JPH0439729B2 - - Google Patents

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Publication number
JPH0439729B2
JPH0439729B2 JP60099912A JP9991285A JPH0439729B2 JP H0439729 B2 JPH0439729 B2 JP H0439729B2 JP 60099912 A JP60099912 A JP 60099912A JP 9991285 A JP9991285 A JP 9991285A JP H0439729 B2 JPH0439729 B2 JP H0439729B2
Authority
JP
Japan
Prior art keywords
magnetic
recording medium
magnetic recording
auxiliary yoke
pole
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 - Lifetime
Application number
JP60099912A
Other languages
Japanese (ja)
Other versions
JPS61258312A (en
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 filed Critical
Priority to JP9991285A priority Critical patent/JPS61258312A/en
Publication of JPS61258312A publication Critical patent/JPS61258312A/en
Publication of JPH0439729B2 publication Critical patent/JPH0439729B2/ja
Granted legal-status Critical Current

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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
    • G11B5/1278Structure or manufacture of heads, e.g. inductive specially adapted for magnetisations perpendicular to the surface of the record carrier

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  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Magnetic Heads (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は記録、再生効率の向上した垂直磁気
ヘツドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] This invention relates to a perpendicular magnetic head with improved recording and reproducing efficiency.

〔従来の技術〕[Conventional technology]

従来、この種の垂直の垂直磁気ヘツドとして、
第5図に示すものがあつた。図において、1aは
磁性フエライト等で構成された補助ヨーク、2は
パーマロイ、Co−Zr−Nb等を蒸着、スパツタ等
で形成した強磁性薄膜で構成された主磁極、3は
巻線のコイル導体、4はガラス等の非電導性非磁
性材料、5は磁気テープ、磁気デイスク等の磁気
記録媒体、aは擬似ギヤツプであり、主磁極2と
補助ヨーク1a間の距離である。
Conventionally, this type of vertical perpendicular magnetic head
The one shown in Figure 5 was found. In the figure, 1a is an auxiliary yoke made of magnetic ferrite, etc., 2 is a main pole made of a ferromagnetic thin film made of permalloy, Co-Zr-Nb, etc. by vapor deposition or sputtering, and 3 is a coil conductor of a winding. , 4 is a non-conductive non-magnetic material such as glass, 5 is a magnetic recording medium such as a magnetic tape or a magnetic disk, and a is a pseudo gap, which is the distance between the main magnetic pole 2 and the auxiliary yoke 1a.

従来の垂直磁気ヘツドは、上記のように構成さ
れ、主磁極2に巻かれたコイル導体3に電流を流
すことによつて、磁束が発生する。発生した磁束
は透磁率の高い主磁極2の内部を流れ、磁気記録
媒体5を磁化し、補助ヨーク1aに磁束は誘導さ
れる。
The conventional vertical magnetic head is constructed as described above, and magnetic flux is generated by passing current through the coil conductor 3 wound around the main pole 2. The generated magnetic flux flows inside the main magnetic pole 2 having high magnetic permeability, magnetizes the magnetic recording medium 5, and is induced into the auxiliary yoke 1a.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

上記のような従来の垂直磁気ヘツドでは、擬似
ギヤツプaが数mmあるため、主磁極2から、磁気
記録媒体5を介して補助ヨーク1aに誘導される
磁束は弱まり記録効率、再生効率が低下するとい
う問題点があつた。
In the conventional perpendicular magnetic head as described above, since the pseudo gap a is several mm, the magnetic flux induced from the main pole 2 to the auxiliary yoke 1a via the magnetic recording medium 5 is weakened, resulting in a decrease in recording efficiency and reproduction efficiency. There was a problem.

この発明は、かかる問題点を解決するためにな
されたもので、高い記録効率、再生効率をもつ垂
直磁気ヘツドを得ることを目的とする。
The present invention was made to solve these problems, and an object of the present invention is to obtain a perpendicular magnetic head with high recording efficiency and high reproduction efficiency.

