JPS6341127B2 - - Google Patents
Info
- Publication number
- JPS6341127B2 JPS6341127B2 JP2892480A JP2892480A JPS6341127B2 JP S6341127 B2 JPS6341127 B2 JP S6341127B2 JP 2892480 A JP2892480 A JP 2892480A JP 2892480 A JP2892480 A JP 2892480A JP S6341127 B2 JPS6341127 B2 JP S6341127B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- metal
- gap
- core body
- metal magnetic
- 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
Links
- 239000002184 metal Substances 0.000 claims description 18
- 239000000696 magnetic material Substances 0.000 claims description 10
- 230000004907 flux Effects 0.000 claims description 6
- 229910000702 sendust Inorganic materials 0.000 claims description 5
- 239000000463 material Substances 0.000 claims description 4
- 230000035699 permeability Effects 0.000 claims description 4
- 229910000889 permalloy Inorganic materials 0.000 claims description 3
- 229910000859 α-Fe Inorganic materials 0.000 claims description 3
- 229910001004 magnetic alloy Inorganic materials 0.000 claims description 2
- 239000010408 film Substances 0.000 description 12
- 239000011521 glass Substances 0.000 description 4
- 239000010409 thin film Substances 0.000 description 4
- 230000007423 decrease Effects 0.000 description 3
- 239000013590 bulk material Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000003754 machining Methods 0.000 description 2
- 238000004544 sputter deposition Methods 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 229910004298 SiO 2 Inorganic materials 0.000 description 1
- 238000005219 brazing Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000002500 effect on skin Effects 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 239000012528 membrane Substances 0.000 description 1
- 230000008929 regeneration Effects 0.000 description 1
- 238000011069 regeneration method Methods 0.000 description 1
- 230000003252 repetitive effect Effects 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
- 238000004804 winding 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
- G11B5/187—Structure or manufacture of the surface of the head in physical contact with, or immediately adjacent to the recording medium; Pole pieces; Gap features
Description
【発明の詳細な説明】
本発明は磁気ヘツドに関し、すぐれた性能を有
する超狭トラツク幅の磁気ヘツドが容易に得られ
るようにすることを目的とする。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic head, and an object of the present invention is to make it possible to easily obtain a magnetic head with excellent performance and an ultra-narrow track width.
従来、家庭用VTR用ビデオヘツドの様に数十
μm程度の狭トラツク幅を必要とする磁気ヘツド
は耐摩耗性を確保し、コア能率を高めまた隣接ト
ラツクからのクロストークの影響を減少させる事
のために、第1図a,bの様にメガヘルツ帯での
透確率が高いMn―Zn系各種フエライト(単結
晶、ホツトプレス、配向、その他)よりなる厚さ
100〜数百μmのコア1,1′のギヤツプ2の近傍
のみに所定のトラツク幅TWを残す様に切欠き3
を設け、切欠き部にガラス等の非磁性体3′を充
填した構造にしているのが一般的である。しかし
この様な構造のヘツドは、トラツク幅10μm程度
以下の超狭トラツク幅化に対しては、切欠き部近
傍のトラツク幅形成部4,4′の厚さが極端に薄
い事によりこの部分の磁気抵抗が高くなるので相
対的にトラツク側面からの漏洩磁束の割合が高く
なり、コア能率の低下およびこの部分での磁気的
飽和を招きやすくなる。またヘツド加工において
も、切欠き部の機械加工時に折損を生じやすく、
またエツチングやレーザー加工の場合でも所定の
トラツク幅精度を同時に実現する事は非常に困難
である。 Conventionally, magnetic heads, such as video heads for home VCRs, which require narrow track widths of several tens of micrometers, have been designed to ensure wear resistance, increase core efficiency, and reduce the effects of crosstalk from adjacent tracks. Therefore, as shown in Figure 1 a and b, the thickness is made of various Mn-Zn ferrites (single crystal, hot pressed, oriented, etc.) that have high permeability in the megahertz band.
The notch 3 is made so as to leave a predetermined track width TW only in the vicinity of the gap 2 of the cores 1 and 1', which are 100 to several hundred μm.
It is common to have a structure in which the notch is filled with a non-magnetic material 3' such as glass. However, a head with such a structure cannot be used for ultra-narrow track widths of about 10 μm or less because the thickness of the track width forming portions 4, 4' near the notch is extremely thin. Since the magnetic resistance becomes high, the proportion of leakage magnetic flux from the side surfaces of the track becomes relatively high, which tends to cause a decrease in core efficiency and magnetic saturation in this part. In addition, when machining the head, breakage is likely to occur when machining the notch.
