JPH0490108A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPH0490108A JPH0490108A JP20240090A JP20240090A JPH0490108A JP H0490108 A JPH0490108 A JP H0490108A JP 20240090 A JP20240090 A JP 20240090A JP 20240090 A JP20240090 A JP 20240090A JP H0490108 A JPH0490108 A JP H0490108A
- Authority
- JP
- Japan
- Prior art keywords
- core
- magnetic
- length
- core base
- magnetic head
- 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
- 238000011144 upstream manufacturing Methods 0.000 claims abstract description 8
- 239000010409 thin film Substances 0.000 claims description 12
- 230000004907 flux Effects 0.000 claims description 6
- 238000005336 cracking Methods 0.000 abstract description 5
- 230000035699 permeability Effects 0.000 description 7
- 229910045601 alloy Inorganic materials 0.000 description 6
- 239000000956 alloy Substances 0.000 description 6
- 239000000696 magnetic material Substances 0.000 description 5
- 239000000758 substrate Substances 0.000 description 4
- 229910000859 α-Fe Inorganic materials 0.000 description 4
- 230000001154 acute effect Effects 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 2
- 229910000676 Si alloy Inorganic materials 0.000 description 2
- QCWXUUIWCKQGHC-UHFFFAOYSA-N Zirconium Chemical compound [Zr] QCWXUUIWCKQGHC-UHFFFAOYSA-N 0.000 description 2
- 229910000808 amorphous metal alloy Inorganic materials 0.000 description 2
- 229910017052 cobalt Inorganic materials 0.000 description 2
- 239000010941 cobalt Substances 0.000 description 2
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 description 2
- 229910052726 zirconium Inorganic materials 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 1
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 1
- 229910001289 Manganese-zinc ferrite Inorganic materials 0.000 description 1
- ZOKXTWBITQBERF-UHFFFAOYSA-N Molybdenum Chemical compound [Mo] ZOKXTWBITQBERF-UHFFFAOYSA-N 0.000 description 1
- 229910001053 Nickel-zinc ferrite Inorganic materials 0.000 description 1
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- JIYIUPFAJUGHNL-UHFFFAOYSA-N [O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[Mn++].[Mn++].[Mn++].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Zn++].[Zn++] Chemical compound [O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[O--].[Mn++].[Mn++].[Mn++].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Fe+3].[Zn++].[Zn++] JIYIUPFAJUGHNL-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052790 beryllium Inorganic materials 0.000 description 1
- ATBAMAFKBVZNFJ-UHFFFAOYSA-N beryllium atom Chemical compound [Be] ATBAMAFKBVZNFJ-UHFFFAOYSA-N 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
- 239000011651 chromium Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 229910052732 germanium Inorganic materials 0.000 description 1
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 229910052735 hafnium Inorganic materials 0.000 description 1
- VBJZVLUMGGDVMO-UHFFFAOYSA-N hafnium atom Chemical compound [Hf] VBJZVLUMGGDVMO-UHFFFAOYSA-N 0.000 description 1
- 229910052738 indium Inorganic materials 0.000 description 1
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical compound [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- XWHPIFXRKKHEKR-UHFFFAOYSA-N iron silicon Chemical compound [Si].[Fe] XWHPIFXRKKHEKR-UHFFFAOYSA-N 0.000 description 1
- -1 iron-aluminum-silicon Chemical compound 0.000 description 1
