JPH01227206A - Magnetic head - Google Patents

Magnetic head

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Publication number
JPH01227206A
JPH01227206A JP63054206A JP5420688A JPH01227206A JP H01227206 A JPH01227206 A JP H01227206A JP 63054206 A JP63054206 A JP 63054206A JP 5420688 A JP5420688 A JP 5420688A JP H01227206 A JPH01227206 A JP H01227206A
Authority
JP
Japan
Prior art keywords
magnetic
substrate
layer
target
insulating material
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
Application number
JP63054206A
Other languages
Japanese (ja)
Inventor
Takeshi Hirota
健 廣田
Mitsuo Satomi
三男 里見
Koichi Kugimiya
公一 釘宮
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP63054206A priority Critical patent/JPH01227206A/en
Publication of JPH01227206A publication Critical patent/JPH01227206A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To make the thermal expansion coefficient of layer insulators of multilayer structure close to the coefficient of a metallic material by making the layer mainly out of an oxide of Al and Si and including simultaneously the crystal phases of both cristobalite and mullite by the oxide of Al and Si. CONSTITUTION:A substrate material is mirror-finished to form a substrate 1, Ar is led into a pressure reducing vessel, a sputtering is performed by using a target of composition CoSiNb13Zr6 and a noncrystalline alloy film 2a is manufactured. Next, when powder of composition in which the weight inclusion ratio of Al2O3 to SiO2 is 40:60 is calcined, crushed, formed and baked to manufacture a target, the mullite and the cristobalite coexist in its composition and a thermal expansion coefficient alpha becomes 115X10<-7>/ deg.C. Next, a layer insulating material 3 is made on the noncrystalline alloy film 2a by a spatter by using the target, and a block of three-layer structure is obtained with the noncrystalline alloy film and the layer insulating material as 2b, 3b and 2c alternately in the same way. Next, a laminated core is obtained by joining the substrate 1 and a substrate 5 made of the same material through an adhesive glass layer 4, a coil window 6 is processed and after that, laminated core half- bodies 1'-5' of the same structure are joined 7 together.

Description

【発明の詳細な説明】 産業上の利用分野 この発明は、電気・電子工業に用いられる磁気ヘッドに
関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application This invention relates to a magnetic head used in the electrical and electronic industries.

従来の技術 従来より、磁気ヘッド用コア材として、耐磨耗性が良い
という特長から、フェライトが広(使用されているが、
飽和磁束密度Bsが合金材料に比べて30〜50%低い
ので、近年登場してきた高 。
Conventional technology Ferrite has been widely used as a core material for magnetic heads due to its good abrasion resistance.
Since the saturation magnetic flux density Bs is 30 to 50% lower than that of alloy materials, high-density metals that have appeared in recent years.

抗磁力の高密度記録用媒体に使用した場合、ヘッドコア
の磁気飽和が問題となり、このような観点から、高密度
記録媒体への対応ヘッドとして、パーマロイやセンダス
トなどの合金材料を使った磁気ヘッドが実用化されてい
る。
When used for high-density recording media with coercive force, magnetic saturation of the head core becomes a problem.From this perspective, magnetic heads using alloy materials such as permalloy and sendust are recommended as heads compatible with high-density recording media. It has been put into practical use.

他方、耐磨耗性、磁気特性とも優れた材料として、非晶
質合金が脚光を浴びてきている。これらの合金材料を、
磁気へラドコア材料として、使用した場合、材料自身の
比抵抗が70〜120μΩCmと低いので高周波領域で
、渦電流による損失が大きいため、通常積層構造により
、改善を図っている。
On the other hand, amorphous alloys have been attracting attention as materials with excellent wear resistance and magnetic properties. These alloy materials,
When used as a magnetic helad core material, the resistivity of the material itself is as low as 70 to 120 .mu..OMEGA.Cm, resulting in large losses due to eddy currents in the high frequency region, so improvements are usually made by using a laminated structure.

オーディオヘッドに於いては、トラック幅が数100μ
mと太き(、周波数領域も低いので一枚当たりのコアの
厚みも200〜300μmと厚く、積層及びギャップ形
成は、エボ牛シ樹脂等の所謂接着剤が使用されている。
In audio heads, the track width is several hundred microns.
Since the frequency range is low, the thickness of each core is as thick as 200 to 300 μm, and so-called adhesives such as ebo-shi resin are used for lamination and gap formation.

