本発明に係る磁気抵抗効果材料は、体心立方構造の
Feを主成分とする平均結晶粒径5nm以下の微細結晶
粒が希土類金属元素およびTi、Zr、Hf、V、N
b、Ta、Wの群から選択される少なくとも1種または
2種以上の元素MとNまたはOとの化合物を含む非晶質
相中に分散されてなり、前記非晶質相が体積比率で組織
の少なくとも20%以上を占める割合とされ、かつ、非
晶質相の比抵抗が102μΩm以上であり、前記微細結
晶粒の粒子相互間の距離が、平均3〜10nmとされて
なるものである。BEST MODE FOR CARRYING OUT THE INVENTION Hereinafter, the present invention will be described in more detail. In the magnetoresistive effect material according to the present invention, fine crystal grains having a body-centered cubic structure as a main component and having an average crystal grain size of 5 nm or less and rare earth metal elements and Ti, Zr, Hf, V, and N are used.
b, Ta, W dispersed in an amorphous phase containing a compound of at least one or two or more elements M and N or O selected from the group consisting of b, Ta, and W, and the amorphous phase in a volume ratio. A ratio that occupies at least 20% or more of the structure, a resistivity of the amorphous phase is 10 2 μΩm or more, and a distance between the fine crystal grains is 3 to 10 nm on average. Is.
【0008】本発明で前記の構造とする場合、組成を以
下の組成式で表されるものとすることが好ましい。 Fe a M b N c ただしこの組成式における組成比a,b,cは、原子%で、
60≦a≦70、10≦b≦15、19≦c≦25なる関
係を満足するものとする。前記のFe-M-N組成系にお
いて具体的には、FeTiN、FeZrN、FeHf
N、FeVN、FeNbN、FeTaN、FeWNなる
組成系、あるいは、元素Mとして、Ti、Zr、Hf、
V、Nb、Ta、Wの群から選択される2種以上を用い
ても良い。前記の組成において、Fe含有量を60〜7
0原子%、元素Mの含有量を10〜15原子%、N含有
量を19〜25原子%としたのは、これらの組成範囲か
ら外れると、体心立方晶のFeが生成され難くなるか、
窒化鉄が析出する傾向があるためである。また、これら
の範囲内であれば、高いΔρが得られ易い。When the above structure is used in the present invention, the composition is preferably represented by the following composition formula. Fe a M b N c However, the composition ratio a, b, c in this composition formula is
It is assumed that the relations of 60 ≦ a ≦ 70, 10 ≦ b ≦ 15, 19 ≦ c ≦ 25 are satisfied. In the above Fe-M-N composition system, specifically, FeTiN, FeZrN, FeHf
N, FeVN, FeNbN, FeTaN, FeWN composition system, or as the element M, Ti, Zr, Hf,
You may use 2 or more types selected from the group of V, Nb, Ta, and W. In the above composition, the Fe content is 60 to 7
The content of 0 atom%, the content of the element M is 10 to 15 atom%, and the content of N is 19 to 25 atom%. ,
This is because iron nitride tends to precipitate. Further, within these ranges, a high Δρ is easily obtained.
【0009】次に、本発明で前記の構造とする場合、組
成を以下の各組成式で表されるものとすることが好まし
い。 Fe d M e O f ただし、この組成式における組成比d,e,fは、原子%
で、40≦d≦50、10≦e≦30、20≦f≦40な
る関係を満足するものとする。前記のFeMO組成系に
おいて具体的には、FeTiO、FeZrO、FeHf
O、FeVO、FeNbO、FeTaO、FeWOなる
組成系、あるいは、元素Mとして、Ti、Zr、Hf、
V、Nb、Ta、Wの群から選択される2種以上を用い
ても良い。前記の組成において、Fe含有量を40〜7
0原子%、元素Mの含有量を5〜30原子%、N含有量
を10〜40原子%としたのは、これらの組成範囲から
外れると、非晶質単相状態か、あるいは結晶質単相状態
になり易くなる。また、これらの範囲内であれば、高い
比抵抗を有する非晶質相を介した伝導電子のスピン依存
トンネリングにより、高いΔρが得られ易い。Next, when the above structure is used in the present invention, the composition is preferably represented by the following composition formulas. Fe d Me O f However, the composition ratio d, e, f in this composition formula is atomic%
Then, the relations 40 ≦ d ≦ 50, 10 ≦ e ≦ 30, and 20 ≦ f ≦ 40 are satisfied. In the above FeMO composition system, specifically, FeTiO, FeZrO, FeHf
O, FeVO, FeNbO, FeTaO, FeWO composition system, or as element M, Ti, Zr, Hf,
You may use 2 or more types selected from the group of V, Nb, Ta, and W. In the above composition, the Fe content is 40 to 7
0 atom%, the content of element M is 5 to 30 atom%, and the content of N is 10 to 40 atom%. It becomes easy to enter into a phase state. Further, within these ranges, high Δρ is easily obtained by spin-dependent tunneling of conduction electrons through an amorphous phase having a high specific resistance.
