JPH0461012A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPH0461012A
JPH0461012A JP17337590A JP17337590A JPH0461012A JP H0461012 A JPH0461012 A JP H0461012A JP 17337590 A JP17337590 A JP 17337590A JP 17337590 A JP17337590 A JP 17337590A JP H0461012 A JPH0461012 A JP H0461012A
Authority
JP
Japan
Prior art keywords
thin film
magnetic
core half
gap
face
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
JP17337590A
Other languages
Japanese (ja)
Inventor
Satoru Ota
哲 太田
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.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo Electric 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 Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP17337590A priority Critical patent/JPH0461012A/en
Publication of JPH0461012A publication Critical patent/JPH0461012A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To improve the track width accuracy of a magnetic gap and to execute good recording and reproducing even in a high-frequency region by joining and fixing a 1st core half body and a 2nd core half body while the end face of 1st laminated thin films and the front surface of a 3rd ferromagnetic metallic thin film are held butted on each other via a nonmagnetic material to constitute a magnetic gap. CONSTITUTION:The width of the end face of the 1st laminated thin films 16 exposed on the gap forming surface is set equal to the desired track width of the magnetic gap 27 and the width of the gap butt part of the 2nd ferromagnetic metallic thin film 25 of the 2nd core half body 12b is set larger than the desired track width of the magnetic gap 2 in the case of forming a core block 32 by butting the 1st, 2nd core half body blocks 30a, 30b by melting and solidifying a glass layer 26 in the state in which the end face 31 on the gap forming side of the 1st core half block 30a and the glass layer 26 face each other. The track width of the magnetic gap 27 is set exactly by the film thickness of the 1st laminated thin films 16 at all times in this way and the good recording and reproducing are executed even in a high-frequency region.

Description

【発明の詳細な説明】 (イ)産業上の利用分野 本発明は高周波信号を効率良く、記録再生するのに好適
な磁気へVドに関する。
DETAILED DESCRIPTION OF THE INVENTION (a) Industrial Application Field The present invention relates to a magnetic V-drive suitable for efficiently recording and reproducing high frequency signals.

(ロ)従来の技術 従来、VTR等の高周波信号を記録再生する装置におい
ては、ビデオへンド用磁性材料として高周波損失の少な
いフェライト材料が用いられている。しかし、近年にな
って高品位VTRやデジタル〜7TRのように更に広帯
域の信号を取り扱うシステムの開発が盛んになってきて
おり、記録媒体もこのような大量の情報を記録する為の
高密度化の流れの中で酸化鉄系から合金粉末媒体や金属
蒸着媒体等の高抗磁力媒体・\移行しつつある。これに
対してフェライトヘッドではその最大磁束密度が高々5
000ガウス程度であり、又短波長信号を効率よく再生
する為には狭ギャップにする必要があり、上述のような
保磁力Haが10000e以上の高抗磁力媒体ではギャ
ップ先端部のフエライトコアが飽和し、十分な記録が出
来ない。そこで最大磁束密度の高いセンダストやアモル
ファス磁性合金等の金属磁性材料を用いた磁気へtドの
開発が行!つれている。
(b) Prior Art Conventionally, in devices for recording and reproducing high frequency signals such as VTRs, ferrite materials with low high frequency loss have been used as magnetic materials for video ends. However, in recent years, the development of systems that handle even wider band signals, such as high-quality VTRs and digital to 7TRs, has become active, and recording media have also become denser to record such large amounts of information. In this trend, there is a shift from iron oxide based media to high coercive force media such as alloy powder media and metal evaporated media. On the other hand, in ferrite heads, the maximum magnetic flux density is at most 5
000 Gauss, and in order to efficiently reproduce short wavelength signals, it is necessary to make the gap narrow, and in the case of a high coercive force medium with a coercive force Ha of 10000e or more as mentioned above, the ferrite core at the tip of the gap becomes saturated. However, sufficient records cannot be recorded. Therefore, we have developed magnetic materials using metal magnetic materials such as sendust and amorphous magnetic alloy, which have a high maximum magnetic flux density! I'm tired.

