JPH0622049B2 - Combined type magnetic head - Google Patents
Combined type magnetic headInfo
- Publication number
- JPH0622049B2 JPH0622049B2 JP58163254A JP16325483A JPH0622049B2 JP H0622049 B2 JPH0622049 B2 JP H0622049B2 JP 58163254 A JP58163254 A JP 58163254A JP 16325483 A JP16325483 A JP 16325483A JP H0622049 B2 JPH0622049 B2 JP H0622049B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- composite
- head
- core
- magnetic core
- 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.)
- Expired - Lifetime
Links
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
- G11B5/187—Structure or manufacture of the surface of the head in physical contact with, or immediately adjacent to the recording medium; Pole pieces; Gap features
-
- 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
-
- 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
- G11B5/1278—Structure or manufacture of heads, e.g. inductive specially adapted for magnetisations perpendicular to the surface of the record carrier
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Magnetic Heads (AREA)
Description
【発明の詳細な説明】 〔発明の利用分野〕 本発明は垂直磁気記録用の磁気ヘッドに係り、特に高密
度での記録再生特性に優れた複合型磁気ヘツドに関す
る。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic head for perpendicular magnetic recording, and more particularly to a composite magnetic head having excellent recording and reproducing characteristics at high density.
面内記録媒体の高保磁力化に伴ない、該媒体に有効に記
録を行なうため、高飽和磁束密度磁性体を被着せしめた
フエライトブロツクから形成される複合型磁気ヘツドが
提案されていた。ところがこれらの複合型磁気ヘツドに
おいては、該被着部境界面が擬似ギヤツプとして機能す
るため、いわゆるコンタ効果を生じ易く、再生出力の周
波数特性が波打ち現象を起こしており、これを回避する
ために種々の工夫がなされていた。例えば、特開昭56
−129214号公報には、磁気空隙構成部分を他のコ
ア部分よりも高飽和磁束密度の材料とし、かつギヤツプ
部と斜交せしめるという提案がなされている。Along with the increase in coercive force of the in-plane recording medium, a composite magnetic head formed from a ferrite block coated with a high saturation magnetic flux density magnetic material has been proposed in order to effectively perform recording on the medium. However, in these composite magnetic heads, since the boundary surface of the adhered portion functions as a pseudo gear, a so-called contour effect is likely to occur, and the frequency characteristic of the reproduction output causes a wavy phenomenon. Various ideas were made. For example, JP-A-56
In Japanese Patent Laid-Open No. 129214, it is proposed that the magnetic air gap constituent portion is made of a material having a higher saturation magnetic flux density than the other core portions and is obliquely crossed with the gear portion.
ところが、上記複合型磁気ヘツドでは、第1、第2の磁
気コアに被着せしめた高飽和磁束密度磁性体が同一材料
でしかも膜厚もほぼ等しいため、記録磁界分布がギヤツ
プ部に対して対称で、充分急峻な垂直方向の記録磁界成
分が得られず、本ヘツドをそのまま垂直磁気記録装置に
適用しても特に高飽和磁化の媒体に対して理想的な垂直
磁気記録ができないという欠点があつた。However, in the above-mentioned composite magnetic head, since the high saturation magnetic flux density magnetic materials applied to the first and second magnetic cores are made of the same material and the film thicknesses thereof are almost the same, the recording magnetic field distribution is symmetrical with respect to the gear part. However, a sufficiently steep perpendicular recording magnetic field component cannot be obtained, and even if this head is directly applied to a perpendicular magnetic recording apparatus, there is a drawback that ideal perpendicular magnetic recording cannot be performed especially on a medium with high saturation magnetization. It was
本発明の目的は、記録磁界の媒体に垂直な方向の成分が
急峻で、高密度記録の可能な垂直磁気記録用の複合型磁
気ヘツドを提供することにある。It is an object of the present invention to provide a composite magnetic head for perpendicular magnetic recording in which the component of the recording magnetic field in the direction perpendicular to the medium is steep and high density recording is possible.