【0010】本発明に係る磁気抵抗効果材料は、汎用の
技術、例えば、スパッタや蒸着等の薄膜形成装置を用い
て磁気抵抗効果材料膜として得ることができる。また、
成膜装置として高周波2極スパッタ装置、DCスパッ
タ、マグネトロンスパッタ、3極スパッタ、イオンビー
ムスパッタ、対向ターゲット式スパッタ等の装置を利用
することができる。更に、スパッタ−ゲートとしてFe
ターゲット上に、Ti、Zr、Hf、V、Nb、Ta、
Wなどからなるペレットを配置した複合ターゲット等を
使用することができる。また、OまたはNを膜中に添加
する方法としては、Ar等の不活性ガス中に酸素ガスま
たは窒素ガスを混合したAr+O2 またはAr+N2 混
合雰囲気ガスでスパッタを行なう反応性スパッタが有効
である。また、Fe、FeM、あるいはFeM系の合金
ターゲットの上に、Fe、元素M、あるいはそれらの酸
化物または窒化物を配置した複合ターゲットを用いてA
r等の不活性ガス中で作製することもできる。The magnetoresistive material according to the present invention can be obtained as a magnetoresistive material film using a general-purpose technique, for example, a thin film forming apparatus such as sputtering or vapor deposition. Also,
As the film forming device, a high frequency bipolar sputtering device, a DC sputtering device, a magnetron sputtering device, a tripolar sputtering device, an ion beam sputtering device, a facing target type sputtering device and the like can be used. Further, as a sputter gate, Fe
Ti, Zr, Hf, V, Nb, Ta, on the target
A composite target in which pellets of W or the like are arranged can be used. As a method of adding O or N into the film, reactive sputtering is effective in which sputtering is performed in an Ar + O 2 or Ar + N 2 mixed atmosphere gas in which an oxygen gas or a nitrogen gas is mixed in an inert gas such as Ar. . In addition, a composite target in which Fe, element M, or an oxide or nitride thereof is arranged on Fe, FeM, or FeM-based alloy target is used.
It can also be produced in an inert gas such as r.
【0011】図1にこの種の薄膜形成装置の一構造例を
示す。この例の装置は、底部に排気孔1を有し側部に雰
囲気ガス供給孔2を有して排気可能に構成された減圧容
器3と、この減圧容器3の内部に図示略の基板ホルダに
よって支持された基板4と、基板4に対向配置されたタ
ーゲット5を主体として構成されている。また、ターゲ
ット5は、本発明の磁気抵抗効果材料の基本組成となる
Fe製のターゲット本体5aと、添加成分元素に対応し
た元素の複数のチップ5bを備えて構成されている。図
1に示す装置を用い、排気孔1から減圧容器2の内部の
空気を排出することで減圧容器2の内部を減圧するとと
もに、ガス供給孔2から、目的の組成に応じてArガ
ス、Arガス+N2ガス、あるいは、Arガス+O2ガス
を供給してスパッタを行い、ターゲット5から粒子を飛
ばして基板4の表面に堆積させ、目的の組成の磁気抵抗
効果材料膜7を得ることができる。FIG. 1 shows an example of the structure of this type of thin film forming apparatus. The apparatus of this example has a decompression container 3 configured to have an exhaust hole 1 at the bottom and an atmosphere gas supply hole 2 at the side so as to be evacuated, and a substrate holder (not shown) inside the decompression container 3. It is mainly composed of a supported substrate 4 and a target 5 arranged to face the substrate 4. Further, the target 5 is configured to include a target body 5a made of Fe, which is the basic composition of the magnetoresistive effect material of the present invention, and a plurality of chips 5b of elements corresponding to the additive component elements. Using the apparatus shown in FIG. 1, the inside of the decompression container 2 is decompressed by exhausting the air inside the decompression container 2 from the exhaust hole 1, and the Ar gas, Ar gas and Ar gas are supplied from the gas supply hole 2 according to the target composition. Gas + N 2 gas or Ar gas + O 2 gas is supplied to perform sputtering, particles are blown from the target 5 and deposited on the surface of the substrate 4, and a magnetoresistive material film 7 having a desired composition can be obtained. .
【0012】以上の如く得られた磁気抵抗効果材料膜7
は、図2に示すように、非晶質相7aのマトリックスの
内部にbccFeを主体とする微細結晶粒7bが多数析
出された構造となる。従って図2に示す磁気抵抗効果材
料膜7は、元素M、あるいはO、Nを多く含む非晶質相
7aの内部に強磁性金属の微細結晶粒7bが多数分散さ
れた構造となる。Magnetoresistive material film 7 obtained as described above
2 has a structure in which a large number of fine crystal grains 7b mainly composed of bccFe are deposited inside the matrix of the amorphous phase 7a, as shown in FIG. Therefore, the magnetoresistive effect material film 7 shown in FIG. 2 has a structure in which a large number of fine crystal grains 7b of ferromagnetic metal are dispersed inside the amorphous phase 7a containing a large amount of the element M or O or N.