しかしながら、ビデオ、コンピュータ、計測機用磁気ヘ
ッドとなると、トラック幅が小さく(例えば数10μm
)、且つギャップ長が非常に短い(例えば0.3μm以
下)ので、接着剤による磁気ヘッド構成では、高精度の
ギャップを維持することは、困難である。
However, when it comes to magnetic heads for videos, computers, and measuring instruments, the track width is small (for example, several tens of μm).
), and the gap length is very short (for example, 0.3 μm or less), so it is difficult to maintain a highly accurate gap in a magnetic head configuration using adhesive.

又、トラック幅が小さ(、且つ使用周波数領域も数MH
zないしは10MHzと高いので、−枚当たりのコアの
厚みも10μmあるいはそれ以下が望ましい。
In addition, the track width is small (and the frequency range used is several MH)
Since the frequency is as high as 10 MHz or 10 MHz, the thickness of each core is preferably 10 μm or less.

このような厚みの磁気コアをいわゆるバルク材料から作
製するには、現在の加工技術では、困難であり、超急冷
法によるリボンアモルファスやリボンセンダストでも厚
みが20μm以下では、均一な厚みのものを得ることは
難しい。
It is difficult to produce a magnetic core of such thickness from so-called bulk materials using current processing technology, and even with ribbon amorphous or ribbon Sendust produced by ultra-quenching, it is difficult to obtain a magnetic core with a uniform thickness at a thickness of 20 μm or less. That's difficult.

従って、上記観点より、磁性材料である非晶質合金やセ
ンダスト合金を、スパッタ法や蒸着法によって薄板化す
る方法が採用されている。これらの方法によると、−枚
当たりのコアの厚みが10μm以下のものが容易に得ら
れ、且つ磁性材料と層間絶縁材料を交互に積層すること
が可能であり各材料間の付着強度も強いので、前記高精
度のギャップを維持することが可能である。
Therefore, from the above point of view, methods have been adopted in which magnetic materials such as amorphous alloys and sendust alloys are made into thin plates by sputtering or vapor deposition. According to these methods, it is easy to obtain cores with a thickness of 10 μm or less per sheet, and it is also possible to alternately laminate magnetic materials and interlayer insulating materials, and the adhesion strength between each material is strong. , it is possible to maintain the high precision gap.

この時の層間絶縁材料として、SiO2が用いられてい
るのは公知である(電子通信学会論文誌別刷Trans
、IECE’74/9  Vol。
It is well known that SiO2 is used as the interlayer insulating material at this time (Trans.
, IECE'74/9 Vol.

57−CNo、9.電気学会研究会資料MAG82−3
6)。又ギャップスペーサ−材料としてをSiO2を用
いるのも公知である。
57-CNo.9. Institute of Electrical Engineers of Japan study group material MAG82-3
6). It is also known to use SiO2 as a gap spacer material.

発明が解決しようとする課題 このような従来の金属磁性材料と眉間絶縁材料であるS
iO2の積層磁芯からなる磁気ヘッドにおいて、積層枚
数を多(してい(と、磁性材料の厚みが同一にもかかわ
らず、透磁率μが低下する傾向が見られた。
Problems to be Solved by the Invention The conventional metal magnetic material and the eyebrow insulating material S
In a magnetic head made of a laminated iO2 magnetic core, there was a tendency for the magnetic permeability μ to decrease when the number of laminated layers was increased, even though the thickness of the magnetic material was the same.

これは、金属磁性材料の磁歪定数λSが完全に零になっ
ていないことを意味するが、又、SiO2の熱膨張係数
α(α:4X10−”/’C)に比べて一桁以上大きい
ことにも起因する。(金属磁性材料のα:110〜15
0xlO−7/℃)。
This means that the magnetostriction constant λS of the metallic magnetic material is not completely zero, but it is also one order of magnitude larger than the thermal expansion coefficient α (α: 4X10-”/'C) of SiO2. (α of metal magnetic material: 110-15
0xlO-7/°C).

又、金属磁性材料と眉間絶縁材料である5i02の積層
磁芯からなる磁気ヘッドを用いて、市販の塗布型メタル
テープによる各種環境下におけるテープ走行試験をした
所、特に低温環境下で磁気ヘッド出力の大きな低下が見
られた。
In addition, using a magnetic head made of a laminated magnetic core of metal magnetic material and 5i02, which is an insulating material between the eyebrows, we conducted tape running tests under various environments using a commercially available coated metal tape. A large decrease was observed.

