JPS63247904A - Thin film magnetic head - Google Patents

Thin film magnetic head

Info

Publication number
JPS63247904A
JPS63247904A JP8321787A JP8321787A JPS63247904A JP S63247904 A JPS63247904 A JP S63247904A JP 8321787 A JP8321787 A JP 8321787A JP 8321787 A JP8321787 A JP 8321787A JP S63247904 A JPS63247904 A JP S63247904A
Authority
JP
Japan
Prior art keywords
film
alumina
thin film
magnetic head
films
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP8321787A
Other languages
Japanese (ja)
Inventor
Hiroshi Nishida
宏 西田
Kazuo Nakamura
和夫 中村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP8321787A priority Critical patent/JPS63247904A/en
Publication of JPS63247904A publication Critical patent/JPS63247904A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/31Structure or manufacture of heads, e.g. inductive using thin films
    • G11B5/3103Structure or manufacture of integrated heads or heads mechanically assembled and electrically connected to a support or housing
    • G11B5/3106Structure or manufacture of integrated heads or heads mechanically assembled and electrically connected to a support or housing where the integrated or assembled structure comprises means for conditioning against physical detrimental influence, e.g. wear, contamination

Abstract

PURPOSE:To decrease the uneven wear characteristic of the sliding surface of a titled head by interposing a nonmagnetic underlying layer to the part of the lower layer of nonmagnetic insulating layers where the layer consists of a material different from the material of the nonmagnetic insulating layers. CONSTITUTION:This ring type thin film magnetic head is constituted by forming a silicone film 12 as the underlying layer on a nonmagnetic 'Fotoceram(R)', substrate 1, then forming alumina films 5-7 as the nonmagnetic insulating films thereon. On the other hand, magnetic materials 2-4 consisting of amorphous Co-Nb-Zr films are formed thereon. A gap 10 is formed between the magnetic materials 3 and 4 and the material is formed of SiO2. The silicone film 13 is formed as the underlying layer on the magnetic material 4. The alumina film 8 is then so formed as to cover the alumina film 7 and the silicone film 13. After the upper part thereof is flattened, a cover substrate 11 is stuck thereto. All the alumina films 5-8 exposed on the sliding surface are thus provided with nearly the equal hardness and the absolute quantity of the unevenwear to be generated between the respective layers is decreased.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、磁気記録媒体に信号を記録再生する場合に用
いる薄膜磁気ヘッドに関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a thin film magnetic head used for recording and reproducing signals on a magnetic recording medium.

従来の技術 従来の薄膜磁気ヘッドは、たとえば第3図に示すように
非磁性の7オトセラム基板1にスバ、ツタリング法によ
りCo −Nb−Zrアモルファス膜からなる磁性体ム
2.磁性体B3.磁性体C4が形成される。これらの磁
性体2.3.41−iギャップ10を含むリング型磁気
ヘッドとしての磁気回路を構成し、又その磁気回路にア
ルミニウム等からなる1ターンコイル9力1鎖交してい
る。コイル9及び磁性体2〜4はアルミナ膜からなる非
磁性絶縁膜6.7によって電気的に絶縁されている。又
同じくアルミナ膜からなる非磁性絶縁膜6.8は、磁性
体2〜4を包むように保護しており、基板1及びカバー
基板11の間でヘッド主要部を支持固定するための構造
体としての役割をはたしている。
2. Description of the Related Art A conventional thin-film magnetic head is manufactured by, for example, as shown in FIG. 3, a magnetic film 2. made of a Co--Nb--Zr amorphous film is deposited on a non-magnetic Otoceram substrate 1 by a tuttering method. Magnetic material B3. A magnetic body C4 is formed. A magnetic circuit as a ring-shaped magnetic head including the magnetic material 2.3.41-i gap 10 is constructed, and a 1-turn coil 9 made of aluminum or the like is interlinked with the magnetic circuit. The coil 9 and the magnetic bodies 2 to 4 are electrically insulated by a nonmagnetic insulating film 6.7 made of an alumina film. The non-magnetic insulating film 6.8, also made of alumina film, protects the magnetic bodies 2 to 4 by enveloping them, and serves as a structure for supporting and fixing the main part of the head between the substrate 1 and the cover substrate 11. playing a role.

