JPS62180507A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPS62180507A JPS62180507A JP2191386A JP2191386A JPS62180507A JP S62180507 A JPS62180507 A JP S62180507A JP 2191386 A JP2191386 A JP 2191386A JP 2191386 A JP2191386 A JP 2191386A JP S62180507 A JPS62180507 A JP S62180507A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic head
- conductor coil
- ferrite
- gap
- conductive coil
- 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
Links
- 229910000859 α-Fe Inorganic materials 0.000 claims abstract description 33
- 239000000696 magnetic material Substances 0.000 claims abstract 3
- 239000004020 conductor Substances 0.000 claims description 57
- 238000006243 chemical reaction Methods 0.000 claims description 3
- 239000000758 substrate Substances 0.000 abstract description 5
- 238000000992 sputter etching Methods 0.000 abstract description 4
- 238000004544 sputter deposition Methods 0.000 abstract description 3
- 239000010409 thin film Substances 0.000 description 6
- 230000000694 effects Effects 0.000 description 5
- 238000004519 manufacturing process Methods 0.000 description 5
- 230000007423 decrease Effects 0.000 description 4
- 238000005516 engineering process Methods 0.000 description 3
- 230000004907 flux Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 238000000227 grinding Methods 0.000 description 2
- 238000003754 machining Methods 0.000 description 2
- 238000001020 plasma etching Methods 0.000 description 2
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 239000003822 epoxy resin Substances 0.000 description 1
- 239000010408 film Substances 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000005012 migration Effects 0.000 description 1
- 238000013508 migration Methods 0.000 description 1
- 238000007747 plating Methods 0.000 description 1
- 229920000647 polyepoxide Polymers 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/133—Structure or manufacture of heads, e.g. inductive with cores composed of particles, e.g. with dust cores, with ferrite cores with cores composed of isolated magnetic particles
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/17—Construction or disposition of windings
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Magnetic Heads (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明□の利用分野〕
本発明は、フェライトコア及び薄膜導体コイルとよりな
り、書込効率の向上及び製造法の簡単化された磁気ヘッ
ドに関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of Invention □] The present invention relates to a magnetic head comprising a ferrite core and a thin film conductor coil, which improves writing efficiency and simplifies the manufacturing method.
従来の薄膜磁気ヘッドの書込効率を向上させる構造とし
て、特開昭55−62523号公報で開示されているも
のが上げられる。第3図はそのリング型薄膜磁気ヘッド
の断面図である。A structure for improving the writing efficiency of a conventional thin film magnetic head is disclosed in Japanese Patent Application Laid-Open No. 55-62523. FIG. 3 is a sectional view of the ring-type thin film magnetic head.
この構造によれば、基板21上に下部磁性層22を形成
し、次いで絶縁層23.導体コイル24を交互に形成す
る。この時、第1絶縁層と第2絶縁層はへラドギャップ
層となる。さらに、導体コイル24の形状は、対向面2
6から遠ざかるにつれてその幅が増大する、従って、断
面積が順次増大するように構成されている。次いで、上
部磁性層25を形成させ、磁気ヘッドが完成される。According to this structure, a lower magnetic layer 22 is formed on a substrate 21, and then an insulating layer 23. Conductor coils 24 are formed alternately. At this time, the first insulating layer and the second insulating layer become Herad gap layers. Furthermore, the shape of the conductor coil 24 is different from that of the opposing surface 2.
The width increases as the distance from 6 increases, and thus the cross-sectional area increases sequentially. Next, an upper magnetic layer 25 is formed to complete the magnetic head.
この様な構造においては、磁気記録媒体に最も近い位置
に巻回された導体コイルの幅によって磁気ヘッドの発生
磁場強さがほぼ規定されるため、媒体から遠い方の位置
のコイル部分の幅を大きくしても書込効率はほとんど変
わらず。In such a structure, the strength of the magnetic field generated by the magnetic head is almost determined by the width of the conductor coil wound at the position closest to the magnetic recording medium. Even if you increase the size, the write efficiency remains almost the same.
