JPS63259813A - Thin film magnetic head - Google Patents

Thin film magnetic head

Info

Publication number
JPS63259813A
JPS63259813A JP9562687A JP9562687A JPS63259813A JP S63259813 A JPS63259813 A JP S63259813A JP 9562687 A JP9562687 A JP 9562687A JP 9562687 A JP9562687 A JP 9562687A JP S63259813 A JPS63259813 A JP S63259813A
Authority
JP
Japan
Prior art keywords
gap
magnetic
head
superconductor
magnetic field
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
JP9562687A
Other languages
Japanese (ja)
Inventor
Hiroshi Yoda
養田 広
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 JP9562687A priority Critical patent/JPS63259813A/en
Publication of JPS63259813A publication Critical patent/JPS63259813A/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
    • G11B5/3109Details
    • G11B5/313Disposition of layers
    • G11B5/3143Disposition of layers including additional layers for improving the electromagnetic transducing properties of the basic structure, e.g. for flux coupling, guiding or shielding

Landscapes

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

Abstract

PURPOSE:To enable efficient reproduction by using a ceramics superconductor to form a nonmagnetic material of a ring type magnetic head forming a magnetic gap. CONSTITUTION:A magnetic core 2 which consists of a ferromagnetic material such as Co, Nb and Zr and is sandwiched by a ceramics base material 1 is joined by gap surfaces. The superconductor 3 consisting of Y-Ba-Cu-O is formed to 0.3mum thickness in the front part gap facing a recording medium and is adhered by low melting point glass 4 of 0.05mum thickness formed in the gap part between the front part and the rear part. A winding window 5 is provided. The Y-Ba-Cu-O of the gap material attains a superconducting state and the infiltration of magnetic fluxes therein is prevented by a Meissner effect under the magnetic field of <=1 lower critical Hc when this head is cooled down to <=80 deg.K. The magnetic field in the gap generated by the recording medium at the time of reproduction is extremely small and does not, therefore, exceed the lower critical magnetic field. Since the superconducting state is maintained, the magnetic fluxes leaking in the gap are eliminated.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は狭ギャップであっても高能率な再生特性を有す
る磁気ヘッドに関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magnetic head having highly efficient reproduction characteristics even with a narrow gap.

従来の技術 磁気記録媒体への信号の記録再生のためにリング型の磁
気ヘッドが広く用いられている。リング型の磁気ヘッド
の構造を第3図に示す。セラミックス基板21に挟まれ
たCoNbZrなどの強磁性体よりなる磁気コア22が
、ギャップ面で接合されている。ギャップ材23として
は、ガラスやS i 02などの非磁性材が用いられる
。24は巻線窓である。
2. Description of the Related Art Ring-shaped magnetic heads are widely used for recording and reproducing signals on magnetic recording media. FIG. 3 shows the structure of a ring-type magnetic head. A magnetic core 22 made of a ferromagnetic material such as CoNbZr is sandwiched between ceramic substrates 21 and joined at a gap surface. As the gap material 23, a non-magnetic material such as glass or S i 02 is used. 24 is a winding window.

リング型の磁気ヘッドでは再生時のギャップロスによる
効率低下を防ぐため、記録密度が上がって記録波長が短
(なるにつれギャップ長Gを小さくする必要がある。と
ころがギャップ長Gを小さくすると、磁気ギャップ部の
磁気抵抗が小さくなるのでギャップ中での磁束の漏洩が
多くなり、コイルに鎖交する磁束が減少してヘッド効率
が低下する。このために、ギャップ材としてCuなとの
金属を用い、渦電流によりギャップ中を漏洩する磁束を
阻止し効率の低下を防ごうとする試みが提案されている
In a ring-type magnetic head, in order to prevent a drop in efficiency due to gap loss during reproduction, as the recording density increases and the recording wavelength becomes shorter (as the recording wavelength becomes shorter), the gap length G must be decreased. As the magnetic resistance of the coil decreases, the leakage of magnetic flux in the gap increases, and the magnetic flux linking the coil decreases, resulting in a decrease in head efficiency.For this reason, a metal such as Cu is used as the gap material. Attempts have been proposed to prevent the decrease in efficiency by blocking magnetic flux leaking through the gap using eddy currents.

