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JPH0444609A - Thin film magnetic head - Google Patents

Thin film magnetic head

Info

Publication number
JPH0444609A
JPH0444609A JP2153207A JP15320790A JPH0444609A JP H0444609 A JPH0444609 A JP H0444609A JP 2153207 A JP2153207 A JP 2153207A JP 15320790 A JP15320790 A JP 15320790A JP H0444609 A JPH0444609 A JP H0444609A
Authority
JP
Japan
Prior art keywords
gap
layer
magnetic
magnetic layer
layers
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
JP2153207A
Other languages
Japanese (ja)
Inventor
Toshio Fukazawa
利雄 深澤
Kumiko Wada
久美子 和田
Yoshihiro Tozaki
善博 戸崎
Yuji Nagata
裕二 永田
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.)
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 JP2153207A priority Critical patent/JPH0444609A/en
Publication of JPH0444609A publication Critical patent/JPH0444609A/en
Pending legal-status Critical Current

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  • Magnetic Heads (AREA)

Abstract

PURPOSE:To prevent permeability from being lowered and to increase efficiency for recording and reproducing by alternately laminating a soft magnetic layer and an insulated layer in a wavy shape to a gap surface at a gap part to which upper and lower magnetic layers are faced through a gap layer. CONSTITUTION:At the time of recording, signal magnetic fields 13-16 are induced by a signal current impressed to a conductive coil 4 and on a cross section perpendicular to the magnetic fields 13-16 flowing in upper and lower magnetic layers 9 and 2, a soft magnetic layer 11 and an insulated layer 12 are alternately arranged so as not to generate any eddy current. Therefore, since the permeability at a gap part (d) between the layers 9 and 2 is not lowered, the satisfactory recording efficiency can be realized. Next, the satisfactory reproducing efficiency can be realized by the similar cause even at the time of reproducing. At the gap part (d), since a layer 12 forming the structure of laminating the layers 9 and 2 is formed wavy to the gap surface, the gap part (d) can become a pseudo gap and because of azimuth loss, however, any influence caused by the pseudo gap is not generated. Thus, satisfactory recording and reproducing can be executed.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は磁気記録再生装置などに用いられる薄膜磁気ヘ
ッドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a thin film magnetic head used in magnetic recording/reproducing devices and the like.

従来の技術 近年、磁気記録再生装置の高記録密度化、データの高転
送速度化に対応して薄膜磁気ヘッドが注目されている。
2. Description of the Related Art In recent years, thin film magnetic heads have been attracting attention in response to higher recording densities and higher data transfer speeds in magnetic recording and reproducing devices.

第6図に従来の薄膜磁気ヘッドの断面図を示す。FIG. 6 shows a cross-sectional view of a conventional thin film magnetic head.

第6図において、従来の巻線型の薄膜磁気ヘッドは、非
磁性基板21上に下部磁性層nが形成され、下部磁性層
η上にギャップとなる所定膜厚の絶縁層nを形成し、さ
らK、絶縁層夙に埋め込まれるようにして導電コイルゐ
を形成し、上部磁性層26を形成して構成される。
In FIG. 6, the conventional wire-wound thin film magnetic head includes a lower magnetic layer n formed on a non-magnetic substrate 21, an insulating layer n of a predetermined thickness forming a gap on the lower magnetic layer η, and K. A conductive coil is formed so as to be embedded in an insulating layer, and an upper magnetic layer 26 is formed.

上記構成により、記録時には導電コイル部に信号電流を
印加し、これにより、ギャップ部で発生する磁界により
記録媒体に記録を行い、また、再生時にはギャップ部か
ら流入する記録媒体上の信号磁界を導電コイルδにより
検出する。
With the above configuration, during recording, a signal current is applied to the conductive coil section, thereby recording is performed on the recording medium by the magnetic field generated in the gap section, and during playback, the signal magnetic field flowing in from the gap section on the recording medium is conducted. Detected by coil δ.

発明が解決しようとする課題 上記従来例における巻線型の薄膜磁気ヘッドでは、高周
波領域での動作時に漏電流損失などが生じ、また、高周
波領域では透磁率が低下するなどの問題が生じて効率よ
く記録再生することが困雌であった。
Problems to be Solved by the Invention In the conventional wire-wound thin film magnetic head described above, problems such as leakage current loss occur when operating in a high frequency region, and problems such as a decrease in magnetic permeability occur in a high frequency region. It was difficult to record and play back.