- WPBNNNQJVZRUHP-UHFFFAOYSA-L manganese(2+);methyl n-[[2-(methoxycarbonylcarbamothioylamino)phenyl]carbamothioyl]carbamate;n-[2-(sulfidocarbothioylamino)ethyl]carbamodithioate Chemical compound [Mn+2].[S-]C(=S)NCCNC([S-])=S.COC(=O)NC(=S)NC1=CC=CC=C1NC(=S)NC(=O)OC WPBNNNQJVZRUHP-UHFFFAOYSA-L 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 229910052750 molybdenum Inorganic materials 0.000 description 1
- 239000011733 molybdenum Substances 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- 229910052758 niobium Inorganic materials 0.000 description 1
- 239000010955 niobium Substances 0.000 description 1
- GUCVJGMIXFAOAE-UHFFFAOYSA-N niobium atom Chemical compound [Nb] GUCVJGMIXFAOAE-UHFFFAOYSA-N 0.000 description 1
- 229910052698 phosphorus Inorganic materials 0.000 description 1
- 239000011574 phosphorus Substances 0.000 description 1
- 230000002250 progressing effect Effects 0.000 description 1
- 230000003014 reinforcing effect Effects 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 229910052718 tin Inorganic materials 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、磁気ヘッドに係り、特に磁気ギャップと対向
する方の側面が磁気ギャップ面に対して傾斜してなるコ
ア基体と、そのコア基体の磁気ギャップに対向する方の
側面に被着された高飽和磁束密度を有する磁性材料より
なる磁性薄膜とを備えたコア半体を有する磁気ヘッドに
関する。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a magnetic head, and in particular to a core base whose side surface facing a magnetic gap is inclined with respect to the magnetic gap plane, and the core base. The present invention relates to a magnetic head having a core half having a magnetic thin film made of a magnetic material having a high saturation magnetic flux density and deposited on the side surface facing the magnetic gap.
磁気記録の高密度化にともない、磁気記録媒体の保持力
が高められ、この磁気記録媒体に記録可能な磁気ヘッド
として、少なくとも磁気ギャップと対向する部分を高飽
和磁束密度を有する磁性材料で構成した磁気ヘッドの開
発が進められている。With the increase in the density of magnetic recording, the coercive force of magnetic recording media has been increased, and a magnetic head capable of recording on this magnetic recording medium is made of a magnetic material having a high saturation magnetic flux density, at least in the portion facing the magnetic gap. Development of magnetic heads is progressing.
第3図はこの種の従来の磁気ヘッドの1例として挙げた
磁気ヘッドの平面図、第4図は第3図のイーイ線断面図
である。この磁気ヘッドは磁気ディスク再生装置に用い
られるもので、ヘッド保持体(図示せず)に取り付けら
れる。FIG. 3 is a plan view of a magnetic head as an example of this type of conventional magnetic head, and FIG. 4 is a sectional view taken along the line E-II in FIG. This magnetic head is used in a magnetic disk reproducing device and is attached to a head holder (not shown).
再生ヘッド21は、トラック走行方向Aの上流側に位置
する第1コア半体24と、それと対向する第2コア半体
25と、第2コア半体25に設けたコイル溝26に巻装
される励磁コイル27とから主として構成されている。The reproducing head 21 is wound around a first core half 24 located on the upstream side in the track running direction A, a second core half 25 opposite thereto, and a coil groove 26 provided in the second core half 25. It mainly consists of an excitation coil 27.
28はガラス等の非磁性体からなる補強層で、第1コア
半体24と第2コア半体25の接合部近傍に設けられて
いる。A reinforcing layer 28 made of a non-magnetic material such as glass is provided near the joint between the first core half 24 and the second core half 25.
第1コア半体24は、磁気ギャップ35と対向する側面
のほぼ中央に山形の突出部29を有し、高透磁率のフェ
ライトからなる第1コア基体30と、前記側面に被着さ
れた高飽和磁束密度と高透磁率を有する金属磁性材料よ
りなる第1磁性薄膜31とから構成されている。The first core half 24 has a chevron-shaped protrusion 29 approximately in the center of the side surface facing the magnetic gap 35, and includes a first core base 30 made of ferrite with high magnetic permeability and a high It is composed of a first magnetic thin film 31 made of a metallic magnetic material having a saturation magnetic flux density and high magnetic permeability.
第2コア半体25も第1コア半体24と同様に。The second core half 25 is similar to the first core half 24.
