JPS58182125A - Thin film magnetic head - Google Patents

Thin film magnetic head

Info

Publication number
JPS58182125A
JPS58182125A JP6591782A JP6591782A JPS58182125A JP S58182125 A JPS58182125 A JP S58182125A JP 6591782 A JP6591782 A JP 6591782A JP 6591782 A JP6591782 A JP 6591782A JP S58182125 A JPS58182125 A JP S58182125A
Authority
JP
Japan
Prior art keywords
magnetic field
lead
magnetic head
thin film
bias magnetic
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
JP6591782A
Other languages
Japanese (ja)
Inventor
Shuzo Hakoda
箱田 修三
Kazuo Yokoyama
和夫 横山
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 JP6591782A priority Critical patent/JPS58182125A/en
Publication of JPS58182125A publication Critical patent/JPS58182125A/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
    • G11B5/33Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
    • G11B5/39Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects
    • G11B5/3903Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects using magnetic thin film layers or their effects, the films being part of integrated structures

Abstract

PURPOSE:To apply optimum bias magnetic fields to plural magneto-resistance effect element independently, by adjusting a current for applying the bias magnetic fields at the inside of a head. CONSTITUTION:The magneto-resistance effect element 14 is arranged on a conductor layer 12 as a path for the bias magnetic field current with an insulator layer 13 between. Signal lead-out parts 15 are formed at both ends of the magneto-resistance effect element 14. The serial structures of plural resistors 17 are formed at both ends of the conductor layer 12 for applying the bias magnetic field to the magneto-resistance effect element 14, and plural lead terminal parts 18 are provided between the resistors 17 to constitute lead parts 16, respectively. Consequently, lead lines are connected selectively to one of lead terminal parts 18 to vary the current value of the current for the bias magnetic field stepwise, and even when individual magneto-resistance effect elements 14 have variance in characteristics, an optimum bias point is selected inside of the head.

Description

【発明の詳細な説明】 本発明は薄膜磁気ヘッド、特に多数の磁気抵抗効果型子
全備えた多チャンネル?4膜磁気ヘッドにおいて、各チ
ャンネルの磁気抵抗効果素子にバイアス磁界を与えるた
めの構造に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a thin film magnetic head, particularly a multi-channel magnetic head equipped with a large number of magnetoresistive elements. The present invention relates to a structure for applying a bias magnetic field to a magnetoresistive element of each channel in a four-film magnetic head.

磁気抵抗効果素子は、信号磁界に対して磁性体の抵抗値
が変化する現象を利用した素子であシ、一定磁界でその
変化率が一定となる。したがって1ぎ号磁界に対して線
型の抵抗値変化を得るために一般に信号磁界に対して一
定のバイアス磁界を加えている。このバイアスを印刀口
する方法には、固だ磁石により外部から磁気抵抗効果素
子に磁界を加える方法、磁気抵抗効果型素子と並列に接
続した導電体層に電流を分流させ磁界を加える方法、さ
らには磁気抵抗効果素子とは独立にと扛と隣接した導′
亀体層を設け、これに流す電流による磁界を磁気抵抗効
果素子に印加する方法などがある。
A magnetoresistive element is an element that utilizes a phenomenon in which the resistance value of a magnetic material changes in response to a signal magnetic field, and the rate of change is constant in a constant magnetic field. Therefore, a constant bias magnetic field is generally applied to the signal magnetic field in order to obtain a linear change in resistance value with respect to the 1-magnitude magnetic field. Methods for applying this bias include applying a magnetic field to the magnetoresistive element from the outside using a solid magnet, applying a magnetic field by shunting current to a conductive layer connected in parallel with the magnetoresistive element, and is independent of the magnetoresistive element and the conductor adjacent to the magnetoresistive element.
There is a method in which a turtle layer is provided and a magnetic field caused by a current flowing through the turtle layer is applied to the magnetoresistive element.

これらの方法の原理的な構成はそれぞ′n第1図第2図
、および第3図に示す。すなわち、第1図はml疋磁石
により外部から磁気抵抗効果素子にバイアス磁界を加え
る方法の原理的な構成を示す。
The basic configurations of these methods are shown in FIG. 1, FIG. 2, and FIG. 3, respectively. That is, FIG. 1 shows the basic configuration of a method for applying a bias magnetic field to a magnetoresistive element from the outside using a ml magnet.