この問題を解消するため、上部磁性1g122と上部磁
性層拠には、第7図に示すように、軟磁性域27と絶縁
層かを交互Kl1層しでなる積層磁性膜を使用する方法
が知られて゛いる。しかしながら、このような構成にし
ても、ギャップ部a1.CK′おける渦電流損失を避け
ることができない。
In order to solve this problem, a method is known in which a laminated magnetic film is used for the upper magnetic layer 1g122 and the upper magnetic layer, as shown in FIG. I'm being beaten. However, even with such a configuration, the gap portion a1. Eddy current losses in CK' cannot be avoided.

この点についで以下に説明する。This point will be explained below.

まず、記録時においては、第7図に示すように。First, during recording, as shown in FIG.

信号磁界29,30.3’l 、32が誘起される。導
電コイル25(第7図には図示せず)の下に位aする下
部磁性lll122のb部中の信号磁界31に垂直な面
での下部磁性要部の断面は、!8図に示すように、軟磁
性層ごと絶縁層あが交互に並んだ形状をしているため、
#l!縁層281Cより、渦電流の発生か妨げられてい
る。これは導電、]イル5の上に位置するJ一部磁性@
加においしも同材である。しか(7、下部磁性M212
と」二部磁性層26がギャップ層2)を介し、C対向す
るギャップ部aと、F部磁性層22と」′、部磁性ji
126が直接接t−6後部ギャップ部Cでは、。磁界の
流れ30.32に垂直IJ而での上部磁性1i12(5
および下部磁性要部の断面はさらに、断面が一様に軟磁
性層nまたは絶縁膨脂となり、第9図に゛示すように、
軟磁性11127の場合例は信号磁界30.32により
渦電流33を生じて°ギャップ部aや、後部ギャップ部
Cでは透磁率が低ドする。特に、記録媒体と接するギャ
ップ部aKおいで透磁率が低重することは記録効率を十
げる要因とIJる。また、再生時にも記録の場合と同様
な理由により、再生効率が低下する。
Signal magnetic fields 29, 30.3'l, 32 are induced. The cross section of the lower magnetic main part in the plane perpendicular to the signal magnetic field 31 in the part b of the lower magnetic 122 located below the conductive coil 25 (not shown in FIG. 7) is ! As shown in Figure 8, each soft magnetic layer has a shape in which insulating layers are arranged alternately.
#l! The edge layer 281C prevents the generation of eddy currents. This is conductive, J part located above ile 5 is magnetic @
Kanioishi is also made from the same material. But (7, lower magnetic M212
The two-part magnetic layer 26 has a gap part a facing C and a part F magnetic layer 22 through the gap layer 2), part magnetic ji
126 directly contacts the t-6 rear gap section C. The upper magnetic field 1i12 (5
Further, the cross section of the lower magnetic main part is uniformly formed into a soft magnetic layer n or insulating swelling, as shown in FIG.
In the case of soft magnetism 11127, an eddy current 33 is generated by the signal magnetic field 30, 32, and the magnetic permeability is low in the gap part a and the rear gap part C. In particular, low magnetic permeability in the gap aK in contact with the recording medium is considered to be a factor that reduces recording efficiency. Furthermore, during playback, playback efficiency decreases for the same reason as during recording.

以上のような理由により、従来の薄膜磁気・\フドでは
十分な記録再生効率を実現することが困峻であった。
For the reasons mentioned above, it has been difficult to achieve sufficient recording and reproducing efficiency with conventional thin film magnetic/hoods.

また、F部磁性層nと上部磁性−3中のe線層3はギャ
ップ1123と平行に構成されており、テープ摺動面に
露出する絶縁層かは疑似ギャップとなり、この疑似ギャ
ップ部て一不必要な記録再生がなされ、C/N比の劣イ
しなど良好な記録再生かで傘ないという間融があった。
In addition, the F part magnetic layer n and the e-line layer 3 in the upper magnetic layer 3 are configured parallel to the gap 1123, and the insulating layer exposed on the tape sliding surface becomes a pseudo gap, and this pseudo gap part Unnecessary recording/reproduction was performed, and there was a problem with good recording/reproduction due to poor C/N ratio.