磁気ギャップ35と対応する側面のほぼ中央に山形の突
出部32を有する高透磁率のフェライトからなる第2コ
ア基体33と、それの前記側面に被着された高飽和磁束
密度と高透磁率を有する金属磁性材料よりなる第2磁性
薄膜34とから構成されている。第3図に示すように第
1コア半体24側に突出部29ならびに第1磁性薄膜3
1と、第2コア半体25側の突出部32ならびに第2磁
性薄膜34とは、接合部近傍の形状が磁気ギャップ35
を介してほぼ左右対称になっている。この磁気ギャップ
35は約30〜140μm程度の長さを有している。A second core base 33 made of ferrite with high magnetic permeability and having a chevron-shaped protrusion 32 at approximately the center of the side surface corresponding to the magnetic gap 35, and a second core base body 33 made of ferrite with high magnetic permeability and having a high saturation magnetic flux density and high magnetic permeability adhered to the side surface thereof. and a second magnetic thin film 34 made of a metallic magnetic material. As shown in FIG. 3, a protrusion 29 and a first magnetic thin film 3 are provided on the first core half 24 side.
1, the protruding portion 32 on the second core half 25 side, and the second magnetic thin film 34 have a shape near the joint portion that is the magnetic gap 35.
It is almost symmetrical between the left and right sides. This magnetic gap 35 has a length of approximately 30 to 140 μm.
ところで、このように構成しである従来の磁気ヘッドは
、上述したようにコア基体30.33の突出部29.3
2の角度θが鋭角になっていることから、コア半体24
.25の作製時等に突出部29.32の先端部に割れや
欠けを生じやすく、歩留りが悪い不具合がある。By the way, in the conventional magnetic head configured as described above, the protrusion 29.3 of the core base 30.33
Since the angle θ of 2 is an acute angle, the core half 24
.. When manufacturing the protruding parts 29 and 25, cracks and chips tend to occur at the tips of the protruding parts 29 and 32, resulting in poor yield.
またこのようなコア半体の突出部に作製時等に際しての
割れや欠けを防止するために、従来、第5図に示す磁気
コアが提案されている。Furthermore, in order to prevent the protruding portions of such core halves from cracking or chipping during manufacturing, a magnetic core shown in FIG. 5 has been proposed.
第5図に示す磁気コアは、コア半体55.56を形成す
るコア基体57.58のそれぞれの突出部59.60の
先端部に幅の狭い平坦部61.62を設けたものである
。The magnetic core shown in FIG. 5 has a narrow flat portion 61.62 at the tip of each protrusion 59.60 of a core base 57.58 forming a core half 55.56.
しかしながら、この磁気ヘッドでは、前記平坦部が磁気
ギャップに平行であるため、平坦部の長さによっては、
擬似ギャップとなり、再生波形を乱す要因となり得る。However, in this magnetic head, since the flat part is parallel to the magnetic gap, depending on the length of the flat part,
This may result in a pseudo gap, which may disturb the reproduced waveform.
本発明の目的は、コア半体の製作時等におけるコア半体
の突出部の先端部の割れや欠けを抑制するとともに擬似
ギャップによる再生波形の乱れを防止することができる
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 capable of suppressing cracking or chipping of the tip of a protruding portion of a core half during manufacturing of the core half, and preventing disturbance of reproduced waveform due to a pseudo gap. It is in.
上記目的を達成するために本発明は、トラック走行方向
の下流側のコア半体における突出部のトラック幅方向の
長さをLls上流側の突出部のトラック幅方向の長さを
L!とするとき、L 2 / L 1=0〜0.8と設
定したものである。In order to achieve the above object, the present invention sets the length in the track width direction of the protrusion in the core half on the downstream side in the track running direction to Lls, and the length in the track width direction of the protrusion on the upstream side to L! In this case, L 2 /L 1 is set as 0 to 0.8.
これによって、擬似ギャップに起因するエラーレートは
実質的に無視し得る程度であり、またコア半体の突出部
の先端の割れや欠けを抑制できる。As a result, the error rate caused by the pseudo gap is substantially negligible, and cracking or chipping of the tip of the protruding portion of the core half can be suppressed.
以下、本発明を図面に基づいて説明する。 Hereinafter, the present invention will be explained based on the drawings.