Furthermore, even in the case of etching or laser processing, it is extremely difficult to simultaneously achieve a predetermined track width accuracy.
この様な点から第2図aに示すように、高飽和
磁束密度を有するパーマロイやセンダスト等の金
属磁性材料を蒸着やスパツタ法で形成し膜厚に等
しいトラツク幅を形成した構造のヘツドも知られ
ている。この構造のヘツドは第2図bの様にコア
半体の形状をしたガラス等の非磁性体基板5上
に、センダスト等の金属磁性体層6をスパツタリ
ング法等で形成し、第2図cの様にガラス等の非
磁性体基板7上で一対のコアを突合せ固定しギヤ
ツプを形成して第2図aの如き構造のヘツドを完
成するものである。この構造は基本的には磁性体
厚さがトラツク幅となるので数μm程度の超狭ト
ラツク幅を形成する事が可能であるが、反面、磁
性薄膜のみで磁気回路を構成するので磁気抵抗が
高くなりコア能率の低下を招きやすい。また第2
図b,cに見られる様に、能率的にギヤツプを形
成する方法を得難い構造であるという欠点をも持
つ。 From this point of view, as shown in Figure 2a, a head with a structure in which a metal magnetic material such as permalloy or sendust having a high saturation magnetic flux density is formed by vapor deposition or sputtering to form a track width equal to the film thickness is also known. It is being The head of this structure is made by forming a magnetic metal layer 6 such as Sendust on a non-magnetic substrate 5 such as glass in the shape of a half core by sputtering or the like, as shown in Fig. 2c. A pair of cores are abutted and fixed on a non-magnetic substrate 7 such as glass to form a gap, thereby completing a head having the structure as shown in FIG. 2a. In this structure, the track width is basically the thickness of the magnetic material, so it is possible to form an ultra-narrow track width of several μm. On the other hand, since the magnetic circuit is composed of only a magnetic thin film, the magnetic resistance is low. becomes high and tends to cause a decrease in core efficiency. Also the second
As seen in Figures b and c, the structure also has the disadvantage that it is difficult to find a way to efficiently form the gap.
本発明は、上記従来のヘツドの狭トラツク化に
際して生じる問題点を解決した優れた性能の構造
を与えるものである。以下に図面を用い本発明の
実施例を説明する。 The present invention provides a structure with excellent performance that solves the problems that arise when narrowing the track of the conventional head. Embodiments of the present invention will be described below with reference to the drawings.
第3図a,b,cはそれぞれ本発明による磁気
ヘツドの第1の実施例を示す。図において16お
よび16′はトラツク幅部を形成し高飽和磁束密
度を有する金属磁性体膜であり、センダストやア
モルフアス磁性合金のスパツタリング膜あるいは
高硬度パーマロイの蒸着膜等により構成されてい
る。またこれら左右一対の磁性体膜の突合せ部に
は、非磁性ギヤツプ12が形成されている。1
1,11′は前記の金属磁性体膜16,16′と磁
気的に連続するコア主体部であり、Mn―Zn フ
エライト、センダスト等の高透磁率を有するバル
ク材料からなつている。13および13′は前記
の薄膜トラツク幅部を支持あるいは保護し、かつ
ヘツド前面の耐摩耗強度を確保するために設けら
れた例えばガラス、ロウ材あるいは樹脂等の非磁
性体充填部である。10は巻線用窓である。なお
ここで第3図bはギヤツプ12近傍における金属
磁性体膜16,16′およびバルク材のコア主体
部11,11′の関係を明瞭にするために非磁性
体充填部13,13′を除去した図である。また
第3図cは、同ヘツドをテープ摺動面から見た図
である。本発明においては、金属磁性体膜16,
16′の厚みは所定のトラツク幅(数μm)に等
しく極めて薄い。そのために磁気抵抗が高く側面
からの漏洩磁束の割合が増加して、コア能率の低
下および磁性体膜部での磁気的飽和を生じやすい
ので、ギヤツプ深さ方向の広がり寸法Dおよび媒
体走行方向の広がり寸法Lは極力小さくする必要
があり、大略トラツク幅T、Wの10倍程度以下に
するのがよい。この様に薄膜のトラツク構成部は
必要最小限とし、磁気回路的にはコア幅が広く磁
気抵抗の小さいバルク材よりなるコア主体部1
1,11′に連続する構造となつている。また金
属磁性体部とバルク部との磁気的持続を完全なも
のとするためにバルク部の先端部でギヤツプ形成
面に平行な断面の面積は徐々に減じる構造となつ
ている。 3a, b and c each show a first embodiment of a magnetic head according to the invention. In the figure, reference numerals 16 and 16' designate metal magnetic films that form track width portions and have high saturation magnetic flux density, and are composed of sputtered films of sendust or amorphous magnetic alloy, or vapor-deposited films of high hardness permalloy. Further, a non-magnetic gap 12 is formed at the abutting portion of the pair of left and right magnetic films. 1