媒体に垂直な方向の記録磁界成分を急峻にするために
は、磁気コア構造を磁気的に非対称にすることが有効で
あると考え、フエライトブロツク上に被着せしめる高飽
和磁束密度磁性膜の材質、特性、構造を種々変えて実際
に複合膜ヘツドを試作し特性を評価した結果、磁気記録
媒体対向面における断面形状が突出している突起物を有
する高透磁率フエライトブロツクの該突起物の少なくと
も両側面上に該フエライトより飽和磁束密度の高い非晶
質磁性膜を被着せしめた第1の磁気コアと、少なくとも
作動ギヤツプ近傍に該フエライトより飽和磁束密度の高
い多結晶質磁性体が高透磁率フエライトブロツク上に被
着された第2の磁気コアとで該突起部の先端部において
作動ギヤツプを介して相対峙して形成した複合型磁気ヘ
ツドは、特に高密度での記録再生特性が優れていること
が明らかになつた。また、該第2のコアも磁気記録媒体
対向面における断面形状が突出している突起物を有して
いる場合にはコンター効果分がさらに少なくより好まし
く、さらに、前記多結晶質磁性材料の方が非晶質磁性材
料よりも飽和磁束密度が高い場合には、特に良好な記録
密度特性が得られた。In order to make the recording magnetic field component in the direction perpendicular to the medium steep, it is considered effective to make the magnetic core structure magnetically asymmetric, and the material of the high saturation magnetic flux density magnetic film to be deposited on the ferrite block is considered. , A composite film head was actually manufactured by changing various characteristics and structures and the characteristics were evaluated. As a result, at least both sides of the projection of the high permeability ferrite block having a projection with a protruding cross-sectional shape on the magnetic recording medium facing surface A first magnetic core having an amorphous magnetic film having a saturation magnetic flux density higher than that of the ferrite coated on its surface, and a polycrystalline magnetic material having a saturation magnetic flux density higher than that of the ferrite at least in the vicinity of the operating gear. The composite magnetic head formed by the second magnetic core deposited on the ferrite block and the second magnetic core, which are relatively opposed to each other at the tip of the protrusion via the operating gear, has a particularly high density. It is found that the alien have excellent recording and reproduction characteristics of. Further, when the second core also has a protrusion having a protruding cross-sectional shape on the surface facing the magnetic recording medium, it is more preferable that the amount of the contour effect is smaller, and the polycrystalline magnetic material is more preferable. Particularly good recording density characteristics were obtained when the saturation magnetic flux density was higher than that of the amorphous magnetic material.
以下、本発明の一実施例を第1図により説明する。同図
(a),(b)はそれぞれ斜視図と平面図とを示し、11はM
n−Znフエライト、Ni−Znフエライト等の高透磁
率ブロツク、12は周知のCo−Zr−Mo,Co−Z
r−Nb,Co−Zr−W,Co−Ni−Zrなどの非
晶質磁性合金、もしくはそれらとSiO2,Al2O3などの絶
縁層との積層物、13はSiO2,Al2O3などで形成される
作動ギヤツプ部、14はガラス接着物などの非磁性充填
材、15は周知のFe−Si−Ru,Fe−Si−A
l,Fe−Ti,Ni−Feなので多結晶質磁性合金、
もしくはそれらとSiO2,Al2O3などの絶縁層との積層
物、16はMn−Znフエライト、Ni−Znフエライ
トなどの高透磁率ブロツクである。An embodiment of the present invention will be described below with reference to FIG. Same figure
(a) and (b) show a perspective view and a plan view, respectively, and 11 is M
High permeability blocks such as n-Zn ferrite and Ni-Zn ferrite, and 12 are well-known Co-Zr-Mo and Co-Z.
Amorphous magnetic alloys such as r-Nb, Co-Zr-W, and Co-Ni-Zr, or a laminate of them with an insulating layer such as SiO 2 or Al 2 O 3 , 13 is SiO 2 , Al 2 O. An operating gear portion formed of 3, etc., 14 is a non-magnetic filler such as a glass adhesive, and 15 is a well-known Fe-Si-Ru, Fe-Si-A.
l, Fe-Ti, Ni-Fe, so polycrystalline magnetic alloy,
Or laminates of insulating layers such as those with SiO 2, Al 2 O 3, 16 is a high permeability blocks such as Mn-Zn ferrite, Ni-Zn ferrite.
第2、第3、第4図にはそれぞれ他の実施例を示す。2
1〜26,31〜36,41〜46はそれぞれ11〜1
6に対応するものであり、第2図で25は26の下部ま
で達していてもいなくても良い。Other embodiments are shown in FIGS. 2, 3, and 4, respectively. Two
1-26, 31-36, 41-46 are 11-1 respectively
6 corresponds to 25, and 25 in FIG. 2 may or may not reach the lower part of 26.