発明が解決しようとする問題点 このような薄膜磁気ヘッドでは複数の非磁性絶縁膜が慴
動面に現われる。しかし各層は必ずしも下地条件が同じ
でないために膜質が異なる事があり摩耗特性が異なる場
合がある。例えば第3図の例では、フォトセラム基板1
の上に形成されたアルミナ膜5〜7の硬さは、アルミナ
膜8のうちで、アモルファス膜4の上に形成された部分
の硬さよりも軟らかいために、この部分で優先的な摩耗
が起こるという事が確認できた。このようlアルξす膜
の偏摩耗はへラド摺動面の凹凸音生じさせ、記録媒体と
の良好な接触が損なわれる。
Problems to be Solved by the Invention In such a thin film magnetic head, a plurality of nonmagnetic insulating films appear on the sliding surface. However, since the underlying conditions of each layer are not necessarily the same, the film quality may differ and the wear characteristics may differ. For example, in the example shown in FIG.
Since the hardness of the alumina films 5 to 7 formed thereon is softer than that of the part of the alumina film 8 formed on the amorphous film 4, preferential wear occurs in this part. This was confirmed. Such uneven wear of the film causes uneven noise on the sliding surface of the spatula, impairing good contact with the recording medium.

このようなことは、アルミナ膜に限らずよく使用される
絶縁膜たとえば5102膜でも生起する。
This kind of thing occurs not only with alumina films but also with commonly used insulating films, such as 5102 films.

又このような現象は」二記のようなリングタイプのへ・
ノドに限らず、框直ヘッド等でも起こりうる。
Also, this phenomenon is caused by the ring type as described in 2.
It can occur not only on the throat but also on the straight head of the stile.

問題点を解決するための手段 上記問題点を解決するために本発明では、非磁性絶縁層
の下層が上記非磁性絶縁層とは異なる材料より成ってい
る部分には非磁性下地層を介在させる、。
Means for Solving the Problems In order to solve the above problems, in the present invention, a nonmagnetic underlayer is interposed in the portion where the lower layer of the nonmagnetic insulating layer is made of a different material from the nonmagnetic insulating layer. ,.

作用 このような下地層を設けることにより、各非磁性層は下
地条件がほぼ等しくなりほぼ等しい膜質で成長するよう
になり、摩耗特性がそろうようになる。その結果、偏摩
耗が起こりにくくなる。
Effect: By providing such an underlayer, each nonmagnetic layer has approximately the same underlayer conditions, grows with approximately the same film quality, and has uniform wear characteristics. As a result, uneven wear becomes less likely to occur.

実施例 まず、本発明を導くに至った実験結果を述べる。Example First, the experimental results that led to the present invention will be described.

フォトセラム基板上及びCo−Nb−Zrアモルファス
膜が既に3μm形成されているフォトセラム基板上にR
Fマグネトロンスパヮタ法でアルミナ膜7μmを形成し
、形成したアルミナ膜のヌープ硬さを測定した。ヌープ
硬さは荷重6g一定で測定した。結果を表1の1.2に
示す。
R was applied on the photoceram substrate and on the photoceram substrate on which the Co-Nb-Zr amorphous film had already been formed to a thickness of 3 μm.
An alumina film of 7 μm was formed using the F magnetron sputter method, and the Knoop hardness of the formed alumina film was measured. Knoop hardness was measured under a constant load of 6 g. The results are shown in 1.2 of Table 1.

