JPH08235548A - Information reading and writing device - Google Patents

Information reading and writing device

Info

Publication number
JPH08235548A
JPH08235548A JP7041586A JP4158695A JPH08235548A JP H08235548 A JPH08235548 A JP H08235548A JP 7041586 A JP7041586 A JP 7041586A JP 4158695 A JP4158695 A JP 4158695A JP H08235548 A JPH08235548 A JP H08235548A
Authority
JP
Japan
Prior art keywords
recording
reproducing
magnetic
medium
center
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
JP7041586A
Other languages
Japanese (ja)
Inventor
Naoki Koyama
直樹 小山
Naoki Kodama
直樹 兒玉
Norifumi Miyamoto
詔文 宮本
Hisayasu Honma
久康 本間
Mitsuo Suda
三雄 須田
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP7041586A priority Critical patent/JPH08235548A/en
Publication of JPH08235548A publication Critical patent/JPH08235548A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE: To shorten the time together with the switching of a recording operation and reproducing operation by optimizing the arrangement of recording elements and reproducing elements from characteristics in terms of magnetic recording. CONSTITUTION: A magnetic reluctance effect element 31 is used as the reproducing element and is held by magnetic shielding layer 32, 33. Further, an induction type head 34 is laminated as the recording element. A lower magnetic pole is commonly used as an upper shielding layer 33 and an upper magnetic pole 36 is laminated via a gap layer 35 on the lower magnetic pole in the recording element. The geometrical center in the track width direction of the magnetic reluctance effect element 31 is the center of the spacing of electrodes 37 existing on both sides of the element. The geometrical center of the recording head is the center of the magnetic pole width of the upper magnetic head. Then, the spacing between the geometrical centers of the recording element and the reproducing element in the direction normal to a straight line connecting the axis of an actuator and the recording element is L0. The degradation in the throughput of the data based on the switching of the recording operation and the reproducing operation in the track is minimized in such a manner.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はディスクドライブの分野
に係り、特にデータトラック上での、記録素子および再
生素子の配置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the field of disk drives, and more particularly to the arrangement of recording elements and reproducing elements on data tracks.

【0002】[0002]

【従来の技術】磁気ディスクドライブ装置では回転式の
媒体と、回転軸を有するアクチュエータとこれに付随し
た再生素子と記録素子を含むスライダーからなる。ここ
で媒体上の所望のトラックにスライダーが移動する時
に、その軌跡はアクチュエータの軸と中心とした円弧を
描く。記録素子と再生素子はいずれかがある特定のトラ
ック上に配置されるとき、他方の素子はトラックから外
れる。一方の素子が外れる大きさは、トラックの半径の
関数として変動する。このトラックの不整合は、装置特
性に影響を与えるため、これを防止する方法として、同
一トラックで記録動作または再生動作から他方の動作に
切り替わるとき、記録素子または再生素子が所望のトラ
ック上に来るように再位置決めする方法が取られてい
る。この再位置決めに要する時間を短縮する解決策とし
て、ドライブにおけるトラックのすべてに対する再位置
決めの距離を最小になるように記録素子と再生素子を配
置する技術に関して、特開平4−232610号公報に
開示されている。本従来技術では、(1)個々のドライ
ブ製造時にいくつかのトラック位置で記録素子と再生素
子の位置ずれ量を測定して再位置決め量を求める。
(2)記録と再生の切り替えに伴うスライダーの移動距
離を最小にしてデータのスループットを向上するため
に、記録素子と再生素子の配置にオフセットを与える。
ことが開示されている。
2. Description of the Related Art A magnetic disk drive device comprises a rotary medium, an actuator having a rotary shaft, and a slider including a reproducing element and a recording element associated with the actuator. Here, when the slider moves to a desired track on the medium, its locus describes an arc centered on the axis of the actuator. When either the recording element or the reproducing element is placed on a particular track, the other element is off the track. The amount by which one element deviates varies as a function of track radius. This track misalignment affects the device characteristics, and as a method for preventing this, when the recording operation or the reproducing operation is switched to the other operation in the same track, the recording element or the reproducing element comes on the desired track. The repositioning method has been adopted. As a solution for shortening the time required for this repositioning, a technique for arranging a recording element and a reproducing element so that the repositioning distance with respect to all the tracks in a drive is minimized is disclosed in JP-A-4-232610. ing. In this prior art, (1) the repositioning amount is obtained by measuring the amount of positional deviation between the recording element and the reproducing element at several track positions during the manufacture of each drive.
(2) An offset is given to the arrangement of the recording element and the reproducing element in order to minimize the moving distance of the slider accompanying the switching between recording and reproduction and improve the data throughput.
It is disclosed.