第1図は本発明の磁気ヘッドの一実施例を示す平面図、
第2図は他の実施例を示す平面図である。FIG. 1 is a plan view showing an embodiment of the magnetic head of the present invention;
FIG. 2 is a plan view showing another embodiment.
図において、第3図〜第5図の従来例と同一構成部分は
、第3図〜第5図と同一符号で示している。In the figures, the same components as those in the conventional example shown in FIGS. 3 to 5 are indicated by the same reference numerals as in FIGS. 3 to 5.
第1図の実施例において、再生ヘッド21の第1コア半
体24を構成する第1コア基体30の突出部29は、そ
の角度θが鋭角であるが、第2コア半体25を構成する
第2コア基体33の突出部32の先端部には、トラック
幅の1/20〜115の範囲の長さL2を有する平坦部
62が形成されている。In the embodiment shown in FIG. 1, the protrusion 29 of the first core base 30 constituting the first core half 24 of the reproducing head 21 has an acute angle θ; A flat portion 62 having a length L2 in a range of 1/20 to 115 of the track width is formed at the tip of the protruding portion 32 of the second core base 33.
第2図の実施例では、第1コア半体24を構成する第1
コア基体30の突出部29の先端部、及び第2コア半体
25を構成する第2コア基体33の突出部32の先端部
のいずれにも平坦部61゜62を形成し、第1コア基体
30側の平坦部61の長さL+を第2コア基体25側の
平坦部62の長さL2より小としたものである。In the embodiment of FIG. 2, the first
Flat portions 61 and 62 are formed at both the tip of the protrusion 29 of the core base 30 and the tip of the protrusion 32 of the second core base 33 constituting the second core half 25, and the first core base The length L+ of the flat portion 61 on the 30 side is made smaller than the length L2 of the flat portion 62 on the second core base 25 side.
いずれの実施例においても、磁性薄膜31.34は平坦
部61.62を含む突出部29.32の側面全体にほぼ
均一な厚さ、例えば50μmの厚さで被着されている。In both embodiments, the magnetic thin film 31.34 is applied to the entire side surface of the projection 29.32, including the flat portion 61.62, to a substantially uniform thickness, for example 50 μm.
前記再生ヘッド側の第1コア基体30および第2コア基
体33、例えばマンガン−亜鉛フェライトやニッケルー
亜鉛フェライトのような高透磁率を有するフェライトが
用いられる。一方、前記磁性薄膜31.34には、高飽
和磁束密度ならびに高透磁率を存する結晶質合金や非晶
質合金が用いられる。この結晶質合金としては鉄−アル
ミニウム−ケイ素合金、鉄−ケイ素合金ならびに鉄−ニ
ッケル系合金などがある。また非晶質合金としては、鉄
、ニッケル、コバルトのグループから選択された1種以
上の元素と、リン、炭素、ホウ素、ケイ素、のグループ
から選択された1種以上の元素とからなる合金、または
これらを主成分として、アルミニウム、ゲルマニウム、
ベリリウム、スズ、モリブテン、インジュウム、タング
ステン、チタン、マンガン、クロム、ジルコニウム、ハ
フニウム、ニオブなどの元素を添加した合金あるいはコ
バルト、ジルコニウムを主成分として前述の添加元素を
含んだ合金などがある。本発明において、磁性薄膜には
特に非晶質合金が特に望ましい。The first core substrate 30 and the second core substrate 33 on the read head side are made of ferrite having high magnetic permeability, such as manganese-zinc ferrite or nickel-zinc ferrite. On the other hand, for the magnetic thin films 31 and 34, a crystalline alloy or an amorphous alloy having high saturation magnetic flux density and high magnetic permeability is used. Examples of such crystalline alloys include iron-aluminum-silicon alloys, iron-silicon alloys, and iron-nickel alloys. Examples of amorphous alloys include alloys consisting of one or more elements selected from the group of iron, nickel, and cobalt and one or more elements selected from the group of phosphorus, carbon, boron, and silicon; Or with these as main components, aluminum, germanium,
Examples include alloys to which elements such as beryllium, tin, molybdenum, indium, tungsten, titanium, manganese, chromium, zirconium, hafnium, and niobium are added, and alloys containing cobalt and zirconium as main components and the above-mentioned additional elements. In the present invention, an amorphous alloy is particularly desirable for the magnetic thin film.
