JPS60256908A - Thin film magnetic head - Google Patents

Thin film magnetic head

Info

Publication number
JPS60256908A
JPS60256908A JP11254984A JP11254984A JPS60256908A JP S60256908 A JPS60256908 A JP S60256908A JP 11254984 A JP11254984 A JP 11254984A JP 11254984 A JP11254984 A JP 11254984A JP S60256908 A JPS60256908 A JP S60256908A
Authority
JP
Japan
Prior art keywords
magnetic
thin film
permeable
film
magnetically permeable
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
JP11254984A
Other languages
Japanese (ja)
Inventor
Hiroshi Yoda
養田 広
Kiyoshi Sasaki
清志 佐々木
Kazuo Nakamura
和夫 中村
Nobumasa Kaminaka
紙中 伸征
Tomoaki Izumi
智紹 泉
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 JP11254984A priority Critical patent/JPS60256908A/en
Publication of JPS60256908A publication Critical patent/JPS60256908A/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
    • G11B5/3906Details related to the use of magnetic thin film layers or to their effects
    • G11B5/3916Arrangements in which the active read-out elements are coupled to the magnetic flux of the track by at least one magnetic thin film flux guide
    • G11B5/3919Arrangements in which the active read-out elements are coupled to the magnetic flux of the track by at least one magnetic thin film flux guide the guide being interposed in the flux path

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

Abstract

PURPOSE:To reproduce a signal efficiently up to a high recording density by forming a magnetic gap oppositely in facing with a magnetic recording medium and specifying the ratio of the thickness of the permeable thin film to the length of the magnetic air gap in a couple of magnetic cores from one permeable thin film. CONSTITUTION:One side core is formed by imbedding a nonmagnetic substance 12 such as glass to a permeable substance 11. An MR element 15 comprising a permeable film 13 and a conductive film 14 is coupled magnetically to the surface of the permeable substance 11 via a nonmagnetic insulating film 16. The other end of the MR element 15 is coupled magnetically with the permeable thin film core 17 made of an amorphous magnetic film or the like via the nonmagnetic insulation film 16. The magnetic gap length GL formed by the permeable substance 11 and the permeable thin film core 17 and the thickness T of the thin film cre 17 have a relation of T/GL=0.5-2. Since the MR element is inserted in a magnetic path having magnetic air gap formed with the permeable substance 11 and the permeable thin film core 17 as both ends, the increase in the magnetic resistance of the magnetic path is less and an excellent characteristic is obtained.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、高密度磁気記録媒体の再生に用いる薄膜磁気
ヘッドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a thin-film magnetic head used for reproducing high-density magnetic recording media.

従来例の構成とその問題点 電磁変換表子、たとえば磁気抵抗効果素子(以下rMR
素子」ど称り)を用いた[q生ヘッドとして、従来、第
1図に−示すような、リング型ヘッドの磁路中にMR累
子を電気的に絶縁しで挿入しICヘッドがあった。第1
図において、1はフエライ4−などの透磁性材、2は非
磁性材、3は非磁性絶縁材、4はパーマロイなどの磁気
抵抗効果を有する透磁性膜、5は透磁性膜4とどもにM
R素子6を構成する導電性薄膜、7はパーマロイなどの
透磁性体である。通常、磁気空隙長GLは0.3μ而、
−7ラツクスガイド厚Tはリング動作には厚い方が望ま
しいが実用的に1.5μm程度の値が選ばれる。
Conventional structure and its problems Electromagnetic transducer, for example, magnetoresistive element
Conventionally, an IC head has been used as a q-type head using an electrically insulated MR element inserted into the magnetic path of a ring-shaped head, as shown in Figure 1. Ta. 1st
In the figure, 1 is a magnetically permeable material such as Ferray 4-, 2 is a non-magnetic material, 3 is a non-magnetic insulating material, 4 is a permeable film having a magnetoresistive effect such as permalloy, and 5 is a magnetically permeable film 4. M
The conductive thin film 7 constituting the R element 6 is a magnetically permeable material such as permalloy. Normally, the magnetic gap length GL is 0.3μ,
-7 Lux guide thickness T is preferably thicker for ring operation, but for practical purposes a value of about 1.5 μm is selected.

このヘッドで面内記録媒体に記録された信号磁化を再生
する揚台、磁気ギャップ両端の磁位差に応じた磁束が流
れ、MR素子6により抵抗変化として検出される。記録
密麿特性を規定覆るものは磁気空隙長である。
This head reproduces the signal magnetization recorded on the longitudinal recording medium, and a magnetic flux flows in accordance with the magnetic potential difference between both ends of the magnetic gap, which is detected by the MR element 6 as a resistance change. What determines the recording density characteristics is the magnetic gap length.

