JPS6292213A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPS6292213A
JPS6292213A JP23256385A JP23256385A JPS6292213A JP S6292213 A JPS6292213 A JP S6292213A JP 23256385 A JP23256385 A JP 23256385A JP 23256385 A JP23256385 A JP 23256385A JP S6292213 A JPS6292213 A JP S6292213A
Authority
JP
Japan
Prior art keywords
magnetic layer
magnetic
thickness
leading end
layer
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
JP23256385A
Other languages
Japanese (ja)
Inventor
Hiroshi Miyazawa
弘 宮沢
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson Corp
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 Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP23256385A priority Critical patent/JPS6292213A/en
Publication of JPS6292213A publication Critical patent/JPS6292213A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/31Structure or manufacture of heads, e.g. inductive using thin films
    • G11B5/3109Details
    • G11B5/3116Shaping of layers, poles or gaps for improving the form of the electrical signal transduced, e.g. for shielding, contour effect, equalizing, side flux fringing, cross talk reduction between heads or between heads and information tracks

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Magnetic Heads (AREA)

Abstract

PURPOSE:To intensify the recording magnetic field, enable high-density recording and carry out precise information recording by differentiating the film thicknesses of the lower magnetic layer and the upper magnetic layer in accordance with the distance from the leading end. CONSTITUTION:The film thickness of the leading end of the lower magnetic layer 1 of the magnetic head is regulated to t1 and the thickness of the part from a position l1 from the leading end to the terminal end is controlled to t2. The film thickness of the leading end part of the upper magnetic layer 2 is adjusted to t3 and the thickness of the part from a position l2 from the leading end to the terminal end is regulated to t4. A coil 3 consisting of a conductor layer and an interlayer insulating layer 4 for insulating the magnetic layer 1 from the magnetic layer 2 are formed between the magnetic layers 1 and 2. The film thicknesses t1 and t2 of the leading end parts of the respective magnetic films 1 and 2 are optimally determined in accordance with the recording wavelength. The film thicknesses t3 and t4 as described above are made as thick as possible in the range where the constraint conditions of the process are satisfied, thereby reducing the magnetoresistance of the magnetic head.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、磁気ヘッドの構造に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to the structure of a magnetic head.

〔発明の概要〕[Summary of the invention]

本発明は磁気ヘッドの構造において、下部磁性層上部磁
性層の各々の磁性層厚さを磁性層先端部分とそれ以外の
部々との厚さを変え、厚さの変わる位置の畢適値な決め
たことKより、書込効率再生効率の高い磁気へ9ドh;
得られる。
In the structure of a magnetic head, the present invention changes the thickness of each magnetic layer of the lower magnetic layer and the upper magnetic layer between the tip portion of the magnetic layer and the other portions, and adjusts the thickness to an appropriate value at the position where the thickness changes. From what I decided to do, I went to magnetism with high write efficiency and playback efficiency;
can get.

〔従来技術〕[Prior art]

従来の磁気ヘッド構造は、下部磁性層、上部磁性層とも
に各1層で構成する構造で磁性層の厚さが均一なものや
、磁性層の厚みが先端は近で薄くなって出来な絞り込む
と同じに磁気抵抗を下げるために先端付近以外では厚く
するように構成され  □たものや、下部磁性層、上部
磁性層を複数層積層構造と、プロセスにおいて下部磁性
層と上部磁性層との接合部分の段差の緩和を目的とし友
ものや上記のように磁性層の先端付近のみ薄くなるよう
に積層するといつ層構造がとられていた。
Conventional magnetic head structures have a structure in which both the bottom magnetic layer and the top magnetic layer are composed of one layer each, and the thickness of the magnetic layer is uniform, or the thickness of the magnetic layer is thinner near the tip. Similarly, in order to lower the magnetic resistance, the thickness is increased except near the tip, or the bottom magnetic layer and the top magnetic layer are multi-layered, and the junction between the bottom magnetic layer and the top magnetic layer is formed in the process. For the purpose of alleviating the step difference between magnetic layers, a layered structure was created in which the layers were stacked so that only the tip of the magnetic layer was thinner, as described above.