図に示すように、高透磁率磁性体よりなる磁気抵抗効果
菓子10両端に、信号取り出しのためのリード部2が設
けられており、後部にバイアス磁界を加えるための永久
磁石゛3力畑己置されている。第2図は磁気抵抗効果素
子と並列に配した導電体膜に電流を分流させて磁界を加
える方法の原理的な構成を示し、導電体層4と磁気抵抗
効果素子5とを重ね合わせ、それらの両端に、信号取り
出しとさらには導電体層4に電流を分流し、磁界を発生
させるためのリード部6がそnぞれ設けらnている。5
g3図は磁気抵抗効果素子とは独立にこれと隣接した導
電体j−を設け、これに流す′電流による磁界を磁気抵
抗効果索子に加える方法の原理的な構成を示している。
As shown in the figure, a magnetoresistive confectionery 10 made of a high magnetic permeability magnetic material is provided with lead parts 2 at both ends for signal extraction, and a permanent magnet 2 for applying a bias magnetic field at the rear. It is placed. Figure 2 shows the basic configuration of a method of applying a magnetic field by branching a current to a conductive film arranged in parallel with a magnetoresistive element, in which a conductive layer 4 and a magnetoresistive element 5 are superimposed and Lead portions 6 are provided at both ends of the conductive layer 4 to take out signals, furthermore, to shunt current to the conductor layer 4 and generate a magnetic field. 5
Figure g3 shows the basic structure of a method in which a conductor j- is provided independently of and adjacent to the magnetoresistive element, and a magnetic field caused by a current flowing through it is applied to the magnetoresistive element.

図に示すように導電体ノー7の上に絶縁7* 8 ’に
介して磁気抵抗効果素子9を重ね信号J451り出しの
ために磁気抵抗効果素子9の両端にリード部10が、ま
た磁気抵抗効果素子9にバイアス磁界を加えるための導
電体ノー7に電流を流すためにリード部11がそnぞn
設けら扛ている。
As shown in the figure, the magnetoresistive element 9 is placed on the conductor No. 7 through an insulator 7*8', and lead portions 10 are placed at both ends of the magnetoresistive element 9 for outputting the signal J451. The lead portion 11 is connected to the conductor 7 for applying a bias magnetic field to the effect element 9.
It's not set up.

ヰ ここで前者の揚台では基本的に多数ある各磁気抵抗効果
素子に磁気抵抗効果素子構成による一定の磁界が加わる
のに対して、後者ではバイアス磁界4電体層を各磁気抵
抗効果素子それぞ扛に対応させて設け、こnに流す電流
値を調整することにより、独立にバイアス磁界を調整す
ることができる。したがって、独立バイアス式の薄膜磁
気抵抗効果型磁気ヘッドでは、磁気抵抗効果素子の磁気
特性にばらつきがあっても、バイアス点′ff:最適に
選ぶことによって、その特性を最大限引出すことができ
る。
ヰHere, in the former case, a fixed magnetic field is basically applied to each of the many magnetoresistive elements by the magnetoresistive element configuration, whereas in the latter case, the bias magnetic field is applied to each of the four magnetoresistive elements. The bias magnetic field can be adjusted independently by providing a bias magnetic field corresponding to the magnetic field and adjusting the value of the current flowing therethrough. Therefore, in the independent bias type thin-film magnetoresistive magnetic head, even if there are variations in the magnetic properties of the magnetoresistive element, by optimally selecting the bias point 'ff, the properties can be maximized.

しかしながら、このような利点を有する独立バイアス式
磁気ヘッドもそのバイアス磁界電流を、こ扛に接続する
外部回路で調整した場合、多数の磁気記録再生装置の間
の互換性、すなわち磁気ヘッドを交換する場合の互換性
が損われるという欠点がある。
However, an independent bias type magnetic head with such advantages can also be compatible with a large number of magnetic recording and reproducing devices if its bias magnetic field current is adjusted by an external circuit connected to the magnetic head, that is, the magnetic head can be replaced. The disadvantage is that compatibility is compromised.

本発明は、上述の問題を解決したものであって複数の煩
気抵抗効果累子そnぞnにバイアス磁界を与えるための
専一体ノーに流す電流をヘッド内部で調整できるよう構
成した博模飾気ヘッドを提供することを目的とする。こ
の薄膜磁気ヘッドにおいては、互換性があり、かつ各磁
気抵抗効果素子に対して独立に最適のバイアス磁界を印
加することができるため、特性に(資)れ、さらに各磁
気抵抗効果素子の磁気特1生のばらつきを吸収すること
ができるために、製造時の特性歩留が縄いという利点が
ある。
The present invention solves the above-mentioned problem, and is a model having a structure in which the current flowing through a dedicated unit for applying a bias magnetic field to a plurality of resistance effect elements can be adjusted inside the head. The purpose is to provide an elegant head. This thin-film magnetic head is compatible and can independently apply an optimal bias magnetic field to each magnetoresistive element, which contributes to the characteristics and further improves the magnetic field of each magnetoresistive element. Since it is possible to absorb variations in characteristics, it has the advantage of improving the characteristic yield during manufacturing.