Reference numerals 1 and 11' denote core main parts that are magnetically continuous with the metal magnetic films 16 and 16', and are made of a bulk material having high magnetic permeability such as Mn--Zn ferrite or sendust. Numerals 13 and 13' are filled with non-magnetic material such as glass, brazing material, resin, etc., which are provided to support or protect the thin film track width portion and to ensure wear resistance on the front surface of the head. 10 is a winding window. In addition, in FIG. 3b, the non-magnetic material filling portions 13, 13' are removed in order to clarify the relationship between the metal magnetic films 16, 16' and the bulk core main body portions 11, 11' in the vicinity of the gap 12. This is a diagram. FIG. 3c is a view of the head viewed from the tape sliding surface. In the present invention, the metal magnetic film 16,
The thickness of 16' is extremely thin and equal to the predetermined track width (several μm). For this reason, the magnetic resistance is high and the proportion of magnetic flux leaking from the sides increases, which tends to reduce core efficiency and cause magnetic saturation in the magnetic film. The spread dimension L must be made as small as possible, and is preferably about 10 times or less the track widths T and W. In this way, the thin film track component is kept to the minimum necessary, and in terms of the magnetic circuit, the core main body 1 is made of a bulk material with a wide core width and low magnetic resistance.
1 and 11'. Further, in order to ensure complete magnetic continuity between the metal magnetic material portion and the bulk portion, the structure is such that the area of the cross section parallel to the gap forming surface gradually decreases at the tip of the bulk portion.
第4図は本発明による磁気ヘツドの第2の実施
例を示し、ギヤツプ12を介して対向する左右の
磁性体膜16,16′をトラツクの幅に関して同
一側に配置している。 FIG. 4 shows a second embodiment of the magnetic head according to the present invention, in which left and right magnetic films 16 and 16' facing each other with a gap 12 in between are arranged on the same side with respect to the width of the track.
第5図a,b,cは同じく本発明の第3の実施
例を示し、ギヤツプ極近傍のみの磁性体膜16,
16′をギヤツプ形成面と直交させ、コア主体部
11,11′との接合面はギヤツプ形成面と所定
の角度θをなす様にし、傾斜部が隣接トラツク部
にかかる場合に所定のアジマス損失を生じさせて
クロストークの減少を図つたものである。上記の
様にバルクコアの切欠き部での再生作用を防止す
る必要のない場合には、第6図の本発明の第4の
実施例を示す様に、コア主体部11,11′と磁
性体膜16,16′との接合面がギヤツプ形成面
と平行となる様に構成してもよい。 5a, b, and c similarly show a third embodiment of the present invention, in which the magnetic film 16 only near the gap pole,
16' is perpendicular to the gap forming surface, and the joint surfaces with the core main body parts 11, 11' form a predetermined angle θ with the gap forming surface, so that when the inclined part touches the adjacent track part, a predetermined azimuth loss is achieved. This is intended to reduce crosstalk. In the case where it is not necessary to prevent the regeneration effect at the notch portion of the bulk core as described above, as shown in the fourth embodiment of the present invention shown in FIG. The bonding surface with the membranes 16, 16' may be configured to be parallel to the gap forming surface.
第7図は同じく本発明の第5の実施例を示す。
この場合、トラツク幅T.Wは金属磁性体層17
とSiO或はSiO2等の非磁性絶縁体層18とを交互
にした積層体により構成されている。従つて金属
磁性体層の厚みを表皮効果による損失の生じない
厚みにまで薄くする一方積層枚数を増して所定の
トラツク幅を構成する事によりこの部分での磁気
抵抗を理想的な状態にまで小さくすることができ
る。なお実施例を示す図において、共通な要素に
は同一記号を付し、重復的説明は避けた。 FIG. 7 also shows a fifth embodiment of the present invention.
