JPH02108207A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPH02108207A
JPH02108207A JP26014288A JP26014288A JPH02108207A JP H02108207 A JPH02108207 A JP H02108207A JP 26014288 A JP26014288 A JP 26014288A JP 26014288 A JP26014288 A JP 26014288A JP H02108207 A JPH02108207 A JP H02108207A
Authority
JP
Japan
Prior art keywords
magnetic
gap
head
flux density
magnetic flux
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
JP26014288A
Other languages
Japanese (ja)
Inventor
Toshikatsu Narumi
利勝 鳴海
Yoshiyuki Nanba
義幸 難波
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP26014288A priority Critical patent/JPH02108207A/en
Publication of JPH02108207A publication Critical patent/JPH02108207A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To narrow the interval of a gap and to attain the high density recording the providing a metallic magnetic film with a large saturated magnetic flux density on the surface of the head core opposite to a recording medium. CONSTITUTION:A metallic magnetic film 8 composed of Fe-Al-Si is provided on the surface of a magnetic head 1 opposite to a magnetic disk 2. Thus, by providing the metallic magnetic film 8 with a large saturated magnetic flux density, the magnetic flux density to pass through a gap 4 in the same way as an MIG head can be increased, and thus, in a recording medium 5 of the magnetic disk 2, the magnetic flux density necessary for the recording and reproducing of the information can be secured. The metallic magnetic film 8 can be formed by the sputtering method, etc., the magnetic film 8 is brought into contact with the head core 3 composed of ferrite, since it is extended in the surface direction, it does not work as a gap, for this reason, the generation of the pseudo peak can be prevented, and since the tip of the gap is composed of the metallic magnetic body with the large saturated magnetic flux density, the interval (gap length) of the gap can be narrowed and thus, the high density recording can be executed.

Description

【発明の詳細な説明】 〔概要〕 磁気ディスクの記録媒体に信号の記録と再生とを行う磁
気ヘッドに関し、 記録密度の向上を目的とし、 記録媒体に対向するヘッドコアの表面に飽和磁束密度の
大きな金属磁性膜を設けて磁気ヘッドを構成する。
[Detailed Description of the Invention] [Summary] Regarding a magnetic head that records and reproduces signals on a recording medium of a magnetic disk, for the purpose of improving the recording density, a magnetic head with a high saturation magnetic flux density is provided on the surface of the head core facing the recording medium. A magnetic head is constructed by providing a metal magnetic film.

〔産業上の利用分野〕[Industrial application field]

本発明は高密度記録を可能とする磁気ヘッドに関する。 The present invention relates to a magnetic head that enables high-density recording.

磁気ディスクはアルミニウム(AI)合金などの非磁性
金属からなる円板上に磁性記録媒体をスピンコード法、
真空蒸着法、スパッタ法などの方法により111m未満
の厚さに薄膜化して磁性膜を形成している。
A magnetic disk is a disk made of a non-magnetic metal such as an aluminum (AI) alloy, and a magnetic recording medium is placed on a disk using a spin code method.
The magnetic film is formed by reducing the thickness to less than 111 m using methods such as vacuum evaporation and sputtering.

すなわち、記録媒体がT−フェライ)(r −Pe20
、)やバリウム・フェライト(BaO・6Pez03)
のような酸化物からなるものに就いてはスピンコード法
が用いられており、一方、コバルト・クローム(Co−
Cr)やニッケル・コバルト・燐(Ni−Co−P)の
ような磁性合金膜を用いるものについては真空蒸着法や
スパッタ法が用いられている。
That is, the recording medium is T-ferrai)(r-Pe20
) and barium ferrite (BaO・6Pez03)
The spin code method is used for oxides such as cobalt chromium (Co-
For those using magnetic alloy films such as Cr) or nickel-cobalt-phosphorus (Ni-Co-P), vacuum evaporation and sputtering methods are used.