なお、第1図に示す第1コア基体30の突出部29の角
度θは45″〜90″程度の鋭角、すなわち比較的小さ
い角度に設定されている。第2コア半体25の第2コア
基体33の突出部32の角度も同様である。Note that the angle θ of the protrusion 29 of the first core base 30 shown in FIG. 1 is set to an acute angle of about 45'' to 90'', that is, a relatively small angle. The same applies to the angle of the protrusion 32 of the second core base 33 of the second core half 25.
次に、この様な構成からなる磁気ヘッドについて、発明
者等は種々の実験、測定を行い、擬似ギャップの発生(
再生エラーレートの大小)、及び生産性(コア基体突出
部先端の欠け、割れ)について検討した。その結果、ト
ラック走行方向と上流側のコア基体の突出部の幅り、と
下流側のコア基体の突出部の幅L2との関係をL+/L
t=0〜0.8、好ましくはLl /L! =0〜0.
5の範囲に設定すれば擬似ギャップの発生もなくまた生
産性も所定レベル以上のものとすることができることを
見出した。Next, the inventors conducted various experiments and measurements on the magnetic head constructed as described above, and found that the occurrence of pseudo gaps (
The size of playback error rate) and productivity (chips and cracks at the tip of the protruding portion of the core base) were investigated. As a result, the relationship between the track running direction, the width of the protruding part of the upstream core base, and the width L2 of the protruding part of the downstream core base is determined as L+/L.
t=0-0.8, preferably Ll/L! =0~0.
It has been found that if it is set within the range of 5, no pseudo gap will occur and the productivity can be increased to a predetermined level or higher.
以下に抽出したサンプルを表1として示す0表1では第
1図に示す本発明の第1実施例、漱2は第2図に示す第
2実施例、Nα3は第3図に示す第1従来例、Nα4は
第5図に示す第2従来例の磁気ヘッドを各々示している
。The samples extracted below are shown in Table 1.Table 1 shows the first embodiment of the present invention shown in FIG. 1, Sō2 shows the second embodiment shown in FIG. 2, and Nα3 shows the first conventional example shown in FIG. For example, Nα4 indicates the second conventional magnetic head shown in FIG.
表1
表1かられかるように、トラック走行方向の下流側に位
置するコア基体の突出部先端に平坦部が無い場合、即ち
Lt=Oの場合コア基体の欠け、割れにより生産性が著
しく低下する。また、上流側突出部先端の平坦部の長さ
り、が下流側平坦部の長さL2に等しいか若しくはそれ
以上であると、擬似ギャップが発生する。Table 1 As shown in Table 1, when there is no flat part at the tip of the protruding part of the core base located on the downstream side in the truck running direction, that is, when Lt=O, productivity decreases significantly due to chips and cracks in the core base. do. Furthermore, if the length of the flat portion at the tip of the upstream protrusion is equal to or greater than the length L2 of the downstream flat portion, a pseudo gap occurs.
以上のように本発明によれば、トラック走行方向の上流
側に位置するコア基体の突出部のトラック幅方向の長さ
Llと、下流側に位置するコア基体の突出部のトラック
幅方向の長さLxとの関係をL+/Lz=0.8とした
ため、擬似ギャップの発生ニヨる再生波形の乱れを防止
でき、またコア基体の突出部の割れや欠けを抑制して生
産性の良好な磁気ヘッドを得ることができる。As described above, according to the present invention, the length Ll in the track width direction of the protrusion of the core base located on the upstream side in the track running direction, and the length Ll in the track width direction of the protrusion of the core base located on the downstream side. Since the relationship with Lx is set to L+/Lz=0.8, it is possible to prevent the disturbance of the reproduced waveform caused by the occurrence of pseudo gaps, and also to suppress cracks and chips on the protruding parts of the core base, resulting in a magnetic system with good productivity. You can get the head.