〔問題点を解決するための手段〕[Means for solving problems]

この発明の垂直磁気ヘツドは磁性主磁極ヨー
ク、この主磁極ヨークに設けられ、端面が磁気記
録媒体に対向する磁性主磁極、巻線用窓を設け、
上記主磁極を通る磁束の磁路となるとともに端面
が上記磁気記録媒体に対向する磁性補助ヨーク、
及び上記巻線用窓を通つて設けられている巻線を
備えるものにおいて、上記磁気記録媒体との対向
部における上記補助ヨークと主磁極を70〜250μm
の範囲に、かつ上記補助ヨークの上記磁気記録媒
体と対向する端面と上記磁気記録媒体の空〓を50
〜100μmの範囲にしたものである。
The perpendicular magnetic head of the present invention includes a magnetic main pole yoke, a magnetic main pole provided on the main pole yoke and whose end face faces the magnetic recording medium, and a winding window.
a magnetic auxiliary yoke that serves as a magnetic path for magnetic flux passing through the main magnetic pole and whose end face faces the magnetic recording medium;
and a winding provided through the winding window, the distance between the auxiliary yoke and the main pole at the portion facing the magnetic recording medium is 70 to 250 μm.
and the space between the end surface of the auxiliary yoke facing the magnetic recording medium and the magnetic recording medium is 50 mm.
~100μm range.

〔作用〕[Effect]

この発明においては、磁気記録媒体との対向部
における補助ヨークと主磁極の空隙を250μm以下
と狭くすることにより主磁極より補助ヨークに誘
導される磁束が強くなる。なお、70μm以下では
磁気記録媒体を通らずに直接補助ヨークにもれる
磁束が多くなるので、70〜250μmの範囲にするこ
とにより、垂直磁気ヘツドの記録効率、再生効率
が向上する。また、補助ヨークの磁気記録媒体と
対向する端面と磁気記録媒体の空〓を50μm以上
にすると、ゴーストによるノイズに対する磁気記
録媒体内の磁束密度が急激に減少する。なお、
100μm以上になると信号再生効率が低下するた
め、50〜100μmの範囲にすることになり、再生波
形のゴーストを減少できる。
In this invention, by narrowing the gap between the auxiliary yoke and the main magnetic pole to 250 μm or less in the portion facing the magnetic recording medium, the magnetic flux induced in the auxiliary yoke is stronger than that in the main magnetic pole. Note that if the diameter is 70 μm or less, a large amount of magnetic flux leaks directly to the auxiliary yoke without passing through the magnetic recording medium, so by setting the magnetic flux in the range of 70 to 250 μm, the recording efficiency and reproduction efficiency of the perpendicular magnetic head can be improved. Furthermore, if the gap between the end face of the auxiliary yoke facing the magnetic recording medium and the magnetic recording medium is set to 50 μm or more, the magnetic flux density within the magnetic recording medium against noise caused by ghosts will decrease rapidly. In addition,
Since the signal reproduction efficiency decreases when the diameter exceeds 100 μm, the range is set to 50 to 100 μm, which can reduce ghosts in the reproduced waveform.

〔実施例〕〔Example〕

第1図は、この発明に係わる垂直磁気ヘツドを
示す正面図であり、2〜5は従来のヘツドと同様
のものである。1aは従来と同様に磁性フエライ
ト等で構成された補助ヨークであり、1bは磁性
フエライト等で構成された主磁極ヨークである。
主磁極2の端面は磁気記録媒体5と対向してい
る。補助ヨーク1aは巻線用窓6が設けられ、主
磁極2を通る磁束の磁路となるとともに端面が磁
気記録媒体と対向している。aは磁気記録媒体5
との対向部における補助ヨーク1aと主磁極2の
空隙(擬似ギヤツプ)を表わし70〜250μmの範囲
で、この場合は150μmであり、その間にはガラス
等、非電導性非磁性材料をモールドした。
FIG. 1 is a front view showing a perpendicular magnetic head according to the present invention, and numerals 2 to 5 are similar to conventional heads. 1a is an auxiliary yoke made of magnetic ferrite or the like as in the conventional case, and 1b is a main pole yoke made of magnetic ferrite or the like.
The end face of the main pole 2 faces the magnetic recording medium 5. The auxiliary yoke 1a is provided with a winding window 6, serves as a magnetic path for the magnetic flux passing through the main pole 2, and has an end face facing the magnetic recording medium. a is the magnetic recording medium 5
The gap (pseudo-gap) between the auxiliary yoke 1a and the main pole 2 at the opposing portion thereof is in the range of 70 to 250 μm, in this case 150 μm, and a non-conductive non-magnetic material such as glass is molded in between.