(以下余 白) 父上記のアルミナ膜の下地膜としてDCマグネトロンス
パッタによるシリコン膜を設けた場合についても同様の
実験を行った。その結果を同表の3.4に示す。
(Left below) Similar experiments were also conducted in the case where a silicon film was provided by DC magnetron sputtering as the base film for the alumina film described above. The results are shown in 3.4 of the same table.

シリコン膜は多結晶シリコンターゲットを用いて形成条
件は、投入電力I Kw 、スパッタガス圧5 X 1
0”” TOrr 、基板ターゲット間距離100鵡と
した。又、アルミナ膜は、焼結アルミナターゲットを用
いて、形成条件は、投入電力1.5Kw、スパッタガス
圧3X10  T:orr、  基板ヌープ、。
The silicon film is formed using a polycrystalline silicon target, and the formation conditions are: input power I Kw, sputtering gas pressure 5 x 1
0"" TOrr, and the distance between the substrate and target was 100 mm. The alumina film was formed using a sintered alumina target, and the formation conditions were: input power of 1.5 Kw, sputtering gas pressure of 3×10 T:orr, and Knoop substrate.

ト間距離65Wsとした。フォトセラム上にシリコン下
地層なしで形成されたアルミナ膜のヌープ硬さは800
〜9oOであった。一方Co −Nb−Zrアモルファ
ス膜を介して形成されたアルミナ膜のそれは13oO〜
1400とかなり大きい値を示した。この差が先に述べ
た偏摩耗の現象に対応していると思われる。
The distance between the two ends was set at 65 Ws. The Knoop hardness of an alumina film formed on photoceram without a silicon underlayer is 800.
~9oO. On the other hand, that of the alumina film formed via the Co-Nb-Zr amorphous film is 13oO~
It showed a fairly large value of 1400. This difference seems to correspond to the phenomenon of uneven wear mentioned above.

次に上記2種類の各アルミナ膜に下地層として0.1μ
m厚のシリコン膜を形成した時のヌープ硬さを測定した
ところ共に120o〜130oであった。すなわち膜厚
0.1μmのシリコン膜がその上に形成されるアルミナ
膜の膜質を支配し、結果として硬さが一定の範囲におさ
まったものと考えられる。
Next, a base layer of 0.1 μm was applied to each of the above two types of alumina films.
When the Knoop hardness of a silicon film having a thickness of m was measured, it was 120° to 130° in both cases. In other words, it is considered that the silicon film with a thickness of 0.1 μm dominates the film quality of the alumina film formed thereon, and as a result, the hardness falls within a certain range.

このような知識をもとに、実際の薄膜へ、ンドにおいて
、アルミナ絶縁膜が異種材料の上に形成される部分には
、すべてシリコンの下地層を介在させて成膜したところ
、アルミナ各層間の偏摩耗が極めて小さくなることがわ
かった。
Based on this knowledge, when forming an actual thin film, we formed a film with a silicon underlayer interposed in all parts where the alumina insulating film was formed on a different material, and found that the alumina insulating film was deposited with a silicon base layer interposed between each layer. It was found that the uneven wear of the steel was extremely small.

なおアルミナ膜の下層がアルミナ膜である場合上部のア
ルミナ膜の膜質は下層のそれと同じになることも実験的
に確認された。
It has also been experimentally confirmed that when the lower layer of the alumina film is an alumina film, the film quality of the upper alumina film is the same as that of the lower layer.