本発明は」−記従末の問題を解決するもので、ギャップ
部の上部磁性層およびト部磁性層での渦電流損失などに
よる高周波領域での透磁率の低下と疑似ギャップの影響
か1j<良好な記録再生特性を得ることができる薄膜磁
気ヘッドを提供することを目的とするものである3゜ muを解決するための手段 上記課題を解決するために本発明の薄膜磁気ヘッドは、
1部磁性層と下部磁性層は軟磁性−と絶縁層か交互に積
層された構成を有し、前記上部磁性層とギャップ層と前
記下部磁性層とからなる磁気回路の、前記上部磁性−と
F部磁性−が前&4ギャップ鳴を介して対向する少fL
 くともギャップ部で前記上部磁性層と下部磁性層を構
成する積層磁性膜の軟磁性層と絶縁層かギャップ面に対
し、て波型形状またはギャップ面に平行な面を有しない
折れ線形状に交互に積層された構成を有するものである
The present invention is intended to solve the problems mentioned above, and is concerned with the decrease in magnetic permeability in the high frequency region due to eddy current loss in the upper magnetic layer of the gap part and the magnetic layer of the lower part, and the influence of the pseudo gap 1j< The object is to provide a thin film magnetic head that can obtain good recording and reproducing characteristics.Means for solving the problem of 3㎜mu In order to solve the above problems, the thin film magnetic head of the present invention has the following features:
The first magnetic layer and the lower magnetic layer have a structure in which soft magnetic layers and insulating layers are alternately laminated, and the upper magnetic layer and the lower magnetic layer of the magnetic circuit consisting of the upper magnetic layer, the gap layer, and the lower magnetic layer. Small fL where F section magnetic - faces through front & 4 gap ring
At least in the gap part, the soft magnetic layer and the insulating layer of the laminated magnetic film constituting the upper magnetic layer and the lower magnetic layer are alternately formed into a wave shape or a polygonal shape having no plane parallel to the gap surface with respect to the gap surface. It has a laminated structure.

作  用 上記構成により、ギャップ面に対して波型形状またはギ
ャップ面に平行な面を有し5ない折れ線形状に軟磁性域
と絶縁層とを交互に積層するので、ギャップ部を流れる
磁界の方向に:垂直な方向の上部磁性層およびF部磁性
廣の断面か軟磁性域と絶縁層が交互に配置された形状と
なり、これにより、渦11流の発生が阻害されて、透磁
率は低下せず。
Effect With the above configuration, the soft magnetic regions and the insulating layers are alternately laminated in a wavy shape with respect to the gap surface or a polygonal shape with a surface parallel to the gap surface, so that the direction of the magnetic field flowing through the gap portion is A: The vertical cross-section of the upper magnetic layer and the F section magnetic field has a shape in which soft magnetic regions and insulating layers are alternately arranged, which inhibits the generation of vortex 11 flow and reduces magnetic permeability. figure.

良好な記録再生効率が得られる。また、上部磁性層と下
部磁性層を構成する積層磁性膜中の絶縁層がギャップ部
でギャップ面に対して波型形状、または、ギャップ面に
平行な面を有し7ない折れ線形状をしでいるので、絶縁
層が疑似ギャップとなってもアジマス損失により疑似ギ
ャップによる1曽は生じることなく良好な記録再生が可
能となる。
Good recording and reproducing efficiency can be obtained. In addition, the insulating layer in the laminated magnetic film constituting the upper magnetic layer and the lower magnetic layer has a wavy shape with respect to the gap plane at the gap portion, or a polygonal line shape with a plane parallel to the gap plane. Therefore, even if the insulating layer becomes a pseudo-gap, good recording and reproducing is possible without causing azimuth loss due to the pseudo-gap.

実施例 以下、本発明の実施例について図面を参照し2ながら説
明する。
Embodiments Hereinafter, embodiments of the present invention will be described with reference to the drawings.