なお、後述する空隙bは運転状態の時のもので
浮上距離も含んで考えている。
It should be noted that the gap b, which will be described later, is for when the vehicle is in operation and is considered to include the flying distance.

第2図は上記のように構成された垂直磁気ヘツ
ドにおける主磁極2直下の磁気記録媒体5内での
磁界強度と擬似ギヤツプの関係を、補助ヨーク1
aの磁気記録媒体5と対向する端面と磁気記録媒
体の空隙b(第3図参照)をパラメータとして示
す特性図である。縦軸は磁束密度Tを、横軸は擬
似ギヤツプaを表わしている。擬似ギヤツプaが
70μm以下となると、主磁極2と補助ヨーク1a
の間で磁気記録媒体を通らずに漏れる磁束が増大
し、主磁極直下での垂直方向磁界強度は減少す
る。また、擬似ギヤツプaが250μm以上になる
と、補助ヨーク1aにまで誘導される磁束が減少
する。第2図からわかるように擬似ギヤツプaの
大きさが70μm以上250μm以下のときに主磁極直
下の磁界強度が大きくなり、さらに100μm以上
200μm以下のときに最も大きくなり、高い記録効
率、再生効率が期待できる。
FIG. 2 shows the relationship between the magnetic field strength and the pseudo gap in the magnetic recording medium 5 directly below the main magnetic pole 2 in the perpendicular magnetic head constructed as described above.
FIG. 4 is a characteristic diagram showing the gap b (see FIG. 3) between the end face of the magnetic recording medium 5 facing the magnetic recording medium 5 and the magnetic recording medium as parameters. The vertical axis represents the magnetic flux density T, and the horizontal axis represents the pseudo gap a. Pseudo gap a
If it is less than 70 μm, the main magnetic pole 2 and the auxiliary yoke 1a
The magnetic flux that leaks without passing through the magnetic recording medium between the main magnetic poles increases, and the perpendicular magnetic field strength immediately below the main magnetic pole decreases. Further, when the pseudo gap a becomes 250 μm or more, the magnetic flux induced even to the auxiliary yoke 1a decreases. As can be seen from Figure 2, when the size of the pseudo gap a is 70 μm or more and 250 μm or less, the magnetic field strength directly under the main pole increases, and even more so when the size of the pseudo gap a is 70 μm or more and 250 μm or less.
It is largest when it is 200 μm or less, and high recording efficiency and playback efficiency can be expected.

この結果から、擬似ギヤツプaを70〜250μmに
することにより性能のよい垂直磁気ヘツドを、ま
た100〜200μmにすることにより、さらに性能の
よいものを得ることができる。
From this result, a perpendicular magnetic head with good performance can be obtained by setting the pseudo gap a to 70 to 250 .mu.m, and an even better performance can be obtained by setting the pseudo gap a to 100 to 200 .mu.m.

なお、第1図に示す垂直磁気ヘツドでは再生波
形のゴーストが長波長の記録再生を行う際には、
大きな問題となり、ノイズとなつて表われる。
In addition, in the perpendicular magnetic head shown in Fig. 1, the ghost of the reproduced waveform occurs when recording and reproducing a long wavelength.
This becomes a big problem and appears as noise.