かつ導体コイル24の両端間の電気抵抗を大幅に減少さ
せることができる。さらに、本構造は、媒体対向面に最
も近い導体コイルの先端部とギャップ深さGd=Oとの
距離Cが数μm以下と小さいため、書込効率を向上させ
た構造となっている等の利点を有している。しかしなが
ら。Moreover, the electrical resistance between both ends of the conductor coil 24 can be significantly reduced. Furthermore, in this structure, the distance C between the tip of the conductor coil closest to the medium facing surface and the gap depth Gd=O is as small as several μm or less, resulting in improved writing efficiency. It has advantages. however.
媒体対向面に最も近い位置に巻回された導体コイル24
に、一定の記録電流を流した場合、最も電流密度が高く
なる為、導体コイル24を覆う絶縁層23のテーパ角Q
1が大きい程、導体コイル24の側面部を覆う絶縁層2
3の有効膜厚aが減少し、上部磁性層25との隙間が狭
まくなり、絶縁劣化を生じ易く、信頼性に問題が生じ易
くなる。また1図の如く、多層構造を有した薄膜磁気ヘ
ッドは、素子形成時の製造工程を増やすことになり、磁
気ヘッド性能のバラツキ要因を多く持ち、歩留り低下を
きたしやすくなっている。Conductor coil 24 wound at the position closest to the medium facing surface
When a constant recording current is passed through, the current density is the highest, so the taper angle Q of the insulating layer 23 covering the conductor coil 24 is
The larger 1 is, the more the insulating layer 2 covering the side surface of the conductor coil 24 is.
The effective film thickness a of No. 3 decreases, and the gap with the upper magnetic layer 25 narrows, making insulation deterioration more likely to occur and reliability problems more likely to occur. Further, as shown in FIG. 1, a thin film magnetic head having a multilayer structure requires an additional manufacturing process when forming an element, has many factors that cause variations in magnetic head performance, and is likely to cause a decrease in yield.
一方、磁気ヘッド構造を簡単化し、歩留り低下を防止で
きる様な構造も提案されている。その−例が、特開昭5
7−78615に示されるもので、第4図にて、概略を
説明する。フェライト基体31に導体コイル34を形成
する部分に、フォトリングラフ及び反応性イオンエツチ
ング法を用いて、その上にアルミナの絶縁層37を付着
(ヘッドギャップ部となる)させ、その後、溝内の絶縁
層37の上に導体コイル34を形成し、最後にフェライ
ト閉磁体32をフェライト基体31に結合して磁気ヘッ
ドが完成される。このような構造においては、磁気変換
ギャップ近傍のアペックス角Q′は、磁気ヘッドの効率
に大きな影響を与えるため、溝加工する際のアペックス
角となる傾斜角Qを十分な精度に仕上げなければ、磁気
ヘッドの性能にバラツキが生じ、歩留り低下の原因とな
る。これを避ける為には、フォトリングラフ及び反応性
イオンエツチング法等による溝加工には、Qを厳密にお
さえるために高度な技術と高度な作業管理を必要とされ
る。On the other hand, a structure has also been proposed that simplifies the magnetic head structure and prevents a decrease in yield. An example of this is JP-A No. 5
7-78615, and its outline will be explained with reference to FIG. An insulating layer 37 of alumina is deposited on the portion of the ferrite base 31 where the conductor coil 34 is to be formed using photoringraph and reactive ion etching (to form the head gap portion), and then the insulating layer 37 in the groove is A conductor coil 34 is formed on the insulating layer 37, and finally the ferrite closed magnetic body 32 is bonded to the ferrite base 31 to complete the magnetic head. In such a structure, the apex angle Q' near the magnetic transducer gap has a large effect on the efficiency of the magnetic head, so unless the inclination angle Q, which is the apex angle when machining the groove, is finished with sufficient precision, This causes variations in the performance of the magnetic head, causing a decrease in yield. In order to avoid this, advanced technology and advanced work management are required for groove processing using photoringraph, reactive ion etching, etc. in order to strictly suppress Q.
本発明の目的は、前述した高度な精度や製造技術を必要
とせず、書込効率の向上を計り、かつ、導体コイルの電
気抵抗を低減させ性能の変動を少なくし高信頼性を確保
した磁気ヘッドを容易に製造できる磁気ヘッド構造を提
供することにある。The purpose of the present invention is to improve the writing efficiency without requiring the above-mentioned high precision and manufacturing technology, and to reduce the electrical resistance of the conductor coil to reduce fluctuations in performance and ensure high reliability. An object of the present invention is to provide a magnetic head structure that allows the head to be manufactured easily.