磁気ディスク装置はか\る磁気ディスクを高速回転せし
め、これによる揚力によって磁気ヘッドを内蔵したスラ
イダを微少間隙を隔て\浮上せしめ、磁気ヘッドのコイ
ルに高周波の信号電流を通じ、コイルから発生する磁力
線によって磁気ディスフの記録媒体を磁化して記録を行
い、また、磁化している記録媒体からの磁力線を磁気ヘ
ッドのコイルが受けて電気信号に替え、記録の再生を行
うものである。
A magnetic disk drive rotates a magnetic disk at high speed, and uses the resulting lifting force to levitate a slider with a built-in magnetic head across a small gap.A high-frequency signal current is passed through the coil of the magnetic head, and the magnetic field lines generated from the coil cause the slider to float. Recording is performed by magnetizing the recording medium of a magnetic disc, and the magnetic field lines from the magnetized recording medium are received by the coil of the magnetic head and converted into electric signals to reproduce the recorded data.

〔従来の技術〕[Conventional technology]

磁気ディスクの記録密度を向上する方法として磁気ヘッ
ドのギヤ・7プを狭くすることが行われている。
As a method of improving the recording density of a magnetic disk, narrowing the gear 7 of the magnetic head has been carried out.

第2図はM I G(M6tal in Gapの略称
)ヘッドの構成を示すものであるが、これを用いて磁気
ヘッドの構造を説明する。
FIG. 2 shows the structure of an MIG (abbreviation for M6tal in gap) head, and the structure of the magnetic head will be explained using this.

磁気ヘッド1は0.2μm程度の微少間隔を保って磁気
ディスク2の上に浮揚しており、フェライトよりなるヘ
ッドコア3に設けられているギャップ4からの磁力線に
より磁気ディスク2の記録媒体5が磁化し、情報の記録
が行われている。
The magnetic head 1 floats above the magnetic disk 2 with a minute interval of about 0.2 μm maintained, and the recording medium 5 of the magnetic disk 2 is magnetized by lines of magnetic force from the gap 4 provided in the head core 3 made of ferrite. Information is being recorded.

こ\で、磁気ヘッド1はベツドコア3にコイル6を捲回
したものであり、磁気ディスク2に対向する位置に設け
られているコアのギャップ(通称ギャップ長)4が狭く
なるに従って磁力線の分布が狭くなるために記録媒体5
において1ビツトの所要面積が少なくて済むことからギ
ャップ4を狭くすることにより、記録密度を向上するこ
とができる。
The magnetic head 1 has a coil 6 wound around a bed core 3, and as the gap (commonly known as gap length) 4 of the core provided at a position facing the magnetic disk 2 narrows, the distribution of magnetic lines of force changes. Recording medium 5 to become narrower
Since the area required for one bit is small, recording density can be improved by narrowing the gap 4.

こ\で、磁気ディスク2の記録媒体5に対する情報の記
録はギャップ4を通る磁力線の水平成分によって行われ
るために、ギャップ4を狭くするに従って、コイル6の
信号電流を増し、磁束密度を増加させる必要がある。
Here, since information is recorded on the recording medium 5 of the magnetic disk 2 by the horizontal component of the lines of magnetic force passing through the gap 4, as the gap 4 is narrowed, the signal current of the coil 6 is increased and the magnetic flux density is increased. There is a need.

然し、ヘッドコア3を構成するフェライトの飽和磁束密
度(Bs)は最大でも5000G (ガウス)程度であ
り、コイル6の信号電流を増加させても飽和してしまう
ために磁束密度の増加には貢献しない。
However, the saturation magnetic flux density (Bs) of the ferrite constituting the head core 3 is about 5000G (Gauss) at maximum, and even if the signal current of the coil 6 is increased, it will reach saturation and will not contribute to an increase in the magnetic flux density. .

そのため、ギャップ4を狭くするほど磁気ディスク2の
記録媒体への磁束密度は減少し、オーバライド特性が悪
化する。
Therefore, as the gap 4 becomes narrower, the magnetic flux density to the recording medium of the magnetic disk 2 decreases, and the override characteristic deteriorates.

そこで、この対策として、飽和磁束密度の大きな金属磁
性膜7を第2図に示すようにギャップ4の片面あるいは
両面に設けたMIGヘッドが実用化されている。
As a countermeasure against this problem, an MIG head has been put into practical use in which a metal magnetic film 7 having a high saturation magnetic flux density is provided on one or both sides of the gap 4, as shown in FIG.