【0003】しかしながら、最適オフセット量を求める
方法に関しては、幾何学的な配置からオフセット量を求
める技術が開示されているが、ヘッド媒体の特性を含め
た磁気記録的な観点からの技術は開示されていなかっ
た。
However, regarding the method for obtaining the optimum offset amount, a technique for obtaining the offset amount from a geometrical arrangement is disclosed, but a technique from the magnetic recording viewpoint including the characteristics of the head medium is disclosed. Didn't.

【0004】[0004]

【発明が解決しようとする課題】本発明では、記録動作
と再生動作の切り替えに伴う時間の短縮を図るために、
磁気記録的な特性から、記録素子と再生素子の配置の最
適化を図った情報読み取り・書き込み装置を提供するも
のである。
SUMMARY OF THE INVENTION In the present invention, in order to reduce the time required for switching between the recording operation and the reproducing operation,
It is intended to provide an information reading / writing device in which the arrangement of a recording element and a reproducing element is optimized from the characteristics of magnetic recording.

【0005】[0005]

【課題を解決するための手段】媒体の最内部において磁
気記録上の記録素子中心と再生素子中心の位置ずれを媒
体半径方向に射影した値と、媒体最外部において磁気記
録上の記録素子中心と再生素子中心の位置ずれ量を媒体
半径方向に射影した値とを等しくなるように記録素子と
再生素子とを配置する。
A value obtained by projecting a positional deviation between a recording element center and a reproducing element center on the magnetic recording in the innermost part of the medium in the radial direction of the medium and a recording element center on the magnetic recording in the outermost part of the medium. The recording element and the reproducing element are arranged so that the positional deviation amount of the reproducing element center becomes equal to the value projected in the radial direction of the medium.

【0006】[0006]

【作用】媒体の最内周部分と最外周部分における記録中
心と再生中心の磁気記録的な間隔と、また最外周部にお
ける記録中心と再生中心の磁気記録的な間隔とを媒体半
径方向に射影した距離が等しくなるように、記録ヘッド
と再生ヘッドを配置するので、媒体の最外周と最内周の
全範囲における記録素子と再生素子の位置合わせに必要
な再位置決めの平均的な距離が最小にでき、記録動作と
再生動作の切り替えに伴う時間の短縮を図ることができ
る。
The magnetic recording distance between the recording center and the reproduction center at the innermost and outermost peripheral portions of the medium and the magnetic recording distance between the recording center and the reproduction center at the outermost peripheral portion are projected in the radial direction of the medium. Since the recording head and the reproducing head are arranged so that the distances are equal, the average repositioning distance required for aligning the recording element and the reproducing element in the entire outermost and innermost areas of the medium is minimized. Therefore, it is possible to shorten the time required for switching the recording operation and the reproducing operation.

【0007】[0007]

【実施例】図1にディスクドライブの概略図を示す。こ
こでディスクドライブは回転中心11をもつ媒体10
と、回転軸13をもつロータリーアクチュエータ12
と、アクチュエータ先端に読み取り・書き込み素子をも
つヘッドスライダー14などの構成要素からなる。先端
のヘッドスライダーは回転軸13を中心として円弧を描
きながら媒体上の所望の記録トラック上に移動する。図
2は媒体上のヘッドの最内周位置21および最外周位置
22とヨー角の関係を示す。ここで最内周のヨー角をθ
1で示し、最外周のヨー角をθ2で示す。ヨー角はアク
チュエータの回転軸13からヘッド先端の記録素子又は
再生素子を結んだ直線と媒体運動方向の接線のなす角度
で定義される。ここで各位置におけるヨー角の値は媒体
回転中心11から媒体各位置の間の距離、即ち半径と、
媒体の回転中心と11アクチュエータの回転中心13と
の距離、そしてアクチュエータの回転軸とスライダー先
端の素子までの距離、これらの距離からヨー角は一義的
に決定される。
DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 shows a schematic diagram of a disk drive. Here, the disk drive is a medium 10 having a center of rotation 11.
And a rotary actuator 12 having a rotary shaft 13
And a head slider 14 having a read / write element at the tip of the actuator. The head slider at the tip moves on a desired recording track on the medium while drawing an arc around the rotation axis 13. FIG. 2 shows the relationship between the innermost peripheral position 21 and the outermost peripheral position 22 of the head on the medium and the yaw angle. Here, the yaw angle of the innermost circumference is θ
1 and the yaw angle of the outermost circumference is indicated by θ2. The yaw angle is defined as an angle formed by a tangent line in the medium movement direction and a straight line connecting the recording element or the reproducing element at the head tip from the rotary shaft 13 of the actuator. Here, the value of the yaw angle at each position is the distance between the medium rotation center 11 and each position of the medium, that is, the radius,
The yaw angle is uniquely determined from the distance between the rotation center of the medium and the rotation center 13 of the actuator 11, the distance between the rotation axis of the actuator and the element at the tip of the slider, and these distances.

