JPH01191308A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPH01191308A JPH01191308A JP63013892A JP1389288A JPH01191308A JP H01191308 A JPH01191308 A JP H01191308A JP 63013892 A JP63013892 A JP 63013892A JP 1389288 A JP1389288 A JP 1389288A JP H01191308 A JPH01191308 A JP H01191308A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- superconductor
- thin film
- head
- 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
- 239000010409 thin film Substances 0.000 claims abstract description 21
- 239000002887 superconductor Substances 0.000 claims abstract description 20
- 229910052751 metal Inorganic materials 0.000 claims description 11
- 239000002184 metal Substances 0.000 claims description 11
- 229910000702 sendust Inorganic materials 0.000 claims description 4
- 229910000808 amorphous metal alloy Inorganic materials 0.000 claims description 3
- 239000000758 substrate Substances 0.000 abstract description 13
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 abstract description 7
- 230000000694 effects Effects 0.000 abstract description 7
- 230000004907 flux Effects 0.000 abstract description 7
- 239000011521 glass Substances 0.000 abstract description 6
- 229910052681 coesite Inorganic materials 0.000 abstract description 3
- 229910052906 cristobalite Inorganic materials 0.000 abstract description 3
- 239000010408 film Substances 0.000 abstract description 3
- 239000000377 silicon dioxide Substances 0.000 abstract description 3
- 235000012239 silicon dioxide Nutrition 0.000 abstract description 3
- 229910052682 stishovite Inorganic materials 0.000 abstract description 3
- 229910052905 tridymite Inorganic materials 0.000 abstract description 3
- 230000007423 decrease Effects 0.000 abstract description 2
- 230000003247 decreasing effect Effects 0.000 abstract 1
- 230000004927 fusion Effects 0.000 abstract 1
- 238000010030 laminating Methods 0.000 abstract 1
- 239000000463 material Substances 0.000 description 9
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 6
- 238000000034 method Methods 0.000 description 5
- 239000007788 liquid Substances 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 4
- 229910052757 nitrogen Inorganic materials 0.000 description 3
- 238000004804 winding Methods 0.000 description 3
- 239000000853 adhesive Substances 0.000 description 2
- 230000001070 adhesive effect Effects 0.000 description 2
- 229910045601 alloy Inorganic materials 0.000 description 2
- 239000000956 alloy Substances 0.000 description 2
- AYJRCSIUFZENHW-UHFFFAOYSA-L barium carbonate Chemical compound [Ba+2].[O-]C([O-])=O AYJRCSIUFZENHW-UHFFFAOYSA-L 0.000 description 2
- 238000009835 boiling Methods 0.000 description 2
- 239000010949 copper Substances 0.000 description 2
- 238000005520 cutting process Methods 0.000 description 2
- 238000010304 firing Methods 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 229910000859 α-Fe Inorganic materials 0.000 description 2
- 229910001020 Au alloy Inorganic materials 0.000 description 1
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910003271 Ni-Fe Inorganic materials 0.000 description 1
- 229910052788 barium Inorganic materials 0.000 description 1
- DSAJWYNOEDNPEQ-UHFFFAOYSA-N barium atom Chemical compound [Ba] DSAJWYNOEDNPEQ-UHFFFAOYSA-N 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000000748 compression moulding Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 238000007499 fusion processing Methods 0.000 description 1
- 239000003353 gold alloy Substances 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-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
- 238000003475 lamination Methods 0.000 description 1
- 229910001004 magnetic alloy Inorganic materials 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 239000011812 mixed powder Substances 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 229910000889 permalloy Inorganic materials 0.000 description 1
- 238000005498 polishing Methods 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 239000004576 sand Substances 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 239000007858 starting material Substances 0.000 description 1
- 229910052712 strontium Inorganic materials 0.000 description 1
- CIOAGBVUUVVLOB-UHFFFAOYSA-N strontium atom Chemical group [Sr] CIOAGBVUUVVLOB-UHFFFAOYSA-N 0.000 description 1
- 238000007738 vacuum evaporation Methods 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VTRまたは、デジタルオーディオ等に用いら
れる高保磁力の磁気記録媒体に高周波信号を記録するの
に好適な磁気ヘッドに関する。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magnetic head suitable for recording high frequency signals on a high coercive force magnetic recording medium used for VTRs, digital audio, and the like.