本発明は、フェライト基体とフェライト閉磁体を貼り合
わせた磁気ヘッド構造において、少なくとも導体コイル
の一部が、前記フェライト基体あるいは、フェライト閉
磁体に形成される磁気ヘッドのギャップ内に配置された
ことを特徴とする。また前記導体コイルの一部が、前記
したギャップ内に配置され、かつ媒体対向面から遠ざか
るにつれ、導体コイルの断面積が順次増大させるような
形状としたことを特徴とするものである。The present invention provides a magnetic head structure in which a ferrite base and a ferrite closed magnetic body are bonded together, in which at least a part of the conductor coil is disposed within the gap of the magnetic head formed on the ferrite base or the ferrite closed magnetic body. Features. Further, a portion of the conductor coil is disposed within the gap described above, and the cross-sectional area of the conductor coil gradually increases as the distance from the medium facing surface increases.
以下1本発明の一実施例を第1図及び第2図により説明
する。An embodiment of the present invention will be described below with reference to FIGS. 1 and 2.
第1図は本発明による磁気ヘッド構造を示し。FIG. 1 shows a magnetic head structure according to the present invention.
第2図は断面図を示している。まず比抵抗の大きいNi
−Zn等のフェライト基体1上に、AQ20..5in
2等からなるギャップ層3をスパッタ等で形成する。次
いで、導体コイルを形成するための溝9をイオンミリン
グ等により、所望の形状で導体コイル4が埋設されるよ
うに溝加工する。この時、媒体対向面側に最も近い位置
に巻回される導体コイル4が、フェライト基体1とフェ
ライト閉磁体2とを貼り合わせた際、フェライト閉磁体
2の溝加工されていない、媒体対向面側10の領域内に
あるような1位置に溝加工する。次いで、溝加工された
ギャップ層3内に導体コイル4(例えばAu、Al1.
Cu。FIG. 2 shows a cross-sectional view. First, Ni has a high specific resistance.
- AQ20. .. 5in
A gap layer 3 made of 2 etc. is formed by sputtering or the like. Next, the groove 9 for forming the conductor coil is processed by ion milling or the like so that the conductor coil 4 is buried in a desired shape. At this time, when the ferrite base 1 and the ferrite closed magnetic body 2 are bonded together, the conductor coil 4 wound at the position closest to the medium facing surface side Groove at one location, such as in the area of side 10. Next, a conductor coil 4 (for example, Au, Al1.
Cu.
Ag等)をメッキ、蒸着、スパッタ等により前述したギ
ャップ層3の膜厚以下(例えばギャップ層を1μm厚さ
とすれば、0.8μmの厚さで)形成する。次いでイオ
ンミリング等で所望の形状となるよう加工する。この際
、埋設される導体コイル4は、媒体対向面11から遠ざ
かるにつれてその幅を増大させ、断面積が順次増大する
ような形状としても良い。さらに前述した溝加工されな
い媒体対向面側10の領域内に複数の導体コイルがあっ
ても良い。この様にしてギャップ層3内に埋設するよう
に導体コイル4を形成したフェライト基体1を作る。Ag, etc.) is formed by plating, vapor deposition, sputtering, etc. to a thickness equal to or less than that of the gap layer 3 described above (for example, if the gap layer is 1 μm thick, the thickness is 0.8 μm). Next, it is processed into a desired shape by ion milling or the like. At this time, the buried conductor coil 4 may have a shape such that its width increases as it moves away from the medium facing surface 11, and its cross-sectional area gradually increases. Furthermore, there may be a plurality of conductor coils in the region of the medium facing surface side 10 that is not grooved. In this way, a ferrite base 1 having a conductor coil 4 formed thereon so as to be buried within the gap layer 3 is produced.
もう一方のフェライト閉磁体2は、まず、所望の磁気ヘ
ッドのトラック幅となる様に、フェライト材をガラス層
7により分離した一体化した棒状に造り、次に所望の厚
さに切断し板状にし、フェライト基体1との合せ面側を
ラップ仕上げをし、その抜溝5及び、溝5′を機械研削
加工等により加工する。この詩情5の位置は。The other ferrite closed magnetic body 2 is first made of ferrite material into an integrated rod shape separated by a glass layer 7 so as to have the desired track width of the magnetic head, and then cut into a desired thickness to form a plate. The surface to be mated with the ferrite base 1 is finished by lapping, and the grooves 5 and 5' are processed by mechanical grinding or the like. What is the position of this poem 5?