【0008】図3はアクチュエータ先端にあるスライダ
ーの端部にある記録素子および再生素子を浮上面側から
見た図を示す。図の下方にアクチュエータの回転軸があ
ることになり、またスライダーは省略してある。同図に
おいて、再生素子として磁気抵抗効果素子31を用い、
これを磁気シールド層32、33で挾み、さらに記録素
子として誘導型ヘッド34を積層している。記録素子で
は、下部磁極は上部シールド層33と兼用しており、そ
のうえにギャップ層35を介して上部磁極36を積層し
ている。同図において磁気抵抗効果素子のトラック幅方
向の幾何学的中心は素子の両側にある電極37の間隔の
中心であり、記録ヘッドの幾何学的中心は、上部磁気ヘ
ッドの磁極幅の中心である。したがって本特許で規定し
たアクチュエータの軸と記録素子を結んだ直線の法線方
向の記録素子と再生素子の幾何学的中心の間隔は同図に
示すL0となる。また、再生素子の幾何学中心と磁気記
録的な中心のトラック幅方向の間隔はΔRとなる。磁気
記録的中心の求め方、および値については後で述べる。
また、アクチュエータの軸と記録素子を結んだ直線方向
の記録素子と再生素子の磁気記録的な間隔は図中のbの
ようになり、その値および求め方は後で示す。
FIG. 3 is a view of the recording element and the reproducing element at the end of the slider at the tip of the actuator as seen from the air bearing surface side. The rotary shaft of the actuator is located at the bottom of the figure, and the slider is omitted. In the figure, a magnetoresistive effect element 31 is used as a reproducing element,
This is sandwiched between the magnetic shield layers 32 and 33, and an inductive head 34 is further stacked as a recording element. In the recording element, the lower magnetic pole also serves as the upper shield layer 33, and the upper magnetic pole 36 is laminated on the upper shield layer 33 via the gap layer 35. In the figure, the geometric center of the magnetoresistive effect element in the track width direction is the center of the distance between the electrodes 37 on both sides of the element, and the geometric center of the recording head is the center of the magnetic pole width of the upper magnetic head. . Therefore, the distance between the geometric centers of the recording element and the reproducing element in the direction of the straight line connecting the axis of the actuator and the recording element defined in this patent is L0 shown in FIG. The distance between the geometric center of the reproducing element and the magnetic recording center in the track width direction is ΔR. The method of obtaining the magnetic recording center and the value will be described later.
Further, the magnetic recording distance between the recording element and the reproducing element in the linear direction connecting the axis of the actuator and the recording element is as shown by b in the figure, and its value and the method of obtaining it will be described later.

【0009】ここで図3のような形状を持つヘッドが、
ヨー角θをもって図2のディスク上にあるとき記録素子
と再生素子の磁気記録的な位置ずれ量は次の式で表され
る。
Here, a head having a shape as shown in FIG.
When the yaw angle θ is present on the disc of FIG. 2, the amount of magnetic recording misalignment between the recording element and the reproducing element is expressed by the following equation.

【0010】[0010]

【数1】(L0+ΔR)cosθ−bsinθ または## EQU1 ## (L 0 + ΔR) cos θ−bsin θ or

【0011】[0011]