第3図はこの発明の実施例の垂直磁気ヘツドを
示す正面図で、補助ヨーク1aの磁気記録媒体と
対向する端面と磁気記録媒体5摺動面の間に
50μm以上100μm以下の空隙bを設け、補助ヨー
ク1aの磁気記録媒体と対向する端面に平行部分
を設けたものである。図において、bは補助ヨー
ク1aと磁気記録媒体5摺動面までの距離、Cは
補助ヨーク1aの磁気記録媒体摺動面に平行な部
分の長さで、磁束が飽和しない程度に設けてい
る。
FIG. 3 is a front view showing a perpendicular magnetic head according to an embodiment of the present invention, in which there is a gap between the end surface of the auxiliary yoke 1a facing the magnetic recording medium and the sliding surface of the magnetic recording medium 5.
A gap b of 50 μm or more and 100 μm or less is provided, and a parallel portion is provided on the end surface of the auxiliary yoke 1a facing the magnetic recording medium. In the figure, b is the distance between the auxiliary yoke 1a and the sliding surface of the magnetic recording medium 5, and C is the length of the portion of the auxiliary yoke 1a parallel to the sliding surface of the magnetic recording medium, which is set to an extent that the magnetic flux is not saturated. .

第4図は上記のように構成された垂直磁気ヘツ
ドにおける主磁極2直下の磁気記録媒体5内での
磁界強度と補助ヨーク1aの磁気記録媒体5と対
向する端面と磁気記録媒体5の空隙(距離b)の
関係を擬似ギヤツプaをパラメータとして示す特
性図である。縦軸は信号に対する磁束密度T及び
ノイズに対する磁束密度Tを、横軸は補助ヨーク
と磁気記録媒体の空隙bを表わす。なお実線は記
録信号に対する磁気記録媒体内の磁束密度、破線
はゴーストによるノイズに対する磁気記録媒体内
の磁束密度を表わす。補助ヨーク1aと磁気記録
媒体の空隙bが50μm以上になると信号に対する
磁束密度はわずかしか減少しないが、ゴーストに
よるノイズに対する磁気記録媒体内の磁束密度は
急激に減少するため、また100μm以上になると信
号再生効率が低下するため、空隙bは50〜100μm
が適している。
FIG. 4 shows the magnetic field strength within the magnetic recording medium 5 directly below the main magnetic pole 2 in the perpendicular magnetic head configured as described above, the end face of the auxiliary yoke 1a facing the magnetic recording medium 5, and the gap between the magnetic recording medium 5 ( FIG. 7 is a characteristic diagram showing the relationship between the distance b) and the pseudo gap a as a parameter. The vertical axis represents the magnetic flux density T for signals and the magnetic flux density T for noise, and the horizontal axis represents the air gap b between the auxiliary yoke and the magnetic recording medium. Note that the solid line represents the magnetic flux density within the magnetic recording medium for recording signals, and the broken line represents the magnetic flux density within the magnetic recording medium for noise due to ghosts. When the gap b between the auxiliary yoke 1a and the magnetic recording medium becomes 50 μm or more, the magnetic flux density for the signal decreases only slightly, but the magnetic flux density in the magnetic recording medium for noise caused by ghosts decreases rapidly. The gap b should be 50 to 100 μm because the regeneration efficiency will decrease.
is suitable.

なお、このノイズは補助ヨーク1aの一部先端
に磁束が集中するため、コイルを鎖交する磁束数
が急激に変化するため発生する。この大きなノイ
ズの発生を防ぐため、さらに補助ヨーク1aの磁
気記録媒体5と対向する端面に磁気記録媒体摺動
面に平行な部分を磁束が飽和しない程度に設ける
とよい。
Note that this noise occurs because the magnetic flux concentrates on a part of the tip of the auxiliary yoke 1a, and the number of magnetic fluxes interlinking the coils changes rapidly. In order to prevent the generation of this large noise, it is preferable to further provide a portion parallel to the sliding surface of the magnetic recording medium on the end surface of the auxiliary yoke 1a facing the magnetic recording medium 5 to such an extent that the magnetic flux is not saturated.