フェライト基体1と合わせた際導体コイル4の媒体対向
面に最も近い位置には対向せず、2番目以降の導体コイ
ルに対向する位置になるようにする事がのぞましい。こ
のようにしてフェライト閉磁体2を完成する。When combined with the ferrite base 1, it is preferable that the conductor coil 4 not face the position closest to the medium facing surface, but be located at a position facing the second and subsequent conductor coils. In this way, the ferrite closed magnetic body 2 is completed.
次にフェライト基体1とフェライト閉磁体2をエポキシ
樹脂9等により貼り合わせる。この時、第2図に示すよ
うに前述した。媒体対向側に最も近い位置に巻回された
導体コイル後端とフェライト閉磁体2のアペックス部の
相対位置aが多少変動してもかまわない。そして、導体
コイル4の一部であるバッド8及び8′は、磁気ヘッド
駆動回路へ接続するためのワイヤ(図示せず)を接続す
るために設けられており、溝5′は、そのワイヤ接続の
逃げ溝となっている。Next, the ferrite base 1 and the ferrite closed magnetic body 2 are bonded together using an epoxy resin 9 or the like. At this time, as shown in FIG. 2, as described above. It does not matter if the relative position a between the rear end of the conductor coil wound at the position closest to the medium facing side and the apex portion of the ferrite closed magnetic body 2 varies somewhat. The pads 8 and 8', which are part of the conductor coil 4, are provided for connecting wires (not shown) for connection to the magnetic head drive circuit, and the grooves 5' are for connecting the wires. It serves as an escape groove.
そして1機械加工により、ギャップ深さ加工して、磁気
ヘッドを完成させる。Then, the gap depth is processed by one machining process to complete the magnetic head.
この様にして構成した磁気ヘッドは、第2図で示される
様に、導体コイル4の一部が、媒体対向面に十分近い位
置にあるため、書込効率の良い、磁気ヘッドを得る事が
出来る。さらに。In the magnetic head constructed in this way, as shown in FIG. 2, a part of the conductor coil 4 is located sufficiently close to the medium facing surface, so that a magnetic head with good writing efficiency can be obtained. I can do it. moreover.
導体コイル4は、磁気変換ギャップ部内で、媒体対向面
側に容易に近づけることが可能であるため、より書込効
率の向上した磁気ヘッドを得る事が可能である。Since the conductor coil 4 can be easily brought close to the medium facing surface within the magnetic conversion gap, it is possible to obtain a magnetic head with improved writing efficiency.
また、磁気変換ギャップ近傍のアペックス角Qは、研削
等機械加工で行う事が出来るため。In addition, the apex angle Q near the magnetic conversion gap can be adjusted by mechanical processing such as grinding.
アペックス角Qや、溝5の位置を正確に加工を行なうこ
とができ、さらに、第2図中で示される導体コイル後端
とアペックス部の相対位置aが、フェライト基体1とフ
ェライト閉磁体2を貼り合わせる際、第2図中の8寸法
が多少変動しても前述したように、導体コイルが媒体対
向面に十分近い位置にあるため、ヘッド効率はほとんど
変わらない。従ってこのように構成した磁気ヘッドは高
度な製造技術を必要とせず1M単化されるため、書込効
率が良く、性能の揃った、かつ高信頼性を確保した磁気
ヘッドを容易に作製する事が出来る。The apex angle Q and the position of the groove 5 can be precisely machined, and the relative position a between the rear end of the conductor coil and the apex portion shown in FIG. When bonding, even if the dimension 8 in FIG. 2 changes somewhat, the head efficiency will hardly change because the conductor coil is located sufficiently close to the medium facing surface, as described above. Therefore, since the magnetic head configured in this manner does not require advanced manufacturing technology and can be made into a single 1M unit, it is possible to easily manufacture a magnetic head with good writing efficiency, uniform performance, and high reliability. I can do it.
第5図は、本発明の他の一実施例を示す断面図である。FIG. 5 is a sectional view showing another embodiment of the present invention.