このMIGへラドを使用することにより磁束密度が増し
、狭いギヤノブでも充分なオーバライド特性を得ること
が可能となった。
By using RAD for this MIG, the magnetic flux density increases, making it possible to obtain sufficient override characteristics even with a narrow gear knob.

然し、金属磁性膜7とへラドコア3との境界がギャップ
として働き、再生に当たって第3図(B)に示すような
擬似ピークを生じ、検出器がこの擬似ピークを信号とし
て見誤り易いと云う問題を生じ、解決が必要であった。
However, there is a problem in that the boundary between the metal magnetic film 7 and the herad core 3 acts as a gap, causing pseudo peaks as shown in FIG. 3(B) during reproduction, and it is easy for the detector to mistake these pseudo peaks as signals. occurred, and a solution was needed.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

以上記したように磁気ディスクの記録密度を増大するに
は磁気ヘッドのギャップを狭くする必要があり、これに
よる磁気ディスクへの磁束密度の減少を防ぐ方法として
MIGベツドが使用されている。
As described above, in order to increase the recording density of a magnetic disk, it is necessary to narrow the gap of the magnetic head, and the MIG bed is used as a method to prevent the decrease in magnetic flux density to the magnetic disk.

然し、MIGベツドを構成する金属磁性膜とへラドコア
との界面がギャップとして働(ために擬似ピークが発生
し、信頬性が損なわれている点が問題で、これを解消す
ることが課題である。
However, the problem is that the interface between the metal magnetic film that makes up the MIG bed and the herad core acts as a gap (therefore, pseudo peaks are generated, impairing reliability), and solving this problem is a challenge. be.

〔課題を解決するための手段〕[Means to solve the problem]

上記の問題は磁気ディスクの記録媒体に対向するヘッド
コアの表面に飽和磁束密度の大きな金属磁性膜を設けて
磁気ヘッドを構成することにより解決することができる
The above problem can be solved by constructing a magnetic head by providing a metal magnetic film with a high saturation magnetic flux density on the surface of the head core facing the recording medium of the magnetic disk.

〔作用〕[Effect]

本発明は第1図に示すように金属磁性膜8を磁気ディス
ク2と対向する磁気ヘッド1の表面に設けるものである
In the present invention, a metal magnetic film 8 is provided on the surface of the magnetic head 1 facing the magnetic disk 2, as shown in FIG.

このように飽和磁束密度の大きな金属磁性膜8を設ける
とMIGヘッドと同様にギャップ4を通る磁束密度を増
加することができ、これにより磁気ディスク2の記録媒
体5において情報の記録および再生に必要な磁束密度を
確保することができる。
By providing the metal magnetic film 8 with a high saturation magnetic flux density in this way, it is possible to increase the magnetic flux density passing through the gap 4 similarly to the MIG head, which is necessary for recording and reproducing information on the recording medium 5 of the magnetic disk 2. It is possible to ensure a high magnetic flux density.

こ\で、金属磁性膜8はスパッタ法などによって形成で
きるが、このような構造とすると金属磁性膜8とへラド
コア3との境界面はMIGヘッドの場合と同様にギャッ
プとして働くように思われるが、スパッタ法などの物理
的な方法で析出した金属磁性膜8はフェライトからなる
ヘッドコア3に密着しており、また面方向に伸びている
ため、ギャップとしては働かない。
Here, the metal magnetic film 8 can be formed by sputtering or the like, but with such a structure, the interface between the metal magnetic film 8 and the helad core 3 seems to act as a gap, similar to the case of the MIG head. However, since the metal magnetic film 8 deposited by a physical method such as sputtering is in close contact with the head core 3 made of ferrite and extends in the plane direction, it does not function as a gap.

第3図(A)はこのように形成した磁気ヘッドの再生出
力波形を示すもので、同図(B)のMIGヘッドに較べ
て擬似ピークが発生しないことが判る。
FIG. 3(A) shows the reproduced output waveform of the magnetic head formed in this way, and it can be seen that no pseudo peaks occur compared to the MIG head of FIG. 3(B).