【0013】また、この磁気抵抗効果材料膜7を200
〜500℃の温度で熱処理し、非晶質相7aの中から更
に微細結晶粒7bを析出させることもできる。また、そ
の際に、静磁場中で熱処理することが好ましい。従っ
て、非晶質相7aと微細結晶粒7bが混相状態となって
いる組織が好ましいと推定でき、その場合に非晶質相7
aは、体積比率で20%以上必要、より好ましくは50
%以上必要と思われる。Further, the magnetoresistive material film 7 is formed into 200
It is also possible to heat-treat at a temperature of up to 500 ° C. to further precipitate fine crystal grains 7b from the amorphous phase 7a. At that time, it is preferable to perform heat treatment in a static magnetic field. Therefore, it can be presumed that a structure in which the amorphous phase 7a and the fine crystal grains 7b are in a mixed phase is preferable, and in that case, the amorphous phase 7a
a is required to be 20% or more by volume ratio, more preferably 50
It seems that more than% is necessary.
【0014】そしてこの構造において、微細結晶粒7b
の大きさは、5nm以下であることが好ましく、分散す
る多数の微細結晶粒7bの間の相互の距離は、平均3〜
10nmであることが好ましい。これら微細結晶粒7b
間の間隔が平均3nmより小さいようであると、通常の
電流の流れになってしまう傾向が強く、10nmより大
きいとトンネル電流が流れ難くなって優れたMR効果を
得られなくなるので好ましくない。以上のように結晶粒
径5nm以下のFeの微細結晶粒を有し、微細結晶粒間
の間隔が3〜10nmであり、比抵抗102μΩm以上
の高い抵抗値を有する非晶質相からなる磁気抵抗効果材
料膜7であれば、比抵抗の高い非晶質相7a中に導電性
のbccFeの微細結晶粒7bが好適な距離を介して分
散するので、隣接する微細結晶粒のスピンの向きに依存
した伝導電子のトンネル効果により電流が流れるように
なり、高いMR効果を得ることができる。In this structure, fine crystal grains 7b
Is preferably 5 nm or less, and the mutual distance between a large number of dispersed fine crystal grains 7b is 3 to 3 on average.
It is preferably 10 nm. These fine crystal grains 7b
If the distance between them is smaller than 3 nm on average, there is a strong tendency for the current to flow normally, and if it is larger than 10 nm, it becomes difficult for the tunnel current to flow and an excellent MR effect cannot be obtained, which is not preferable. As described above, the amorphous phase has fine crystal grains of Fe having a crystal grain size of 5 nm or less, an interval between the fine crystal grains is 3 to 10 nm, and a high specific resistance of 10 2 μΩm or more. In the case of the magnetoresistive effect material film 7, since the conductive fine crystal grains 7b of bccFe are dispersed in the amorphous phase 7a having a high specific resistance through a suitable distance, the spin directions of the adjacent fine crystal grains are A current flows due to the tunneling effect of conduction electrons depending on, and a high MR effect can be obtained.
【0015】なお、この種の非晶質相7a中にbccF
eの微細結晶粒7bが析出した構造の磁気抵抗効果材料
膜7にあっては、微細結晶粒7bの電気抵抗は、非晶質
相の比抵抗に比べて非常に小さいので、磁気抵抗効果材
料膜7の比抵抗を非晶質相7aの比抵抗と見ることがで
きる。また、前記磁気抵抗効果材料膜7を静磁場中で2
00〜500℃で熱処理したものは、単位磁界あたりの
磁気抵抗変化の割合が大きくなる。以上の如く構成され
た磁気抵抗効果材料膜7は、磁界印加に応じて大きな抵
抗変化(Δρ)を生じるので、磁界センサ、磁気ヘッド
などへ適用できる。In this type of amorphous phase 7a, bccF is added.
In the magnetoresistive effect material film 7 having the structure in which the fine crystal grains 7b of e are deposited, the electric resistance of the fine crystal grains 7b is much smaller than the specific resistance of the amorphous phase. The specific resistance of the film 7 can be regarded as the specific resistance of the amorphous phase 7a. In addition, the magnetoresistive effect material film 7 is applied in a static magnetic field 2
In the case of heat treatment at 00 to 500 ° C., the rate of change in magnetoresistance per unit magnetic field is large. The magnetoresistive material film 7 configured as described above causes a large resistance change (Δρ) in response to application of a magnetic field, and thus can be applied to a magnetic field sensor, a magnetic head, and the like.
【0016】[0016]
【実施例】以下、図面を参照して本発明の実施例につい
て説明するが、本発明が以下の実施例で限定されないの
は勿論である。高周波マグネトロンスパッタ装置によ
り、Fe-Hf系の合金ターゲットを適宜用い、Ar+
O2 (0.1〜2.0%)ガス雰囲気で成膜を行ない、磁
気抵抗効果材料膜を得た。主なスパッタ条件を以下に示
す。 予備排気 1×10-5Pa以下 高周波電力 400W Arガス圧 0.8〜1.0Pa 基板 ガラス基板(間接水冷) 電極間距離 40〜70mmEXAMPLES Examples of the present invention will be described below with reference to the drawings, but it goes without saying that the present invention is not limited to the following examples. Using a high-frequency magnetron sputtering device, using an Fe-Hf-based alloy target as appropriate, Ar +
Film formation was carried out in an O 2 (0.1 to 2.0%) gas atmosphere to obtain a magnetoresistive material film. The main sputtering conditions are shown below. Preliminary exhaust 1 × 10 −5 Pa or less High frequency power 400 W Ar gas pressure 0.8 to 1.0 Pa Substrate Glass substrate (indirect water cooling) Distance between electrodes 40 to 70 mm
【0017】各磁気抵抗効果材料膜の組成は、誘導結合
プラズマ(ICP)発光分析法および、X線マイクロア
ナライザー(EPMA)により決定した。なお、試料の
形状は、幅4.5〜5.0mm、長さ22.5〜24m
m、厚さ約1〜2μmとした。これらの各試料を得たな
らば、各試料についてMRテスタを用いてMR特性の測
定を行った。The composition of each magnetoresistive material film was determined by inductively coupled plasma (ICP) emission spectrometry and X-ray microanalyzer (EPMA). The sample has a width of 4.5 to 5.0 mm and a length of 22.5 to 24 m.