〔発明が解決しようとする問題点及び目的〕しかし前述
の従来技術では、上下各磁性層原人が均一なものでは、
記録波長により磁性層厚さが決められてしまう几め高密
度記録においては厚さが薄くなり磁気抵抗が高くなって
しまう。また磁性層1層で先端は近のみな薄くシ友もの
や複数層積層しtもので先端は近のみt薄<L7tもの
け記録再生する先端のみ薄くそれ以外の分部では厚い几
め磁気抵抗h;大きくならず上記問題点を解決している
。しかし厚さの変わる位置までの距離のとり方/l(大
きすぎれば記録再生時ともに磁性層が厚くなる部分まで
磁束がまわらずにまわりにもれてしまう。ま之逆に先端
まで近ずけすぎれば記録時に磁束は下部磁性層から上部
磁性層(ま几は上部磁性層から下部磁性層)に磁束がま
わってしまってギャップ部からの磁束が減ってしまうと
いつ九問題点を有する。そこで本発明けこのような問題
点を解決するもので、その目的とするところは、磁性層
の先端から淳さの変わるまでの距離の最適値を決めるこ
とにより効率の高い磁気へリド構造な提供するところK
ある。
[Problems and objects to be solved by the invention] However, in the above-mentioned prior art, if the upper and lower magnetic layers are uniform,
In precise high-density recording where the thickness of the magnetic layer is determined by the recording wavelength, the thickness becomes thinner and the magnetic resistance becomes higher. In addition, with a single magnetic layer, the tip is thin only at the near end, or a multi-layer laminated one, where the tip is thin only at the near end <L7t.Only the tip for recording and reproduction is thin, and the other parts are thick. h: The above problem is solved without becoming large. However, if the distance to the point where the thickness changes (l) is too large, the magnetic flux will not reach the thick part of the magnetic layer during recording and playback, but will leak around.On the other hand, if it is too close to the tip, For example, during recording, when the magnetic flux goes around from the lower magnetic layer to the upper magnetic layer (in other words, from the upper magnetic layer to the lower magnetic layer) and the magnetic flux from the gap decreases, this causes nine problems. This invention solves these problems, and its purpose is to provide a highly efficient magnetic helidic structure by determining the optimum distance from the tip of the magnetic layer to the point where the thickness changes. K
be.

〔問題点を解決する几めの手段〕[Elaborate means to solve problems]

本発明の磁気へ・ノドけ、上下各日性層の膜厚が不均一
の薄膜磁気ヘッドにおいて、磁性層先端から下部磁性層
の膜厚の変わる部分までの距離をtx上部磁性層の膜厚
の変わる部分までの距離を12とし之ときに以下の構成
要件ζ・・有することを時機とする。
Regarding the magnetism of the present invention, in a thin film magnetic head in which the thickness of the upper and lower magnetic layers is uneven, the distance from the tip of the magnetic layer to the part where the thickness of the lower magnetic layer changes is tx the thickness of the upper magnetic layer. When the distance to the changing part is 12, it is assumed that the following constituent requirements ζ... are satisfied.

α) 4μm≦t1≦15μm b)  1μm≦t2≦j Ottm 〔作用〕 本発明の上記構成によれば、磁性層先端部と先端部以外
の部分の膜厚を彎え、その寸度範囲を決め次ことにより
、磁気抵抗が小さく磁界のもhbz少なく書込時のギャ
ップ近傍の磁界強度の最適値1!It得られる。
α) 4 μm≦t1≦15 μm b) 1 μm≦t2≦j Ottm [Function] According to the above structure of the present invention, the thickness of the magnetic layer tip and the portion other than the tip is reduced and the dimensional range is determined. Due to the following, the magnetic resistance is small, the magnetic field is small, and the magnetic field strength near the gap during writing is the optimum value 1! It is obtained.