第2図で示した実施例と異なる点は、導体コイルの一部
がギャップ内に配置されかつこの導体コイル4が媒体対
向面から遠ざかるにつれて、導体コイルの断面積が順次
増大するように構成されている事にある。この様な構造
では、第2図で示した実施例での効果の他に、導体コイ
ル4が媒体対向面11から遠ざかるにつれてその幅が従
って、断面積を順次増大するように構成されているため
、導体コイル4の両端間の電気抵抗を大幅に減少するこ
とが可能となり、電流が流れる事による発熱量を低減す
ることが可能であり磁気ヘッドの駆動回路の負担を軽減
する事も出来る効果がある。第5図は、媒体対向面から
除々に導体コイルの幅をひろげその断面積を除々に増大
させていく構造を示しているが、本発明の特徴は、W体
対向面に最も近い導体コイルの位置が前記したギャップ
内に配置したことに特徴があるので、2番目以降の導体
コイルは、前記した最も近い導体コイルの幅より広番プ
れば第5図で示しを構造と同様の効果があり、2番目以
降は除々J導体コイル幅を増大させなくても良い。ま晶
述した構造は、フェライト基体に、ギャップ層□及び導
体コイルを形成した構造となっているが、フェライト閉
磁体側に、ギャップ層、あるいは導体コイルを形成した
構造としても、前記したと同様の効果がある。The difference from the embodiment shown in FIG. 2 is that a portion of the conductor coil 4 is disposed within the gap, and as the conductor coil 4 moves away from the medium facing surface, the cross-sectional area of the conductor coil increases sequentially. It is because of the fact that In this structure, in addition to the effect of the embodiment shown in FIG. 2, as the conductor coil 4 moves away from the medium facing surface 11, its width and cross-sectional area gradually increase. , it is possible to significantly reduce the electrical resistance between both ends of the conductor coil 4, it is possible to reduce the amount of heat generated due to the flow of current, and it is also possible to reduce the burden on the drive circuit of the magnetic head. be. FIG. 5 shows a structure in which the width of the conductor coil is gradually expanded from the surface facing the medium and its cross-sectional area is gradually increased. Since the position is characterized by being placed within the above-mentioned gap, if the width of the second and subsequent conductor coils is wider than the width of the nearest conductor coil, the same effect as the structure shown in Fig. 5 can be obtained. Yes, there is no need to gradually increase the J conductor coil width from the second onwards. The structure described above is a structure in which a gap layer □ and a conductor coil are formed on a ferrite substrate, but a structure in which a gap layer or a conductor coil is formed on the ferrite closed magnetic body side can also be used in the same manner as described above. effective.
本発明によれば、磁気ヘッドの媒体対向面のすぐ近くに
導体コイルが配置されているため、導体コイルに電流を
流す事により発生する磁界が、余分な所に漏えいするこ
となく、はとんど記録媒体を記録するための磁界として
有効に働く、また再生時も同様、I!体から検出された
磁束が、すぐ近くの導体コンルに電圧として変換される
、さらに、媒体対向面から数えて2番目以降の導体コイ
ルに対向するフェライト閉磁体には、アペックス角Qを
形成する溝5が設けられているため、2番目以降の導体
コイルから発生する記録磁束はフェライト基体1とフェ
ライト閉磁体6との間の2番目以降の導体コイル4の部
分でショートすることなくギャップ先端の方までまわり
、有効に働く、また再生時も同様である。この様に記録
及び再生効率の良い磁気ヘッドが得られる。According to the present invention, since the conductor coil is placed very close to the medium facing surface of the magnetic head, the magnetic field generated by passing a current through the conductor coil can be easily transmitted without leaking to unnecessary places. I! works effectively as a magnetic field for recording on any recording medium, and also during playback. The magnetic flux detected from the body is converted into voltage to a nearby conductor coil.Furthermore, the ferrite closed magnetic body facing the second and subsequent conductor coils counting from the medium facing surface has a groove forming an apex angle Q. 5, the recording magnetic flux generated from the second and subsequent conductor coils is directed toward the tip of the gap without shorting in the second and subsequent conductor coils 4 between the ferrite base 1 and the ferrite closed magnetic body 6. It works effectively, and the same holds true during playback. In this way, a magnetic head with good recording and reproducing efficiency can be obtained.