m and the thickness was about 1 to 2 μm. Once these samples were obtained, the MR characteristics of each sample were measured using an MR tester.
【0018】図3(a)はFe88Hf2O10なる組成の
比較例試料の成膜のままの状態(as-deposited状態)の
室温における磁気抵抗変化(ρ-H曲線)を示し、図3
(b)はFe55Hf11O34なる組成の比較例試料の成膜
のままの状態の磁気抵抗変化を示し、図3(c)はFe
44Hf20O36なる組成の本発明試料の成膜のままの状態
の室温における磁気抵抗変化を示す。なお、図3(a)
〜(c)において、(II)で示す○印を結ぶ曲線が電流
と外部磁界を平行にした場合の測定値、(L)で示す●
印を結ぶ曲線が電流と外部磁界を垂直にした場合の測定
値であることを示す。図3(a)と図3(b)に示す比
較例試料では、IIとLの場合で磁界に対する磁気抵抗変
化の傾向が異なっており、通常の磁性金属に見られる異
方性磁気抵抗効果(AMR)が得られている。図3
(c)に示す示す本発明試料では、IIの場合もLの場合
も抵抗は磁界に対して減少しており、Δρで56.6μ
Ωm、Δρ/ρ0で4%の巨大磁気抵抗効果(GMR)
が得られていることがわかる。FIG. 3 (a) shows the magnetoresistance change (ρ-H curve) at room temperature in the as-deposited state (as-deposited state) of the comparative sample having the composition Fe 88 Hf 2 O 10 . Three
FIG. 3B shows a change in magnetoresistance of a comparative sample having a composition of Fe 55 Hf 11 O 34 in the as-deposited state, and FIG.
4 shows changes in magnetoresistance at room temperature in the as-deposited state of a sample of the present invention having a composition of 44 Hf 20 O 36 . FIG. 3 (a)
In (c), the curve connecting the circles shown in (II) is the measured value when the current and the external magnetic field are parallel, and shown in (L).
The curve connecting the marks shows the measured values when the current and the external magnetic field are perpendicular. The comparative samples shown in FIGS. 3 (a) and 3 (b) have different tendencies of change in magnetoresistance with respect to the magnetic field in the cases of II and L, and the anisotropic magnetoresistive effect (see AMR) has been obtained. FIG.
In the sample of the present invention shown in (c), the resistance decreased with respect to the magnetic field in both cases of II and L, and Δρ was 56.6 μm.
4% giant magnetoresistive effect (GMR) in Ωm and Δρ / ρ 0
It can be seen that is obtained.
【0019】次に、図4(a)にFe55Hf11O34なる
組成の比較例試料の静磁場中熱処理(UFA)後の磁気
抵抗効果材料膜の室温における磁気抵抗変化を示し、図
4(b)にFe44Hf20O36なる組成の本発明試料につ
いての静磁場中熱処理(UFA)後の磁気抵抗効果材料
膜の室温における磁気抵抗変化を示す。図4(a)に示
す比較例試料は、IIとLの場合で磁界に対する磁気抵抗
変化の傾向が異なっており、通常の磁性金属に見られる
異方性磁気抵抗効果(AMR)が得られている。図4
(b)に示す本発明試料ではΔρで30μΩm、Δρ/
ρ0で約3%であるが、成膜したままの状態に比べて変
化が急峻になっている。Next, FIG. 4A shows a change in magnetoresistance at room temperature of the magnetoresistive material film after heat treatment in a static magnetic field (UFA) of a comparative sample having a composition of Fe 55 Hf 11 O 34 . (B) shows the magnetoresistance change at room temperature of the magnetoresistive material film after the static magnetic field heat treatment (UFA) for the sample of the present invention having the composition of Fe 44 Hf 20 O 36 . The comparative sample shown in FIG. 4A has different tendencies of change in magnetoresistance with respect to the magnetic field in the cases of II and L, and the anisotropic magnetoresistive effect (AMR) found in ordinary magnetic metal is obtained. There is. FIG.
In the sample of the present invention shown in (b), Δρ is 30 μΩm, Δρ /
Although ρ 0 is about 3%, the change is steeper than in the as-deposited state.