この出力が低下した磁気ヘッドのテープ摺動面を観察し
たところ、層間絶縁材料であるSiO2付近に選択的に
付着物があり、その程度は段差計により測定したところ
、最大500〜600Aであった。この付着物をオージ
ェ分析により分析した所、付着成分はメタルテープ中の
磁性材料成分であり、段差計による値とオージェ分析に
よる深さが一致した。又程度は少ないがギャップ上にも
少し付着物が見られた。
When we observed the tape sliding surface of the magnetic head where the output had decreased, we found that there was selective deposits near the SiO2 interlayer insulating material, and the extent of this was measured using a step meter and found to be a maximum of 500 to 600 A. . When this deposit was analyzed by Auger analysis, it was found that the adhered component was a magnetic material component in the metal tape, and the value determined by the step meter and the depth determined by Auger analysis matched. In addition, some deposits were also observed on the gap, although to a lesser extent.

このように、塗布型メタルテープを低湿環境下で走行す
ると、金属磁性材料を用いた磁気ヘッドの層間絶縁材料
であるSiO2付近に、選択的にメタルテープ中の磁性
材料が付着し、この付着物により、ヘッドとテープ間に
隙間が生じ、よってスペーシングロスにより、ヘッド出
力が低下することが分かった。
As described above, when a coated metal tape is run in a low humidity environment, the magnetic material in the metal tape selectively adheres to the vicinity of SiO2, which is the interlayer insulating material of the magnetic head using a metal magnetic material, and this adhered material It was found that a gap was created between the head and the tape, resulting in a spacing loss and a decrease in head output.

課題を解決するための手段 多層構造の磁性体から成る磁気ヘッドにおいて、前記多
層構造の眉間絶縁材を、アルミニュウム及びシリコンの
酸化物を主成分とし、このアルミニュウム及びシリコン
の酸化物が、クリストバライトとムライト双方の結晶相
を同時に含有するように構成する。
Means for Solving the Problems In a magnetic head made of a magnetic material with a multilayer structure, the glabella insulating material of the multilayer structure is mainly composed of oxides of aluminum and silicon, and the oxides of aluminum and silicon are composed of cristobalite and mullite. It is configured to contain both crystal phases at the same time.

作用 本発明は、上記構成により、眉間絶縁材料の熱膨張係数
がSiO2やAl2O3に比べて、−桁以上大きく、よ
り金属磁性材料の熱膨張係数に近くなるので、特に積層
枚数が多くなった時の磁性材料材料に対する応力の影響
が少なくなり、磁気ヘッド特性の劣化が少なくなる。
Effects of the present invention With the above configuration, the coefficient of thermal expansion of the glabella insulating material is greater than that of SiO2 or Al2O3 by more than an order of magnitude, and is closer to the coefficient of thermal expansion of the metal magnetic material. The influence of stress on the magnetic material is reduced, and deterioration of magnetic head characteristics is reduced.

又、シリコンの酸化物をSiO2単体の形で使用せず、
ムライト(2A1203・3SiOz)として使用する
ことにより、磁気テープからの磁性粉の層間絶縁材への
付着も減少する。
In addition, silicon oxide is not used in the form of SiO2 alone,
By using it as mullite (2A1203.3SiOz), the adhesion of magnetic powder from the magnetic tape to the interlayer insulation material is also reduced.

実施例 本発明の一実施例を第1図、第2図を用いて説明する。Example An embodiment of the present invention will be described with reference to FIGS. 1 and 2.

市販の基板材料を鏡面研摩し、充分洗浄して基板1とし
て、真空槽内を3X10−7Torrに排気した後、A
rガスを導入して2X 10−3Torrとし、組成式
CoaINbz3Zrsのターゲットを用いてスパッタ
して10μmの非晶質合金膜2aを作製した。
A commercially available substrate material was polished to a mirror surface, thoroughly cleaned, and used as substrate 1. After evacuating the inside of the vacuum chamber to 3X10-7 Torr,
An amorphous alloy film 2a having a thickness of 10 μm was produced by introducing r gas to a pressure of 2×10 −3 Torr and sputtering using a target having a compositional formula of CoaINbz3Zrs.