従来、このような欠点を解消するため、例えば特開昭6
2−33309号公報(G11B5./147C等に開
示されているような高周波用積層型磁気ヘッドが提案さ
れている。
Conventionally, in order to eliminate such drawbacks, for example, Japanese Patent Application Laid-open No. 6
A multilayer magnetic head for high frequency has been proposed as disclosed in Japanese Patent No. 2-33309 (G11B5./147C).

この磁気ヘッドは、第8図に示すように非磁性基板(1
)(]’)間にセンダスト等の強磁性金属薄膜(2)と
S IOを等の絶縁薄膜(3)との積層薄膜(4)が被
着形成されている一対の第1、第2コア半体(5a)(
5b)の前記積層薄膜(4)(4)の端面同士を磁気ギ
ヤツプ(6)となる非磁性材料(7)を介して衝き合わ
すことにより形成されている。前記−対の第1、第2コ
ア半体(5a)(5b)のうち一方の第1コア半体(5
a)には巻線溝(8)が形成されており、該巻線溝(8
)には巻線(9)が巻回されている。前記磁気ギャップ
(6)のギャフプ長は前記非磁性材料(7)の厚みによ
り決定し、トラ/り幅は積層薄膜(4,)(4)の端面
同士が衝き合わされている部分の厚みにより決定する。
This magnetic head consists of a non-magnetic substrate (1
)(]') A pair of first and second cores, between which a laminated thin film (4) of a ferromagnetic metal thin film (2) such as Sendust and an insulating thin film (3) such as SIO is adhered. Half (5a) (
It is formed by abutting the end faces of the laminated thin films (4) (4) of 5b) with a non-magnetic material (7) serving as a magnetic gap (6) interposed therebetween. One of the first core halves (5a, 5b) of the pair of first and second core halves (5a)
A winding groove (8) is formed in a).
) is wound with a winding (9). The gap length of the magnetic gap (6) is determined by the thickness of the non-magnetic material (7), and the gap width is determined by the thickness of the portion where the end surfaces of the laminated thin films (4,) (4) abut against each other. do.

しかし乍ら、上記従来の磁気ヘッドでは、第1、第2コ
ア半体(5a)(5b)の積層薄膜(4X4 )の端面
同士を正確に衝き合わせることが困難であり、磁気ギャ
ップ(6)のトラック幅を高精度に規定することは困難
である。
However, in the conventional magnetic head described above, it is difficult to accurately abut the end surfaces of the laminated thin films (4×4) of the first and second core halves (5a) (5b), and the magnetic gap (6) It is difficult to define the track width with high precision.

上述の欠点を解消した磁気ヘッドとしては、例えば特開
昭63−269310号公報(GLIB5 / 127
 )等に開示されているものがある。
As a magnetic head that eliminates the above-mentioned drawbacks, for example, Japanese Patent Application Laid-Open No. 63-269310 (GLIB5/127
), etc.