従来の技術
VTR,デジタルオーディオ等の高密度磁気記録再生装
置においては、磁気記録媒体の保磁力Hcを大きくすれ
ば、有利であることは良く知られているが、高保磁力の
磁気記録媒体に情報を記録するためには強い磁場が必要
になる。ところが現在磁気ヘッドに多用されているフェ
ライト材は、その飽和磁束密度が4000〜5000ガ
ウス程度であるため、得られる記録磁界の強さに限界が
あり、磁気記録媒体の保磁力が1000エルステツド程
度以上になると記録が不十分になるという欠点を有して
いる。Conventional Technology It is well known that it is advantageous to increase the coercive force Hc of a magnetic recording medium in high-density magnetic recording and reproducing devices such as VTRs and digital audio. A strong magnetic field is required to record. However, the ferrite material currently widely used in magnetic heads has a saturation magnetic flux density of about 4,000 to 5,000 Gauss, so there is a limit to the strength of the recording magnetic field that can be obtained, and the coercive force of the magnetic recording medium is about 1,000 Oe or more. This has the disadvantage that records are insufficient.
一方、金属磁性材料で総称されるFe−Aj!−St金
合金センダストと称される)、Ni−Fe合金(パーマ
ロイ)等の結晶質磁性合金、或は非晶質合金を用いた磁
気ヘッドは、一般にフェライト材より飽和磁束密度が高
く、かつ、摺動ノイズも少ないと言う優れた特徴を有す
るが、加工が難しく、歩留りが悪いためコストが高くな
るという欠点を有していた。On the other hand, Fe-Aj! is a generic name for metallic magnetic materials. Magnetic heads using crystalline magnetic alloys such as -St gold alloy sendust), Ni-Fe alloys (permalloy), or amorphous alloys generally have a higher saturation magnetic flux density than ferrite materials, and Although it has an excellent feature of low sliding noise, it has the drawbacks of being difficult to process and having a low yield, resulting in high costs.
特に、金属磁性薄膜を主コアとして用いる場合には、通
常これを適当な基板上に接着した後所定の厚さに研磨し
、同様の基板で金属磁性薄膜を挟み込むようにして接着
した後加工、ヘッド化される。In particular, when a metal magnetic thin film is used as the main core, it is usually bonded onto a suitable substrate, polished to a predetermined thickness, and then bonded between similar substrates to sandwich the metal magnetic thin film, and then processed. Becomes a head.
発明が解決しようとする課題
しかしながら、高密度記録においてはトラック幅は益々
狭くなる傾向にあり、それを規定する金属磁性薄膜の厚
さが薄くなると上記のような構造を有する磁気ヘッドの
効率が低下し所望の出力が得られなくなるという欠点を
有している。Problems to be Solved by the Invention However, in high-density recording, the track width tends to become narrower and narrower, and as the thickness of the metal magnetic thin film that defines it becomes thinner, the efficiency of the magnetic head with the above structure decreases. However, it has the disadvantage that the desired output cannot be obtained.
課題を解決するための手段
本発明は、上記課題について、基板として、超伝導体を
用いることにより解決を図ろうとするものである。基板
として超伝導体を用いることにより、磁気ヘッドの側面
は超伝導体によって覆われる構成となり、マイスナー効
果によって金属磁性薄膜が構成する磁路の側面の磁束の
漏洩を著しく減少させることができ、磁気ヘッドの効率
を著しく向上させることができる。Means for Solving the Problems The present invention attempts to solve the above problems by using a superconductor as a substrate. By using a superconductor as a substrate, the sides of the magnetic head are covered with the superconductor, and the Meissner effect can significantly reduce the leakage of magnetic flux on the sides of the magnetic path made up of the metal magnetic thin film. Head efficiency can be significantly improved.
作用
基板材として超伝導体を用いることにより金属磁性薄膜
を主コアとする高性能な磁気ヘッドの製造が容易となる
。By using a superconductor as a working substrate material, it becomes easy to manufacture a high-performance magnetic head whose main core is a metal magnetic thin film.
実施例
第1図は、本発明の構造を示す磁気ヘッドの斜視図であ
る。主コアである金属磁性薄膜1の両面を超伝導体2が
挟持する構造となっている。以下にこのヘッドの具体的
な製造方法を示す。Embodiment FIG. 1 is a perspective view of a magnetic head showing the structure of the present invention. It has a structure in which superconductors 2 sandwich both sides of a metal magnetic thin film 1, which is the main core. A specific method for manufacturing this head will be shown below.