【0020】また、このような急峻なMR変化は低温に
おいても得られる。図5(a)は、Fe44Hf20O36な
る組成の本発明試料についての成膜のままの状態の77
Kにおける比抵抗の関係を示し、図5(b)は、同試料
の室温と77Kにおける場合の外部印加磁界と磁化との
関係を示す。この図から、外部磁界の変化に応じる磁化
の変化が77Kのほうが室温より急峻であることがわか
り、これに伴って比抵抗の変化も急峻となる。Further, such a steep MR change can be obtained even at a low temperature. FIG. 5A shows the state of the as-deposited film of the sample of the present invention having the composition of Fe 44 Hf 20 O 36.
5B shows the relationship between the specific resistance at K and FIG. 5B shows the relationship between the externally applied magnetic field and the magnetization of the same sample at room temperature and 77K. From this figure, it can be seen that the change in magnetization in response to the change in the external magnetic field is steeper at 77K than at room temperature, and accordingly, the change in resistivity is also steep.
【0021】図6は、FeHfO系における比抵抗(ρ
0/μΩm)と組成の関係を示す三角組成図、図7はF
eHfO系における抵抗変化量(Δρ/μΩm)と組成
の関係を示す三角組成図を示す。これらの三角組成図か
ら、102ρ0/μΩm以上の高い比抵抗を得るために
は、40≦Fe≦50、10≦Hf≦30、20≦O≦
40なる関係を満足することが好ましいことが明らかで
ある。また、この範囲内でも40≦Fe≦50、15≦
Hf≦25、25≦O≦40なる関係を満足することが
より好ましい。FIG. 6 shows the specific resistance (ρ in the FeHfO system).
0 / μΩm) and the composition diagram showing the relationship between the composition and FIG.
FIG. 6 is a triangular composition diagram showing the relationship between the resistance change amount (Δρ / μΩm) and the composition in the eHfO system. From these triangular composition diagrams, in order to obtain a high specific resistance of 10 2 ρ 0 / μΩm or more, 40 ≦ Fe ≦ 50, 10 ≦ Hf ≦ 30, 20 ≦ O ≦
It is clear that it is preferable to satisfy the relationship of 40. Even within this range, 40 ≦ Fe ≦ 50, 15 ≦
It is more preferable to satisfy the relationships of Hf ≦ 25 and 25 ≦ O ≦ 40.
【0022】図8はFe44Hf20O36なる組成の本発明
試料の組織の高分解能TEM(透過型電子顕微鏡)像を
模写した図を示し、図9はFe55Hf11O34なる組成の
比較例試料の組織の高分解能TEM(透過型電子顕微
鏡)像を模写した図を示す。各図における不定形の粒が
bcc構造のFeを主体とする微細結晶粒である。図8
と図9に示す組織の比較から明らかなように、本発明に
係る試料の微細結晶粒の粒径は5nm以下であるのに対
し、比較例試料の結晶粒の粒径は5nmを超えるものが
多いことが判明した。FIG. 8 shows a copy of a high resolution TEM (transmission electron microscope) image of the texture of the sample of the present invention having the composition of Fe 44 Hf 20 O 36 , and FIG. 9 shows the composition of Fe 55 Hf 11 O 34 . The figure which imitated the high resolution TEM (transmission electron microscope) image of the structure | tissue of a comparative example sample is shown. The amorphous grains in each figure are fine crystal grains composed mainly of Fe having a bcc structure. FIG.
As is clear from a comparison between the structures shown in FIG. 9 and FIG. 9, the sample according to the present invention has a fine grain size of 5 nm or less, whereas the comparative sample has a grain size of more than 5 nm. It turned out to be many.
【0023】次に、図8に符号で示す微細結晶粒部分
のナノビーム(電子線の径が1nm以下)EXD(エネ
ルギー分散型X線分析装置)による組成分析結果を図1
0に示し、同部分のナノビーム(電子線の径が1nm以
下)電子回折像を図11に示すとともに、図8に符号
で示す非晶質相部分のナノビームEXDによる組成分析
結果を図12に示し、同部分のナノビーム電子回折像を
図13に示す。これらの図の比較から、図8のに示す
微細結晶粒の部分では、結晶組織に特有の回折像が得ら
れており、Feの含有量が多いのに比較すると、に示
す非晶質相の部分では、非晶質に特有の回折像が得ら
れ、の部分よりもFeの含有量が少なくなりHfとO
の割合が多くなっている。従って、非晶質相部分に元素
MのHfと、Oが多く含まれていることが明らかになっ
た。Next, FIG. 1 shows the results of composition analysis by nanobeams (electron beam diameter of 1 nm or less) EXD (energy dispersive X-ray analyzer) of the fine crystal grain portions indicated by the reference numeral in FIG.
No. 0, the electron beam diffraction image of the nanobeam (electron beam diameter is 1 nm or less) of the same portion is shown in FIG. 11, and the composition analysis result by the nanobeam EXD of the amorphous phase portion shown in FIG. 8 is shown in FIG. 13 shows a nanobeam electron diffraction image of the same portion. From the comparison of these figures, a diffraction image peculiar to the crystal structure was obtained in the portion of the fine crystal grains shown in FIG. 8, and compared with the fact that the content of Fe is large, the amorphous phase of In the portion, a diffraction image peculiar to amorphous is obtained, the Fe content is smaller than in the portion, and Hf and O
Is increasing. Therefore, it was revealed that the amorphous phase portion contained a large amount of Hf of the element M and O.