【数2】(L0−ΔR)cosθ−bsinθ ここで数1と数2の違いは、ΔRの符号である。再生素
子の幾何学中心と磁気記録的な中心のトラック幅方向の
間隔ΔRは、磁気抵抗効果素子の磁化の方向や出力検出
用の電流を流す方向によって系統的に方向が変わるため
である。この記録と再生の位置ずれを最内周から最外周
の全面にわたって最小限にすることによって、記録動作
と再生動作の切り替えに伴うヘッド移動の時間を短縮で
きる。このためには最内周と最外周での位置ずれ量を同
じ値にし、ずれ方向が逆になるようにL0を求めること
によって実現できる。即ち、中周位置における位置ずれ
量がゼロになるようにL0を設定することによって実現
できる。これを次式に示す。
Difference Equation 2] of (L 0 -ΔR) cosθ-bsinθ where the number 1 and number 2 is the sign of [Delta] R. This is because the distance ΔR between the geometric center of the reproducing element and the magnetic recording center in the track width direction systematically changes depending on the direction of magnetization of the magnetoresistive effect element and the direction of the current for output detection. By minimizing the positional deviation between recording and reproduction over the entire surface from the innermost circumference to the outermost circumference, it is possible to shorten the time required to move the head when switching between the recording operation and the reproducing operation. This can be realized by setting the same amount of positional deviation between the innermost circumference and the outermost circumference and obtaining L0 so that the deviation directions are opposite. That is, it can be realized by setting L0 so that the amount of displacement at the middle position is zero. This is shown in the following equation.

【0012】[0012]

【数3】(L0+ΔR)cosθ1−bsinθ1=bsinθ2−(L
0+ΔR)cosθ2 または
## EQU3 ## (L 0 + ΔR) cos θ1−bsin θ1 = bsin θ2− (L
0 + ΔR) cos θ2 or

【0013】[0013]

【数4】(L0−ΔR)cosθ1−bsinθ1=とbsinθ2−
(L0−ΔR)cosθ2 ここで、bの値、即ち、アクチュエータの軸と記録素子
を結んだ直線方向の記録素子と再生素子の磁気記録的な
間隔は以下のようにして求める。記録後再生を行ない、
記録素子と再生素子のトラック幅方向の磁気記録的なず
れ量をヨー角を変えながら測定し、ずれ量のヨー角依存
性を評価する。ここで磁気記録的なずれ量はヘッドをオ
フトラックさせて得た出力のオフトラック分布におい
て、出力のピークと記録の中心位置との差である。ずれ
量のヨー角依存性において、ヨー角の正接に対するずれ
量の変化の傾きが記録素子と再生素子の磁気記録的な間
隔bの値となる。
(4) (L 0 −ΔR) cos θ1−bsin θ1 = and bsin θ2−
(L 0 −ΔR) cos θ 2 Here, the value of b, that is, the magnetic recording interval between the recording element and the reproducing element in the linear direction connecting the axis of the actuator and the recording element is determined as follows. Play back after recording,
The amount of magnetic recording deviation between the recording element and the reproducing element in the track width direction is measured while changing the yaw angle, and the yaw angle dependence of the deviation amount is evaluated. Here, the magnetic recording deviation amount is the difference between the output peak and the recording center position in the output off-track distribution obtained by off-tracking the head. In the yaw angle dependence of the shift amount, the slope of the change in the shift amount with respect to the tangent of the yaw angle becomes the value of the magnetic recording distance b between the recording element and the reproducing element.

【0014】幾何学的に記録素子と再生素子の間隔が異
なるヘッド(約2.0μm〜5.0μm)を用い、媒体
保磁力(2200 Oe〜3500 Oe)および浮上量
(媒体磁性膜とヘッド素子面との間隔:40nm〜80
nm)を変えて、ヨー角をパラメータにオフトラック出
力分布を求めて磁気記録的間隔bの値を測定したとこ
ろ、いずれも磁気抵抗効果素子から上部磁極のギャップ
面側までの幾何学寸法と寸法測定精度(±0.1μm)
内でほぼ同等であった。したがって、アクチュエータの
軸と記録素子を結んだ直線方向の記録素子と再生素子の
磁気記録的な間隔bは、磁気抵抗効果素子から上部磁極
のギャップ面側までの幾何学寸法に対応することがわか
った。
A head (about 2.0 μm to 5.0 μm) having a geometrically different distance between the recording element and the reproducing element is used, and the medium coercive force (2200 Oe to 3500 Oe) and the flying height (medium magnetic film and head element). Distance from surface: 40 nm to 80
nm), the off-track output distribution was obtained using the yaw angle as a parameter, and the value of the magnetic recording distance b was measured. In both cases, the geometrical dimensions and dimensions from the magnetoresistive effect element to the gap surface side of the upper magnetic pole were measured. Measurement accuracy (± 0.1 μm)
It was almost the same within. Therefore, it is found that the magnetic recording distance b between the recording element and the reproducing element in the linear direction connecting the axis of the actuator and the recording element corresponds to the geometrical dimension from the magnetoresistive effect element to the gap surface side of the upper magnetic pole. It was