〔実施例〕〔Example〕

第1図は本発明の実施例の磁気ヘッドの断面図であり、
下部磁性層1け先端部膜厚t!であり、先端から距離7
+以降の膜厚はt2になるように構成されている。下部
磁性層2も同様に先端部の膜厚はt3であり先端からの
距離12以降の膜厚はt4になるように構成されている
。下部磁性層1と上部磁性層2にはさまれ九部分は導体
層から成るコイル3とコイル及び上下各日性層との絶縁
をとるためて層間絶I#膚から成り、磁気へノドを構成
している。
FIG. 1 is a cross-sectional view of a magnetic head according to an embodiment of the present invention.
The thickness of the tip of the lower magnetic layer 1 is t! and the distance from the tip is 7
The film thickness after + is configured to be t2. Similarly, the lower magnetic layer 2 has a thickness of t3 at the tip and a thickness of t4 at a distance of 12 and beyond from the tip. The nine parts sandwiched between the lower magnetic layer 1 and the upper magnetic layer 2 consist of a coil 3 made of a conductor layer and an interlayer I# skin to insulate the coil and the upper and lower magnetic layers, forming a magnetic node. are doing.

下部磁性層1の先端部膜厚tlと上部磁性層2の膜厚t
3は、記録波長によって最適値があり決められてしま5
゜磁性層先端以外の部分の膜厚is、i+はプロセスの
制約条件が許す範囲で厚くする方が磁気へノドの磁気抵
抗を下げる几め忙望ましい。第2図は、下部磁性層1の
膜厚がtlからhに変わる距離6と、下部磁性層2の膜
厚がムからムに変わる距7111i72を変化させt時
にギャップ部5から発生する磁束密度を示す図であり、
7け下部磁性Nj1+を変化させ次時の曲線であり、8
け上部磁性層12を変化させ次ときの曲線である。2+
が4μmから15μ常の時が一番強くなっている。tl
の距離が小さくなれば、上部磁性層1との間でもれてし
まってギャップ部5゛の宙乗密度bz減少してくる。ま
之1+が小さくなると第1図に示す上部磁性層の立上り
角度6が大きくなって上部−磁性層の形成が行ないにく
くなる几め、1+け望ましくけ6μm以上が良い。
Thickness tl of the tip of the lower magnetic layer 1 and thickness t of the upper magnetic layer 2
3 has an optimum value determined by the recording wavelength5.
゜It is desirable to increase the film thickness is, i+ of the portion other than the tip of the magnetic layer as thick as the process constraints allow in order to reduce the magnetic resistance at the magnetic node. Figure 2 shows the magnetic flux density generated from the gap portion 5 at time t when the distance 6 where the film thickness of the lower magnetic layer 1 changes from tl to h and the distance 7111i72 where the film thickness of the lower magnetic layer 2 changes from mu to mu. It is a diagram showing
The following curve is obtained by changing the lower magnetic field Nj1+ by 7 digits, and 8
This is a curve obtained when the upper magnetic layer 12 is changed. 2+
It is strongest when it is between 4μm and 15μm. tl
If the distance becomes smaller, leakage occurs between the upper magnetic layer 1 and the spacer density bz of the gap portion 5' decreases. If 1+ becomes smaller, the rising angle 6 of the upper magnetic layer shown in FIG. 1 becomes larger, making it difficult to form the upper magnetic layer.

逆にtlが大きくなりすぎればギャップ部からの磁束密
度が減るため15μm以下で更に望ましくは13μm以
下h以下良い。上部磁性層の距離t2と磁束密度の関係
は1μmから6μm才では磁束密度の変化量は少なく6
μm以上で低下のt「合h″−大きくなり、10μm以
上では約半分近くまで低下してしまうことより、 tz
の範囲は1μmから10μmの範囲h;良く特に良いの
け1μmから6μmの範囲である。
On the other hand, if tl becomes too large, the magnetic flux density from the gap portion decreases, so it is preferably 15 μm or less, more preferably 13 μm or less h. The relationship between the distance t2 of the upper magnetic layer and the magnetic flux density is that from 1 μm to 6 μm, the amount of change in magnetic flux density is small6
The decrease in t "total h" - becomes large at 10 μm or more, and decreases to nearly half at 10 μm or more, so tz
The range h is preferably from 1 μm to 10 μm; particularly preferably from 1 μm to 6 μm.