第1図(a、lは本発明の第1の実施例における薄膜磁
気ヘッドの平面図、第1図(b)は第1図(a、l[お
けるA・−A゛断面図5第1図(e)は第1図(a)K
おけるB−B’断面図である。第1図(al (bl 
(dにおいて、薄膜磁気ヘッドは非磁性基板1上に下部
磁性層2が形成され、第1の絶縁層3を介して導電コイ
ル4が形成され、さらに、第2の絶縁層5で導電コイル
4は上部磁性層9と絶縁されている。ギャップ部dでは
ギャップ層7を介して、上部磁性層9と下部磁性層2が
対向しており、後部ギャップ部fでは上部磁性層9と下
部磁性層2は接している。
FIG. 1 (a, l is a plan view of a thin film magnetic head in the first embodiment of the present invention, FIG. 1 (b) is a cross-sectional view of A--A in FIG. Figure (e) is Figure 1 (a) K
It is a BB' sectional view in . Figure 1 (al (bl)
(In d, in the thin film magnetic head, a lower magnetic layer 2 is formed on a non-magnetic substrate 1, a conductive coil 4 is formed via a first insulating layer 3, and a conductive coil 4 is formed on a second insulating layer 5. is insulated from the upper magnetic layer 9. In the gap part d, the upper magnetic layer 9 and the lower magnetic layer 2 face each other with the gap layer 7 in between, and in the rear gap part f, the upper magnetic layer 9 and the lower magnetic layer 2 are in contact.

上部磁性層9と下部磁性層2は、第2図に示すように、
e磁性層11と絶縁層りを積層した積層磁性膜からなり
、また、ギャップ層(第2図中には図示せず)を介して
上部磁性層9と下部磁性層2が対向するギャップ部dで
上部磁性m9と下部磁性層2はギャップ面に対し波型形
状に軟磁性層11と絶縁層12が交互に積層された構成
を有している。
As shown in FIG. 2, the upper magnetic layer 9 and the lower magnetic layer 2 are
e Consisting of a laminated magnetic film in which a magnetic layer 11 and an insulating layer are laminated, and a gap portion d where the upper magnetic layer 9 and the lower magnetic layer 2 face each other via a gap layer (not shown in FIG. 2). The upper magnetic layer m9 and the lower magnetic layer 2 have a structure in which soft magnetic layers 11 and insulating layers 12 are alternately laminated in a wavy shape with respect to the gap plane.

上記構成によりギャップ部dの上部磁性層9と下部磁性
層2においては渦電流を生じないので透磁率の低下もな
く、良好な記録再生効率が得られる。これについて第2
図および第3図を用いて説明する。
With the above structure, no eddy current is generated in the upper magnetic layer 9 and the lower magnetic layer 2 in the gap d, so there is no decrease in magnetic permeability, and good recording and reproducing efficiency can be obtained. Regarding this, the second
This will be explained using the diagram and FIG.

まず、記録時には導電コイル4に印加された信号電流に
より、第2図に示すように、信号磁界13.14,15
.16が誘起される。導電コイル4の上に位置する上部
磁性層9を流れる信号磁界13に垂直な方向の断面は、
第3図に示すように、軟磁性層11と絶縁層12が交互
に配置されたものとなっているので渦電流は生じない。
First, during recording, a signal current applied to the conductive coil 4 creates a signal magnetic field 13, 14, 15, as shown in FIG.
.. 16 is induced. The cross section in the direction perpendicular to the signal magnetic field 13 flowing through the upper magnetic layer 9 located above the conductive coil 4 is as follows:
As shown in FIG. 3, since the soft magnetic layers 11 and the insulating layers 12 are alternately arranged, no eddy current is generated.