【0015】次に、再生素子の幾何学中心と磁気記録的
な中心のトラック幅方向の間隔ΔRに関して検討した。
すでに磁気抵抗効果素子を用いたヘッドでは、再生感度
の中心と幾何学的中心がずれる場合があることは知られ
ている。本発明では磁気抵抗効果素子の信号磁界侵入方
向の幅(以下素子高さと記す。)と、ΔRの関係を実験
的に明らかにした。幾何学的なトラック幅を3μmに固
定して、0.8μmから5.0μmまで素子高さを変え
てΔRを評価した。素子高さの増加に伴ってΔRは増加
するがある一定値で飽和する傾向が見られる。ΔRの増
加の勾配は素子高さのおおよそ1/4である。また飽和
する素子高さの値は測定するときの信号磁界の記録密度
に依存する傾向が見られ、記録密度が高くなるとΔRが
飽和する素子高さが小さくなり、逆に記録密度が低くな
るとΔRが飽和する素子高さが大きくなる。この記録密
度と飽和する素子高さの関係は、おおよそ、信号の侵入
深さと一致する。
Next, the distance ΔR between the geometric center of the reproducing element and the magnetic recording center in the track width direction was examined.
It is already known that in a head using a magnetoresistive effect element, the center of reproduction sensitivity may deviate from the geometric center. In the present invention, the relationship between the width of the magnetoresistive effect element in the signal magnetic field penetration direction (hereinafter referred to as element height) and ΔR was clarified experimentally. The geometric track width was fixed at 3 μm, and the device height was changed from 0.8 μm to 5.0 μm to evaluate ΔR. It can be seen that ΔR increases as the element height increases, and that ΔR tends to saturate at a certain value. The slope of the increase in ΔR is approximately 1/4 of the element height. Also, the value of the element height that saturates tends to depend on the recording density of the signal magnetic field at the time of measurement. When the recording density increases, ΔR saturates the element height decreases, and conversely when the recording density decreases, ΔR decreases. The element height at which is saturated becomes large. The relationship between the recording density and the height of the element that saturates approximately corresponds to the penetration depth of the signal.

【0016】磁気抵抗効果素子を高効率で動作させるに
は、素子高さを信号磁界侵入深さと同程度にすることが
好ましいことが一般に知られている。従って、記録密度
に応じて適切な動作をさせるためには、素子高さを磁界
侵入深さと同等にする必要があり、こうすると上で述べ
たΔRの値は飽和が生じる前になるので、ΔRは素子高
さの約1/4に比例することになる。
It is generally known that in order to operate the magnetoresistive effect element with high efficiency, it is preferable to make the element height approximately equal to the signal magnetic field penetration depth. Therefore, in order to perform an appropriate operation according to the recording density, it is necessary to make the element height equal to the magnetic field penetration depth. If this is done, the value of ΔR described above is before saturation occurs. Is proportional to about 1/4 of the element height.