次に本発明の薄膜磁気ヘッドの実施例について図面を用
いて、mAに述べる。
Next, embodiments of the thin film magnetic head of the present invention will be described in terms of mA with reference to the drawings.

第4図はその一実施例の要部斜視図であり、バイアスo
ii界用電流の通路となる導電体層の上に絶縁ノー全弁
して磁気抵抗効果索子となる磁性体ノーを設けた薄膜磁
気ヘッドにおいて、前記導電体ノーのリード部が複数個
の抵抗体の直列構造全なし、上記抵抗体間に複数個のリ
ード端子部を設け、IJ−ドaを選択的に前記端子部に
接続することによりバイアス磁界用電流値を段階的に可
変できるようにしたものである。図に示すように導電体
層12敏 の上に絶婦体71113’i介して磁気抵抗効果素子1
4が配置されており、この磁気抵抗効果素子14の両端
に信号取り出しのためのリード部15が設けらnている
。そして磁気抵抗効果素子14にバイアス磁界を加える
ための専′成体層12の両端にはそれぞf″Lgi、数
個の抵抗体17の直列構造をなし、抵抗体17の間に複
数個のリード端子部18が設けらnたリード部16が配
置さ扛ている。
FIG. 4 is a perspective view of essential parts of one embodiment, and shows the bias o
(ii) In a thin film magnetic head in which a magnetic material layer serving as a magnetoresistive effect cable is provided by insulating the insulation layer on a conductive layer serving as a path for a field current, the lead portion of the conductive material layer has a plurality of resistors. The current value for the bias magnetic field can be varied step by step by providing a plurality of lead terminals between the resistors and selectively connecting the IJ-door a to the terminals. This is what I did. As shown in the figure, the magnetoresistive effect element 1 is placed on the conductor layer 12 through the intervening body 71113'i.
4 is arranged, and lead portions 15 for signal extraction are provided at both ends of the magnetoresistive element 14. The dedicated layer 12 for applying a bias magnetic field to the magnetoresistive element 14 has f″Lgi at both ends thereof, several resistors 17 are connected in series, and a plurality of leads are connected between the resistors 17. A lead portion 16 provided with a terminal portion 18 is arranged.

このような構成のヘッドにおいて複数個のリード端子部
18のいずれかにリードa(図示せず)を選択的に接続
することにより、バイアス磁界用電流lIl!’r:段
階的に可変でき、個々の磁気抵抗効果索子14の特性の
ばらつきがあっても、バイアス点を最適に辿ぶことによ
って、その特性を最大限り1き出せるように構成するこ
とが、ヘッド内部でできる。
In the head having such a configuration, by selectively connecting the lead a (not shown) to one of the plurality of lead terminal portions 18, the bias magnetic field current lIl! 'r: Can be varied in stages, and even if there are variations in the characteristics of individual magnetoresistive cables 14, the structure can be configured so that the characteristics can be maximized by tracing the bias point optimally. , can be done inside the head.

捷た、抵抗体17が導電体層12を構成する物面と同一
の物質よりなる薄膜体とすることができる。たとえばこ
の物質としてチタンを用いた一合その比抵抗は660c
m程度であり、適当な抵抗体の役目を兼ねさせることが
できる。この場合には抵抗体全蒸着する工程を独立に設
ける必要がないため、工程を簡略化できる。
The resistor 17 may be a thin film made of the same material as the conductive layer 12. For example, if titanium is used as this material, its specific resistance is 660c.
m, and can also serve as a suitable resistor. In this case, there is no need to provide an independent process for completely vapor-depositing the resistor, so the process can be simplified.

次に、本発明の第2の実施クリの薄膜磁気ヘッドについ
て、第6図を用いて説明する。この実施列はリード部の
抵抗体と!−子部が、バイアス磁界用導′屯体層を構成
する物質と同一の物質よりなる博1換体であり、リード
部が抵抗体となる小寸法幅の部分と端子となる大寸法幅
の部分で構成さnてい介して磁気抵抗効果素子21が形
成されており、この磁気抵抗効果素子21の両端に悟号
取り出しのためのリード部22がそれぞ扛設けらnてい
る。
Next, a thin film magnetic head according to a second embodiment of the present invention will be described with reference to FIG. This implementation row is the resistor of the lead part! - The child part is made of the same material as the material constituting the conductor layer for bias magnetic field, and the lead part is a small width part that becomes a resistor and a large part that becomes a terminal. A magnetoresistive element 21 is formed through the magnetoresistive element 21, and lead portions 22 for taking out the Gogo are provided at both ends of the magnetoresistive element 21, respectively.