本発明によれば磁気コアの磁気特性が非対称であるた
め、垂直方向の記録磁界強度が強くしかも急峻となるた
め、例えば飽和磁化500emu/cc、膜厚0.25μm、保磁力
500OeのCo−Cr薄膜を0.9μmのCo−Zr−
Mo磁性膜で裏打ちした2層膜垂直媒体を用いて、相対
速度1.25m/sで特性を評価した場合に、第5図に示す
ように特に優れた記録特性が得られる。ここで、51
は、第1図に示した構造のヘッドの特性で、11,16
を飽和磁束密度0.52TのMn−Znフエライト、1
2を飽和磁束密度0.9T、膜厚5μmのCo−Zr−
Nbを0.1μmのSiO2層を介してそれぞれ4層積層し
た非晶質磁性層、ギヤツプ13はSiO2で形成し、ギヤツ
プ長は0.15μm、14は充填ガラス、15は飽和磁束密
度0.9T、膜厚1μmのNi−Fe−Moを0.04μm
のSiO2層を介してそれぞれ15層積層した多結晶磁性層
であり、θ1は約60゜、θ2は約90゜としたもので
ある。また、52は、第2図に示した構造のヘツドの特
性で、該ヘツド21,26をNi−Znフエライト、2
2を飽和磁束密度1.1T、膜厚6μmのCo−Zr−
Moを0.08μmのAl2O3層を介してそれぞれ6層積
層した非晶質磁性層、ギヤツプ23はSiO2を0.2μm
付着せしめて形成し、24は充填ガラス、25は飽和磁
束密度1.0T、膜厚1.5μmのNi−Feを0.06μ
mのSiO2を介してそれぞれ8層積層した多結晶磁性層で
ありθ3は約50゜としたものである。53は第4図に
示した構造のヘツドの特性で、41,46はMn−Zn
フエライトコア、42は飽和磁束密度1.14T、膜厚
20μmのCo−Zr−W単層膜、43はAl2O3より成
るギヤツプ長0.25μmのギヤツプ、44は充填ガラス、
45は飽和磁束密度1.5T、膜厚0.2μmのFe−
Tiを0.05μmのAl2O3を介してそれぞれ50層形成し
たものである。同図には、第4図に示した構造で、4
2,45ともに20μmのCo−Zr−Wで形成した場
合の特性を54に示すが、本発明による構造のヘツドの
方が特に高密度での特性に優れていることがわかる。According to the present invention, since the magnetic characteristics of the magnetic core are asymmetric, the recording magnetic field strength in the perpendicular direction is strong and steep. For example, the saturation magnetization is 500 emu / cc, the film thickness is 0.25 μm, and the coercive force is
CoO-Cr thin film of 500 Oe with Co-Zr-of 0.9 μm
When the characteristics are evaluated at a relative speed of 1.25 m / s using a double-layered perpendicular medium lined with a Mo magnetic film, particularly excellent recording characteristics are obtained as shown in FIG. Where 51
Is the characteristic of the head having the structure shown in FIG.
A Mn-Zn ferrite with a saturation magnetic flux density of 0.52T, 1
2 is Co-Zr-having a saturation magnetic flux density of 0.9 T and a film thickness of 5 μm.
An amorphous magnetic layer in which four layers of Nb were laminated with each 0.1 μm SiO 2 layer, the gap 13 was made of SiO 2 , the gap length was 0.15 μm, 14 was filled glass, and 15 was a saturated magnetic flux density of 0. Ni-Fe-Mo with 9T and film thickness of 1μm is 0.04μm
Is a polycrystalline magnetic layer in which 15 layers are laminated with each SiO 2 layer interposed therebetween, θ 1 is about 60 °, and θ 2 is about 90 °. Further, 52 is a characteristic of the head having the structure shown in FIG. 2, in which the heads 21 and 26 are replaced with Ni-Zn ferrite.
2 is Co-Zr-having a saturation magnetic flux density of 1.1 T and a film thickness of 6 μm.
An amorphous magnetic layer in which 6 layers of Mo were laminated with Al 2 O 3 layers of 0.08 μm each, and the gap 23 was 0.2 μm of SiO 2 .