次に、アルミナ(A 1203)とシリカ(Si02)
の含有比(重量%)が40/60の組成の粉末を130
0℃で仮焼し、ボールミルで粉砕、乾燥、造粒、成形し
、1450〜1500℃で焼成し、ターゲットを作製し
た。このターゲットをX−線により解析したところ、ム
ライトとクリストバライトの結晶構造が共存していた。
Next, alumina (A 1203) and silica (Si02)
Powder with a composition of 40/60 in the content ratio (wt%) of 130
It was calcined at 0°C, pulverized with a ball mill, dried, granulated, molded, and fired at 1450 to 1500°C to produce a target. When this target was analyzed by X-rays, it was found that the crystal structures of mullite and cristobalite coexisted.

更にこのターゲットの熱膨張係数αを測定したところ、
αは、115X 10−7/℃であった。次に、このタ
ーゲットを用いて、非晶質合金ll2a上にAr圧4X
10  ”Torrでスパッタして約1000Aの眉間
絶縁材料3aを作製した。尚、本発明のスパッタにより
形成された層間絶縁材料は、X−Mにより、ムライトと
クリストバライト双方が同時に存在するものであった。
Furthermore, when we measured the thermal expansion coefficient α of this target, we found that
α was 115×10−7/°C. Next, using this target, Ar pressure 4X was applied onto the amorphous alloy ll2a.
A glabellar insulating material 3a of about 1000 A was produced by sputtering at 10" Torr. Note that the interlayer insulating material formed by sputtering of the present invention contained both mullite and cristobalite at the same time due to X-M. .

以下同様に、非晶質合金膜と眉間絶縁材料を交互に2b
、3b、2cとスパッタし、非晶質合金膜が3層構造の
ブロックを得た。
Similarly, the amorphous alloy film and the glabella insulating material are alternately applied to 2b.
, 3b, and 2c to obtain a block having a three-layer structure of amorphous alloy films.

他方基板1と同じ材料の基板5を、接着用ガラス層4を
介して接着を行い積層コアを得た。
A substrate 5 made of the same material as the other substrate 1 was bonded via an adhesive glass layer 4 to obtain a laminated core.

次にギャップ突き合わせ面に巻線窓6を加工した後、突
き合わせ面をダイヤモンドペーストで鏡面に加工した後
、この面にギャップスペーサ−材を所定の厚みにスパッ
タして、ギャップ形成用の片側が完成する。
Next, after processing the winding window 6 on the gap abutting surface, the abutting surface is processed into a mirror surface with diamond paste, and then a gap spacer material is sputtered to a predetermined thickness on this surface, completing one side for gap formation. do.

このブロックと全(同じ構造1′〜5°からなる積層コ
ア半休を突き合わせ、接着用ガラス7により、ギャップ
形成を行った。
This block was abutted against a half-laminated core having the same structure of 1' to 5°, and a gap was formed using adhesive glass 7.

この一対の棒より所定のヘッドを切り出し磁気ヘッドを
完成した。
A predetermined head was cut out from this pair of rods to complete a magnetic head.

これらの磁気ヘッドをビデオテープレコーダーVTR(
ヘッド/テープ相対速度3.8m/秒)に取り付け、市
販の塗布型メタルテープを用いて各環境下におけるテー
プ走行試験をした所、従来のSiO2のみで眉間絶縁材
料もしくはギャップ材を構成した磁気ヘッドでは、低湿
環境下で磁気ヘッド出力の大幅な低下が見られたのにた
いして、本発明の材料を眉間絶縁又は、ギャップ材で構
成した磁気ヘッドでは、総ての環境下で安定した出力が
得られた。
These magnetic heads are used in video tape recorders (VTRs).
The head/tape relative speed was 3.8 m/sec), and tape running tests were conducted under various environments using a commercially available coated metal tape. In contrast to the fact that a significant drop in magnetic head output was observed in a low humidity environment, a magnetic head made of the material of the present invention as a glabellar insulator or a gap material could provide stable output in all environments. Ta.

