JPH0192909A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPH0192909A JPH0192909A JP24780787A JP24780787A JPH0192909A JP H0192909 A JPH0192909 A JP H0192909A JP 24780787 A JP24780787 A JP 24780787A JP 24780787 A JP24780787 A JP 24780787A JP H0192909 A JPH0192909 A JP H0192909A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- core
- track width
- glass
- flux density
- 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
- 230000001105 regulatory effect Effects 0.000 claims abstract description 14
- 239000000758 substrate Substances 0.000 claims description 8
- 230000004907 flux Effects 0.000 abstract description 17
- 239000011521 glass Substances 0.000 abstract description 14
- 238000004519 manufacturing process Methods 0.000 abstract description 8
- 230000013011 mating Effects 0.000 abstract description 4
- 230000010485 coping Effects 0.000 abstract 1
- 239000006185 dispersion Substances 0.000 abstract 1
- 238000012856 packing Methods 0.000 abstract 1
- 239000000696 magnetic material Substances 0.000 description 8
- 230000000694 effects Effects 0.000 description 7
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 238000004544 sputter deposition Methods 0.000 description 4
- 238000004804 winding Methods 0.000 description 4
- 238000005520 cutting process Methods 0.000 description 3
- 238000005498 polishing Methods 0.000 description 3
- 229910052681 coesite Inorganic materials 0.000 description 2
- 229910052906 cristobalite Inorganic materials 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 239000010410 layer Substances 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 239000000377 silicon dioxide Substances 0.000 description 2
- 235000012239 silicon dioxide Nutrition 0.000 description 2
- 239000002356 single layer Substances 0.000 description 2
- 229910052682 stishovite Inorganic materials 0.000 description 2
- 238000003860 storage Methods 0.000 description 2
- 229910052905 tridymite Inorganic materials 0.000 description 2
- 238000007740 vapor deposition Methods 0.000 description 2
- 229910000808 amorphous metal alloy Inorganic materials 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 238000005304 joining Methods 0.000 description 1
- 238000003754 machining Methods 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 230000002250 progressing effect Effects 0.000 description 1
- 229910000702 sendust Inorganic materials 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Magnetic Heads (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、磁気ディスク装置等の磁気記憶装置に搭載さ
れる磁気ヘッドに係り、特に高抗磁力磁気記録媒体と組
合せて使用可能な磁気ヘッドに関する。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a magnetic head mounted on a magnetic storage device such as a magnetic disk device, and particularly to a magnetic head that can be used in combination with a high coercive force magnetic recording medium. Regarding.
磁気ディスク装置等の磁気記憶装置におげろ大容量化の
要求は高く、それに伴ない、磁気記録媒体の高抗磁力化
が進んでおり、磁気ヘッドとしても、高飽和磁束密度磁
性材料の研究が進められている。第9図は、従来の高抗
磁力磁気記録媒体に対応するために高飽和磁束密度磁性
膜を形成したヘッドコアの斜視図である。ヘッドコア1
は、巻線窓6を有するCコアと■コアを磁気ギャップ5
をはさんでガラスボンディングにより接合され一体とな
っている。Cコア及び■コアは、磁性材料又は非磁性材
料の基板2,2′上に蒸着又はスパッタリングによりセ
ンダスト又は非晶質合金磁性材料等の高飽和磁束密度磁
性膜5.3′を形成しである。この場合、高飽和磁束密
度磁性[3,3’によるコンタ効果を防止する為に磁気
ギャップ5と不平行になる様に傾斜させている。その為
、ヘッドコア10両側面部における磁性膜5,3′の・
・ガレを防止する為とCコア及び■コアとの接合力を増
す為にトラック幅7の両側にガラス4を充填しである。There is a high demand for higher capacity in magnetic storage devices such as magnetic disk drives, and as a result, magnetic recording media are becoming increasingly high in coercive force, and research into high saturation magnetic flux density magnetic materials is also underway for magnetic heads. It is progressing. FIG. 9 is a perspective view of a head core in which a high saturation magnetic flux density magnetic film is formed in order to correspond to a conventional high coercive force magnetic recording medium. head core 1
C core with winding window 6 and ■ core with magnetic gap 5
They are joined together by glass bonding across the two sides, making them a single piece. The C core and the (2) core are formed by forming a high saturation magnetic flux density magnetic film 5.3' of sendust or an amorphous alloy magnetic material by vapor deposition or sputtering on the substrates 2, 2' of magnetic or non-magnetic material. . In this case, it is tilted so as not to be parallel to the magnetic gap 5 in order to prevent the contour effect due to the high saturation magnetic flux density magnetism [3, 3'. Therefore, the magnetic films 5 and 3' on both side surfaces of the head core 10 are
- Glass 4 is filled on both sides of the track width 7 to prevent galling and to increase the bonding force between the C core and the ■ core.