実施例1
第2図に示すように、厚さ1flの超伝導体基板2の両
面にCOを主成分とするアモルファス合金薄膜lを厚さ
21μmにスパッタリングにより形成し、その上に保護
層として0.5〜1μmの厚さのS i O2膜(図面
では省略)を形成する。さらに、前記と同様の超伝導体
基板の両面に厚さ3μmのガラス層(図面では省略)を
形成したものを用意し、前者3枚、後者4枚(ただし、
外側に積層される基板にはガラス層は片側にのみ形成す
る)を交互に積層し、ガラス融着温度(500℃)にて
接着し積層ブロック3を得る。次に第3図の点線に示す
ように所定のアジマス角に応じて切断し、第4図に示す
コア半体対4.4°を得る。一方のコア、半体4に巻線
溝加工を施した後、コア半休4゜4゛の突合せ面を研磨
加工した後所定のギャップ長になるようギャップ材とし
てSiO2および接着ガラスの薄膜を形成し、電気炉中
にて加熱(500℃)、接着することによりギャップ形
成バー5を得る。その後破線に示すように積層ピッチに
応じて切断して第6図に示すスライスパー6を得、さら
に破線で示すように巻線溝ピッチに応じて切断すること
により第1図に示すようなヘッドチップが得られる。ヘ
ッドチップはベース板に接着されテープ摺動面の曲面加
工研磨、巻線等の工程を経て磁気ヘッドとして完成する
。Example 1 As shown in FIG. 2, an amorphous alloy thin film l containing CO as a main component was formed by sputtering on both sides of a superconductor substrate 2 with a thickness of 1 fl to a thickness of 21 μm. A SiO2 film (not shown in the drawing) with a thickness of .5 to 1 μm is formed. Furthermore, we prepared superconductor substrates similar to those described above with glass layers (omitted in the drawing) having a thickness of 3 μm formed on both sides, 3 of the former and 4 of the latter (however,
Glass layers are formed on only one side of the substrates to be laminated on the outside) are alternately laminated and bonded at a glass fusing temperature (500° C.) to obtain a laminated block 3. Next, it is cut according to a predetermined azimuth angle as shown by the dotted line in FIG. 3 to obtain a pair of core halves of 4.4° as shown in FIG. After winding grooves are formed on one of the cores and half body 4, the abutting surfaces of the core halves 4° and 4° are polished, and then a thin film of SiO2 and adhesive glass is formed as a gap material to obtain a predetermined gap length. The gap forming bar 5 is obtained by heating (500° C.) in an electric furnace and bonding. Thereafter, the slicer 6 shown in FIG. 6 is obtained by cutting according to the lamination pitch as shown by the broken line, and the head as shown in FIG. 1 is obtained by cutting according to the winding groove pitch as shown by the broken line. You get chips. The head chip is adhered to a base plate, and the magnetic head is completed through processes such as curved surface processing and polishing of the tape sliding surface, and winding.
以上のような工程において、主コアである金属磁性薄膜
の蒸着基板かつ保持材として超伝導体を用いるので、マ
イスナー効果によりヘッドの側面から漏洩する磁束を大
幅に減少させることができるためヘッド効率を向上させ
ることができるとともに、テープとの摺動において同効
果により適度な間隙を有するため偏摩耗の発生が少なく
良好な摺動面を維持し得る等価れた特徴を多く有してお
り、磁気特性が良好なヘッドを製造できる。In the process described above, a superconductor is used as the evaporation substrate and holding material for the metal magnetic thin film that is the main core, so the Meissner effect can significantly reduce the magnetic flux leaking from the sides of the head, thereby improving head efficiency. In addition, due to the same effect when sliding with the tape, it has an appropriate gap, so it has many equivalent features that can maintain a good sliding surface with less occurrence of uneven wear, and magnetic properties. can produce good heads.
実施例2
実施例1のアモルファス合金薄膜1の代わりに、超伝導
体基板2の両面に、センダスト薄膜を真空蒸着により2
1μmの厚さに形成する。その他は実施例1と同様の工
程でヘッドを作成することができる。本実施例の場合に
はセンダスト薄膜の耐熱性により、積層ブロック、ギャ
ップ形成バーを得る際の加熱温度は800℃程度が可能
であり、高い融着温度(800℃)の接着ガラスを用い
た。Example 2 Instead of the amorphous alloy thin film 1 of Example 1, two Sendust thin films were deposited on both sides of the superconductor substrate 2 by vacuum evaporation.
It is formed to a thickness of 1 μm. Otherwise, the head can be manufactured using the same steps as in Example 1. In the case of this example, due to the heat resistance of the sendust thin film, the heating temperature for obtaining the laminated block and the gap forming bar can be about 800°C, and adhesive glass with a high fusing temperature (800°C) was used.
こうして得られた磁気ヘッドの磁気特性、および摩耗特
性は、実施例1と同様に良好なものである。The magnetic properties and wear characteristics of the magnetic head thus obtained are as good as in Example 1.