この磁気ヘッドは第9図に示すように巻線溝(8)が形
成されている第1コア半体(5a)は、上述の第8図に
示した磁気ヘッドと同様に非磁性基板(1)(1’)間
に積層薄膜(4)が形成された構造であるのに対して、
第2コア半体(5b)は非磁性体(10)のギャップ形
成側の端面(10a)全域に単層の強磁性金属薄膜(1
1)を被着形成し、該強磁性金属薄膜(11)上にギャ
ップスペーサとなる非磁性薄膜(7)を被着形成した構
造である。前記第1、第2コア半体(5a)(5b)は
積層薄膜(4)の端面と非磁性薄膜(7)の上面とが衝
き合わされた状態で接合固定され、磁気ギヤツプ(6)
を形成している。この磁気へ、・ドでは、磁気ギャップ
(6)のトラ/り幅は、第1、第2コア半体(5a)(
5b)の衝き合わせ精度には関係なく、積層薄膜(4)
のllN厚により規定され、トラック精度を非常に高め
ることができる。
As shown in FIG. 9, this magnetic head has a first core half (5a) in which a winding groove (8) is formed, and a non-magnetic substrate (1) as in the magnetic head shown in FIG. ) (1') In contrast to the structure in which a laminated thin film (4) is formed between
The second core half (5b) has a single-layer ferromagnetic metal thin film (1
1) is deposited, and a non-magnetic thin film (7) serving as a gap spacer is deposited on the ferromagnetic metal thin film (11). The first and second core halves (5a) and (5b) are bonded and fixed in a state where the end face of the laminated thin film (4) and the upper face of the non-magnetic thin film (7) are brought into contact with each other, and a magnetic gap (6) is formed.
is formed. In this magnetic field, the width of the magnetic gap (6) is the width of the first and second core halves (5a) (
Regardless of the alignment accuracy of 5b), the laminated thin film (4)
The tracking accuracy can be greatly improved.

しかし乍ら、この構造の磁気ヘッドにおいても、高周波
領域で記録再生を行う場合、第2コア半体(5b)の強
磁性金属薄膜(11)の膜厚を薄くする必要があるが、
逆に前記強磁性金属薄膜(11)が薄くなると、該薄膜
(11)がすぐに磁気飽和してしまい、良好な記録を行
うことが出来ないという問題が生じる。
However, even in a magnetic head with this structure, when recording and reproducing in a high frequency region, it is necessary to reduce the thickness of the ferromagnetic metal thin film (11) of the second core half (5b).
Conversely, if the ferromagnetic metal thin film (11) becomes thin, the thin film (11) quickly becomes magnetically saturated, causing a problem that good recording cannot be performed.

(ハ)発明が解決しようとする課題 本発明は上記従来例の欠点に鑑み為されたものであり、
磁気ギャップのトラック精度が高く、且つ磁気飽和を起
こすことなく、高周波領域においても良好な記録再生を
行うことが出来る磁気ヘッドを提供することを目的とす
るものである。
(c) Problems to be Solved by the Invention The present invention has been made in view of the drawbacks of the above-mentioned conventional examples.
It is an object of the present invention to provide a magnetic head that has high tracking accuracy of a magnetic gap and can perform good recording and reproduction even in a high frequency range without causing magnetic saturation.

(ニ)課題を解決するための手段 本発明は一対の非磁性基板間に第1の強磁性金属薄膜と
絶縁薄膜とよりなり、厚みが磁気ギヤツプの所望のトラ
ンク幅に等しい第1の積層薄膜が被着形成され、ギャッ
プ形成側の端面に前記積層薄膜の端面が露出している第
1コア半体と、非磁性体のギャップ形成側の端面のうち
媒体摺接面とは反対側に溝を備え、該溝内に第2の強磁
性金属薄膜と絶縁薄膜とよりなり、上面が前記非磁性体
のギャップ形成側の端面と面一である第2の積層薄膜が
被着形成され、該第2の積層薄膜上に幅が前記第1の積
層薄膜の厚みより大きい第3の強磁性金属薄膜が被着形
成されている第2コア半体とから成り、前記第1コア半
体と前記第2コア半体とを上記第1の積層薄膜の端面と
上記第3の強磁性金属薄膜の上面とが磁気ギャップとな
る非磁性材料を介して衝き合わされた状態で接合固定し
たことを特徴とする。
(d) Means for Solving the Problems The present invention comprises a first ferromagnetic metal thin film and an insulating thin film between a pair of non-magnetic substrates, the first laminated thin film having a thickness equal to the desired trunk width of the magnetic gap. a first core half on which is deposited and the end face of the laminated thin film is exposed on the end face on the gap forming side, and a groove on the end face on the gap forming side of the non-magnetic material on the side opposite to the medium sliding contact surface. A second laminated thin film comprising a second ferromagnetic metal thin film and an insulating thin film, the upper surface of which is flush with the end surface on the gap forming side of the non-magnetic material, is deposited in the groove; a second core half on which a third ferromagnetic metal thin film having a width larger than the thickness of the first laminated thin film is deposited on the second laminated thin film; The second core half is bonded and fixed in a state where the end face of the first laminated thin film and the upper face of the third ferromagnetic metal thin film are brought into contact with each other with a non-magnetic material forming a magnetic gap. do.