第10図は、第9図の記録媒体対向面の拡大図である。FIG. 10 is an enlarged view of the surface facing the recording medium in FIG. 9.
ヘッドコア1は、Cコア及びIコアは磁気ギャップ5を
介して対向する面を研摩加工等によって鏡面に仕上げる
際にトラック幅7になる様に行うが、磁性膜3,5′の
両側に傾斜面を有している為、加工量のバラツキにより
、コア幅8゜8′とトラック幅7を一致させることは難
しく、又。In the head core 1, the surfaces of the C core and I core that face each other across the magnetic gap 5 are polished to a mirror surface so as to have a track width of 7, but there are sloped surfaces on both sides of the magnetic films 3 and 5'. Because of this, it is difficult to match the core width of 8° 8' and the track width of 7 due to variations in the amount of processing.
Cコアと■コアとの接合時に位置ズレな生じることもあ
り、製造歩留が著しく悪いものであった。Misalignment may occur when the C core and the (2) core are joined, resulting in a significantly poor manufacturing yield.
なお、この種のへラドコアとして関連するものには例え
ば特開昭59−207415号が挙げられる。Incidentally, related to this type of heradocore, for example, Japanese Patent Application Laid-Open No. 59-207415 can be mentioned.
上記従来技術は、磁性又は非磁性基板上に高飽和磁束密
度磁性膜を形成してヘッドコアを製造する際の生産性の
点について配慮がされておらず、トラック幅精度が悪く
、製造歩留を低下させるという問題があった。The above-mentioned conventional technology does not give consideration to productivity when manufacturing a head core by forming a high saturation magnetic flux density magnetic film on a magnetic or non-magnetic substrate, resulting in poor track width accuracy and lower manufacturing yield. There was a problem of lowering the
本発明の目的は、かかる欠点をな(し、生産性の高いト
ラック幅精度のよい高抗磁力磁気記録媒体に対応出来る
磁気ヘッドを提供することにある。SUMMARY OF THE INVENTION An object of the present invention is to provide a magnetic head that overcomes these drawbacks and can be used with high coercive force magnetic recording media with high productivity and good track width accuracy.
上記目的は、磁性又は非磁性基板上に高飽和磁束密度磁
性膜を形成した後ガラスを充填する前に前記高飽和磁束
密度磁性膜にトラック幅に相当するトラック幅規制溝を
加工することKより達成される。The above purpose is to process a track width regulating groove corresponding to the track width in the high saturation magnetic flux density magnetic film after forming the high saturation magnetic flux density magnetic film on a magnetic or non-magnetic substrate and before filling the high saturation magnetic flux density magnetic film with glass. achieved.
磁性又は非磁性基板上に形成した高飽和磁束密度磁性膜
に磁気ギャップ面に対して直角のトラック幅規制溝を加
工し、ガラスを充填した後、磁気−ギャップ合せ面を研
摩加工で仕上げる際に、前記トラック幅規制溝によって
、その加工量のバラツキによるトラック幅の変動は防止
出来る。After cutting a track width regulating groove perpendicular to the magnetic gap surface into a high saturation magnetic flux density magnetic film formed on a magnetic or non-magnetic substrate and filling it with glass, when finishing the magnetic-gap mating surface by polishing. The track width regulating groove can prevent variations in the track width due to variations in the amount of processing.