Formed by adhering, 24 is filled glass, 25 is saturation magnetic flux density 1.0 T, film thickness 1.5 μm Ni-Fe 0.06 μm
It is a polycrystalline magnetic layer in which eight layers are respectively laminated via m of SiO 2 and θ 3 is set to about 50 °. 53 is the characteristic of the head having the structure shown in FIG. 4, and 41 and 46 are Mn-Zn.
A ferrite core, 42 is a Co-Zr-W single layer film having a saturation magnetic flux density of 1.14 T and a film thickness of 20 μm, 43 is a gear cup made of Al 2 O 3 and has a gear length of 0.25 μm, and 44 is filled glass.
45 is Fe- with a saturation magnetic flux density of 1.5 T and a film thickness of 0.2 μm.
Fifty layers of Ti are each formed through 0.05 μm of Al 2 O 3 . In the figure, the structure shown in FIG.
The characteristics of both Nos. 2 and 45 formed with Co-Zr-W of 20 μm are shown in 54. It can be seen that the head of the structure according to the present invention is particularly excellent in high density characteristics.
第6図には第3図に示した構造の複合ヘツドで飽和磁化
350emu/cc、膜厚0.2μm、保磁力700OeのCo−
Cr薄膜を1.5μmのCo−Zr−W磁性膜で裏打ち
した2層膜媒体に、相対速度2.5m/sで記録再生した場
合の特性を示す。61は、第3図で31,36をMn−
Znフエライト、32を飽和磁化13.5T、膜厚7μ
mのCo−Zr−Bを、0.1μmのSiO2層を介してそ
れぞれ5層積層した膜、33を0.2μmのSiO2、34
を充填ガラス、35を飽和磁化1.9T、膜厚0.1μ
mのFe−Si−Ruを、膜厚0.005μmのNi−Fe
とそれぞれ50層積層した多結晶磁性膜とした複合ヘツ
ドの特性であり、62は35部を飽和磁化1T、膜厚
0.2μmのNi−Feを、膜厚0.007μmのSiO2でそ
れぞれ31層積層した多結晶磁性膜と変えた複合ヘツド
の特性で、いずれも優れた特性が得られてはいるが、特
に、多結晶質磁性材35部の飽和磁束密度が、非晶質磁
性材料部32部の飽和磁束密度よりも高い方がより特性
が良いことが分かる。FIG. 6 shows the saturation magnetization of the composite head with the structure shown in FIG.
Coe with 350emu / cc, film thickness 0.2μm and coercive force 700Oe
The characteristics when recording and reproducing were performed on a two-layer film medium in which a Cr thin film was lined with a Co-Zr-W magnetic film of 1.5 μm at a relative speed of 2.5 m / s. 61 is Mn-31 and 36 in FIG.
Zn ferrite, 32, saturation magnetization 13.5 T, film thickness 7 μ
m of Co-Zr-B, each of which was laminated with 5 layers of 0.1 μm of SiO 2 layer, 33 was 0.2 μm of SiO 2 , 34.
Is a filled glass, 35 is a saturation magnetization of 1.9 T, and the film thickness is 0.1 μ.
Fe-Si-Ru with a thickness of 0.005 μm Ni-Fe
And 62 are characteristics of the composite head made of a polycrystalline magnetic film laminated by 50 layers respectively, and 62 is a saturation magnetization 1T in 35 parts, Ni-Fe with a film thickness of 0.2 μm, and SiO 2 with a film thickness of 0.007 μm is 31 layers each. Although excellent characteristics are obtained by the characteristics of the laminated polycrystalline magnetic film and the composite head in which the polycrystalline magnetic film is changed, the saturation magnetic flux density of the polycrystalline magnetic material 35 parts is particularly high. It is understood that the higher the saturation magnetic flux density of the part, the better the characteristics.
以上いわゆる狭ギヤツプのリング型ヘツドに関する実施
例について説明したが、この効果は、特にギヤツプ長と
高飽和磁束密度材の膜厚とを大幅に変えた第7図に示す
構造でも第5図52に示したものと同程度の特性が得ら
れた。なおここで、71,76はMn−Znフエライ
ト、72は膜厚20μmのCo−Zr−W非晶質磁性
膜、73,73′は各々2μm厚のSiO2ギヤツプ長、7
4は充填ガラス、75は飽和磁化1.8T、膜厚0.05μ
mのFe−Si−Ruと膜厚0.005μmのCoとをそれ
ぞれ4層積層した多結晶磁性膜である。Although the embodiments relating to the so-called narrow head type ring head have been described above, this effect can be seen in FIG. 5 even in the structure shown in FIG. Properties similar to those shown were obtained. Here, 71 and 76 are Mn-Zn ferrite, 72 is a Co-Zr-W amorphous magnetic film having a film thickness of 20 μm, 73 and 73 ′ are SiO 2 gap lengths having a film thickness of 2 μm, and 7
4 is filled glass, 75 is saturation magnetization 1.8 T, film thickness 0.05 μ
It is a polycrystalline magnetic film in which four layers of Fe-Si-Ru of m and Co of 0.005 μm each are laminated in four layers.