一方、面内記録と比べて高密度記録の可能性のある垂直
記録媒体に記録された信号磁化を再生するためには、第
2図に示すようh1パーマロイなどの透磁性膜8とフェ
ライトなどの透磁性体9及びコイル10などからなる補
助磁極励磁型のヘッドが用いられている。
On the other hand, in order to reproduce the signal magnetization recorded on a perpendicular recording medium, which has the possibility of higher density recording than longitudinal recording, it is necessary to An auxiliary magnetic pole excitation type head consisting of a magnetically permeable material 9, a coil 10, etc. is used.

ところで、同一のm器で異なる記録媒体、たとえば面内
と垂直との双方の記録済テープを再生しようとする場合
、同一の再生ヘッドで異なる記録媒体を再生できること
が望ましいが、第1図に示すヘッドで垂直記録媒体を再
生した場合、第3図に示すように、磁気空隙長による凹
よりも低い記録密度から7ラツクスガイドwrに対応し
た記録密度特性の凹凸を生じ、低記録密度でしか使用で
きない。一方、第2図に示Jヘッドで面内記録媒体を再
生した場合、磁束の捕集効率が悪く小さな出力しか得ら
れないので実用は困ガである。
By the way, when trying to play back different recording media with the same device, for example, both in-plane and perpendicular recorded tapes, it is desirable to be able to play back different recording media with the same playback head. When a perpendicular recording medium is reproduced with a head, as shown in Figure 3, unevenness of recording density characteristics corresponding to the 7 lux guide WR occurs from a recording density lower than the concave due to the magnetic gap length, and it can only be used at low recording densities. . On the other hand, when reproducing a longitudinal recording medium using the J head shown in FIG. 2, the magnetic flux collection efficiency is poor and only a small output can be obtained, making it difficult to put it into practical use.

、発明の目的 本発明は上記従来の欠点を解消するもので、面内、垂直
いずれの記録媒体に記録された信号磁化も効率良くしか
も高記録密度まで再生可能な薄膜磁気ヘッドを提供する
ことを目的とする。
OBJECTS OF THE INVENTION The present invention solves the above-mentioned conventional drawbacks, and aims to provide a thin-film magnetic head that can efficiently reproduce signal magnetization recorded on either in-plane or perpendicular recording media and at high recording densities. purpose.

発明の構成 上記目的を達成するため、本発明の薄II!磁気へ゛ラ
ドは、磁気記録媒体に面しC互いに相対向して磁気空隙
を形成しかつ一方が透磁性薄膜からなる一対の磁気コア
と、この一対の狂1気コアをっなぐ磁路中に配置された
電磁変換素子とを備え、前記透磁性薄膜の厚さに対゛す
る磁気空隙の長さの比を0.5〜2に設定し1.:もの
である。
Structure of the Invention In order to achieve the above object, the thin II! The magnetic helad includes a pair of magnetic cores that face the magnetic recording medium and face each other to form a magnetic gap, one of which is made of a magnetically permeable thin film, and a magnetic path that connects this pair of crazy cores. 1. The ratio of the length of the magnetic gap to the thickness of the magnetically permeable thin film is set to 0.5 to 2. :It is something.

かかる構成によれば、従来!1!自記録媒体に記録され
た信号磁化を再生した場合に生じていた記録密度特性の
凹凸は、最初の凹を磁気空隙により生じる凹とほば同じ
波長にできるため、実用範囲内でなくなり、平坦な特性
が杓られる。従って面内記録媒体はもちろんのこと、垂
直記録媒体ら実用的に再生可能となるのである。
According to this configuration, conventional! 1! The unevenness of the recording density characteristics that occurs when reproducing signal magnetization recorded on the own recording medium is eliminated from the practical range because the initial depression can be made to have almost the same wavelength as the depression caused by the magnetic gap, and it becomes flat. Characteristics are exploited. Therefore, it is possible to practically reproduce not only longitudinal recording media but also perpendicular recording media.

実施例の説明 以下、本発明の一実施例について、図面に基づいて説明
する。
DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings.