第一の実施例を第1図に従って説明する。第1図はリン
グ型薄膜磁気ヘッドの一例に本発明を適用した図であり
、摺動面から見た図面である。非磁性のフォトセラム基
板1のうえに下地層として膜厚0.1 μmのシリコン
膜をDOマグネトロンスパッタリング法で形成した後、
非磁性絶縁膜としてのアルミナ膜6〜7をRFマグネト
ロンスパッタリング法で形成する。一方co −Nb 
−zr  アモルファス膜からなる磁性体2〜4をRF
スパ・ンタリング法で形成する。なお磁性体3と4の間
にはギヤ・ツブ10が形成されており材料は5102で
RFスパッタ法で形成される。上記磁性体4のうえに先
と同じように下地層として膜厚0.1μmのシリコン膜
13を形成する。この後、アルミナ膜7とシリコン膜1
3をおおうようにしてアルミナ膜8が形成される。この
上部をう・ンピング法等で平坦化した後、カバー基板1
1が貼り合せられる。
A first embodiment will be described with reference to FIG. FIG. 1 is a diagram in which the present invention is applied to an example of a ring-type thin film magnetic head, as seen from the sliding surface. After forming a silicon film with a thickness of 0.1 μm as an underlayer on the nonmagnetic photoceram substrate 1 by DO magnetron sputtering method,
Alumina films 6 to 7 as nonmagnetic insulating films are formed by RF magnetron sputtering. On the other hand, co -Nb
-zr Magnetic bodies 2 to 4 made of amorphous film are RF
Formed by spun-interning method. A gear knob 10 is formed between the magnetic bodies 3 and 4, and is made of 5102 material by RF sputtering. A silicon film 13 having a thickness of 0.1 μm is formed as a base layer on the magnetic body 4 in the same manner as before. After this, alumina film 7 and silicon film 1
An alumina film 8 is formed to cover 3. After flattening this upper part by a rolling method etc., the cover substrate 1
1 is pasted.

このような構成にする事により、摺動面に露出したすべ
てのアルミナ膜6〜8がほぼ等しい硬さになり、各層の
間に発生する偏摩耗の絶対量は、160Å以下となった
。なお、従来例である第3図におけるこの値は600人
であった。
With this configuration, all the alumina films 6 to 8 exposed on the sliding surface had approximately the same hardness, and the absolute amount of uneven wear occurring between each layer was 160 Å or less. In addition, this value in FIG. 3, which is a conventional example, was 600 people.

第2の実施例を第2図に従って説明する。第2図aは、
主磁極型垂直ヘッドの一例に本発明を適用した場合の断
面図である。フェライト基板14のうえに、下地層とし
てシリコン膜12を膜厚0.1μmだけDCマグネトロ
ンスパッタ法で形成し、その上にアルミナ膜6.7をR
Fマグネトロン法で形成する。さらにGo −Wb−Z
r  アモルファス膜からなる主磁極16を形成後、上
記と同じようにして膜厚0.1μmのシリコン膜13を
形成する。この後アルミナ膜8を形成して、う・ンビン
グによる平坦化を経て、カバー基板11とはり合わせら
れる。第2図すが摺動面から見た図面で、この面に露出
しているアルミナ膜6〜8は全て、t’hぼ等しい硬さ
になっており、アルミナ膜各層の間での偏摩耗の絶対値
は、120人であった。なお下地層としてのシリコン膜
を設けない場合の値は約SOO入であった。
A second embodiment will be described with reference to FIG. Figure 2 a is
FIG. 3 is a cross-sectional view when the present invention is applied to an example of a main pole type vertical head. On the ferrite substrate 14, a silicon film 12 is formed as a base layer to a thickness of 0.1 μm by DC magnetron sputtering, and an alumina film 6.7 is formed on it by R.
Formed by F magnetron method. Furthermore, Go-Wb-Z
After forming the main magnetic pole 16 made of an amorphous film, a silicon film 13 having a thickness of 0.1 μm is formed in the same manner as described above. Thereafter, an alumina film 8 is formed, flattened by rolling, and then bonded to the cover substrate 11. Figure 2 is a drawing seen from the sliding surface, and the alumina films 6 to 8 exposed on this surface all have approximately the same hardness t'h, and uneven wear between each alumina film layer. The absolute value was 120 people. Note that the value when no silicon film was provided as an underlayer was about SOO.