(ホ)作 用 上記構成に依れば、第1コア半体と第2コア半体の衝き
合わせに多少のズレが生じても、前記第1コア半体の第
1の積層薄膜の端面は、その全幅において非磁性材料を
介して前記第2コア半体の第3の強磁性金属薄膜に衝き
合わされ、前記積層薄膜の端面の幅が磁気ギャノブのト
ラック幅となり、また、第2コア半体は第2の積層薄膜
によ)、高周波領域においても渦電流損失は抑えられ、
しかもこの部分での磁気飽和は起こらない。
(E) Effect According to the above configuration, even if some misalignment occurs in the abutment between the first core half and the second core half, the end face of the first laminated thin film of the first core half , whose entire width abuts against the third ferromagnetic metal thin film of the second core half through a non-magnetic material, the width of the end face of the laminated thin film becomes the track width of the magnetic ganob, and the second core half (by the second laminated thin film), eddy current loss is suppressed even in the high frequency range,
Moreover, magnetic saturation does not occur in this part.

(へ)実施例 以下、図面を参照しつつ本発明の一実施例を詳細に説明
する。
(F) Embodiment Hereinafter, an embodiment of the present invention will be described in detail with reference to the drawings.

第1図は本実施例の磁気ヘッドの外観を示す斜視図であ
る。
FIG. 1 is a perspective view showing the appearance of the magnetic head of this embodiment.

図中、(12a)(12b)は第1、第2コア半体であ
り、そのうち一方の第1コア半体(12a)は結晶化ガ
ラス、非磁性セラミック等よりなる非磁性基板(13)
上にセンダスト等の膜厚5gmの第1の強磁性金属薄膜
(14)と8102等の膜厚0.1μmの絶縁薄膜(1
5)とよりなる第1の積層薄膜(16)が被着形成され
ており、該第1の積層薄膜(16)上には接着材として
作用する高融点のガラス層(17)により結晶化ガラス
、非磁性セラミ7り等よりなる非磁性基板り13°)が
接合固定されている。前記第1コア半体(12a)のギ
ャンプ形成側の端面には巻線il!(18)が形成され
ている。
In the figure, (12a) and (12b) are first and second core halves, one of which, the first core half (12a), is a nonmagnetic substrate (13) made of crystallized glass, nonmagnetic ceramic, etc.
A first ferromagnetic metal thin film (14) with a film thickness of 5 gm such as Sendust and an insulating thin film (14) with a film thickness of 0.1 μm such as 8102 are placed on top.
A first laminated thin film (16) consisting of 5) is deposited on the first laminated thin film (16), and a high melting point glass layer (17) acting as an adhesive is applied to the crystallized glass. , a non-magnetic substrate (13°) made of non-magnetic ceramic 7, etc. is bonded and fixed. A winding il! is provided on the end face of the first core half (12a) on the gap formation side. (18) is formed.

また、前記第2コア半体(12b)は、結晶化ガラス、
非磁性セラミック等よりなり前記第1コア半体(12a
)と厚みが等しい非磁性体(19)のギャップ形成側の
端面のうち媒体摺接面とは反対側(バ/クギャップ側)
に斜面(20)を有する溝(21)が形成されている。
Further, the second core half (12b) includes crystallized glass,
The first core half (12a) is made of non-magnetic ceramic or the like.
) of the end face on the gap forming side of the non-magnetic material (19) with the same thickness as the side opposite to the media sliding contact surface (back/back gap side)
A groove (21) having a slope (20) is formed in the groove.