〔実施例〕 □
以下、本発明の一実施例を第1図〜第8図により説明す
る。[Example] □ An example of the present invention will be described below with reference to FIGS. 1 to 8.
第1図は、本発明の一実施例のへラドコアの斜視図、第
2図は、第1図の記録媒体対向面の゛拡大図である。ヘ
ッドコア1は、巻線窓6を有するCコアと1コアを磁気
ギャップ5をはさんでガラス4により接合されて一体と
なっている。磁気ギャップ5は、S i O2又はガラ
、ス等の非磁性材料により構成される。Cコア及びIコ
アは、磁性又は非磁性材料の基板2,2′上K、各々高
飽和磁束密度磁性膜3,3′を蒸着又はスパッタリング
により形成した後、Cコア及びIコアのコア幅8,8′
が規定。FIG. 1 is a perspective view of a helad core according to an embodiment of the present invention, and FIG. 2 is an enlarged view of the surface facing the recording medium in FIG. 1. The head core 1 is made up of a C core having a winding window 6 and one core joined by a glass 4 with a magnetic gap 5 in between. The magnetic gap 5 is made of a non-magnetic material such as SiO2 or glass. The C core and I core are formed by depositing or sputtering high saturation magnetic flux density magnetic films 3 and 3' on the substrates 2 and 2' of magnetic or non-magnetic material, respectively, and then forming the core width 8 of the C core and I core. ,8'
is stipulated.
のトラック幅7になるようにトラック幅規制溝9゜9′
を加工しである。その溝深さ10 、10’はCコア及
びエコアを磁気ギャップ5を介して接合した際に記録再
生時に影響を与えない程度、例えば100μm以上であ
ればよい。Track width regulating groove 9°9' so that the track width is 7.
It is processed. The groove depths 10 and 10' may be such that when the C core and the echo core are joined through the magnetic gap 5, there is no effect on recording and reproduction, for example, 100 μm or more.
次に本発明のへラドコアの製造方法の一実施例を第4図
〜第8図により説明する。第4図はCコアの磁性又は非
磁性基板2の加工斜視図である。Next, an embodiment of the method for manufacturing a herad core according to the present invention will be described with reference to FIGS. 4 to 8. FIG. 4 is a processed perspective view of the magnetic or nonmagnetic substrate 2 of the C core.
高飽和磁束密度磁性膜の形成面側に、巻線窓6の為の溝
加工及び前記高飽和磁束密度磁性膜によるコンタ効果を
防止する一策として、磁気ギャップ面と不平行くなる様
に傾斜をもつ突起部形成溝11゜12の加工を施しであ
る。又、■コアの基板2′の場合には、巻11!6の溝
加工はな(、突、起部形成溝if 、 12のみの加工
を行う。第5図は、Cコアの基板2上に高飽和磁束密着
磁性膜5を形成した図であり、蒸着又はスパッタリング
等により形成される。この場合、磁性膜5は、磁性材料
のみの単層膜で形成してもよく、又、磁性材料の高周波
数特性を向上させる為に中間層に5zOz等の非磁性材
を介して積層する多層膜構成であってもよい。As a measure to prevent the contour effect caused by the groove processing for the winding window 6 and the contour effect caused by the high saturation magnetic flux density magnetic film on the side where the high saturation magnetic flux density magnetic film is formed, an inclination is made so as not to be parallel to the magnetic gap surface. The protrusion forming grooves 11 and 12 are processed. In addition, in the case of the board 2' of the core, only the grooves of winding 11!6 (, protrusions, protrusion forming grooves, if, 12) are processed. This is a diagram in which a high saturation magnetic flux adhesion magnetic film 5 is formed by vapor deposition, sputtering, etc. In this case, the magnetic film 5 may be formed as a single layer film of only magnetic material, or may be formed of a single layer of magnetic material only. In order to improve the high frequency characteristics of the multi-layer structure, the intermediate layer may be laminated with a non-magnetic material such as 5 ozOz interposed therebetween.