以上の説明では薄膜リングヘッド及び薄膜垂直ヘッドを
例にとって本発明の実施例を示したが、更に広く一般に
膜質差に起因する硬さの不均一による偏摩耗の問題を有
するような場合に本発明を適用することができる。
In the above explanation, the embodiments of the present invention have been shown by taking a thin film ring head and a thin film vertical head as examples, but the present invention can be applied more broadly to cases where uneven wear is a problem due to uneven hardness caused by differences in film quality. can be applied.

又非磁性絶縁膜はA/20.のスパッタ膜の場合を示し
たが、5in2のスパッタ膜でも同様の効果が得られた
Also, the non-magnetic insulating film is A/20. Although the case of a sputtered film of 5 in 2 was shown, similar effects were obtained with a 5 in 2 sputtered film.

更に下地層としては、以下のように種々の検討を行なっ
た。
Furthermore, various studies were conducted regarding the base layer as described below.

まず金属としては、 ムl 、 Qn 、 Ti 、 
Or各各の蒸着膜又はスパッタ膜を試みたところ、これ
らにいずれもSlと同様の効果が得られた。
First of all, as metals, Mul, Qn, Ti,
When we tried vapor deposited films or sputtered films of Or, each of them produced the same effect as Sl.

半導体では、Go の蒸着膜又はスパッタ膜を試みたと
ころ、8iと同様の効果が得られた。
For semiconductors, we tried using a vapor-deposited or sputtered Go film, and the same effect as 8i was obtained.

誘電体では、まず酸化物系では、概して極めて大きな効
果は見られなかったが、その上に付着するム1203等
の膜質差を少なくする傾向を有していることは確認され
た。これに対して窒化物系、特にSiN のスバ・フタ
膜ではSiと同様の顕著な効果が見られた。
As for dielectric materials, first of all, although a very large effect was not observed in the case of oxide-based materials, it was confirmed that they tend to reduce the difference in film quality of the film 1203 etc. that adheres thereon. On the other hand, a remarkable effect similar to that of Si was observed in the nitride-based sub-lid film, especially SiN.

このように本発明における下地膜の選択幅は非常に広い
ことが確認された。
As described above, it was confirmed that the selection range of the base film in the present invention is very wide.

発明の効果 本発明によれば、ヘッド摺動面に露出したすべての非磁
性絶縁膜の硬さが等しくなるために、ヘッド摺動面の偏
摩耗が極めて小さくなり、ヘッドと媒体のスペース損失
の小さい薄膜磁気ヘリドを得る事ができる。
Effects of the Invention According to the present invention, all the nonmagnetic insulating films exposed on the head sliding surface have the same hardness, so uneven wear on the head sliding surface is extremely small, and space loss between the head and the medium is reduced. Small thin film magnetic helides can be obtained.

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

第1図は本発明の第1の実施例を示す断面図、第2図は
第2の実施例を示す断面図、第3図は従来flJ ’(
r−示す断面図である。 1・・・・・・基板、2〜4・・・・・磁性体A〜C,
s〜8・・・・・非磁性絶縁膜ム〜D、9・・・・・・
コイル、10・・・・・ギャフプ、11・・・・・カバ
ー基板、12.13・・・・・・ンリコン膜、14.・
・・・・・フェライト基板、15・・・・・磁性体、1
6・・・・・主6極。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名f−
1瀉1 2−−一話+王イ1ミ4 3−=、   B 4=−=C 5−xp*nIelhpXs 8−、     ρ ’0−+1’yデ 1f−−−カIぐ一羞不j イ2.13−−−ンリゴソ刀稟 第3図
FIG. 1 is a sectional view showing a first embodiment of the present invention, FIG. 2 is a sectional view showing a second embodiment, and FIG. 3 is a sectional view showing a conventional flJ'(
FIG. 1...Substrate, 2-4...Magnetic materials A-C,
s~8...Nonmagnetic insulating film M~D, 9...
Coil, 10...Gap, 11...Cover substrate, 12.13...Nilicon film, 14.・
... Ferrite substrate, 15 ... Magnetic material, 1
6... Main 6 poles. Name of agent: Patent attorney Toshio Nakao and 1 other person f-
1〉1 2--Episode + King I 1 Mi 4 3-=, B 4=-=C 5-xp*nIelhpXs 8-, ρ '0-+1'y de 1f---K Iguichi shame j A2.13 --- Nrigoso sword drawing 3