前記溝(21)内にはセンダスト等の膜厚5μmの第2
の強磁性金属薄膜(22)とSin、等の膜厚0.1μ
mの絶縁薄膜(23)とよりなる第2の積層薄膜(24
)が被着形成されている。前記非磁性体(19)のギャ
ップ形成側の端面(191)と前記第2の積層薄膜(2
4)の上面(241)とは面一であり、該端面(191
)から第2の積層薄膜(24)の上面(241)に亘っ
てはセンダスト等よりなる膜厚5μmの第3の強磁性金
属薄膜(25)が被着形成されている。前記第3の強磁
性金属薄膜(25)上には、ギャップスペーサ用の低融
点のガラス層(非磁性材料) (26)が被着形成され
ている。
In the groove (21), a second film of Sendust or the like having a thickness of 5 μm is placed.
The film thickness of ferromagnetic metal thin film (22) and Sin, etc. is 0.1μ.
a second laminated thin film (24) consisting of an insulating thin film (23) of m
) is deposited. The gap forming side end face (191) of the non-magnetic material (19) and the second laminated thin film (2
4) is flush with the top surface (241), and the end surface (191)
) to the upper surface (241) of the second laminated thin film (24), a third ferromagnetic metal thin film (25) made of sendust or the like and having a thickness of 5 μm is deposited. A low melting point glass layer (non-magnetic material) (26) for use as a gap spacer is deposited on the third ferromagnetic metal thin film (25).

前記第1、第2コア半体(1,2a)(12b)は、第
1コア半体(12a)のギャノブ形成側の端面と@記ガ
ラス層(26)とが衝き合わされた状態で接合されて3
す、この接合は前記ガラス層(26)の溶融同化により
為されている。前記ガラス層(26)は磁気ギャップ(
27)として作用し、該磁気ギヤノブ(27)のキャッ
プ長は前記ガラス層(17)の厚みに等しく、トランク
幅は前記第1の積層薄膜(16)の膜厚に等しい。
The first and second core halves (1, 2a) (12b) are joined with the end surface of the first core half (12a) on the Ganob formation side and the glass layer (26) abutting each other. te3
This bonding is achieved by melting and assimilating the glass layer (26). The glass layer (26) has a magnetic gap (
27), the cap length of the magnetic gear knob (27) is equal to the thickness of the glass layer (17), and the trunk width is equal to the thickness of the first laminated film (16).

次に、上記実施例の磁気ヘッドの製造方法について説明
する。
Next, a method of manufacturing the magnetic head of the above embodiment will be explained.

先ず、第2図に示すように非磁性基板(13)の上面に
第1の強磁性金属薄膜(14)と絶縁薄膜(15)とか
らなる所望のトラック幅に等しい膜厚の第1の積層薄膜
(16)及び高融点のガラス層(17)がスパッタリン
グ等で被着形成されている積層基板(競)を複数枚、前
記ガラス(17)により接合固定して積層ブロック(2
9)を形成する。
First, as shown in FIG. 2, a first laminated layer consisting of a first ferromagnetic metal thin film (14) and an insulating thin film (15) with a film thickness equal to the desired track width is formed on the upper surface of the nonmagnetic substrate (13). A plurality of laminated substrates (components) each having a thin film (16) and a high melting point glass layer (17) formed by sputtering or the like are bonded and fixed by the glass (17) to form a laminated block (2).
9).

次に、前記積層ブロック(29)を破線A−A’にィa
って切断して第1コア半体ブロツク(30a)を形成し
、第3図に示すように前記第1コア半体ブロツク(30
a)の切断面、即ち積層薄膜(16)の端面(+61)
が露出しているギャップ形成側の端面(31)に巻線溝
(18)を形成する。
Next, move the laminated block (29) along the broken line AA'.
to form a first core half block (30a), and then cut the first core half block (30a) as shown in FIG.
The cut surface of a), that is, the end surface (+61) of the laminated thin film (16)
A winding groove (18) is formed on the end face (31) on the gap forming side where the wire is exposed.