In this case, the track width TW is the metal magnetic layer 17.
It is constituted by a laminated body in which layers 18 of non-magnetic insulating material such as SiO or SiO 2 are alternately arranged. Therefore, by reducing the thickness of the metal magnetic layer to a thickness that does not cause loss due to the skin effect, and increasing the number of laminated layers to form a predetermined track width, the magnetic resistance in this area can be reduced to an ideal state. can do. In the drawings showing the embodiments, common elements are given the same symbols and repetitive explanations are avoided.
以上のように、本発明による磁気ヘツドはギヤ
ツプ近傍のトラツク幅構成部のみを、高飽和磁束
密度の磁性体薄膜で構成し、他の部分を高透磁率
の磁性体で構成しているので、記録特性および再
生特性の極めて優れた超狭トラツク幅の磁気ヘツ
ドとなつている。 As described above, in the magnetic head according to the present invention, only the track width component near the gap is made of a magnetic thin film with a high saturation magnetic flux density, and the other parts are made of a magnetic material with a high magnetic permeability. It is a magnetic head with an ultra-narrow track width and excellent recording and reproducing characteristics.
第1図a,bはそれぞれ従来の磁気ヘツドの上
面図および斜視図、第2図a,b,cはそれぞれ
従来の他の磁気ヘツドについて説明するための斜
視図、第3図a,b,cはそれぞれ本発明の第1
の実施例である磁気ヘツドの斜視図、同磁気ヘツ
ドの要部の斜視図、および同磁気ヘツドの上面
図、第4図は本発明の第2の実施例である磁気ヘ
ツドの上面図、第5図a,b,cはそれぞれ本発
明の第3の実施例である磁気ヘツドの上面図、斜
視図および同磁気ヘツドの要部の斜視図、第6
図、第7図はそれぞれ本発明の第4、第5の実施
例である磁気ヘツドの上面図である。
11,11′……コア主体部、12……ギヤツ
プ、13,13′……非磁性体充填部、16,1
6′……金属磁性体膜。
1A and 1B are a top view and a perspective view of a conventional magnetic head, respectively, FIGS. 2A, B, and C are perspective views for explaining another conventional magnetic head, and FIGS. 3A, B, c is the first of the present invention, respectively.
FIG. 4 is a perspective view of a magnetic head according to a second embodiment of the present invention, a perspective view of essential parts of the magnetic head, and a top view of the same magnetic head. Figures 5a, b, and c are respectively a top view, a perspective view, and a perspective view of essential parts of a magnetic head according to a third embodiment of the present invention.
7 are top views of magnetic heads which are fourth and fifth embodiments of the present invention, respectively. 11, 11'...Core main body part, 12...Gap, 13, 13'...Nonmagnetic material filling part, 16,1
6'...Metal magnetic film.
Claims (1)
れぞれの一端が互いに対向してギヤツプを形成し
かつ上記金属磁性体膜のギヤツプ形成部における
厚さがトラツク幅に対応し、かつ透磁率が高い磁
性体よりなるコア本体に上記金属磁性体膜の他端
側が接合したことを特徴とする磁気ヘツド。 2 金属磁性体膜とコア本体との接合面がトラツ
ク方向と平行していないことを特徴とする特許請
求の範囲第1項記載の磁気ヘツド。 3 金属磁性体膜とコア本体との接合面積がギヤ
ツプ形成面の面積よりも充分大であることを特徴
とする特許請求の範囲第1項又は第2項記載の磁
気ヘツド。 4 コア本体のギヤツプに近い側の面がトラツク
方向に対し傾斜していることを特徴とする特許請
求の範囲第1項記載の磁気ヘツド。 5 金属磁性体膜が非磁性体を間にはさんだ金属
磁性体の積層体で構成されていることを特徴とす
る特許請求の範囲第1項記載の磁気ヘツド。 6 コア本体の材料としてフエライトを用いかつ
金属磁性体膜の材料としてパーマロイ、センダス
トおよびアモロフアス磁性合金よりなるグループ
のなかより選択された少なくとも一つを用いたこ
とを特徴とする特許請求の範囲第1項記載の磁気
ヘツド。[Scope of Claims] 1. One ends of each of a pair of metal magnetic films having high saturation magnetic flux density face each other to form a gap, and the thickness of the metal magnetic film at the gap forming portion corresponds to the track width. A magnetic head characterized in that the other end side of the metal magnetic film is bonded to a core body made of a magnetic material having high magnetic permeability. 2. The magnetic head according to claim 1, wherein the bonding surface between the metal magnetic film and the core body is not parallel to the track direction. 