以上のように、本発明による複合型磁気ヘツドは、記録
再生特性がすぐれているのみでなく、コンター効果も十
分に小さく、垂直磁気記録用としてすぐれており、特に
高密度での記録再生特性がすぐれている。As described above, the composite magnetic head according to the present invention not only has excellent recording / reproducing characteristics, but also has a sufficiently small contour effect and is excellent for perpendicular magnetic recording, and particularly has high recording / reproducing characteristics. It is excellent.
第1図(a),(b)、第2図(a),(b)、第3図および第4図
は本発明の各実施例における複合型ヘツドの斜視図もし
くは記録媒体対抗面の作動ギヤツプ近傍の平面図、第5
図、第6図は該ヘツドの特性を示すグラフ、第7図は他
の実施例より成る複合型ヘツドの斜視図を示す。 11,16,21,26,31,36,71,76……
フエライトブロツク、12,22,32,42,72…
…非晶質磁性材からなる薄膜、15,25,35,4
5,75……多結晶質磁性材から成る薄膜、14,2
4,34,44,74……非磁性充填材、13,23,
33,43,73,73′……ギツプ部、51,52,
53,61,62……本発明より成る複合ヘツドの特
性、54……従来ヘツドの特性。FIGS. 1 (a), (b), 2 (a), (b), 3 and 4 are perspective views of composite heads in each embodiment of the present invention or actuation of the recording medium facing surface. Plan view of the vicinity of the gear, No. 5
6 and 6 are graphs showing the characteristics of the head, and FIG. 7 is a perspective view of a composite head according to another embodiment. 11,16,21,26,31,36,71,76 ...
Ferrite block, 12, 22, 32, 42, 72 ...
... Thin film made of amorphous magnetic material, 15, 25, 35, 4
5,75 ... Thin film made of polycrystalline magnetic material, 14, 2
4,34,44,74 ... Non-magnetic filler, 13,23,
33, 43, 73, 73 '... Gap portion, 51, 52,
53, 61, 62 ... Characteristics of the composite head according to the present invention, 54 ... Characteristics of conventional head.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 熊坂 登行 東京都国分寺市東恋ヶ窪1丁目280番地 株式会社日立製作所中央研究所内 (72)発明者 品川 公成 東京都国分寺市東恋ヶ窪1丁目280番地 株式会社日立製作所中央研究所内 (56)参考文献 特開 昭56−169214(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Climbing Kumasaka, the inventor 1-280 Higashikoigakubo, Kokubunji, Tokyo Inside the Central Research Laboratory, Hitachi, Ltd. (72) Kosei Shinagawa 1-280 Higashikoigakubo, Kokubunji, Tokyo Central Research Laboratory, Hitachi, Ltd. (56) Reference JP-A-56-169214 (JP, A)
Claims (5)
トより飽和磁束密度の高い磁性体が被着された第1の磁
気コアと第2の磁気コアとが上記磁性体の面が互いに向
き合った状態で作動ギャップを介して相対峙している複
合型磁気ヘッドにおいて、上記第1の磁気コアを構成す
る上記高透磁率フェライトブロックは磁気記録媒体との
対向面部において上記作動ギャップに向かって尖った形
状の突起物を有しており、上記第2の磁気コアを構成す
る磁性体は、上記第1の磁気コアを構成する磁性体より
も大きな飽和磁束密度を有する材料からなることを特徴
とする複合型磁気ヘッド。1. A first magnetic core and a second magnetic core, wherein a magnetic material having a saturation magnetic flux density higher than that of the ferrite is coated on a high-permeability ferrite block, with the surfaces of the magnetic material facing each other. In the composite type magnetic head which is relatively opposed via the working gap, the high magnetic permeability ferrite block constituting the first magnetic core has a shape pointed toward the working gap at the surface facing the magnetic recording medium. A composite type having a protrusion and the magnetic body forming the second magnetic core is made of a material having a saturation magnetic flux density higher than that of the magnetic body forming the first magnetic core. Magnetic head.