また、導電コイル4の下に位置する下部磁性層2を流れ
る信号磁界15の場合も同様である。さらに、ギャップ
部dの上部磁性層9と下部磁性層2を流れる信号磁界1
4に垂直な方向の断面は、第4図に示すように、軟磁性
層11と絶縁層12が交互に配置されたものとなってい
るので渦電流は生じない。したかって、上部磁性層9と
下部磁性層2のギャップ部dにおける透磁率は従来のよ
うに低下しないため、良好な記録効率を実現できる。次
に、再生時にも同様の理由で、上部磁性層9と下部磁性
層2のギャップ部dにおける透磁率は低下しないため、
良好な再生録効率を実現できる。また、ギャップ部dで
は上部磁性層9と下部磁性層2の積層構造を形成する絶
縁層12はギャップ面に対し波型形状をしているため、
疑似ギャップとなり得るが、アジマス損失により疑似ギ
ャップによる影響は生じない。よって良好な記録再生が
できる。
The same applies to the signal magnetic field 15 flowing through the lower magnetic layer 2 located below the conductive coil 4. Furthermore, the signal magnetic field 1 flowing through the upper magnetic layer 9 and the lower magnetic layer 2 in the gap portion d
4, the soft magnetic layers 11 and the insulating layers 12 are alternately arranged, so that no eddy current occurs. Therefore, since the magnetic permeability at the gap d between the upper magnetic layer 9 and the lower magnetic layer 2 does not decrease as in the conventional case, good recording efficiency can be achieved. Next, during reproduction, for the same reason, the magnetic permeability at the gap d between the upper magnetic layer 9 and the lower magnetic layer 2 does not decrease.
Good playback/recording efficiency can be achieved. Furthermore, in the gap part d, the insulating layer 12 forming the laminated structure of the upper magnetic layer 9 and the lower magnetic layer 2 has a wave-like shape with respect to the gap surface.
Although it can be a pseudo gap, the effect of the pseudo gap does not occur due to azimuth loss. Therefore, good recording and reproduction can be performed.

なお、本実施例において、上部磁性層2と下部磁性層9
を波型形状に積層したのはギャップ部dのみであったが
、後部ギャップ部fにおいても上部磁性層2と下部磁性
層9をギャップ部dと同様に波型形状に積層することに
より、後部ギャップ部fにおける透磁率を低下させない
ことが可能で、さらに記録再生特性を向上させることが
できる。
Note that in this embodiment, the upper magnetic layer 2 and the lower magnetic layer 9
It was only in the gap part d that the upper magnetic layer 2 and the lower magnetic layer 9 were laminated in a wave-like shape in the same way as in the gap part d, so that the rear gap part f was laminated in a wave-like shape. It is possible not to reduce the magnetic permeability in the gap part f, and it is possible to further improve the recording and reproducing characteristics.

また、上部磁性層2と下部磁性Mlt9の導電コイル4
の上下に位置する部分eにおいてもギャップ部dと同様
に波型形状に積層しても磁界の流れに垂直な方向の断面
は軟磁性層11と絶縁層12が交互に配置されたものと
なっているので、やはり、渦電流は発生せず、透磁率の
低下も生じない。よって、上部磁性層と下部磁性層のす
べての部分で波型形状に積層しても、良好な記録再生効
率を実現できる。
Moreover, the conductive coil 4 of the upper magnetic layer 2 and the lower magnetic Mlt9
Similarly to the gap portion d, in the portion e located above and below the layer, even if the layers are laminated in a wave-like shape, the cross section in the direction perpendicular to the flow of the magnetic field shows that the soft magnetic layer 11 and the insulating layer 12 are arranged alternately. Therefore, no eddy current is generated and no decrease in magnetic permeability occurs. Therefore, good recording and reproducing efficiency can be achieved even if all the upper and lower magnetic layers are laminated in a wave-like shape.

次に、第2の実施例について第5図を用いて説明する。Next, a second embodiment will be described using FIG. 5.

第5図(atは第2の実施例における薄膜磁気ヘッドの
平面図、第5図1alは第5図(at中のD−D°断面
図、第5図(c)は第5図(at中のE−E’断面図で
あり、1図と同一の構成要素には同一番号を付してその
説明を省略する。第5図1al (bl (c)におい
て上部磁性層19ど下部磁性層美は軟磁性層17と絶縁
層18を積層した積層磁性膜からなり、さらに、ギャッ
プ部gで上部磁性1119と下部磁性層加はギャップ面
に平行な面を有しない折れ線形状に軟磁性1117と絶
縁層18が交互に積層された構成を有している。
FIG. 5 (at is a plan view of the thin film magnetic head in the second embodiment, FIG. 5 1al is a DD degree cross-sectional view in FIG. 5 is a cross-sectional view taken along the line EE' in FIG. 1, and the same components as in FIG. The magnetic layer consists of a laminated magnetic film in which a soft magnetic layer 17 and an insulating layer 18 are laminated, and the upper magnetic layer 1119 and the lower magnetic layer 1117 are formed in a polygonal shape with no plane parallel to the gap plane at the gap g. It has a structure in which insulating layers 18 are stacked alternately.