〔発明の効果〕〔Effect of the invention〕

この発明は以上説明したとおり、磁性主磁極ヨ
ーク、この主磁極ヨークに設けられ、端面が磁気
記録媒体に対向する磁性主磁極、巻線用窓を設
け、上記主磁極を通る磁束の磁路となるとともに
端面が上記磁気記録媒体に対向する磁性補助ヨー
ク、及び上記巻線用窓を通つて設けられている巻
線を備えるものにおいて、上記磁気記録媒体との
対向部における上記補助ヨークと主磁極の空隙を
70〜250μmの範囲に、かつ上記補助ヨークの上記
磁気記録媒体と対向する端面と上記磁気記録媒体
の空〓を50〜100μmの範囲にすることにより、高
い記録効率、再生効率をもつ再生効率をもち、か
つ再生波形のゴーストを減少でき、その結果ノイ
ズの発生を防止できる垂直磁気ヘツドが得られる
効果がある。
As explained above, the present invention includes a magnetic main pole yoke, a magnetic main pole provided on the main pole yoke and whose end face faces the magnetic recording medium, and a winding window, and a magnetic path for magnetic flux passing through the main pole. and a magnetic auxiliary yoke whose end face faces the magnetic recording medium, and a winding provided through the winding window, wherein the auxiliary yoke and the main magnetic pole at the portion facing the magnetic recording medium. the void of
By setting the distance between the end face of the auxiliary yoke facing the magnetic recording medium and the space between the magnetic recording medium and the magnetic recording medium to be within the range of 50 to 100 μm, high recording efficiency and high playback efficiency can be achieved. This has the effect of providing a perpendicular magnetic head that can hold the magnetic head and reduce ghosts in the reproduced waveform, thereby preventing the generation of noise.

さらに、補助ヨーク1aの磁気記録媒体と対向
する端面と磁気記録媒体の空隙を50〜100μmの範
囲にすることにより、再生波形のゴーストを減少
でき、その結果ノイズの発生を防止できる垂直磁
気ヘツドが得られる。
Furthermore, by setting the gap between the end surface of the auxiliary yoke 1a facing the magnetic recording medium and the magnetic recording medium in the range of 50 to 100 μm, ghosts in the reproduced waveform can be reduced, and as a result, a perpendicular magnetic head that can prevent the generation of noise can be realized. can get.