また、導体コイル4を記録媒体対向面に最も近い導体コ
イルの幅より2番目以降の導体コイルの幅をひろげ(導
体コイルは第1図に示す様に全てつながっている)断面
積を増大させた構造の1のは、記録媒体に最も近い導体
コイルに流れる電流によって生じる磁界が、媒体を記録
するための磁界に最も影響を与え、しかも断面積が媒体
対向面側から数えて2番目以降の導体コイルのどれより
も小さいため、電流を流した時最も電流密度が高くなり
、記録効率の良い磁気ヘッドとなると同時に、2番目以
降の導体コイルの抵抗値を下げる事が可能となり、電流
を流す事による発熱量の低減でき、また2番目以降の導
体コイルに流れる電流密度を小さく出来るためマイグレ
ーションを防止できる等信頼性の良い磁気ヘッドが得ら
れる。In addition, the width of the second and subsequent conductor coils is made wider than the width of the conductor coil closest to the surface facing the recording medium (the conductor coils are all connected as shown in Fig. 1) to increase the cross-sectional area of the conductor coil 4. The first structure is that the magnetic field generated by the current flowing through the conductor coil closest to the recording medium has the greatest effect on the magnetic field for recording the medium, and the cross-sectional area is the second conductor coil closest to the medium facing side. Because it is smaller than any of the coils, the current density is the highest when current is passed through it, making it a magnetic head with high recording efficiency.At the same time, it is possible to lower the resistance value of the second and subsequent conductor coils, making it possible to pass current. Since the amount of heat generated by the magnetic head can be reduced, and the current density flowing through the second and subsequent conductor coils can be reduced, migration can be prevented and a highly reliable magnetic head can be obtained.
第1図(a)は本発明の一実施例の斜視図で。
(b)はそのA部詳細図、第2図は本発明の実施例の断
面図、第3図は従来構造の薄膜磁気ヘッドの断面図、第
4図は従来のフェライトコア+薄膜コイル構造の断面図
、第5図は1本発明による他の実施例を示す断面図であ
る。
1・・・・フェライト基体、2・・・・フェライト閉磁
体、3・・・−ヘッドギャップ層、4,24.34・・
・・導体コイル、5.5’ 、9・・・・溝、21・・
・・基板、22・・・・F部磁性層、25・・・・上部
磁性層、11,26,37・・・・媒体対向面、23・
・・・絶縁層、6・・・・樹脂層、7・・・・ガラス層
。
第5閃FIG. 1(a) is a perspective view of one embodiment of the present invention. (b) is a detailed view of part A, FIG. 2 is a sectional view of an embodiment of the present invention, FIG. 3 is a sectional view of a thin film magnetic head with a conventional structure, and FIG. 4 is a sectional view of a conventional ferrite core + thin film coil structure. 5 is a sectional view showing another embodiment of the present invention. 1... Ferrite base, 2... Ferrite closed magnetic body, 3...-head gap layer, 4, 24.34...
...Conductor coil, 5.5', 9...Groove, 21...
...Substrate, 22...F section magnetic layer, 25...Top magnetic layer, 11, 26, 37...Medium facing surface, 23.
...Insulating layer, 6...Resin layer, 7...Glass layer. 5th flash
Claims (1)
た磁気ヘッドにおいて、磁気ヘッドを構成する変換ギャ
ップ内に、少なくとも導体コイルの一部が埋設されてい
ることを特徴とする磁気ヘッド。1. A magnetic head having a ferrite base and a core piece of ferrite closed magnetic material, characterized in that at least a part of a conductor coil is embedded within a conversion gap that constitutes the magnetic head.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2191386A JPS62180507A (en) | 1986-02-05 | 1986-02-05 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2191386A JPS62180507A (en) | 1986-02-05 | 1986-02-05 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62180507A true JPS62180507A (en) | 1987-08-07 |
Family
ID=12068328
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2191386A Pending JPS62180507A (en) | 1986-02-05 | 1986-02-05 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62180507A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0821347A2 (en) * | 1996-07-25 | 1998-01-28 | Sony Corporation | Magnetic head |
-
1986
- 1986-02-05 JP JP2191386A patent/JPS62180507A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0821347A2 (en) * | 1996-07-25 | 1998-01-28 | Sony Corporation | Magnetic head |
EP0821347A3 (en) * | 1996-07-25 | 1999-01-27 | Sony Corporation | Magnetic head |
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