〔実施例〕〔Example〕

第1図に示す本発明の実施例において、金属磁性膜とし
ては鉄・アルミニウム・シリコン(Fe−八β−5i)
からなるセンダスト合金を用いた。
In the embodiment of the present invention shown in FIG. 1, the metal magnetic film is made of iron, aluminum, silicon (Fe-8β-5i).
Sendust alloy consisting of was used.

この合金の飽和磁束密度は約10000 Gである。The saturation magnetic flux density of this alloy is approximately 10,000G.

この合金をスパッタ法を用い、ヘッドコアの片側表面に
2μmの厚さに形成した。
This alloy was formed to a thickness of 2 μm on one side of the head core using a sputtering method.

第3図(A)はか\る磁気ヘッドの再生出力波形であっ
て、測定条件は同図に示すように、周速は12.5 m
/s、書込み周波数は1MHzである。
Figure 3 (A) shows the reproduced output waveform of the magnetic head, and the measurement conditions were as shown in the figure: the circumferential speed was 12.5 m.
/s, and the writing frequency is 1 MHz.

この図から判るようにMIGヘッドで問題となっている
擬似ピークの発生がなく、また同様に高周波書込みが可
能である。
As can be seen from this figure, there is no generation of pseudo peaks, which is a problem with MIG heads, and high frequency writing is also possible.

〔発明の効果〕〔Effect of the invention〕

本発明の実施により擬似ピークの発生を防止でき、また
キャップの先端が飽和磁束密度の大きな金属磁性体より
なるので、ギャップの間隔(ギャップ長)を狭くするこ
とができ、これにより高密度記録が可能となる。
By implementing the present invention, it is possible to prevent the occurrence of pseudo peaks, and since the tip of the cap is made of a magnetic metal material with a high saturation magnetic flux density, the gap interval (gap length) can be narrowed, which enables high-density recording. It becomes possible.

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

第1図は本発明に係る磁気ヘッドの正面模式図、第2図
はMIGヘッドの正面模式図、 第3図(A)、  (B)はそれぞれ再生出力波形図、 である。 図において、 1は磁気ヘッド、     2は磁気ディスク、3はへ
ラドコア、 5は記録媒体、 である。 4はギヤ、2プ、 7.8は金属磁性膜、 水肩に岨【;づ糸るλ論i−ヘノドの圧jbJkj大C
〕第 1 ■ 芦 3 の
FIG. 1 is a schematic front view of a magnetic head according to the present invention, FIG. 2 is a schematic front view of an MIG head, and FIGS. 3A and 3B are reproduction output waveform diagrams, respectively. In the figure, 1 is a magnetic head, 2 is a magnetic disk, 3 is a helad core, and 5 is a recording medium. 4 is a gear, 2 is a metal magnetic film, and 7.8 is a metal magnetic film.
] No. 1 ■ Reed 3

Claims (1)

【特許請求の範囲】 高速で回転する磁気ディスク面より揚力により浮上し、
磁気ディスクの記録媒体に信号の記録と再生とを行う磁
気ヘッドにおいて、 記録媒体(5)に対向するヘッドコア(3)の表面に飽
和磁束密度の大きな金属磁性膜(8)を設けたことを特
徴とする磁気ヘッド。
[Claims] Floating from the surface of a magnetic disk rotating at high speed due to lift force,
A magnetic head that records and reproduces signals on a magnetic disk recording medium is characterized by a metal magnetic film (8) with a high saturation magnetic flux density provided on the surface of the head core (3) facing the recording medium (5). magnetic head.
JP26014288A 1988-10-14 1988-10-14 Magnetic head Pending JPH02108207A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26014288A JPH02108207A (en) 1988-10-14 1988-10-14 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26014288A JPH02108207A (en) 1988-10-14 1988-10-14 Magnetic head

Publications (1)

Publication Number Publication Date
JPH02108207A true JPH02108207A (en) 1990-04-20

Family

ID=17343888

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26014288A Pending JPH02108207A (en) 1988-10-14 1988-10-14 Magnetic head

Country Status (1)

Country Link
JP (1) JPH02108207A (en)

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