〔発明の効果〕〔Effect of the invention〕

以上述べたように本発明てよれば、下部磁性層と上部磁
性層のり厚を先端からの各々の距離の範囲?決めて不均
一膜厚とし定ことにより、記録憎界が強く発生し、高記
録密度が可能となり、安価で正確な情報記録b′−提供
できる。
As described above, according to the present invention, the thickness of the lower magnetic layer and the upper magnetic layer can be adjusted within the respective distance ranges from the tip. By determining the non-uniform film thickness, a strong recording boundary is generated, a high recording density is possible, and accurate information recording b'- can be provided at low cost.

【図面の簡単な説明】 第1図は本発明の磁気ヘッドな示す断面図。 第2図は磁性層の距離と発生磁束密度を示すグラフ。 1・・・・・・下部磁性層 2・・・・・・上部磁性層 3・・・・・・コイル 4・・・・・・層間絶縁層 5・・・・・・ギャップ部 6・・・・・・立上り角度 7・・・・・・下部磁性/?! 1+の変化と発生磁束
密度8・・・・・・上部磁性層12の変化と発生磁束密
度以  上
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a sectional view showing the magnetic head of the present invention. FIG. 2 is a graph showing the distance between magnetic layers and the generated magnetic flux density. 1...Lower magnetic layer 2...Top magnetic layer 3...Coil 4...Interlayer insulating layer 5...Gap portion 6... ...Rising angle 7...Lower magnetism/? ! Change in 1+ and generated magnetic flux density 8...Change in upper magnetic layer 12 and generated magnetic flux density or more

Claims (1)

【特許請求の範囲】 上下各磁性層の膜厚が不均一の薄膜磁気ヘッドにおいて
、磁性層先端から下部磁性層の膜厚の変わる部分までの
距離をl_1、上部磁性層の膜厚の変わる部分までの距
離をl_2としたときに、以下の構成要件を有すること
を特徴とする磁気ヘッド a)4μm≦l_1≦15μm b)1μm≦l_2≦10μm
[Claims] In a thin-film magnetic head in which the thickness of the upper and lower magnetic layers is non-uniform, the distance from the tip of the magnetic layer to the portion where the thickness of the lower magnetic layer changes is l_1, and the portion where the thickness of the upper magnetic layer changes is defined as l_1. A magnetic head characterized by having the following configuration requirements, where the distance to the top is l_2: a) 4 μm≦l_1≦15 μm b) 1 μm≦l_2≦10 μm
JP23256385A 1985-10-18 1985-10-18 Magnetic head Pending JPS6292213A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23256385A JPS6292213A (en) 1985-10-18 1985-10-18 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23256385A JPS6292213A (en) 1985-10-18 1985-10-18 Magnetic head

Publications (1)

Publication Number Publication Date
JPS6292213A true JPS6292213A (en) 1987-04-27

Family

ID=16941294

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23256385A Pending JPS6292213A (en) 1985-10-18 1985-10-18 Magnetic head

Country Status (1)

Country Link
JP (1) JPS6292213A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04146510A (en) * 1990-10-05 1992-05-20 Tdk Corp Magnetic head
US5195006A (en) * 1990-06-07 1993-03-16 Mitsubishi Denki Kabushiki Kaisha Thin-film magnetic head element having high recording/reproducing characteristics

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5195006A (en) * 1990-06-07 1993-03-16 Mitsubishi Denki Kabushiki Kaisha Thin-film magnetic head element having high recording/reproducing characteristics
JPH04146510A (en) * 1990-10-05 1992-05-20 Tdk Corp Magnetic head

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