【0024】以上のように、Fe-Hf-O膜膜の磁気抵
抗効果の測定を行ったが、現行のパーマロイ(Δρ=
0.7μΩcm)に比べるとΔρについてはFe-Hf-
O膜の方が遥かに大きい値(Δρ=5660μΩcm)
が得られた。As described above, the magnetoresistive effect of the Fe-Hf-O film was measured. The current permalloy (Δρ =
Compared to 0.7 μΩcm), Δρ is Fe-Hf-
Much larger value for O film (Δρ = 5660μΩcm)
was gotten.
【0025】[0025]
【発明の効果】以上説明したように本発明は、体心立方
構造のFeを主成分とする平均結晶粒径5nm以下の微
細結晶粒を、希土類金属元素およびTi、Zr、Hf、
V、Nb、Ta、Wの群から選択される少なくとも1種
または2種以上の元素MとNまたはOとの化合物を含む
非晶質相の中に分散させた構造であり、微細結晶粒の間
隔を3〜5nmとし、非晶質相の比抵抗を102μΩm
以上にしたので、102μΩm以上の比抵抗を有する非
晶質相を通じた伝導電子のスピン依存トンネリングに起
因する巨大磁気抵抗効果により、高い抵抗変化量(Δ
ρ)を得ることができる。As described above, according to the present invention, fine crystal grains having an average crystal grain size of 5 nm or less containing Fe as a main body and having a body-centered cubic structure as a main component are provided with rare earth metal elements and Ti, Zr, Hf,
It has a structure in which it is dispersed in an amorphous phase containing a compound of at least one element or two or more elements M and N or O selected from the group of V, Nb, Ta and W, and has a fine crystal grain structure. The interval is 3 to 5 nm and the resistivity of the amorphous phase is 10 2 μΩm
As described above, due to the giant magnetoresistive effect due to the spin-dependent tunneling of conduction electrons through the amorphous phase having a specific resistance of 10 2 μΩm or more, a high resistance change amount (Δ
ρ) can be obtained.
【0026】次に、Fe a M b N cなる組成系におい
て、組成比a,b,cを原子%で、60≦a≦70、10≦b
≦15、19≦c≦25なる関係を満足させた場合に、
非晶質相の中に微細結晶粒が析出した構造であって、微
細結晶粒どうしの間の間隔が3〜10nmであり、比抵
抗が102μΩm以上となりやすく、高いΔρを得るこ
とができる。Next, in the composition system Fe a M b N c , the composition ratios a, b and c in atomic% are 60 ≦ a ≦ 70 and 10 ≦ b.
When the relationship of ≦ 15, 19 ≦ c ≦ 25 is satisfied,
It has a structure in which fine crystal grains are precipitated in an amorphous phase, the distance between the fine crystal grains is 3 to 10 nm, the specific resistance is easily 10 2 μΩm or more, and high Δρ can be obtained. .
【0027】次に、Fe d M e O fなる組成系におい
て、組成比d,e,fを原子%で、40≦d≦50、10≦e
≦30、20≦f≦40なる関係を満足させた場合に、
非晶質相の中に微細結晶粒が析出した構造であって、微
細結晶粒どうしの間の間隔が3〜10nmであり、比抵
抗が102μΩm以上となりやすく、高いΔρを得るこ
とができる。Next, Fe d M e O f becomes the composition system, a composition ratio d, e, and f in atomic%, 40 ≦ d ≦ 50,10 ≦ e
When the relationship of ≦ 30, 20 ≦ f ≦ 40 is satisfied,
It has a structure in which fine crystal grains are precipitated in an amorphous phase, the distance between the fine crystal grains is 3 to 10 nm, the specific resistance is easily 10 2 μΩm or more, and high Δρ can be obtained. .
【図1】本発明に係る磁気抵抗効果材料膜を製造する装
置の一例を示す図である。FIG. 1 is a diagram showing an example of an apparatus for producing a magnetoresistive material film according to the present invention.
【図2】本発明の磁気抵抗効果材料膜の一構造例を示す
図である。FIG. 2 is a diagram showing a structural example of a magnetoresistive material film of the present invention.
【図3】図3(a)は、Fe88Hf2O10なる組成の比
較例試料の成膜のままの状態の磁気抵抗変化曲線を示す
図、図3(b)は、Fe55Hf11O34なる組成の比較例
試料の成膜のままの状態の磁気抵抗変化曲線を示す図、
図3(c)は、Fe44Hf20O36なる組成の本発明試料
の成膜のままの状態の磁気抵抗変化曲線を示す図であ
る。3 (a) is a diagram showing a magnetoresistive change curve of a comparative sample having a composition of Fe 88 Hf 2 O 10 in the as-deposited state, and FIG. 3 (b) is Fe 55 Hf 11 shows a magnetoresistance change curve remains the deposition of the comparative sample of O 34 having a composition,
FIG. 3C is a diagram showing a magnetoresistance change curve of the sample of the present invention having a composition of Fe 44 Hf 20 O 36 in the as-deposited state.