第−表に23℃、10%相対湿度下に於ける本発明のヘ
ッドと参考までに、従来の磁気ヘッドのヘッド出力を示
す。尚、磁気ヘッド出力は、23℃、70%相対湿度下
の々ヘッド出力を0(dB)で示す。
Table 1 shows the head output of the head of the present invention and, for reference, a conventional magnetic head at 23 DEG C. and 10% relative humidity. Note that the magnetic head output is expressed as 0 (dB) at 23° C. and 70% relative humidity.

(以下余白) 第−表 比較のため、アルミナとシリカの同一組成の成。(Margin below) Table - Table For comparison, the same composition of alumina and silica was prepared.

形体を1300℃で焼成し、その結晶構造がムライト(
熱膨張係数α: 20X10−7/℃)からなるターゲ
ットを用いて作製した磁気ヘッドの出力を第−表に示す
。
The shape was fired at 1300℃, and its crystal structure became mullite (
Table 1 shows the output of a magnetic head manufactured using a target having a thermal expansion coefficient α: 20×10 −7 /° C.).

次に基板に非磁性ステンレスを用い、センダスト合金(
Fe84.5、Si9.7、A15.8各重量%)をタ
ーゲットとして、真空槽内を5×10  ”Torrに
排気した後、Arガスを導入して15X 10−3To
 r rとしてスパッタした。次に、ムライト/クリス
トバライトから構成される層間絶縁材料をターゲットと
して、センダスト膜上にAr圧4x10−2To r 
rでスパッタして約1000Aの居間絶縁材料の膜を形
成した。
Next, non-magnetic stainless steel was used for the substrate, and Sendust alloy (
Targeting Fe84.5, Si9.7, and A15.8% by weight, the inside of the vacuum chamber was evacuated to 5 x 10'' Torr, and then Ar gas was introduced to 15 x 10-3 Torr.
It was sputtered as r r. Next, using an interlayer insulating material composed of mullite/cristobalite as a target, an Ar pressure of 4x10-2 Torr was applied to the sendust film.
A film of about 1000 A of living room insulation material was formed by sputtering at r.

以下同様に、センダスト合金膜と層間絶縁材料を交互に
積層して、多層センダスト膜を作製した。こうして得ら
れた膜の、周波数100kHzに於ける外部磁場1m0
eでの透磁率を第二表に示す。尚、表中の透磁率は、磁
性材料の厚みに対して、即ち、層間絶縁材料は無視して
示しである。
Similarly, the sendust alloy film and the interlayer insulating material were alternately laminated to produce a multilayer sendust film. The film thus obtained was subjected to an external magnetic field of 1 m0 at a frequency of 100 kHz.
The magnetic permeability at e is shown in Table 2. In addition, the magnetic permeability in the table is shown with respect to the thickness of the magnetic material, that is, the interlayer insulating material is ignored.

第二表 尚、上記実施例では、ヘッドコアを基板で挟んだサンド
イッチ構造を有する磁気ヘッドについて述べたが、テー
プ摺動面に基板を含まない、即ち、テープ摺動面が総て
多層構造の磁性体からなる磁気ヘッドでも、同様の効果
を有するものである。
Table 2 In the above embodiment, a magnetic head having a sandwich structure in which a head core is sandwiched between substrates was described, but the tape sliding surface does not include a substrate, that is, the tape sliding surface is entirely made of a multilayer magnetic structure. A magnetic head made of a body also has similar effects.

又、磁性材料も非晶質合金、Co−Nb−Zr系につい
て述べたが他の系、例えばCo−Fe−3i−B、 N
i −3i−B系などについても、同様の効果ががあり
、スパッタ材料に限定されるものではな(、超急冷法に
よるリボンアモルファスや蒸着法等によっても可能であ
る。
In addition, as for magnetic materials, although the amorphous alloy Co-Nb-Zr system has been described, other systems such as Co-Fe-3i-B, N
A similar effect can be achieved with i-3i-B systems, and is not limited to sputtering materials (it is also possible to use ribbon amorphous materials using ultra-quenching methods, vapor deposition methods, etc.).

センダスト合金についても組成の限定は特にな(、Fe
−5i−A1合金組成で効果が有る。この事は、同様に
合金磁性材料であるパーマロイ(Fe−Ni系合金)に
ついても、特に磁歪に対する透磁率の影響が大きいので
同様の効果が期待出来る。
There are no particular compositional limitations for sendust alloys (, Fe
-5i-A1 alloy composition is effective. Similar effects can be expected for permalloy (Fe--Ni alloy), which is a magnetic alloy material, since magnetic permeability has a particularly large influence on magnetostriction.