このように構成することにより、第1の実施例と同様、
ギャップ部gでの磁界の流れに垂直な方向の1frrr
Uは軟磁性層17と絶縁層18が交互に配置されたもの
となっているので、渦電流は発生せず透磁率の低下も生
じない。さらに、絶縁層18はギャップ面に平行な面を
有しない折れ線形状をしているため、疑似ギャップとな
り得るが、アジマス損失により疑似ギャップによる影響
は生じない。よって良好な記録再生ができる。
By configuring in this way, similar to the first embodiment,
1frrr in the direction perpendicular to the flow of the magnetic field at the gap g
Since the U has soft magnetic layers 17 and insulating layers 18 arranged alternately, no eddy current is generated and no decrease in magnetic permeability occurs. Furthermore, since the insulating layer 18 has a polygonal line shape that does not have a plane parallel to the gap plane, it may become a pseudo gap, but the effect of the pseudo gap does not occur due to azimuth loss. Therefore, good recording and reproduction can be performed.

また、上部磁性層19と下部磁性層加の導電コイル4の
手下に位置する部分lにおいてもギャップ層gと同様に
ギャップ面に゛平行な面を有(2ない折i、、 i形状
さ17.でも、渦電流は発生せず透磁率の低下も生じな
いので、後部ギャップ層り苓含む、F部磁性層19と上
部磁性@(イ)の−4べての部分で4−ヤフブ部gと同
様にギャップ面に平行なIiiをイ](、ない拍れ線形
状に積層りでも、良好な記録再生効率を実現でき、るこ
とも第1の実施例さ同様である。
In addition, the portion 1 of the upper magnetic layer 19 and the lower magnetic layer located below the conductive coil 4 also has a surface parallel to the gap plane (i shape 17) similar to the gap layer g. However, since no eddy current is generated and no decrease in magnetic permeability occurs, all parts of the F section magnetic layer 19 and the upper magnetic layer (A), including the rear gap layer, are Similarly to the first embodiment, good recording and reproducing efficiency can be achieved even when the layers are stacked in a straight line shape without parallel to the gap plane.

発明の効果 以上のように本発明の薄膜磁気ヘッドによれば軟磁性層
と絶縁層を交互に積層]2てなる積層磁性膜からなる上
部磁性層と上部磁性層かギャップ層を介し7で一対向す
る少なくともギ轡、フブ部でギャップ面に対j、、て波
型形状、または、ギャップ向に平行y;c rNiを有
しない折れ線形状に軟磁性層と絶縁層が交互に積置され
た横゛成とすることにより、ギャップ層におりる渦電流
損失に起因する透磁率の低下を防ぐことができて記録再
生効率を増大させると−一かできる◆)のである。
Effects of the Invention As described above, according to the thin film magnetic head of the present invention, the upper magnetic layer consisting of the laminated magnetic film consisting of the soft magnetic layer and the insulating layer are laminated alternately. Soft magnetic layers and insulating layers are alternately stacked in a wave-like shape or a polygonal line shape parallel to the gap direction without Ni at least on the opposing gears and the fub portion. By using a horizontal structure, it is possible to prevent a decrease in magnetic permeability caused by eddy current loss flowing through the gap layer, thereby increasing the recording and reproducing efficiency.

また、ナーブ摺動面(C露出する上部磁性−および上部
磁性層を構成する積層磁γを膜中の絶縁−は疑うソ、ギ
ャブブとなるか、この絶縁層は1ニキブブ面に対し2波
型形状、または、ギャップ面に平ht面を有1.ない折
れ線形状に゛露出4るたと)アジ1ス損矢に才り4似ギ
ャップの影響は無視できて良好な記録再生を行うと、と
かで鼻るものである。
In addition, it is doubtful that the nub sliding surface (the exposed upper magnetic layer and the insulation in the film of the laminated magnetic It is said that if the shape or gap surface has a flat surface and a polygonal line shape with no flat surface is exposed, the influence of the gap can be ignored and good recording and playback can be performed. It's something to sniff at.