【図4】図4(a)は静磁場中熱処理(UFA)後のF
e55Hf11O34なる組成の磁気抵抗効果材料膜試料の室
温における磁気抵抗変化曲線を示す図、図4(b)は静
磁場中熱処理(UFA)後のFe44Hf20O36なる組成
の磁気抵抗効果材料膜試料の室温における磁気抵抗変化
曲線を示す図である。FIG. 4 (a) is an F after heat treatment in a static magnetic field (UFA).
FIG. 4B is a diagram showing a magnetoresistance change curve of a magnetoresistive effect material film sample having a composition of e 55 Hf 11 O 34 at room temperature. FIG. 4B shows a composition of Fe 44 Hf 20 O 36 after heat treatment in a static magnetic field (UFA). It is a figure which shows the magnetoresistive change curve at room temperature of a magnetoresistive effect material film sample.
【図5】図5(a)はFe44Hf20O36なる組成の磁気
抵抗効果材料膜試料の77Kにおける磁気抵抗変化曲線
を示す図、図5(b)は同試料の外部磁界に伴う77K
と室温における磁化変化の状態を示す図である。FIG. 5 (a) is a diagram showing a magnetoresistance change curve at 77K of a magnetoresistive effect material film sample having a composition of Fe 44 Hf 20 O 36 , and FIG. 5 (b) is 77K accompanying an external magnetic field of the sample.
It is a figure which shows the state of the magnetization change at room temperature.
【図6】Fe-Hf-O膜の成膜したままの状態における
構造と抵抗変化量(Δρ0)の組成依存性を示す三角組
成図である。FIG. 6 is a triangular composition diagram showing the composition dependence of the structure and the resistance change amount (Δρ 0 ) in the as-deposited state of the Fe—Hf—O film.
【図7】Fe-Hf-O膜の成膜したままの状態における
構造と抵抗変化量(Δρ)の組成依存性を示す三角組成
図である。FIG. 7 is a triangular composition diagram showing the composition dependence of the structure and the resistance change amount (Δρ) in the as-deposited state of the Fe—Hf—O film.
【図8】Fe44Hf20O36なる組成の本発明試料の組織
の高分解能TEM像を模写した図である。FIG. 8 is a diagram showing a high-resolution TEM image of the texture of a sample of the present invention having a composition of Fe 44 Hf 20 O 36 .
【図9】Fe55Hf11O34なる組成の比較例試料の組織
の高分解能TEM像を模写した図である。FIG. 9 is a diagram showing a high-resolution TEM image of the texture of a comparative sample having a composition of Fe 55 Hf 11 O 34 .
【図10】Fe44Hf20O36なる組成の本発明試料の組
織の微細結晶粒部分のEXDによる組成分析結果を示す
図である。FIG. 10 is a diagram showing a composition analysis result by EXD of a fine crystal grain portion of a structure of a sample of the present invention having a composition of Fe 44 Hf 20 O 36 .
【図11】Fe44Hf20O36なる組成の本発明試料の組
織の微細結晶粒部分の電子線回折像を示す模式図であ
る。FIG. 11 is a schematic diagram showing an electron diffraction image of a fine crystal grain portion of the structure of the sample of the present invention having a composition of Fe 44 Hf 20 O 36 .
【図12】Fe44Hf20O36なる組成の本発明試料の組
織の非晶質相部分のEXDによる組成分析結果を示す図
である。FIG. 12 is a diagram showing the result of composition analysis by EXD of the amorphous phase portion of the structure of the sample of the present invention having the composition of Fe 44 Hf 20 O 36 .
【図13】Fe44Hf20O36なる組成の本発明試料の組
織の非晶質相部分のX電子線回折像を示す模式図であ
る。FIG. 13 is a schematic diagram showing an X-ray diffraction image of an amorphous phase portion of the texture of the sample of the present invention having a composition of Fe 44 Hf 20 O 36 .
1 排気孔、 2 導入孔、 3 減圧容器、 4 基板、 5 ターゲット、 5a ターゲット本体、 5b チップ、 7 磁気抵抗効果材料膜、 7a 非晶質相、 7b 微細結晶粒。 1 exhaust hole, 2 introduction hole, 3 decompression container, 4 substrate, 5 target, 5a target body, 5b chip, 7 magnetoresistive effect material film, 7a amorphous phase, 7b fine crystal grains.
─────────────────────────────────────────────────────
─────────────────────────────────────────────────── ───
【手続補正書】[Procedure amendment]
【提出日】平成7年12月20日[Submission date] December 20, 1995
【手続補正1】[Procedure amendment 1]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】図3[Correction target item name] Figure 3
【補正方法】変更[Correction method] Change
【補正内容】[Correction contents]
【図3】図3は、Fe88Hf2O10なる組成の比較例試
料の成膜のままの状態の磁気抵抗変化曲線と、Fe55H
f11O34なる組成の比較例試料の成膜のままの状態の磁
気抵抗変化曲線と、Fe44Hf20O36なる組成の本発明
試料の成膜のままの状態の磁気抵抗変化曲線を示す図で
ある。FIG. 3 is a magnetoresistance change curve of a comparative sample having a composition of Fe 88 Hf 2 O 10 in the as-deposited state and Fe 55 H
The magnetic resistance change curve of the sample of the comparative example having the composition f 11 O 34 in the as-deposited state and the magnetic resistance change curve of the sample of the present invention having the composition of Fe 44 Hf 20 O 36 in the as-deposited state are shown. It is a figure.