第4図は本発明の一実施例における薄膜磁気ヘッドの断
面図で、11はMn−;lnフェライトなどの透磁性体
であり、この透磁性体11にはガラスなどの非磁性材1
2が埋込まれて片側のコアを形成している。パーマロイ
などの磁気抵抗効果を0づる透磁性膜13と金やアルミ
ニウムなどの導電性膜14とよりなるMR素子15は、
SiO2などの非磁性絶縁膜16を介して透磁性体11
の表面に磁気的に結合するような位置に形成されている
。非磁性絶縁膜16は、透磁性体11がNi7nフエラ
イi〜のような高抵抗であれば必らずしも必要ではない
。MR素子15の他端は非磁性絶縁膜16を介して、パ
ーマロイやアモルファス磁性膜などからなる透磁性薄膜
コア17と磁気的に結合している。透磁性体11と透磁
性薄膜コア17とにより形成される磁気空隙超GLは0
.25μmであり、透磁性薄膜コア11の厚さTも0.
25μ而である。さらにSiO2などの非磁性絶縁膜を
介して感光性ガラスやチタン酸バリウムなどのカバーが
接着され(図示せず)、薄lll!!磁気ヘッドとなる
。本実施例ではM R素子15は直接透磁性体11の溝
端と磁気的に結合しているが、透磁性膜13を介しても
よく、要するに、−透磁性体11と透磁性薄膜コア17
トの形成する磁気空隙を両端とする磁路中に非磁性絶縁
膜16を介して挿入されでいることが東要なのである1
゜ 上記構成の薄!B! It気ヘッドぐメタルパウダ・テ
ープなどの面内記録媒体に記録された信号磁化を再生す
る場合、磁気空隙長0.25μ肌のリング型ヘッドとし
て動作Jるため、短波■【の信号まで良好に再生する。
FIG. 4 is a cross-sectional view of a thin film magnetic head according to an embodiment of the present invention, in which 11 is a magnetically permeable material such as Mn-;ln ferrite, and the magnetically permeable material 11 is made of a non-magnetic material such as glass.
2 is embedded to form one side of the core. The MR element 15 is composed of a magnetically permeable film 13 such as permalloy that has no magnetoresistive effect and a conductive film 14 such as gold or aluminum.
A magnetically permeable material 11 is inserted through a non-magnetic insulating film 16 such as SiO2.
is formed at a position where it is magnetically coupled to the surface of the The nonmagnetic insulating film 16 is not necessarily necessary if the magnetically permeable material 11 has a high resistance such as Ni7n ferrite. The other end of the MR element 15 is magnetically coupled via a nonmagnetic insulating film 16 to a magnetically permeable thin film core 17 made of permalloy, an amorphous magnetic film, or the like. The magnetic gap GL formed by the magnetically permeable body 11 and the magnetically permeable thin film core 17 is 0.
.. The thickness T of the magnetically permeable thin film core 11 is also 0.25 μm.
It is 25μ. Furthermore, a cover made of photosensitive glass or barium titanate (not shown) is adhered via a non-magnetic insulating film such as SiO2, and thin lll! ! It becomes a magnetic head. In this embodiment, the MR element 15 is directly magnetically coupled to the groove end of the magnetically permeable body 11, but it may be coupled via the magnetically permeable film 13.
The key point is that the magnetic field is inserted through the non-magnetic insulating film 16 into the magnetic path whose ends are the magnetic gaps formed by the magnetic field.
゜The above structure is thin! B! When reproducing signal magnetization recorded on an in-plane recording medium such as metal powder or tape, the head operates as a ring-shaped head with a magnetic gap length of 0.25 μm, so even shortwave signals can be reproduced well. Reproduce.

一方、コバル]−クロム/パーマロイなどの垂にFlW
A記録媒体を再イ1する場合、コア厚の薄い透磁性薄膜
コア17の方が主磁極として抛らき、その下の記録媒体
の磁化の方向に応じた磁束をMR素子15に導びき、他
の側のコアより記録媒体のパーマロイなどの透磁性膜を
通して戻る閉磁路を形成する。この場合、コア厚が0.
25μmと薄いため、記録密度特性は第L1図に示ずよ
うに 100K B P 1以上の高域まで再生可能で
ある。
On the other hand, FlW
When reproducing the A recording medium, the thin magnetically permeable thin film core 17 serves as the main magnetic pole, and guides magnetic flux to the MR element 15 in accordance with the direction of magnetization of the recording medium below it. A closed magnetic path is formed that returns from the core on the side of the recording medium through a magnetically permeable film such as permalloy of the recording medium. In this case, the core thickness is 0.
Since it is as thin as 25 μm, the recording density characteristic can be reproduced up to a high frequency range of 100K B P 1 or more, as shown in FIG. L1.