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

第1図(al fb) fe)は本発明の第1の実施例
[おける薄膜磁気ヘッドのψ面図、第1図(a) vc
おけるA−A’断面図およびB・−B′断面図、第2図
は同#膜磁気ヘマトの積層磁性層の斜視図、第3図およ
び第4図は同f5薄膜磁気ヘッドの磁性層の断面図、第
5図(aM’b)(e) P第2の実施例におけるW#膜磁気ヘッドの平面図、第
5図(a)におりる丁)−pHlT面図、E−E ’断
面図7゜第6図は従来の薄膜磁気ヘッドの断面図、第7
図は従来の薄膜磁気ヘッドにおける積層磁性層の斜視図
、第8図および第9図は従来の傅膜磁気ヘッドにおける
積層磁性層の断面図である。 2.20・−・下部磁性層、7−・・ギャップ層、9,
19・・・上部磁性層、]、 1 、1.7・−・軟磁
性層、12.18・・・絶縁層、 ・・・ギャッーノ部う 代 理 人 森 本 義 弘 第1図 cj) dρ 4ル、仰Nイ、7′遮p 第 因 !!3 丙 第1図 (/+ 第5図 +b) 第2図
FIG. 1 (al fb) fe) is a ψ plane view of the thin film magnetic head in the first embodiment of the present invention; FIG. 1 (a) vc
Figure 2 is a perspective view of the laminated magnetic layer of the same # film magnetic hematome, and Figures 3 and 4 are the magnetic layer of the same f5 thin film magnetic head. Cross-sectional view, Fig. 5 (aM'b) (e) P Plan view of the W# film magnetic head in the second embodiment, Fig. 5 (a) - pHlT plane view, E-E' Cross-sectional view 7゜Figure 6 is a cross-sectional view of a conventional thin film magnetic head.
The figure is a perspective view of a laminated magnetic layer in a conventional thin-film magnetic head, and FIGS. 8 and 9 are cross-sectional views of the laminated magnetic layer in a conventional thin-film magnetic head. 2.20...lower magnetic layer, 7-...gap layer, 9,
19...Top magnetic layer,], 1, 1.7...Soft magnetic layer, 12.18...Insulating layer,...Yoshihiro Morimoto, agent of Gyakno Department Figure 1cj) dρ 4le, Upward N, 7' interception, the first cause! ! 3 C Figure 1 (/+ Figure 5 + b) Figure 2

Claims (1)

【特許請求の範囲】[Claims] 1、軟磁性層と絶縁層が交互に積層された構成を有する
積層磁性膜からなる上部磁性層および下部磁性層が設け
られる薄膜磁気ヘッドであって、前記上部磁性層とギャ
ップ層と前記下部磁性層とからなる磁気回路の前記上部
磁性層と下部磁性層が前記ギャップ層を介して対向する
少なくともギャップ部で前記上部磁性層と下部磁性層を
構成する前記積層磁性膜の軟磁性層と絶縁層がギャップ
面に対して波型形状またはギャップ面に平行な面を有し
ない折れ線形状に交互に積層された構成を有する薄膜磁
気ヘッド。
1. A thin film magnetic head provided with an upper magnetic layer and a lower magnetic layer made of a laminated magnetic film having a structure in which soft magnetic layers and insulating layers are alternately laminated, wherein the upper magnetic layer, the gap layer, and the lower magnetic layer a soft magnetic layer and an insulating layer of the laminated magnetic film forming the upper magnetic layer and the lower magnetic layer at least at a gap portion where the upper magnetic layer and the lower magnetic layer of the magnetic circuit face each other with the gap layer interposed therebetween; A thin-film magnetic head having a structure in which the layers are alternately stacked in a wave-like shape with respect to the gap plane or in a polygonal line shape with no plane parallel to the gap plane.
JP2153207A 1990-06-11 1990-06-11 Thin film magnetic head Pending JPH0444609A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2153207A JPH0444609A (en) 1990-06-11 1990-06-11 Thin film magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2153207A JPH0444609A (en) 1990-06-11 1990-06-11 Thin film magnetic head

Publications (1)

Publication Number Publication Date
JPH0444609A true JPH0444609A (en) 1992-02-14

Family

ID=15557388

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2153207A Pending JPH0444609A (en) 1990-06-11 1990-06-11 Thin film magnetic head

Country Status (1)

Country Link
JP (1) JPH0444609A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6473265B1 (en) * 1999-12-06 2002-10-29 Seagate Technology Llc High frequency writer with sliced core topology

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6473265B1 (en) * 1999-12-06 2002-10-29 Seagate Technology Llc High frequency writer with sliced core topology

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