Claims (8)

【特許請求の範囲】[Claims] (1)非磁性絶縁層を含む薄膜磁気ヘッドであって、上
記絶縁層の下層が上記絶縁層とは異なる材料である部分
には、非磁性の下地層が介在していることを特徴とする
薄膜磁気ヘッド。
(1) A thin film magnetic head including a non-magnetic insulating layer, characterized in that a non-magnetic underlayer is interposed in a portion where the lower layer of the insulating layer is made of a different material from the insulating layer. Thin film magnetic head.
(2)非磁性絶縁層はAl_2O_3又はSiO_2の
RFスパッタ膜であることを特徴とする特許請求の範囲
第1項記載の薄膜磁気ヘッド。
(2) The thin film magnetic head according to claim 1, wherein the nonmagnetic insulating layer is an RF sputtered film of Al_2O_3 or SiO_2.
(3)下地層は金属層であることを特徴とする特許請求
の範囲第1項記載の薄膜磁気ヘッド。
(3) The thin film magnetic head according to claim 1, wherein the underlayer is a metal layer.
(4)金属層はAl、Cn、Ti、Crの中から選ばれ
た一種であることを特徴とする特許請求の範囲第3項記
載の薄膜磁気ヘッド。
(4) The thin film magnetic head according to claim 3, wherein the metal layer is one selected from Al, Cn, Ti, and Cr.
(5)下地層は半導体層であることを特徴とする特許請
求の範囲第1項記載の薄膜磁気ヘッド。
(5) The thin film magnetic head according to claim 1, wherein the underlayer is a semiconductor layer.
(6)半導体層はSi、Geの中から選ばれた一種であ
ることを特徴とする特許請求の範囲第5項記載の薄膜磁
気ヘッド。
(6) The thin film magnetic head according to claim 5, wherein the semiconductor layer is one selected from Si and Ge.
(7)下地層は誘電体層である事を特徴とする特許請求
の範囲第1項記載の薄膜磁気ヘッド。
(7) The thin film magnetic head according to claim 1, wherein the underlayer is a dielectric layer.
(8)誘電体層は窒化物であることを特徴とする特許請
求の範囲第7項記載の薄膜磁気ヘッド。
(8) The thin film magnetic head according to claim 7, wherein the dielectric layer is made of nitride.
JP8321787A 1987-04-03 1987-04-03 Thin film magnetic head Pending JPS63247904A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8321787A JPS63247904A (en) 1987-04-03 1987-04-03 Thin film magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8321787A JPS63247904A (en) 1987-04-03 1987-04-03 Thin film magnetic head

Publications (1)

Publication Number Publication Date
JPS63247904A true JPS63247904A (en) 1988-10-14

Family

ID=13796147

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8321787A Pending JPS63247904A (en) 1987-04-03 1987-04-03 Thin film magnetic head

Country Status (1)

Country Link
JP (1) JPS63247904A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2834375A1 (en) * 2001-12-28 2003-07-04 Commissariat Energie Atomique INTEGRATED MAGNETIC HEAD FOR MAGNETIC RECORDING AND METHOD OF MANUFACTURING THE MAGNETIC HEAD

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2834375A1 (en) * 2001-12-28 2003-07-04 Commissariat Energie Atomique INTEGRATED MAGNETIC HEAD FOR MAGNETIC RECORDING AND METHOD OF MANUFACTURING THE MAGNETIC HEAD
WO2003056548A1 (en) * 2001-12-28 2003-07-10 Commissariat A L'energie Atomique Integrated magnetic head for magnetic recording and method for making same

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