なお上記実施例では、磁気空隙長OLと透磁性薄膜コア
厚Tとが等しい例を示した。垂直記録媒体を再生した場
合、磁気空隙による記録密度特性の最初の凹は11〜1
.27の波長で、磁気コア厚によるものは11〜1.3
Ql、の波長で起きる。従って、GLとTとをほぼ等し
くすれば、両方の凹は同じ波長に生じ、垂直記録媒体を
再生した場合にも最も平坦な記録密度特性が得られるが
、実用的にはTとGLとの比は、ヘッドの能率や記録媒
体の特性などを考慮して0,5〜2の範囲内で選ばれる
。すなわちG[−の方を人さくすれば面内記録媒体再生
時の出力が増加し、];の方を大きくすれば垂直記録媒
体再生時の出力が増加するのrlそれぞれの記録媒体の
特性に応じて2番目の凹の生じない範囲で選ばれる。
In the above embodiment, an example was shown in which the magnetic gap length OL and the magnetically permeable thin film core thickness T were equal. When reproducing a perpendicular recording medium, the first concavity of the recording density characteristic due to the magnetic gap is 11 to 1.
.. 27 wavelengths, depending on magnetic core thickness 11-1.3
It occurs at a wavelength of Ql. Therefore, if GL and T are made approximately equal, both depressions will occur at the same wavelength, and the flattest recording density characteristic will be obtained even when reproducing a perpendicular recording medium. The ratio is selected within the range of 0.5 to 2, taking into consideration the efficiency of the head and the characteristics of the recording medium. In other words, if G [- is made more sensitive, the output when reproducing a longitudinal recording medium increases, and ]; when it is made larger, the output when reproducing a perpendicular recording medium is increased.rl Depending on the characteristics of each recording medium. Accordingly, it is selected within a range that does not cause the second concavity.

また上記実施例においては、透磁性薄膜コア11に対向
する磁気コアすなわ#l)透磁性体11としてフェライ
トよりなるものを用いたが、これは透磁性薄膜コア17
の厚さに比べて充分厚ければJ、く、非磁性基板上に透
磁性アモルファス膜などを形成したものでもよい。
Further, in the above embodiment, a material made of ferrite was used as the magnetic core 11 facing the magnetically permeable thin film core 11, that is, the magnetically permeable body 11;
A magnetically permeable amorphous film or the like formed on a nonmagnetic substrate may be used as long as it is sufficiently thicker than the thickness of the substrate.

透磁性薄膜コア17の厚さ及0び磁気空隙の長さは、面
内記録媒体と比べて短波長まで特性の良い垂直記録媒体
の信号磁化も再生するため、垂直記録の方が特性の良い
0.5μm以下に設定すれば特に効果がある。
Regarding the thickness of the magnetically permeable thin film core 17 and the length of the magnetic gap, perpendicular recording has better characteristics because it also reproduces the signal magnetization of perpendicular recording media, which has better characteristics up to shorter wavelengths than longitudinal recording media. It is particularly effective if the thickness is set to 0.5 μm or less.

次に本発明の第2の実施例について第6図を用いて説明
する。18はNi7nフJライトなどの高抵抗透磁性体
、19はIn’Sb’a:どの薄膜20と導電性薄膜の
リード線21とにより構成されるホール効果素子、22
は八Ω203などの非磁性絶縁材、23はセンダストな
どの透磁性膜である。前記透磁性膜23のρさは、先@
rは0.3μTn、 Fあるが、ホール効果素子19に
対向する上部では磁気抵抗を減らづために1μmである
。また磁気空隙長は0,3μTrLセある。
Next, a second embodiment of the present invention will be described using FIG. 6. 18 is a high-resistance magnetic permeable material such as Ni7n FJ-lite, 19 is In'Sb'a: a Hall effect element composed of a thin film 20 and a conductive thin film lead wire 21, 22
is a non-magnetic insulating material such as 8Ω203, and 23 is a magnetically permeable film such as Sendust. The ρ of the magnetically permeable film 23 is
Although r is 0.3 μTn, F, the upper portion facing the Hall effect element 19 is 1 μm in order to reduce magnetic resistance. Further, the magnetic gap length is 0.3 μTrL.