第6図は、磁性膜3にトラック幅規制溝9の加工を行っ
た図である。トラック幅規制溝9は、コア幅8がトラッ
ク幅と同一寸法になる様に及びコアピッチ13が規定の
寸法になる様に加工される。FIG. 6 is a diagram showing track width regulating grooves 9 formed in the magnetic film 3. As shown in FIG. The track width regulating groove 9 is processed so that the core width 8 has the same dimension as the track width and the core pitch 13 has a specified dimension.
又、トラック幅規制溝加工深さ14は、磁気ギャップ面
の研摩加工後の溝深さ寸法1oが、記録再生特性に影響
をおよぼさない程度に加工してあればよい。又、トラッ
ク幅規制溝加工を行なうのにマルチカッターを使用すれ
ば、精度よくかっ、製造効率も向上する。第7図は、ト
ラック幅溝加工後にガラス4を充填した図である。この
ガラス4は、磁性膜のハガレ防止及びCコアとIコアと
を磁気ギャップを介して接合する為の接合材料として作
用する。磁気ギャップ合せ面の面仕上げ及びトラック幅
規制溝9が作用する所まで(第7図の人の一点ta線面
)研摩加工等により表面精度のよい状頭に仕上げられる
。次に、Cコア及びIコアの少な(共一方の合せ面に磁
気ギャップ5を構成する為のSiO2又はガラスをスパ
ッタリング等により形成し、第8図に示すようにCコア
と■コアの合せ面をつき合せ、お互いのコア幅8,8′
が規定のトラック幅7になる様に位置決めし、ガラス4
により接合する。この場合、磁気ギャップ材としての5
iChは、ガラスに拡散される為、接合に際しては、特
に問題はない。次K、第8図のB1及びB2の一点[1
で示すようにスライサー等で切断することによりヘッド
コアが出来る。The track width regulating groove machining depth 14 may be such that the groove depth dimension 1o after polishing of the magnetic gap surface does not affect the recording and reproducing characteristics. Furthermore, if a multi-cutter is used to process the track width regulating grooves, the cutting can be done with good precision and manufacturing efficiency can be improved. FIG. 7 is a diagram showing the glass 4 filled after track width groove processing. This glass 4 acts as a bonding material to prevent peeling of the magnetic film and to bond the C core and I core via a magnetic gap. The surface of the magnetic gap mating surface is finished to a surface with good surface precision by polishing and the like up to the point where the track width regulating groove 9 acts (ta line surface at one point in FIG. 7). Next, SiO2 or glass for forming the magnetic gap 5 is formed on the mating surfaces of the C core and the I core by sputtering, etc., and as shown in FIG. and each other's core width 8,8'
Position the glass so that it has the specified track width 7, and
Join by. In this case, 5 as the magnetic gap material
Since iCh is diffused into the glass, there is no particular problem during bonding. Next K, one point B1 and B2 in Figure 8 [1
The head core can be made by cutting with a slicer etc. as shown in .
次に、本発明の他の実施例における記録媒体対向面の拡
大図を第6図に示す。ヘッドコア1を構成するCコア及
び■コアの内、■コア側のコア幅8′が規定のトラック
幅7になる様にトラック幅規制溝9′を加工してあり溝
深さ10′は記録再生特性に影響を与えない量になって
いる。Cコア側のコア幅8は■コアのコア幅8′に比し
、太き(しである。この場合、トラック幅7は、Cコア
とエコアのコア幅8,8′が重なり合った幅になる為、
Cコアとエコアとを磁気ギャップ5を介して接合する際
に、たとえお互い水位置ズレな生じたとしてもCコアの
コア幅8の巾に1コアのコア幅8′が位置。Next, FIG. 6 shows an enlarged view of the surface facing the recording medium in another embodiment of the present invention. Of the C core and ■core that make up the head core 1, a track width regulating groove 9' is machined so that the core width 8' on the ■core side becomes the specified track width 7, and the groove depth 10' is used for recording and reproduction. The amount is set so that it does not affect the characteristics. The core width 8 on the C core side is thicker than the core width 8' of the core. In this case, the track width 7 is the width where the core widths 8 and 8' of the C core and Ecore overlap. To become
When joining the C core and the eco core through the magnetic gap 5, even if the water positions are shifted from each other, the core width 8' of one core is located within the width of the core width 8 of the C core.