一方、第4図に示すように結晶化ガラス、非磁性セラミ
ック等よりなり、前記第1コア半体ブロツク(30a)
に相当する大きさの長方体状の非磁性体(19)を用意
し、該非磁性体(19)の上面即ち、ギャンプ形成側の
端面(191)のうちバックギャンプ側(媒体摺接側の
端面(192)とは反対側)に斜面(20)を有する溝
(21)を形成する。
On the other hand, as shown in FIG. 4, the first core half block (30a) is made of crystallized glass, non-magnetic ceramic, etc.
A rectangular non-magnetic material (19) with a size corresponding to the size of the non-magnetic material (19) is prepared. A groove (21) having a slope (20) is formed on the side opposite to (192).

次に、第5図に示すように前記溝(21)内に第2の強
磁性金属薄膜(22)と絶縁薄膜(23)とよりなる第
2の積層薄膜(24)を該積層薄膜(24)の上面(2
41)が前記非磁性体(19)のギャップ形成側の端面
(191)と面一になるように形成する。これは非磁性
体(19)の上面全域に第2の積層薄膜(24)を形成
した後、該積層薄膜(24)をギャップ形成側の端面(
191)が露出するまで、研磨、エツチング等により除
去することにより形成する。
Next, as shown in FIG. 5, a second laminated thin film (24) consisting of a second ferromagnetic metal thin film (22) and an insulating thin film (23) is placed in the groove (21). ) top surface (2
41) is formed flush with the end surface (191) of the non-magnetic material (19) on the gap forming side. After forming the second laminated thin film (24) on the entire upper surface of the non-magnetic material (19), the second laminated thin film (24) is attached to the end face (on the gap forming side) of the non-magnetic material (19).
191) is removed by polishing, etching, etc. until it is exposed.

次に、第6図に示すように前記非磁性体(19)のギャ
ップ形成側の端面(191)から前記第2の積層薄膜(
24)の上面(241)に亘って第3の強磁性金属薄膜
(25)を被着形成し、該強磁性金属薄膜(25)上に
ギャップスペーサ用のガラス層(26)をスパッタリン
グ等により被着形成して第2コア半体ブロツク(30b
)を形成する。
Next, as shown in FIG. 6, the second laminated thin film (
24) A third ferromagnetic metal thin film (25) is deposited over the upper surface (241), and a gap spacer glass layer (26) is coated on the ferromagnetic metal thin film (25) by sputtering or the like. The second core half block (30b
) to form.

次に、第3図に示す第1コア半体ブロンク(3t)a)
と第6図に示す第2コア半体ブロツク(30b)とを用
意し、該第1、第2コア半体ブロンク(±)(識)を第
7図に示すように第1コア半体ブロンク(30a)のギ
ャップ形成側の端面(31)とガラス1it(26)と
が対向する状態で衝き合わせて該ガラス層(26)を溶
融固化することにより接合してコアブロック(32)を
形成する。
Next, the first core half bronc (3t) a) shown in FIG.
and a second core half-bronch (30b) shown in FIG. The end face (31) on the gap forming side of (30a) and the glass 1it (26) are brought into contact with each other while facing each other, and the glass layer (26) is melted and solidified to join to form a core block (32). .

次に、前記コアブロック(32)を破線B−B’に沿っ
て切断してヘントチツブを複数個形成し、該ヘッドチッ
プに媒体摺接面のR付加工等の外形加工を行い、巻線溝
(18)を通して巻線(33)(33)を巻回して第1
図に示す本実施例の磁気ヘッドを形成する。
Next, the core block (32) is cut along the broken line BB' to form a plurality of hent chips, and the head chip is subjected to external processing such as rounding of the media sliding surface, and winding grooves are formed on the head chip. Winding wires (33) and (33) are wound through (18) and the first
The magnetic head of this example shown in the figure is formed.