このよ)に電磁変換素子としてホール効果素子19を用
いると、磁、路と垂直にホール効果素子薄膜を段間する
こととなるので、MR素子のように薄膜長手方向を磁路
に挿入する場合に比べて、磁路の磁気抵抗の増加が少4
Tり、良好な特性が得られる。
When the Hall effect element 19 is used as an electromagnetic transducer in this case, the Hall effect element thin film is interposed perpendicular to the magnetic path, so when inserting the longitudinal direction of the thin film into the magnetic path like an MR element, Compared to 4, the increase in magnetic resistance of the magnetic path is small.
T, good characteristics can be obtained.

発明の詳細 な説明したように本発明にJ7れば、面内記録媒体と垂
直記録媒体との双方を、特性を損なうことなしに、充分
高密痕なものまで良好に再生づることができる。
As described in detail, according to the present invention, it is possible to successfully reproduce both longitudinal recording media and perpendicular recording media, even those with sufficiently high density marks, without impairing their characteristics.

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

第1図は従来の面内記録媒体再生用の薄膜磁気ヘッドの
断面図、第2図は従来の垂直記録媒体再生用の薄膜磁気
ヘッドのmi ili図、第33図は第1図に示す薄膜
磁気ヘッドにより垂直記録媒体を再生した場合の記録密
度特性の説明図、第4図は本発明の一実施例におGJ8
酵股磁気ヘッドの断面図、第5図は同博膜磁気ヘッドに
まり重両記録媒体を再生した場合の記録密度特性の説明
図、第6図は本発明の別の実施例にお【ノる薄膜磁気ヘ
ッドの断面図である。 11・・・透磁性体、15・・・磁気抵抗効51+素子
、17・・・透磁性簿膜コア、18・・・高抵抗透磁性
体、19・・・ホール効果素子、23・・・透磁性膜 代理人 森 本 義 弘 第1図 i、2図 第3図 ン銀密度 第4図 第51 8と仰庄度 第6図
Fig. 1 is a cross-sectional view of a conventional thin film magnetic head for reproducing in-plane recording media, Fig. 2 is a mi ili diagram of a conventional thin film magnetic head for reproducing perpendicular recording media, and Fig. An explanatory diagram of recording density characteristics when a perpendicular recording medium is reproduced by a magnetic head, FIG.
5 is an explanatory diagram of the recording density characteristics when a double recording medium is played back by the Hakuba magnetic head, and FIG. 6 is a cross-sectional view of another embodiment of the present invention. 1 is a cross-sectional view of a thin film magnetic head. DESCRIPTION OF SYMBOLS 11... Magnetically permeable body, 15... Magnetoresistive effect 51+ element, 17... Magnetically permeable film core, 18... High resistance magnetic permeable body, 19... Hall effect element, 23... Magnetically Permeable Membrane Agent Yoshihiro Morimoto Figures 1, 2, 3, Silver Density, Figure 4, 51 8, and Emphasis, Figure 6

Claims (1)

【特許請求の範囲】 1、磁気記録媒体に面して互いに相対向して磁気空隙を
形成しかつ一方が透磁性薄膜からなる一対の磁気コアと
、この一対の磁気コアをつなぐ磁路中に配置された電磁
変換素子とを備え、前記透磁性薄膜の庁さに対する磁気
空隙の長さの比を0.5〜2に設定した薄膜磁気ヘッド
。 2、透磁性薄膜の厚ざと磁気空隙の長さとをいずれも0
.5μm以下とした特許請求の範囲第1項記載の薄膜磁
気ヘッド。
[Claims] 1. A pair of magnetic cores facing each other facing the magnetic recording medium to form a magnetic gap, one of which is made of a magnetically permeable thin film, and a magnetic path connecting the pair of magnetic cores. A thin film magnetic head comprising: an electromagnetic transducer arranged in the magnetic field, and a ratio of the length of the magnetic gap to the height of the magnetically permeable thin film is set to 0.5 to 2. 2. The thickness of the magnetically permeable thin film and the length of the magnetic gap are both 0.
.. A thin film magnetic head according to claim 1, wherein the thickness is 5 μm or less.
JP11254984A 1984-05-31 1984-05-31 Thin film magnetic head Pending JPS60256908A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11254984A JPS60256908A (en) 1984-05-31 1984-05-31 Thin film magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11254984A JPS60256908A (en) 1984-05-31 1984-05-31 Thin film magnetic head

Publications (1)

Publication Number Publication Date
JPS60256908A true JPS60256908A (en) 1985-12-18

Family

ID=14589436

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11254984A Pending JPS60256908A (en) 1984-05-31 1984-05-31 Thin film magnetic head

Country Status (1)

Country Link
JP (1) JPS60256908A (en)

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