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

第1図はこの発明に係わる垂直磁気ヘツドを示
す正面図、第2図はこの発明に係わる垂直磁気ヘ
ツドにおける主磁極直下の磁気記録媒体内での磁
界強度と擬似ギヤツプの関係を示す特性図、第3
図はこの発明の実施例の垂直磁気ヘツドを示す正
面図、第4図はこの発明の一実施例の垂直磁気ヘ
ツドにおける主磁極直下の磁気記録媒体内での磁
界強度と補助ヨークの磁気記録媒体と対向する端
面と磁気記録媒体の空隙の関係を示す特性図、第
5図は従来の垂直磁気ヘツドを示す正面図であ
る。 図において、1aは補助ヨーク、1bは主磁極
ヨーク、2は主磁極、3は巻線、5は磁気記録媒
体、6は巻線用窓、aは磁気記録媒体との対向部
における補助ヨークと主磁極の空隙(擬似ギヤツ
プ)、bは補助ヨークの磁気記録媒体と対向する
端面と磁気記録媒体の空隙である。なお、図中同
一符号は同一又は相当部分を示す。
FIG. 1 is a front view showing a perpendicular magnetic head according to the present invention, and FIG. 2 is a characteristic diagram showing the relationship between the magnetic field strength and the pseudo gap in the magnetic recording medium directly under the main magnetic pole in the perpendicular magnetic head according to the present invention. Third
The figure is a front view showing a perpendicular magnetic head according to an embodiment of the present invention, and FIG. 4 is a diagram showing the magnetic field strength within the magnetic recording medium immediately below the main pole and the magnetic recording medium of the auxiliary yoke in the perpendicular magnetic head according to an embodiment of the present invention. FIG. 5 is a characteristic diagram showing the relationship between the end face facing the magnetic recording medium and the air gap of the magnetic recording medium. FIG. 5 is a front view showing a conventional perpendicular magnetic head. In the figure, 1a is an auxiliary yoke, 1b is a main magnetic pole yoke, 2 is a main magnetic pole, 3 is a winding, 5 is a magnetic recording medium, 6 is a winding window, and a is an auxiliary yoke at the part facing the magnetic recording medium. The gap (pseudo gap) between the main pole and b is the gap between the end face of the auxiliary yoke facing the magnetic recording medium and the magnetic recording medium. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】 1 磁性主磁極ヨーク、この主磁極ヨークに設け
られ、端面が磁気記録媒体に対向する磁性主磁
極、巻線用窓を設け、上記主磁極を通る磁束の磁
路となるとともに端面が上記磁気記録媒体に対向
する磁性補助ヨーク、及び上記巻線用窓を通つて
設けられている巻線を備えるものにおいて、上記
磁気記録媒体との対向部における上記補助ヨーク
と主磁極の空〓を70〜250μmの範囲にし、かつ上
記補助ヨークの上記磁気記録媒体と対向する端面
と上記磁気記録媒体の空〓を50〜100μmの範囲に
したことを特徴とする垂直磁気ヘツド。 2 磁気記録媒体との対向部における上記補助ヨ
ークと主磁極の空〓を100〜200μmの範囲にした
ことを特徴とする特許請求の範囲第1項記載の垂
直磁気ヘツド。
[Scope of Claims] 1. A magnetic main pole yoke, which is provided with a magnetic main pole whose end face faces the magnetic recording medium, and a winding window, which serves as a magnetic path for magnetic flux passing through the main pole. and a magnetic auxiliary yoke whose end face faces the magnetic recording medium, and a winding provided through the winding window, wherein the auxiliary yoke and the main magnetic pole are connected at the portion facing the magnetic recording medium. 1. A perpendicular magnetic head, characterized in that the gap is in the range of 70 to 250 μm, and the gap between the end face of the auxiliary yoke facing the magnetic recording medium and the magnetic recording medium is in the range of 50 to 100 μm. 2. The perpendicular magnetic head according to claim 1, characterized in that the space between the auxiliary yoke and the main magnetic pole at the portion facing the magnetic recording medium is in the range of 100 to 200 μm.
JP9991285A 1985-05-09 1985-05-09 Vertical magnetic head Granted JPS61258312A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9991285A JPS61258312A (en) 1985-05-09 1985-05-09 Vertical magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9991285A JPS61258312A (en) 1985-05-09 1985-05-09 Vertical magnetic head

Publications (2)

Publication Number Publication Date
JPS61258312A JPS61258312A (en) 1986-11-15
JPH0439729B2 true JPH0439729B2 (en) 1992-06-30

Family

ID=14259984

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9991285A Granted JPS61258312A (en) 1985-05-09 1985-05-09 Vertical magnetic head

Country Status (1)

Country Link
JP (1) JPS61258312A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0315361B1 (en) * 1987-10-30 1994-01-26 Seagate Technology, Inc. Magnetic head for perpendicular magnetic recording system and process

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54103331A (en) * 1978-02-01 1979-08-14 Sony Corp Production of magnetic head
JPS6029909A (en) * 1983-07-28 1985-02-15 Matsushita Electric Ind Co Ltd Magnetic head

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54103331A (en) * 1978-02-01 1979-08-14 Sony Corp Production of magnetic head
JPS6029909A (en) * 1983-07-28 1985-02-15 Matsushita Electric Ind Co Ltd Magnetic head

Also Published As

Publication number Publication date
JPS61258312A (en) 1986-11-15

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