【0017】次にディスクドライブ内の1枚の媒体を挾
んで上下2つのヘッドの組み合わせた場合について述べ
る。上下2つのヘッドは向き合ってアクチュエータの回
転軸を中心に同時に動くので、ウエーハ基盤上にヘッド
を作製するときには、上下のヘッドで磁気記録的な記録
素子中心と再生素子中心は線対称の関係にする必要があ
る。一方、再生素子における幾何学的中心と磁気記録的
な中心のずれΔRは、素子の成膜条件や作成後の磁界印
加処理などが同じであれば同一の方向にずれる。上下の
スライダーによって作製条件や磁界印加処理方法を変え
て、逆方向にΔRをずらせることは不可能ではないが、
プロセスが煩雑になり、またその再現性を確保するため
にはプロセス精度を上げる必要があり複雑になる。この
ため、上下のヘッドを同一成膜条件や同一磁界処理で作
成するためには、予め上下のヘッド用として記録素子と
再生素子の幾何学的中心の間隔L0の異なるヘッドを準
備し、これらを組み合わせて上下1組のヘッドを作製す
る必要がある。このためには、どちらか一方のヘッドの
幾何学的間隔L0にΔRを加えた値と、他方のヘッドの
幾何学的間隔L0にΔRを加えた値との符号が逆で、絶
対値が概ね等しくなるように記録素子と再生素子を配置
する必要がある。これによって、上下のヘッドを組み合
わせた時に磁気記録的な記録素子中心と再生素子中心は
上下で合致し、アクチュエータの動きに対して記録再生
の中心は同時に変化するようになる。なお上記ではΔR
を加えた場合を述べたが、ΔRの符号を逆にとれば、幾
何学的間隔L0からΔRをひいた値の絶対値が等しく、
符号が逆になる場合もある。
Next, a case will be described in which one medium in the disk drive is sandwiched and two upper and lower heads are combined. Since the upper and lower two heads face each other and move simultaneously about the rotation axis of the actuator, when the heads are manufactured on the wafer substrate, the upper and lower heads have a magnetic recording-like recording element center and a reproducing element center in a line-symmetric relationship. There is a need. On the other hand, the deviation ΔR between the geometric center and the magnetically recording center in the reproducing element shifts in the same direction if the film forming conditions of the element and the magnetic field application process after formation are the same. It is not impossible to shift ΔR in the opposite direction by changing the manufacturing conditions and the magnetic field application method with the upper and lower sliders,
The process becomes complicated, and in order to ensure its reproducibility, it is necessary to improve the process accuracy and it becomes complicated. Therefore, in order to form the upper and lower heads under the same film forming conditions and the same magnetic field treatment, heads having different geometrical distances L0 between the recording element and the reproducing element are prepared in advance for the upper and lower heads. It is necessary to fabricate one set of heads by combining them. For this purpose, the sign of the value obtained by adding ΔR to the geometrical interval L0 of either one of the heads and the value obtained by adding ΔR to the geometrical interval L0 of the other head is opposite, and the absolute value is approximately the same. It is necessary to arrange the recording element and the reproducing element so that they are equal to each other. As a result, when the upper and lower heads are combined, the center of the recording element and the center of the reproducing element coincide with each other vertically, and the center of recording and reproduction changes simultaneously with the movement of the actuator. In the above, ΔR
However, if the sign of ΔR is reversed, the absolute value of the value obtained by subtracting ΔR from the geometrical interval L0 is equal,
The sign may be reversed.

【0018】以上の検討を元に、線記録密度が130k
BPIの条件における最適な記録素子と再生素子の配置
を求めた。最外周ヨー角が−20.5度、最内周ヨー角
が−2.4度で、磁気抵抗効果素子と誘導型素子流出端
側のギャップ内側の磁極端部との間隔が2.5μmの場
合、磁気抵抗効果素子の高さを1.6μmにすると、Δ
Rは約0.4μmで、記録素子と再生素子の幾何学的間
隔L0を約0.2μmにすると、最内周と最外周での磁
気記録的な記録素子と再生素子の間隔が等しくすること
ができた。これにより、媒体上の全有効エリア内の記録
動作と再生動作の切り替えに基づくデータの平均的なス
ループットの低下を最小にすることができた。
Based on the above examination, the linear recording density is 130 k.
The optimum arrangement of the recording element and the reproducing element under the BPI condition was obtained. The outermost circumference yaw angle is −20.5 degrees, the innermost circumference yaw angle is −2.4 degrees, and the gap between the magnetoresistive effect element and the magnetic pole end inside the gap on the outflow end side of the inductive element is 2.5 μm. In this case, if the height of the magnetoresistive effect element is set to 1.6 μm, Δ
When R is about 0.4 μm and the geometrical distance L0 between the recording element and the reproducing element is about 0.2 μm, the distance between the magnetic recording element and the reproducing element at the innermost circumference and the outermost circumference should be equal. I was able to. As a result, it is possible to minimize the decrease in the average data throughput due to the switching between the recording operation and the reproducing operation in the entire effective area on the medium.

【0019】また媒体の上下1組のヘッドの他方のヘッ
ドとしては、L0として−0.9μmとすることによ
り、上下のヘッドを組み合わせた時に磁気記録的な記録
素子中心と再生素子中心は上下で合致し、アクチュエー
タの動きに対して記録再生の中心は同時に変化するよう
にできた。
The other head of the pair of heads on the upper and lower sides of the medium is set to have L0 of −0.9 μm, so that when the upper and lower heads are combined, the center of the magnetic recording element and the center of the reproducing element are vertically arranged. In agreement, the center of recording and reproduction could be changed simultaneously with the movement of the actuator.

【0020】[0020]

【発明の効果】以上説明したように本発明によればトラ
ックにおける記録動作と再生動作の切り替えに基づくデ
ータのスループットの低下を最小にすることができる。
As described above, according to the present invention, it is possible to minimize the decrease in the data throughput due to the switching between the recording operation and the reproducing operation in the track.