発明が解決しようとする問題点 ギャップ材として金属を用いても、金属の抵抗により渦
電流の大きさが制限されるので、ギヤップ中の磁束の漏
洩を十分阻止して効率を上げるだけの効果が得られない
。またギャップ材として金属を用いると、記録媒体との
摺動によりギヤ・ツブ部のみが特に摩耗して段差ができ
る偏摩耗が起こりやすく、それにより磁気コアもくずれ
てギヤ・ツブが広がるような問題も起こる。
Problems to be Solved by the Invention Even if metal is used as the gap material, the magnitude of eddy current is limited by the resistance of the metal, so it is not effective enough to sufficiently prevent leakage of magnetic flux during the gap and increase efficiency. I can't get it. Furthermore, when metal is used as the gap material, the gear and knobs are particularly likely to wear due to sliding with the recording medium, causing uneven wear that creates steps, which causes the magnetic core to collapse and the gear and knobs to widen. also happens.

特に薄膜磁気ヘッドではバルク型ヘッドと比べて磁気コ
アの断面積が小さく磁路の磁気抵抗が大きいので、狭ギ
ャップ化による効率の低下は顕著である。
In particular, in thin-film magnetic heads, the cross-sectional area of the magnetic core is smaller and the magnetic resistance of the magnetic path is greater than in bulk-type heads, so the reduction in efficiency due to the narrowing of the gap is significant.

問題点を解決するための手段 強磁性体よりなる磁気コアと、前記磁気コアに鎖交する
コイルと、磁気ギャップを形成する非磁性材よりなるリ
ング型磁気ヘッドにおいて、少なくとも前記非磁性材を
セラミック系超伝導体により構成する。
Means for Solving the Problems In a ring-shaped magnetic head comprising a magnetic core made of a ferromagnetic material, a coil interlinked with the magnetic core, and a non-magnetic material forming a magnetic gap, at least the non-magnetic material is made of ceramic. It is composed of a system superconductor.

作用 本発明によれば、磁気ギャップが超伝導体で出来ている
ために、超伝導状態では完全反磁性になるマイスナー効
果により、再生時にギヤ、ツブ中に漏洩する磁束が無く
なり、磁気ギャップに入った再生磁束は大部分磁気コア
を通りコイルと鎖交する。従って短波長再生のために磁
気ギャップ長を小さくしても、再生効率は低下しない。
Function According to the present invention, since the magnetic gap is made of a superconductor, the Meissner effect, which becomes completely diamagnetic in the superconducting state, eliminates magnetic flux leaking into the gears and hubs during playback, and causes no magnetic flux to enter the magnetic gap. Most of the reproduced magnetic flux passes through the magnetic core and interlinks with the coil. Therefore, even if the magnetic gap length is reduced for short wavelength reproduction, the reproduction efficiency does not decrease.

また超伝導体としてセラミック系の材料を用いているの
で、Nbなとの金属超伝導体を用いた場合と比べ十分な
硬度があり、記録媒体と摺動した場合にギャップ材のみ
が摩耗して、ギャップ近傍の磁気コアが崩れキャップ長
が広がる様な問題も起こらず、安定した性能が得られる
In addition, since a ceramic material is used as the superconductor, it has sufficient hardness compared to the case of using a metal superconductor such as Nb, so that only the gap material is worn out when it slides against the recording medium. , there is no problem of the magnetic core near the gap collapsing and the cap length increasing, and stable performance can be obtained.