3. The magnetic head according to claim 1 or 2, wherein the bonding area between the metal magnetic film and the core body is sufficiently larger than the area of the gap forming surface. 4. The magnetic head according to claim 1, wherein the surface of the core body closer to the gap is inclined with respect to the track direction. 5. The magnetic head according to claim 1, wherein the metal magnetic film is composed of a laminate of metal magnetic materials with a non-magnetic material sandwiched therebetween. 6. Claim 1, characterized in that ferrite is used as the material of the core body, and at least one selected from the group consisting of permalloy, sendust, and amorphous magnetic alloy is used as the material of the metal magnetic film. Magnetic head as described in section.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2892480A JPS56124112A (en) | 1980-03-06 | 1980-03-06 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2892480A JPS56124112A (en) | 1980-03-06 | 1980-03-06 | Magnetic head |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS56124112A JPS56124112A (en) | 1981-09-29 |
JPS6341127B2 true JPS6341127B2 (en) | 1988-08-16 |
Family
ID=12261941
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2892480A Granted JPS56124112A (en) | 1980-03-06 | 1980-03-06 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS56124112A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01149618U (en) * | 1988-04-06 | 1989-10-17 |
Families Citing this family (18)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58155513A (en) * | 1982-03-10 | 1983-09-16 | Hitachi Ltd | Composite magnetic head and its manufacture |
JPS59193235A (en) * | 1983-04-15 | 1984-11-01 | Hitachi Ltd | Co-nb-zr type amorphous magnetic alloy and magnetic head using the same |
JPS6032107A (en) * | 1983-07-30 | 1985-02-19 | Sony Corp | Magnetic head |
JPS60229210A (en) * | 1983-12-30 | 1985-11-14 | Sony Corp | Magnetic head |
CA1236212A (en) * | 1983-12-30 | 1988-05-03 | Heikichi Sato | Magnetic transducer head with slanted thin film |
JPS60182507A (en) * | 1984-02-29 | 1985-09-18 | Sony Corp | Magnetic head |
JPH0656647B2 (en) * | 1985-01-26 | 1994-07-27 | ソニー株式会社 | Magnetic head |
US4819113A (en) * | 1984-03-29 | 1989-04-04 | Sony Corporation | Magnetic transducer head with inclined magnetic gap |
DE3584607D1 (en) * | 1984-09-19 | 1991-12-12 | Hitachi Maxell | MAGNETIC HEAD. |
JPS61126614A (en) * | 1984-11-21 | 1986-06-14 | Victor Co Of Japan Ltd | Magnetic head and its production |
JPH0654527B2 (en) * | 1984-11-26 | 1994-07-20 | ソニー株式会社 | Magnetic head |
JPS61158015A (en) * | 1984-12-29 | 1986-07-17 | Sony Corp | Production of magnetic head |
JPH0658727B2 (en) * | 1985-04-13 | 1994-08-03 | ソニー株式会社 | Magnetic head |
JPH0758527B2 (en) * | 1986-01-10 | 1995-06-21 | 株式会社日立製作所 | Magnetic head |
JPS63228403A (en) * | 1987-03-18 | 1988-09-22 | Akai Electric Co Ltd | Magnetic head and production of magnetic head |
JPH01264610A (en) * | 1989-03-08 | 1989-10-20 | Hitachi Ltd | Compound type magnetic head |
JPH01264611A (en) * | 1989-03-08 | 1989-10-20 | Hitachi Ltd | Manufacture of compound type magnetic head |
JPH04356701A (en) * | 1991-09-13 | 1992-12-10 | Hitachi Ltd | Composite type magnetic head |
-
1980
- 1980-03-06 JP JP2892480A patent/JPS56124112A/en active Granted
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01149618U (en) * | 1988-04-06 | 1989-10-17 |
Also Published As
Publication number | Publication date |
---|---|
JPS56124112A (en) | 1981-09-29 |
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