【図面の簡単な説明】[Brief description of drawings]

【図1】ディスクドライブの概略図。FIG. 1 is a schematic diagram of a disk drive.

【図2】媒体上ヘッドの最内周位置および最外周位置と
ヨー角。
FIG. 2 shows the innermost and outermost positions of the head on the medium and the yaw angle.

【図3】記録素子および再生素子の浮上面側形状。FIG. 3 shows air bearing surface side shapes of a recording element and a reproducing element.

【符号の説明】[Explanation of symbols]

10…媒体、 11…回転中心、 1
2…アクチュエータ、13…回転軸、 14…
ヘッドスライダー、21…最内周位置、 22…最
外周位置、 31…再生素子、32…磁気シールド
層、 33…上部磁気シールド層兼下部磁極、34…記
録素子、 35…磁気ギャップ、 36…上部
磁極、37…電極。
10 ... Medium, 11 ... Center of rotation, 1
2 ... Actuator, 13 ... Rotation axis, 14 ...
Head slider, 21 ... innermost peripheral position, 22 ... outermost peripheral position, 31 ... reproducing element, 32 ... magnetic shield layer, 33 ... upper magnetic shield layer / lower magnetic pole, 34 ... recording element, 35 ... magnetic gap, 36 ... upper part Magnetic poles, 37 ... Electrodes.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 本間 久康 神奈川県小田原市国府津2880番地株式会社 日立製作所ストレージシステム事業部内 (72)発明者 須田 三雄 神奈川県小田原市国府津2880番地株式会社 日立製作所ストレージシステム事業部内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Hisayasu Honma 2880 Kozu, Odawara, Kanagawa Hitachi Storage Systems Division (72) Inventor Mio Suda 2880, Kozu, Odawara, Kanagawa Hitachi Storage Systems Business Department