実施例 本発明の第1の実施例について第1図をもとに説明する
。第1図は本発明のヘッドを示す斜視図であり、セラミ
ックス基板1に挟まれたCoNbZrなどの強磁性体よ
りなる磁気コア2がギャップ面で接合されている。記録
媒体と対向する前部ギャップにはY−Ba−Cu−0よ
りなる超伝導体3が0.3μm厚形成されており、前部
及び後部ギャップ部に形成された0、05μm厚の低融
点ガラス4によって接着されている。5は巻線窓である
。本ヘッドを80に以下に冷却すればギャップ材に用い
たY−Ba−Cu−0は超伝導状態になり、下部臨界磁
界Hcl以下の磁界に対してはマイスナー効果によりそ
の中に磁束が侵入しない。再生時には記録媒体によって
生じるギャップ中磁界は非常に小さいので、下部臨界磁
界を越えることはなく超伝導状態が保たれるので、ギャ
ップ中を漏洩する磁束は無くなる。例えばトラック幅4
0μm、ギャップ長0.3μm、ギャップ深さ25μm
のヘットの再生効率は、磁気コアの透磁率を1000と
して約0.6であるが、これが1に近くなり約1.6倍
出力が向上する。記録時には媒体の抗磁力が小さくギャ
ップ材の下部臨界磁界以下のギャップ中磁界で記録でき
る条件では、記録電流によって生じた磁束はマイスナー
効果によりギャップ中を流れず、記録磁界としてすべて
ギャップ外に出るので、少ない記録電流で効率良く記録
できる。またギャップ材としてセラミック系の超伝導材
料を用いているので、基板や磁気コアとの硬度差が少な
く、記録媒体との摺動による偏摩耗や、ギャップ近傍の
コア材の崩れによるギャップの広がりが生じにくい。
Embodiment A first embodiment of the present invention will be described with reference to FIG. FIG. 1 is a perspective view showing a head of the present invention, in which a magnetic core 2 made of a ferromagnetic material such as CoNbZr is sandwiched between ceramic substrates 1 and joined at a gap surface. A 0.3 μm thick superconductor 3 made of Y-Ba-Cu-0 is formed in the front gap facing the recording medium, and a 0.05 μm thick low melting point superconductor 3 is formed in the front and rear gap portions. It is bonded by glass 4. 5 is a winding window. When this head is cooled to below 80°C, the Y-Ba-Cu-0 used as the gap material becomes superconducting, and magnetic flux does not enter into it due to the Meissner effect for magnetic fields below the lower critical magnetic field Hcl. . During reproduction, the magnetic field in the gap generated by the recording medium is so small that it does not exceed the lower critical magnetic field and the superconducting state is maintained, so that no magnetic flux leaks through the gap. For example, track width 4
0μm, gap length 0.3μm, gap depth 25μm
The regeneration efficiency of this head is about 0.6, assuming the magnetic permeability of the magnetic core as 1000, but this becomes close to 1, and the output is improved by about 1.6 times. During recording, under conditions where the coercive force of the medium is small and recording is possible with a magnetic field in the gap that is less than the lower critical magnetic field of the gap material, the magnetic flux generated by the recording current does not flow through the gap due to the Meissner effect, and all of it exits the gap as a recording magnetic field. , efficient recording is possible with a small recording current. In addition, since a ceramic superconducting material is used as the gap material, there is little difference in hardness between the substrate and the magnetic core, which prevents uneven wear due to sliding with the recording medium and widening of the gap due to collapse of the core material near the gap. Hard to occur.

本発明の第2の実施例について第2図をもとに説明する
。第2図は本発明の薄膜ヘッドの断面図を示すものであ
り、セラミックスの基板の11の上にセンダストやパー
マロイなどの磁気コア12が形成され、その上に、ギャ
ップ材となるLa−Ba−Cu−0などの超伝導体13
が形成されている。更にその上にAIやCuなとのコイ
ル14が、S i O2などの非磁性絶縁材15を介し
て形成されている。更にその上に、もう一方の磁気コア
16となる強磁性薄膜が後部ギャップ部17で磁気コア
11と接合される。ギャップ材が非磁性材の場合には、
ギャップ材が後部ギャップ部17まであっても後部ギャ
ップ部の面積が大きければ磁気抵抗としてはほとんど問
題無いが、超伝導体を用いる場合には後部ギャップ部に
まであると磁束の流れが阻止され非常な効率の低下を招
(ため後部ギャップ部は除く必要がある。コイルに鎖交
しない漏洩磁束は磁気ギャップ中を通るものが大部分で
あるが、コイルを囲う磁気コア間ても多少の漏洩がある
ので、磁気ギャップを形成する超伝導体はコイルと磁気
コアの重なり部分全体に形成した方が、再生効率がより
良くなることは明らかである。またギャップ中での磁束
の漏洩が無ければ、ギャップ深さが大きくても効率の低
下は少ないから、摩耗に対して長寿命のヘッドが実現で
きる。
A second embodiment of the present invention will be explained based on FIG. 2. FIG. 2 shows a cross-sectional view of the thin film head of the present invention, in which a magnetic core 12 made of sendust, permalloy, etc. is formed on a ceramic substrate 11, and on top of that a magnetic core 12 made of a material such as Sendust or Permalloy is placed on a ceramic substrate 11. Superconductor 13 such as Cu-0
is formed. Furthermore, a coil 14 made of AI or Cu is formed thereon via a non-magnetic insulating material 15 such as SiO2. Furthermore, a ferromagnetic thin film serving as the other magnetic core 16 is bonded to the magnetic core 11 at the rear gap portion 17 thereon. If the gap material is non-magnetic,
Even if the gap material extends to the rear gap part 17, there is almost no problem with magnetic resistance as long as the area of the rear gap part is large, but when using a superconductor, if the material extends to the rear gap part, the flow of magnetic flux is blocked and there is a problem. It is necessary to remove the rear gap, which causes a significant decrease in efficiency.Most of the leakage magnetic flux that does not link the coil passes through the magnetic gap, but some leakage also occurs between the magnetic cores surrounding the coil. Therefore, it is clear that regeneration efficiency will be better if the superconductor that forms the magnetic gap is formed over the entire overlap between the coil and the magnetic core.Also, if there is no leakage of magnetic flux in the gap, Even if the gap depth is large, there is little decrease in efficiency, so a head with a long service life against wear can be realized.