なお、上記実施例中、超伝導体材料としては、たとえば
、いわゆる常温超伝導体を用いるか、または、超伝導臨
界温度が室温と液体窒素温度の沸点の間の材料を用いて
液体窒素で冷却するか(図示せず)、もしくは超伝導臨
界温度が液体窒素温度の沸点以下の材料を用いて液体ヘ
リウムで冷却するか(図示せず)をすればよい。常温超
伝導体の一例としては、組成としてストロンチウム(S
r)、バリウム(Ba)、 インドリウム(Y)およ
び銅(Cu)をそれぞれ1:1:1:3の比率で含有す
るセラミック酸化物がある。その製造方法の一例として
は、出発原料として5rCO’。In the above examples, as the superconductor material, for example, a so-called room temperature superconductor is used, or a material whose superconducting critical temperature is between room temperature and the boiling point of liquid nitrogen temperature is used and cooled with liquid nitrogen. (not shown), or cooled with liquid helium using a material whose superconducting critical temperature is below the boiling point of liquid nitrogen temperature (not shown). An example of a room-temperature superconductor is strontium (S) as a composition.
There are ceramic oxides containing barium (Ba), indium (Y) and copper (Cu) in a ratio of 1:1:1:3, respectively. As an example of its production method, 5rCO' is used as a starting material.
BaCO3,Y2O3,CuOのそれぞれの粉体を所定
量混合し、粉砕し、空気中において920℃で5時間焼
成する。この焼成、粉砕を3回操り返し、均質性を高め
る。このようにして処理した混合粉体を冷間圧縮成型し
た後、空気中において1000℃で5時間焼成し、徐冷
することにより製造する。Predetermined amounts of powders of BaCO3, Y2O3, and CuO are mixed, pulverized, and fired in air at 920° C. for 5 hours. This firing and crushing process is repeated three times to improve homogeneity. After cold compression molding the mixed powder treated in this way, it is produced by firing in air at 1000° C. for 5 hours and slowly cooling.
発明の効果
以上のように本発明は、主コアである金属磁性薄膜の蒸
着基板かつ保持材として超伝導体を用いることにより、
そのマイスナー効果によ砂ヘッドの側面から漏洩する磁
束を大幅に減少させることができるためヘッド効率を向
上させることができるとともに、テープとの摺動におい
て同効果により適度な間隙を有するため偏摩耗の発生が
少なく良好な摺動面を維持し得る等価れた特徴を多く有
しており、磁気特性が良好なヘッドを製造できる。Effects of the Invention As described above, the present invention uses a superconductor as the deposition substrate and holding material for the metal magnetic thin film that is the main core.
The Meissner effect can significantly reduce the magnetic flux leaking from the side of the sand head, improving head efficiency, and the same effect creates an appropriate gap when sliding with the tape, reducing uneven wear. It has many equivalent features that can maintain a good sliding surface with less generation, and a head with good magnetic properties can be manufactured.
第1図は本発明の磁気ヘッドの構造を示す斜視図、第2
図から第6図は本発明の実施例におけるヘッドの製造方
法を説明する説明図である。
1・・・・・・金属磁性薄膜、2・・・・・・超伝導体
、3・・・・・・積層ブロック、4,4°・・・・・・
コア半休対、5・・・・・・ギャソフ形成バー、6・・
・・・・スライスバー。
代理人の氏名 弁理士 中尾敏男 はか1名第1図
第2図
第3図
84図
11開平1−191308(4)FIG. 1 is a perspective view showing the structure of the magnetic head of the present invention, and FIG.
6 to 6 are explanatory diagrams illustrating a method of manufacturing a head in an embodiment of the present invention. 1...Metal magnetic thin film, 2...Superconductor, 3...Laminated block, 4,4°...
Core half-rest pair, 5...Gasoff formation bar, 6...
...Slice bar. Name of agent: Patent attorney Toshio Nakao (1 person) Figure 1 Figure 2 Figure 3 Figure 84 Figure 11 Kaihei 1-191308 (4)
Claims (2)
持してなる構造を有する磁気ヘッド。(1) A magnetic head having a structure in which both sides of a metal magnetic thin film, which is the main core, are sandwiched between superconductors.
スト薄膜であることを特徴とする特許請求の範囲第(1
)項記載の磁気ヘッド。(2) Claim No. 1, characterized in that the metal magnetic thin film is an amorphous alloy or a sendust thin film.
) The magnetic head described in section 2.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63013892A JPH01191308A (en) | 1988-01-25 | 1988-01-25 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63013892A JPH01191308A (en) | 1988-01-25 | 1988-01-25 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01191308A true JPH01191308A (en) | 1989-08-01 |
Family
ID=11845834
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63013892A Pending JPH01191308A (en) | 1988-01-25 | 1988-01-25 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01191308A (en) |
-
1988
- 1988-01-25 JP JP63013892A patent/JPH01191308A/en active Pending
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