上述のような本実施例の磁気へノドでは、第1コア半体
(12a)の第1の積層薄膜(16)の膜厚、即ちギャ
ップ形成面に露出している第1の積層薄膜(16)の端
面の幅は磁気ギャップ(27)の所望のトランク幅に等
しく、第2コア半体(1,2b)の第2の強磁性金属薄
膜(25)のギャップ衝き合わせ部の幅は磁気ギャップ
ク27)の所望のトラック幅よりも大きいため、第1、
第2コア半体(12a)(12b)の衝き合わせ位置に
ズレが生じても、磁気ギャップ(27)は前記積層薄膜
(16)の端面に形成されるため、前記磁気ギャップ(
27)のトランク幅は常に前記第1の積層薄膜(16)
の膜厚により正確に規定される。
In the magnetic head of this embodiment as described above, the thickness of the first laminated thin film (16) of the first core half (12a), that is, the first laminated thin film (16) exposed on the gap forming surface is ) is equal to the desired trunk width of the magnetic gap (27), and the width of the gap abutting portion of the second ferromagnetic metal thin film (25) of the second core half (1, 2b) is equal to the desired trunk width of the magnetic gap (27). 27), the first,
Even if the second core halves (12a) and (12b) are misaligned, since the magnetic gap (27) is formed on the end face of the laminated thin film (16), the magnetic gap (
The trunk width of 27) is always the same as that of the first laminated thin film (16).
It is precisely defined by the film thickness.

また、上述の磁気へノドでは、第2コア半体(12b)
の磁路が第2の積層薄膜(24)で形成されているので
高周波領域においても磁気飽和を生じることなく、渦電
流損失を抑え、記録再生特性の劣化を防止出来る。また
、媒体摺接面には前記第2の積層薄膜(24)が露出さ
れておらず、該第2の積層薄膜(24)の絶縁薄膜(2
3)が擬似ギャップとして作用することもない。
In addition, in the above-mentioned magnetic helix, the second core half (12b)
Since the magnetic path is formed by the second laminated thin film (24), magnetic saturation does not occur even in the high frequency range, eddy current loss can be suppressed, and deterioration of recording and reproducing characteristics can be prevented. Further, the second laminated thin film (24) is not exposed on the medium sliding contact surface, and the insulating thin film (24) of the second laminated thin film (24) is not exposed.
3) does not act as a pseudo gap.

(ト)発明の効果 本発明に依れば、磁気ギャップのトランク幅制度が向上
し、且つ高周波領域においても良好な記録再生を行うこ
とが出来る磁気ヘッドを提供し得る。
(G) Effects of the Invention According to the present invention, it is possible to provide a magnetic head that has improved trunk width precision of the magnetic gap and can perform good recording and reproduction even in a high frequency region.