発明の効果 本発明によれば、多層構造の磁性体からなる磁気ヘッド
において、眉間絶縁材料もしくはギャップ材料に、ムラ
イト及びクリストバライト双方の結晶相が共存するS 
i O2/ A I 20 sを主体とする材料を用い
ることで、従来材料より熱膨張係数が一桁以上太き(、
より金属磁性材料に近くなるので、特に、積層枚数が多
(なった時、もしくは、−層の厚みが薄くなった時の磁
性材料に対する応力の影響が少な(なり、磁気ヘッド特
性の劣化が少なくなる。
Effects of the Invention According to the present invention, in a magnetic head made of a multilayered magnetic material, the glabella insulating material or the gap material contains S in which crystal phases of both mullite and cristobalite coexist.
By using a material mainly composed of iO2/AI20s, the coefficient of thermal expansion is more than an order of magnitude larger than that of conventional materials (,
Since it is closer to a metallic magnetic material, the effect of stress on the magnetic material is reduced, especially when the number of laminated layers increases or when the layer thickness becomes thinner, resulting in less deterioration of magnetic head characteristics. Become.

又本発明では、層間絶縁材料もしくはギャップ材料に、
ムライト及びクリストバライト双方の結晶構造が共存す
るS i O2/ A 1203を主体とする材料を用
いることで、実用的に使用される幅広い環境下のテープ
走行に対して、テープ中の磁性材料成分の付着が少な(
なり、従って安定したヘッド出力が得られ、信頼性の高
い磁気ヘッドが供給出来る。
Further, in the present invention, the interlayer insulating material or the gap material,
By using a material mainly composed of SiO2/A 1203, in which the crystal structures of both mullite and cristobalite coexist, the adhesion of magnetic material components in the tape can be improved while the tape is running under a wide range of environments in which it is practically used. is small (
Therefore, stable head output can be obtained and a highly reliable magnetic head can be supplied.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、本発明の一実施例に於ける磁気ヘッドのテー
プ摺動面を示す正面図、第2図は、その側面図である。 1.1゛・・・・基板、2a、2a’・・・・非晶質合
金、3a、3a’・・・・絶縁材料、4.4゛・・・・
接着用ガラス層、5.5°・・・・基板、6・・・・巻
線窓、7・・・・接着用ガラス、8・・・・ギャップ。
FIG. 1 is a front view showing a tape sliding surface of a magnetic head in an embodiment of the present invention, and FIG. 2 is a side view thereof. 1.1゛...Substrate, 2a, 2a'...Amorphous alloy, 3a, 3a'...Insulating material, 4.4゛...
Adhesive glass layer, 5.5°...substrate, 6... winding window, 7... adhesive glass, 8... gap.

Claims (2)

【特許請求の範囲】[Claims] (1)多層構造の磁性体から成る磁気ヘッドにおいて、
前記多層構造の層間絶縁材が、アルミニュウム及びシリ
コンの酸化物を主成分とし、このアルミニュウム及びシ
リコンの酸化物が、クリストバライトとムライト双方の
結晶相を同時に含有することを特徴とする磁気ヘッド。
(1) In a magnetic head made of a multilayered magnetic material,
A magnetic head characterized in that the interlayer insulating material of the multilayer structure contains oxides of aluminum and silicon as main components, and the oxides of aluminum and silicon simultaneously contain crystal phases of both cristobalite and mullite.
(2)多層構造の磁性体が、非晶質合金、センダスト合
金、または、パーマロイ合金からなる請求項1記載の磁
気ヘッド。
(2) The magnetic head according to claim 1, wherein the multilayered magnetic material is made of an amorphous alloy, a sendust alloy, or a permalloy alloy.
JP63054206A 1988-03-08 1988-03-08 Magnetic head Pending JPH01227206A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63054206A JPH01227206A (en) 1988-03-08 1988-03-08 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63054206A JPH01227206A (en) 1988-03-08 1988-03-08 Magnetic head

Publications (1)

Publication Number Publication Date
JPH01227206A true JPH01227206A (en) 1989-09-11

Family

ID=12964078

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63054206A Pending JPH01227206A (en) 1988-03-08 1988-03-08 Magnetic head

Country Status (1)

Country Link
JP (1) JPH01227206A (en)

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