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】回転式の媒体と軸の周りに回転するアクチ
ュエータと媒体にたいして情報を記録する素子と再生す
る素子とを備えた記録再生装置において、媒体の最内部
において磁気記録上の記録素子中心と再生素子中心の位
置ずれ量を媒体半径方向に射影した値と、媒体最外部に
おいて磁気記録上の記録素子中心と再生素子中心の位置
ずれ量を媒体半径方向に射影した値とを等しくなるよう
に記録素子と再生素子とを配置されていることを特徴と
する情報読み取り・書き込み装置。
1. A recording / reproducing apparatus provided with a rotary medium, an actuator rotating about an axis, an element for recording information on the medium, and an element for reproducing information, and a recording element center on magnetic recording at the innermost part of the medium. And the value obtained by projecting the positional deviation amount of the reproducing element center in the radial direction of the medium and the value obtained by projecting the positional deviation amount of the recording element center and the reproducing element center on the magnetic recording in the outermost part of the medium in the radial direction of the medium. An information reading / writing device, characterized in that a recording element and a reproducing element are arranged in the.
【請求項2】アクチュエータの回転軸と記録素子を結ぶ
直線と記録素子部における媒体運動方向接線のなす角度
をヨー角としたときに、媒体の最内部でのヨー角と最外
部でのヨー角をそれぞれθ1、θ2とし、アクチュエー
タの軸と記録素子を結んだ直線の法線方向の記録素子と
再生素子の幾何学的中心の間隔をL0とし、アクチュエ
ータの軸と記録素子を結んだ直線方向の記録素子と再生
素子の磁気記録的な間隔をbとし、再生素子の幾何学中
心と磁気記録的な中心のトラック幅方向の間隔をΔRと
したときに、(L0+ΔR)cosθ1−bsinθ1の値とbsin
θ2−(L0+ΔR)cosθ2の値が概ね等しいか、または
(L0−ΔR)cosθ1−bsinθ1の値とbsinθ2−(L0
ΔR)cosθ2の値が概ね等しいことを特徴とする情報読
み取り・書き込み装置。
2. A yaw angle at the innermost part of the medium and a yaw angle at the outermost part of the medium when a yaw angle is defined by a straight line connecting the rotation axis of the actuator and the recording element and a tangent line of the medium movement direction in the recording element part. Let θ1 and θ2 respectively be the distance between the geometrical centers of the recording element and the reproducing element in the direction of the straight line connecting the axis of the actuator and the recording element, and let L0 be the linear direction connecting the axis of the actuator and the recording element. The value of (L 0 + ΔR) cos θ1−bsin θ1 where b is the magnetic recording distance between the recording element and the reproducing element and ΔR is the distance between the geometric center of the reproducing element and the magnetic recording center. And bsin
The values of θ 2 − (L 0 + ΔR) cos θ 2 are substantially equal, or the values of (L 0 −ΔR) cos θ 1 −bsin θ 1 and bsin θ 2 − (L 0
An information reading / writing device characterized in that the values of ΔR) cos θ2 are substantially equal.
【請求項3】媒体を挾んで対応する記録素子および再生
素子をふくむ1組の磁気ヘッドにおいて、どちらか一方
のヘッドの前記記載の各部の値において(L0+ΔR)
の値と他方のヘッドの(L0+ΔR)の値が概ね等しく
かつ符号が逆であるか、または一方のヘッドの(L0
ΔR)の値と他方のヘッドの(L0−ΔR)の値が概ね
等しくかつ符号が逆であることを特徴とする請求項2記
載の情報読み取り・書き込み装置。
3. A set of magnetic heads including a corresponding recording element and reproducing element sandwiching a medium, wherein (L 0 + ΔR) in the value of each part of either head described above.
Of the other head and the value of (L 0 + ΔR) of the other head are substantially equal and opposite in sign, or (L 0 − of one head).
[Delta] R) of the value and the other head (L 0 - [Delta] R) value generally equal and code information reading and writing apparatus of claim 2, wherein the opposite.
【請求項4】前記再生素子が磁気抵抗効果素子とこれを
はさむ磁気シールド層からなり、前記記録素子が媒体抵
抗面にギャップを持つ誘導型素子からなるヘッドであっ
て、さらに前記アクチュエータの軸と記録素子を結んだ
直線方向の記録素子と再生素子の磁気記録的な間隔b
が、磁気抵抗効果素子と誘導型素子流出端側のギャップ
内側の磁極端部との間隔であることを特徴とする請求項
2ならびに3記載の情報読み取り・書き込み装置。
4. A head, wherein the reproducing element comprises a magnetoresistive effect element and a magnetic shield layer sandwiching the magnetoresistive effect element, and the recording element comprises an inductive type element having a gap on a medium resistance surface, further comprising an axis of the actuator. Magnetic recording distance b between the recording element and the reproducing element in the linear direction connecting the recording elements b
The information reading / writing apparatus according to claim 2 or 3, wherein is a distance between the magnetoresistive effect element and the magnetic pole end inside the gap on the outflow end side of the inductive element.
【請求項5】前記再生素子が磁気抵抗効果素子とこれを
はさむ磁気シールド層からなり、前記再生素子の幾何学
中心と磁気記録的な中心のトラック幅方向の間隔ΔR
が、磁気抵抗効果素子の信号磁界侵入方向の幅の約4分
の1であることを特徴とする請求項4記載の情報読み取
り・書き込み装置。
5. The reproducing element comprises a magnetoresistive effect element and a magnetic shield layer sandwiching the magnetoresistive effect element, and a distance ΔR between a geometric center of the reproducing element and a magnetic recording center in the track width direction.
5. The information reading / writing apparatus according to claim 4, wherein is about 1/4 of the width of the magnetoresistive effect element in the signal magnetic field penetration direction.
【請求項6】前記再生素子の信号磁界侵入方向の幅が2
μm未満であることを特徴とする請求項5記載の情報読
み取り・書き込み装置。
6. The width of the reproducing element in the signal magnetic field penetration direction is 2
The information reading / writing apparatus according to claim 5, wherein the information reading / writing apparatus has a thickness of less than μm.
JP7041586A 1995-03-01 1995-03-01 Information reading and writing device Pending JPH08235548A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7041586A JPH08235548A (en) 1995-03-01 1995-03-01 Information reading and writing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7041586A JPH08235548A (en) 1995-03-01 1995-03-01 Information reading and writing device

Publications (1)

Publication Number Publication Date
JPH08235548A true JPH08235548A (en) 1996-09-13

Family

ID=12612543

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7041586A Pending JPH08235548A (en) 1995-03-01 1995-03-01 Information reading and writing device

Country Status (1)

Country Link
JP (1) JPH08235548A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6456451B1 (en) 1997-12-25 2002-09-24 International Business Machines Corporation Method and apparatus for disk drive seek control

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6456451B1 (en) 1997-12-25 2002-09-24 International Business Machines Corporation Method and apparatus for disk drive seek control
US6597530B2 (en) 1997-12-25 2003-07-22 International Business Machines Corporation Method and apparatus for disk drive seek control

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