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

第1図乃至第6図は本発明に係り、第1図は磁気へノド
の外観を示す斜視図、第2図、第3図、第4図、第5図
、第6図及び第7図は夫々磁気ヘッドの製造方法を示す
斜視図である。第8図及び第9図は夫々従来の磁気ヘッ
ドの外観を示す斜視図である。 (12a)・・・第1コア半体、(12b)・・・第2
コア半体、(13)(13’)・・・非磁性基板、(1
4)・・・第1の強磁性金属薄膜、(15)(23)・
・・絶縁薄膜、(16)・・・第1の積層薄膜、(19
)・・・非磁性体、(21)・・・溝、(22)・・・
第2の強磁性金属薄膜、(24)・・・第2の積層薄膜
、(25)・・・第3の強磁性金属薄膜、(26)・・
・ガラス層(非磁性材料ン、 (27)・・・磁気ギヤ
ノブ、(191)・・ギヤノγ形吸側の端面。 出1人 三洋電機株式会社 代理人 弁理士 西野卓嗣(外2名) 第1図 一’/ 第4図 第8図 第9図
Figures 1 to 6 relate to the present invention; Figure 1 is a perspective view showing the external appearance of the magnetic helix; Figures 2, 3, 4, 5, 6, and 7; 2A and 2B are perspective views showing a method of manufacturing a magnetic head, respectively. FIGS. 8 and 9 are perspective views showing the appearance of conventional magnetic heads, respectively. (12a)...first core half, (12b)...second core half
Core half, (13) (13')...Nonmagnetic substrate, (1
4)...first ferromagnetic metal thin film, (15)(23).
...Insulating thin film, (16)...First laminated thin film, (19
)...Nonmagnetic material, (21)...Groove, (22)...
Second ferromagnetic metal thin film, (24)...Second laminated thin film, (25)...Third ferromagnetic metal thin film, (26)...
・Glass layer (non-magnetic material) (27)...Magnetic gear knob, (191)...End face of gear knob γ type suction side. 1 person, Sanyo Electric Co., Ltd. agent, patent attorney Takuji Nishino (2 others) No. 1 Figure 1' / Figure 4 Figure 8 Figure 9

Claims (1)

【特許請求の範囲】[Claims] (1)一対の非磁性基板間に第1の強磁性金属薄膜と絶
縁薄膜とよりなり、厚みが磁気ギャップの所望のトラッ
ク幅に等しい第1の積層薄膜が被着形成され、ギャップ
形成側の端面に前記積層薄膜の端面が露出している第1
コア半体と、非磁性体のギャップ形成側の端面のうち媒
体摺接面とは反対側に溝を備え、該溝内に第2の強磁性
金属薄膜と絶縁薄膜とよりなり、上面が前記非磁性体の
ギャップ形成側の端面と面一である第2の積層薄膜が被
着形成され、該第2の積層薄膜上に幅が前記第1の積層
薄膜の厚みより大きい第3の強磁性金属薄膜が被着形成
されている第2コア半体とから成り、前記第1コア半体
と前記第2コア半体とを上記第1の積層薄膜の端面と上
記第3の強磁性金属薄膜の上面とが磁気ギャップとなる
非磁性材料を介して衝き合わされた状態で接合固定した
ことを特徴とする磁気ヘッド。
(1) A first laminated thin film consisting of a first ferromagnetic metal thin film and an insulating thin film and having a thickness equal to the desired track width of the magnetic gap is deposited between a pair of nonmagnetic substrates, and a first layer having an end surface with an end surface of the laminated thin film exposed;
A groove is provided on the side opposite to the medium sliding contact surface of the core half and the end face on the gap forming side of the non-magnetic material, a second ferromagnetic metal thin film and an insulating thin film are formed in the groove, and the upper surface is A second laminated thin film is deposited and formed flush with the end face of the non-magnetic material on the gap forming side, and a third ferromagnetic film having a width larger than the thickness of the first laminated thin film is formed on the second laminated thin film. a second core half on which a metal thin film is deposited, and the first core half and the second core half are connected to the end face of the first laminated thin film and the third ferromagnetic metal thin film. 1. A magnetic head characterized in that the upper surface of the magnetic head is bonded and fixed in a state where the upper surfaces thereof are brought into contact with each other through a non-magnetic material that forms a magnetic gap.
JP17337590A 1990-06-29 1990-06-29 Magnetic head Pending JPH0461012A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17337590A JPH0461012A (en) 1990-06-29 1990-06-29 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17337590A JPH0461012A (en) 1990-06-29 1990-06-29 Magnetic head

Publications (1)

Publication Number Publication Date
JPH0461012A true JPH0461012A (en) 1992-02-27

Family

ID=15959227

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17337590A Pending JPH0461012A (en) 1990-06-29 1990-06-29 Magnetic head

Country Status (1)

Country Link
JP (1) JPH0461012A (en)

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