発明の効果 本発明によれば、キャップ材としてセラミック系の超伝
導材を用いたことにより、再生時の磁気ギャップ中の磁
束の漏洩が無くなるため、再生効率が1に近(なり効率
の良い再生が行える。また偏摩耗やギャップのくずれが
起きにくいので長時間安定した特性が保たれる。
Effects of the Invention According to the present invention, by using a ceramic superconducting material as the cap material, there is no leakage of magnetic flux in the magnetic gap during reproduction, so the reproduction efficiency is close to 1 (which means highly efficient reproduction). Also, since uneven wear and gap collapse are less likely to occur, stable characteristics can be maintained for a long time.

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

第1図は、本発明の第1の実施例の磁気ヘッドの斜視図
、第2図は、本発明の第2の実施例の磁気ヘッドの断面
図、第3図は、従来例の磁気ヘッドの斜視図である。 1・・・基板、2・・・磁気コア、3・・・超伝導体、
4・・・ガラス、5・・・巻線窓。 代理人の氏名 弁理士 中尾敏男 はが1名第1図 第2図 第3図
FIG. 1 is a perspective view of a magnetic head according to a first embodiment of the present invention, FIG. 2 is a sectional view of a magnetic head according to a second embodiment of the present invention, and FIG. 3 is a conventional magnetic head. FIG. 1... Substrate, 2... Magnetic core, 3... Superconductor,
4...Glass, 5...Wound window. Name of agent: Patent attorney Toshio Nakao (1 person) Figure 1 Figure 2 Figure 3

Claims (2)

【特許請求の範囲】[Claims] (1)強磁性体よりなる磁気コアと、前記磁気コアに鎖
交するコイルと、磁気ギャップを形成する非磁性材より
なるリング型磁気ヘッドにおいて、少なくとも前記非磁
性材がセラミック系超伝導体よりなることを特徴とする
薄膜磁気ヘッド。
(1) In a ring-shaped magnetic head consisting of a magnetic core made of a ferromagnetic material, a coil interlinked with the magnetic core, and a nonmagnetic material forming a magnetic gap, at least the nonmagnetic material is made of a ceramic superconductor. A thin film magnetic head characterized by:
(2)磁気ギャップを形成するセラミック系超伝導体が
、磁気コアの接合部を除く磁気コアとコイルの重なり部
分全体に延長されていることを特徴とする特許請求の範
囲第1項記載の磁気ヘッド。
(2) The magnetism according to claim 1, characterized in that the ceramic superconductor forming the magnetic gap extends over the entire overlapping portion of the magnetic core and the coil, excluding the joint of the magnetic core. head.
JP9562687A 1987-04-17 1987-04-17 Thin film magnetic head Pending JPS63259813A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9562687A JPS63259813A (en) 1987-04-17 1987-04-17 Thin film magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9562687A JPS63259813A (en) 1987-04-17 1987-04-17 Thin film magnetic head

Publications (1)

Publication Number Publication Date
JPS63259813A true JPS63259813A (en) 1988-10-26

Family

ID=14142734

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9562687A Pending JPS63259813A (en) 1987-04-17 1987-04-17 Thin film magnetic head

Country Status (1)

Country Link
JP (1) JPS63259813A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0367439A2 (en) * 1988-11-01 1990-05-09 Ampex Systems Corporation Magnetic heads with superconductor shields

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0367439A2 (en) * 1988-11-01 1990-05-09 Ampex Systems Corporation Magnetic heads with superconductor shields
EP0367439A3 (en) * 1988-11-01 1991-11-13 Ampex Systems Corporation Magnetic heads with superconductor shields

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