記第1の磁気コアを構成する高透磁率フェライトブロッ
クの形状と、上記第2の磁気コアを構成する高透磁率フ
ェライトブロックの形状とが非対称であることを特徴と
する特許請求の範囲第1項に記載の複合型磁気ヘッド。2. The shape of the high-permeability ferrite block forming the first magnetic core and the shape of the high-permeability ferrite block forming the second magnetic core at the surface facing the magnetic recording medium. The composite magnetic head according to claim 1, wherein the composite magnetic head is asymmetric.
上記第2の磁気コアを構成する高透磁率フェライトブロ
ックは、滑らかな凹形状をなしている特許請求の範囲第
1項又は第2項に記載の複合型磁気ヘッド。3. A surface facing the magnetic recording medium,
The composite magnetic head according to claim 1 or 2, wherein the high-permeability ferrite block forming the second magnetic core has a smooth concave shape.
上記第2の磁気コアを構成する高透磁率フェライトブロ
ックは、上記作動ギャップに向かって尖った形状の突起
物を有している特許請求の範囲第1項又は第2項に記載
の複合型磁気ヘッド。4. A surface facing the magnetic recording medium,
The composite magnetic material according to claim 1 or 2, wherein the high-permeability ferrite block forming the second magnetic core has a protrusion having a sharp shape toward the working gap. head.
晶質磁性材料であり、かつ上記第2の磁気コアを構成す
る磁性体は多結晶磁性材料であることを特徴とする特許
請求の範囲第1項から4項のいずれかに記載の複合型磁
気ヘッド。5. A magnetic material forming the first magnetic core is an amorphous magnetic material, and a magnetic material forming the second magnetic core is a polycrystalline magnetic material. The composite magnetic head according to any one of claims 1 to 4.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58163254A JPH0622049B2 (en) | 1983-09-07 | 1983-09-07 | Combined type magnetic head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58163254A JPH0622049B2 (en) | 1983-09-07 | 1983-09-07 | Combined type magnetic head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6057512A JPS6057512A (en) | 1985-04-03 |
| JPH0622049B2 true JPH0622049B2 (en) | 1994-03-23 |
Family
ID=15770294
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58163254A Expired - Lifetime JPH0622049B2 (en) | 1983-09-07 | 1983-09-07 | Combined type magnetic head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0622049B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2625888B2 (en) * | 1988-05-25 | 1997-07-02 | ソニー株式会社 | Composite magnetic head |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56169214A (en) * | 1980-06-02 | 1981-12-25 | Nippon Hoso Kyokai <Nhk> | Magnetic head |
-
1983
- 1983-09-07 JP JP58163254A patent/JPH0622049B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6057512A (en) | 1985-04-03 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| KR910007861B1 (en) | Magnetic head and method of fabricating same | |
| JPH0477370B2 (en) | ||
| JPS6341127B2 (en) | ||
| JPH0442725B2 (en) | ||
| JPH0622049B2 (en) | Combined type magnetic head | |
| JPH0664703B2 (en) | Magnetic head | |
| US4731299A (en) | Composite magnetic material | |
| JPS5856163B2 (en) | Floating perpendicular magnetic recording/reproducing head | |
| JPH0142815Y2 (en) | ||
| JPS6212909A (en) | Combined erase head | |
| JPH0548244Y2 (en) | ||
| JPH0656646B2 (en) | Magnetic head | |
| JP2502273B2 (en) | Method of manufacturing magnetic head | |
| JP2549150B2 (en) | Perpendicular magnetic head | |
| KR100225346B1 (en) | Method for manufacturing m.i.g. type magnetic head | |
| JPH045046Y2 (en) | ||
| JPS62222412A (en) | Magnetic head and its manufacture | |
| JPS63271707A (en) | magnetic head | |
| JPH07121819A (en) | Magnetic head | |
| JPS61280009A (en) | Magnetic head | |
| JPS6139907A (en) | Magnetic head | |
| JPS6387606A (en) | Composite magnetic head | |
| JPS6356805A (en) | Magnetic head | |
| JPH07296321A (en) | Magnetic head | |
| JPS62177714A (en) | Magnetic head |