していればトラック幅7の変動は生じない。If so, the track width 7 will not fluctuate.
本発明によれば、磁気ギャップ面加工時に−よって生ず
るコア幅及びトラック幅の変動をなくし、かつ、Cコア
及びエコアのつき合せ時に発生するトラック幅の変動を
も抑制出来る為、製造歩留も向上し、生産性の高い高記
録密度化に適した磁気ヘッドを提供出来る効果がある。According to the present invention, it is possible to eliminate fluctuations in the core width and track width that occur during magnetic gap surface processing, and also to suppress fluctuations in the track width that occur when the C core and the echo core are brought together, thereby improving manufacturing yield. This has the effect of providing a magnetic head suitable for high recording density with high productivity and high productivity.
第1図は本発明の一実施例のへラドコアの斜視図、第2
図は第1図の記録媒体対向面の拡大図、第3図は本発明
の他の実施例における記録媒体対向面の拡大図、第4図
〜第8図は第1図に示すヘッドコアの製造方法の一実施
例の説明図、第9図は従来のへラドコアの斜視図、第1
u図は第9図の記録媒体対向面の拡大図である。
1・・・ヘッドコア、2・・・Cコア用基板、2′・・
・■コア用基板、 3 、3’・・・高胞和磁束密度磁
性膜、4・・・ガラス、5・・・磁気ギャップ、6・・
・巻Is2.7・・・トラック幅、 8 、8’・・・
コア幅、 9 、9’・・・トラック幅規制溝、 10
、 in’・・・溝深さ、 11 、12・・・突起
部形成溝、13・・・コアピッチ。
代理人弁理士 小 川 勝 男
夷1国
第2z
第〕聞
晃4凹
第、5目 、5
/2/l
め乙ぬ
あ71El
り
晃8I!lFIG. 1 is a perspective view of a herad core according to an embodiment of the present invention, and FIG.
The figure is an enlarged view of the recording medium facing surface in FIG. 1, FIG. 3 is an enlarged view of the recording medium facing surface in another embodiment of the present invention, and FIGS. 4 to 8 are manufacturing of the head core shown in FIG. 1. An explanatory diagram of one embodiment of the method, FIG. 9 is a perspective view of a conventional herad core, and FIG.
Figure U is an enlarged view of the surface facing the recording medium in Figure 9. 1...Head core, 2...C core board, 2'...
・■ Core substrate, 3, 3'... High cell sum magnetic flux density magnetic film, 4... Glass, 5... Magnetic gap, 6...
・Volume Is2.7... Track width, 8, 8'...
Core width, 9, 9'...Track width regulating groove, 10
, in'...Groove depth, 11, 12...Protrusion forming groove, 13...Core pitch. Representative Patent Attorney Masaru Ogawa Ogawa 1st Country 2nd Edition] Monko 4th, 5th, 5/2/l Meotnua 71El Riko 8I! l
Claims (1)
構成する磁気ヘッドにおいて、磁気ギャップを介して対
向する。少なく共一方の高磁性膜に磁気ギャップとほぼ
直角にトラック幅規制溝を形成してなることを特徴とす
る磁気ヘッド。1. In a magnetic head in which a highly magnetic film is formed on a magnetic or non-magnetic substrate to form a magnetic path, the heads face each other across a magnetic gap. A magnetic head characterized in that a track width regulating groove is formed in at least one highly magnetic film at substantially right angles to a magnetic gap.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24780787A JPH0192909A (en) | 1987-10-02 | 1987-10-02 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24780787A JPH0192909A (en) | 1987-10-02 | 1987-10-02 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0192909A true JPH0192909A (en) | 1989-04-12 |
Family
ID=17168953
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP24780787A Pending JPH0192909A (en) | 1987-10-02 | 1987-10-02 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0192909A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5253953A (en) * | 1990-08-23 | 1993-10-19 | Whidden Jr Malcolm B | Boom for containing oil spills |
-
1987
- 1987-10-02 JP JP24780787A patent/JPH0192909A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5253953A (en) * | 1990-08-23 | 1993-10-19 | Whidden Jr Malcolm B | Boom for containing oil spills |
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