なお、本磁気ヘッドの構造は、再生だけでなく、記録用
ヘッド、記録再生ヘッドにも適用できることは言うまで
もない。It goes without saying that the structure of the present magnetic head can be applied not only to reproducing heads but also to recording heads and recording/reproducing heads.
第1図は本発明の磁気ヘッドの一実施例を示す平面図、
第2図は本発明の磁気ヘッドの他の実施例を示す平面図
、第3図は従来の磁気ヘッドを示す平面図、第4図は第
3図のイーイ線上の断面図第5図は他の従来の磁気ヘッ
ドを示す平面図である。
21・・・・・・・・・再生ヘッド、24・・・・・・
用筆1コア半体、25・・・・・・・・・第2コア半体
、29・・・・・・・・・突出部、30・・・・・・・
・・第1コア基体、31・・・・・・川第1磁性薄膜、
32・・・・・・・・・突出部、33・・・町・・第2
コア基体、34・・・・・・・・・第2磁性薄膜、35
・・・・・・・・・磁気ギヤッ61゜
62・・・・・・・・・平坦部。
図
第
21・・・・・・再生へ51.F
24・・・・第1]ア学仏
25・・・・・・オ2コア午体
29.32・・・大出若p
30・・・・・ 71コアゐ体
31・−・ ・ 71jン袂゛1生淳月更33・・・・
・ 72コア基体
34・・・・・・72五性薄膜
35・・・・・・ル扛気ff”v・・/フ。
61.62・・・干以都FIG. 1 is a plan view showing an embodiment of the magnetic head of the present invention;
FIG. 2 is a plan view showing another embodiment of the magnetic head of the present invention, FIG. 3 is a plan view showing a conventional magnetic head, FIG. 4 is a sectional view taken along the E-I line in FIG. 3, and FIG. FIG. 2 is a plan view showing a conventional magnetic head. 21......Playback head, 24...
Brush 1 core half, 25... Second core half, 29... Protrusion, 30...
...First core substrate, 31... River first magnetic thin film,
32...Protrusion, 33...Town...Second
Core substrate, 34... Second magnetic thin film, 35
......Magnetic gear 61°62...Flat part. Figure 21...Go to playback 51. F 24... 1st] A Gakbutsu 25...O2 core meridian body 29.32...Odewaka p 30...71 core body 31... 71j 33...
・ 72 core base 34...72 pentagonal thin film 35...le air ff"v.../fu. 61.62...hanitsu
Claims (1)
もに前記2つのコア半体の互いに対向する側面に山形の
突出部を有し、その突出部上に高飽和磁束密度を有する
磁性薄膜を被着してなる磁気ヘッドにおいて、トラック
走行方向の下流側のコア半体における前記突出部の先端
のトラック幅方向の長さをL_2、トラック走行方向の
上流側のコア半体における前記突出部の先端のトラック
幅方向の長さをL_1とするとき、L_1/L_2=0
〜0.8と設定したことを特徴とする磁気ヘッド。The two core halves are joined via a magnetic gap, and the two core halves have chevron-shaped protrusions on opposing sides, and the protrusions are covered with a magnetic thin film having a high saturation magnetic flux density. In the magnetic head, the length in the track width direction of the tip of the protrusion in the core half on the downstream side in the track running direction is L_2, and the tip of the protrusion in the core half on the upstream side in the track running direction is L_2. When the length in the track width direction is L_1, L_1/L_2=0
A magnetic head characterized in that the magnetic head is set to 0.8.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20240090A JPH0490108A (en) | 1990-08-01 | 1990-08-01 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20240090A JPH0490108A (en) | 1990-08-01 | 1990-08-01 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0490108A true JPH0490108A (en) | 1992-03-24 |
Family
ID=16456874
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP20240090A Pending JPH0490108A (en) | 1990-08-01 | 1990-08-01 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0490108A (en) |
-
1990
- 1990-08-01 JP JP20240090A patent/JPH0490108A/en active Pending
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