さらにこの磁気抵抗効果素子21にバイアス磁界全顎え
るための導電体層19が、複数個の抵抗体となる小寸法
幅の部分23と複数個のリード端子部となる大寸法幅の
部分24とで構成されている。
Furthermore, the conductor layer 19 for supporting the entire bias magnetic field in the magnetoresistive element 21 has a small width portion 23 that will serve as a plurality of resistors and a large width portion 24 that will serve as a plurality of lead terminal portions. It consists of

リード線ヲ選択的にリード端子部24のいずれかに選択
的に接続することにより、導電体層19に流すバイアス
08界用電流のff1uを段階的に可変できる。したが
って、個々の磁気抵抗効果素子21の特1生のばらつき
があってもそれぞれについてバイアス点を最適に選ぶこ
とができ、そ扛によってその時1生を最大限引き出すこ
とがヘッド内部でできるとともに、リード部の抵抗体と
端子部が、バイアス磁界用4電体ノーヲ構成する物質と
同一の物質により形成できるため、製造工程の大幅な簡
略化かはか扛る。
By selectively connecting the lead wire to one of the lead terminal portions 24, ff1u of the bias 08 field current flowing through the conductor layer 19 can be varied stepwise. Therefore, even if there are variations in the characteristics of the individual magnetoresistive elements 21, the bias point can be optimally selected for each magnetoresistive element 21, and by adjusting the bias point, the maximum characteristics can be brought out inside the head. Since the resistor and the terminal part can be made of the same material as the material constituting the bias magnetic field four-electric node, the manufacturing process can be greatly simplified.

磁気抵抗効果素子にバイアス磁界を印ノ用するための導
電体ノーの材質としてはチタンまたはモリブデンが適し
ている。バイアス磁界形成用導電体層は、短波長信号の
記録再生全可能とするには、できるだけ薄いものである
ことが望ましい。しかしあまり膜厚が薄くなると、製造
工程中に受ける熱履歴のため、隣接する構成膜物質の拡
散を受け、その抵抗直が大きくなる傾向にある。この点
チタンまたはモリブデンは拡散を受けにくい。また、こ
の導゛一体層は磁気抵抗効果を有する磁性体ノーととも
に記録媒体と花立に接触する構成となることもあるが、
チタンまたはモリブデンは耐犀耗性にもV扛、導′屯体
層の材質として通している。
Titanium or molybdenum is suitable as the material for the conductor for applying a bias magnetic field to the magnetoresistive element. It is desirable that the bias magnetic field forming conductive layer be as thin as possible in order to be able to record and reproduce short wavelength signals. However, if the film thickness becomes too thin, the adjacent film materials will diffuse due to the thermal history received during the manufacturing process, and the resistance will tend to increase. In this respect, titanium or molybdenum is less susceptible to diffusion. In addition, this conductive layer may be configured to contact the recording medium and the flower stand together with a magnetic material having a magnetoresistive effect.
Titanium or molybdenum is also used as a material for the V-coat and conductor layers due to its corrosion resistance.

以上のように、本発明の薄膜磁気ヘッド°は磁気抵抗効
果型磁気ヘッドの多数ある磁気抵抗効果素子VCバイア
ス磁界を与えるための導電体ノーに流す亜流を、ヘッド
内部で調贅するための構造を持つため、多数の磁気記録
再生装置の磁気ヘッドを交換する場合の互換性に曖れて
いる。そして、各磁気抵抗効果素子に対して独立に最適
のバイアス磁界を印加することができるため、特性に暖
れ、さらに各磁気抵抗効果素子の磁気%曲のばらつき全
吸収することができるため、時1生歩留の良好なもので
ある。
As described above, the thin-film magnetic head of the present invention has a structure for regulating the subcurrent flowing through the conductor for providing the magnetoresistive element VC bias magnetic field, which is present in many magnetoresistive magnetic heads, inside the head. Because of this, compatibility is unclear when replacing the magnetic heads of many magnetic recording and reproducing devices. Since the optimum bias magnetic field can be applied independently to each magnetoresistive element, the characteristics can be warmed up, and the variation in the magnetic % curvature of each magnetoresistive element can be fully absorbed, so the time It has a good one-year yield.