【手続補正2】[Procedure amendment 2]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】図5[Correction target item name] Fig. 5
【補正方法】変更[Correction method] Change
【補正内容】[Correction contents]
【図5】図5は、Fe44Hf20O36なる組成の磁気抵抗
効果材料膜試料の77Kにおける磁気抵抗変化曲線と、
同試料の外部磁界に伴う77Kと室温における磁化変化
の状態を示す図である。FIG. 5 is a magnetoresistance change curve at 77K of a magnetoresistance effect material film sample having a composition of Fe 44 Hf 20 O 36 ;
It is a figure which shows the state of 77 K and the magnetization change at room temperature with an external magnetic field of the same sample.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 牧野 彰宏 東京都大田区雪谷大塚町1番7号 アルプ ス電気株式会社内 (72)発明者 藤森 啓安 宮城県仙台市青葉区吉成2丁目20−3 (72)発明者 三谷 誠司 宮城県仙台市太白区八木山緑町7番地41− 305号 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Akihiro Makino 1-7 Yukiya Otsuka-cho, Ota-ku, Tokyo Alps Electric Co., Ltd. (72) Inventor Seiji Mitani No. 41-305, 7-Yagiyama Midoricho, Taihaku-ku, Sendai City, Miyagi Prefecture
Claims (3)
結晶粒径5nm以下の微細結晶粒が、希土類金属元素お
よびTi、Zr、Hf、V、Nb、Ta、Wの群から選
択される少なくとも1種または2種以上の元素MとNま
たはOとの化合物を含む非晶質相中に分散されてなり、
前記非晶質相が体積比率で組織の少なくとも20%以上
を占める割合とされ、かつ、非晶質相の比抵抗が102
μΩm以上であり、前記微細結晶粒の粒子相互間の距離
が、平均3〜10nmとされてなることを特徴とする磁
気抵抗効果材料。1. Fine crystal grains having an average crystal grain size of 5 nm or less, which is mainly composed of Fe having a body-centered cubic structure, are selected from the group of rare earth metal elements and Ti, Zr, Hf, V, Nb, Ta and W. Which is dispersed in an amorphous phase containing a compound of at least one or two or more elements M and N or O,
The volume ratio of the amorphous phase accounts for at least 20% or more of the structure, and the resistivity of the amorphous phase is 10 2
A magnetoresistive effect material having a size of μΩm or more and an average distance between the fine crystal grains of 3 to 10 nm.
徴とする請求項1に記載の磁気抵抗効果材料。 Fe a M b N c ただしこの組成式における組成比a,b,cは、原子%で、
60≦a≦70、10≦b≦15、19≦c≦25なる関
係を満足するものとする。2. The magnetoresistive effect material according to claim 1, wherein the composition is represented by the following composition formula. Fe a M b N c However, the composition ratio a, b, c in this composition formula is
It is assumed that the relations of 60 ≦ a ≦ 70, 10 ≦ b ≦ 15, 19 ≦ c ≦ 25 are satisfied.
徴とする請求項1に記載の磁気抵抗効果材料。 Fe d M e O f ただし、組成比d,e,fは、原子%で、40≦d≦50、1
0≦e≦30、20≦f≦40なる関係を満足するものと
する。3. The magnetoresistive effect material according to claim 1, wherein the composition is represented by the following composition formula. Fe d Me O f However, the composition ratio d, e, f is 40% d ≦ 50, 1 in atomic%.
It is assumed that the relationship of 0 ≦ e ≦ 30 and 20 ≦ f ≦ 40 is satisfied.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7203485A JPH0949059A (en) | 1995-08-09 | 1995-08-09 | Material having magnetic resistance effect |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7203485A JPH0949059A (en) | 1995-08-09 | 1995-08-09 | Material having magnetic resistance effect |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0949059A true JPH0949059A (en) | 1997-02-18 |
Family
ID=16474944
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7203485A Pending JPH0949059A (en) | 1995-08-09 | 1995-08-09 | Material having magnetic resistance effect |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0949059A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2012089858A (en) * | 2011-11-28 | 2012-05-10 | Toshiba Corp | Magnetoresistance effect element, magnetic memory, magnetoresistance effect head, and magnetic recording and reproducing device |
| US8351164B2 (en) | 2006-09-28 | 2013-01-08 | Kabushiki Kaisha Toshiba | Magnetoresistive element having free and/or pinned layer magnetic compound expressed by M1M2O |
-
1995
- 1995-08-09 JP JP7203485A patent/JPH0949059A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US8351164B2 (en) | 2006-09-28 | 2013-01-08 | Kabushiki Kaisha Toshiba | Magnetoresistive element having free and/or pinned layer magnetic compound expressed by M1M2O |
| JP2012089858A (en) * | 2011-11-28 | 2012-05-10 | Toshiba Corp | Magnetoresistance effect element, magnetic memory, magnetoresistance effect head, and magnetic recording and reproducing device |
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