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

5N、1図、第2図および第3図はそnぞれ従来の薄膜
磁気ヘッドの薄膜素子の斜視図、第4図および5g5図
はそ扛ぞれ本発明の薄膜磁気ヘッドの実施例における薄
膜素子の斜視図である。 12・・・・・導電体ノー、13・・・・・絶縁体層、
14・・・・・磁気抵抗効果素子、16・・・・・ リ
ード部、・・・・・・抵抗体、24・・・・・・リード
端子部。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 2 ? 第2図 第3図 第4図 6
5N, 1, 2 and 3 are respectively perspective views of thin film elements of a conventional thin film magnetic head, and FIGS. FIG. 2 is a perspective view of a thin film element. 12...Conductor layer, 13...Insulator layer,
14... Magnetoresistive element, 16... Lead portion,... Resistor, 24... Lead terminal portion. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2? Figure 2 Figure 3 Figure 4 Figure 6

Claims (4)

【特許請求の範囲】[Claims] (1)磁気抵抗効果素子と、この磁気抵抗効果素子に印
加すべきバイアス磁界形成用の導′4E体層とをゼし、
前記導電体ノーのリード部が複e1dの抵抗体の直列構
造をなし、かつ前記抵抗体間に複数個のリード端子部金
具−しており、リード國′fc選択的VC+471記端
子部のいずれかに接続することにより、前記導電体、1
−に供給すべき電流の直を段階的に可変としたことを特
徴とする薄膜磁気ヘッド。
(1) A magnetoresistive element and a conductor layer for forming a bias magnetic field to be applied to the magnetoresistive element,
The lead part of the conductor has a series structure of multiple e1d resistors, and a plurality of lead terminal parts metal fittings are provided between the resistors, and the lead part has a plurality of lead terminal parts. The electrical conductor, 1
- A thin film magnetic head characterized in that the directivity of the current to be supplied to the magnetic head is made variable in stages.
(2)抵抗体が導電体層を構成する物質と同一の物置よ
りなる薄膜体でるること全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) A thin-film magnetic head according to claim 1, wherein the resistor is a thin-film body made of the same material as the conductor layer.
(3)リード部の抵抗体と端子部が導電体層會倒成する
物質と同一の物質よりなる薄膜体であり、前記リード部
が前記抵抗体となる小寸法幅の部分と前記端子部となる
大寸法幅の部分とで構成されてい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 resistor of the lead part and the terminal part are thin film bodies made of the same material as the material in which the conductive layer is formed, and the lead part is a thin film body made of the same material as the material in which the resistor and the terminal part are formed. 2. The thin film magnetic head according to claim 1, wherein the thin film magnetic head is comprised of a portion having a large size and width.
(4)導電体層がチタンまたはモリブデンよりなること
を特徴とする特許請求の範囲第1項、第2項または第3
項記載の薄膜磁気ヘッド。
(4) Claim 1, 2 or 3, characterized in that the conductive layer is made of titanium or molybdenum.
The thin film magnetic head described in Section 1.
JP6591782A 1982-04-19 1982-04-19 Thin film magnetic head Pending JPS58182125A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6591782A JPS58182125A (en) 1982-04-19 1982-04-19 Thin film magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6591782A JPS58182125A (en) 1982-04-19 1982-04-19 Thin film magnetic head

Publications (1)

Publication Number Publication Date
JPS58182125A true JPS58182125A (en) 1983-10-25

Family

ID=13300798

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6591782A Pending JPS58182125A (en) 1982-04-19 1982-04-19 Thin film magnetic head

Country Status (1)

Country Link
JP (1) JPS58182125A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0107982A2 (en) * 1982-10-29 1984-05-09 Sony Corporation Magnetic transducer heads utilising magnetoresistance effect
EP0725388A2 (en) * 1995-01-31 1996-08-07 Sony Corporation Magneto-resistance effect type magnetic head operable at optimum biasing point
JP2007093456A (en) * 2005-09-29 2007-04-12 Casio Comput Co Ltd Liquid residual quantity measuring device, liquid residual quantity measuring method, and electronic apparatus

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0107982A2 (en) * 1982-10-29 1984-05-09 Sony Corporation Magnetic transducer heads utilising magnetoresistance effect
EP0107982A3 (en) * 1982-10-29 1987-01-14 Sony Corporation Magnetic transducer heads utilising magnetoresistance effect
EP0725388A2 (en) * 1995-01-31 1996-08-07 Sony Corporation Magneto-resistance effect type magnetic head operable at optimum biasing point
EP0725388A3 (en) * 1995-01-31 1996-12-27 Sony Corp Magneto-resistance effect type magnetic head operable at optimum biasing point
JP2007093456A (en) * 2005-09-29 2007-04-12 Casio Comput Co Ltd Liquid residual quantity measuring device, liquid residual quantity measuring method, and electronic apparatus

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