JPH053044B2 - - Google Patents

Info

Publication number
JPH053044B2
JPH053044B2 JP58012658A JP1265883A JPH053044B2 JP H053044 B2 JPH053044 B2 JP H053044B2 JP 58012658 A JP58012658 A JP 58012658A JP 1265883 A JP1265883 A JP 1265883A JP H053044 B2 JPH053044 B2 JP H053044B2
Authority
JP
Japan
Prior art keywords
recording
magnetic field
magneto
recording medium
optical
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 - Lifetime
Application number
JP58012658A
Other languages
Japanese (ja)
Other versions
JPS59140604A (en
Inventor
Takehiko Shibata
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP1265883A priority Critical patent/JPS59140604A/en
Publication of JPS59140604A publication Critical patent/JPS59140604A/en
Publication of JPH053044B2 publication Critical patent/JPH053044B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Description

【発明の詳細な説明】 技術分野 本発明は光ビームを用いて熱モード材料に情報
の記録を行う光磁気記録装置の記録方式に関し、
特に、一定角速度で記録媒体を回転させてその記
録を行う光磁気記録方法に関する。
Detailed Description of the Invention Technical Field The present invention relates to a recording method of a magneto-optical recording device that records information on a thermal mode material using a light beam.
In particular, the present invention relates to a magneto-optical recording method in which recording is performed by rotating a recording medium at a constant angular velocity.

従来技術 記録媒体を一定角速度で回転させて記録を行う
方式(C.A.V回転方式)による光磁気記録装置に
おいては、外周部トラツクと内周部トラツクとで
は単位面積当りの光エネルギ密度が大幅に異な
り、結果として、垂直磁化ピツトがレーザのオン
またはオフ信号に従つて忠実に形成されない。
Prior Art In a magneto-optical recording device that uses a method (CAV rotation method) in which recording is performed by rotating a recording medium at a constant angular velocity, the optical energy density per unit area is significantly different between the outer track and the inner track. As a result, perpendicular magnetization pits are not formed faithfully according to the laser on or off signal.

すなわち、第1図に示すように、C.A.V回転方
式では露光時間Δtに通過する露光面積が記録媒
体1の外周部から内周部に向けて小となるので、
外周部トラツクT1上のピツト記録面積ΔS1の
エネルギ密度は適当な補償を施さないと、内周部
トラツクT2上のピツト記録面積ΔS2のエネル
ギ密度に比して小さくなる。
That is, as shown in FIG. 1, in the CAV rotation method, the exposed area passing through the exposure time Δt becomes smaller from the outer circumference to the inner circumference of the recording medium 1.
The energy density of the pit recording area .DELTA.S1 on the outer track T1 will be smaller than the energy density of the pit recording area .DELTA.S2 on the inner track T2 unless appropriate compensation is provided.

そこで、従来、その解決法として、外周部トラ
ツクから、内周部トラツクに向けて記録レーザパ
ワーを漸減させて記録媒体に記録してゆくことに
よつて、外周部から内周部へ向けての記録ピツト
を補正する方式が提案されている。そして、この
ようなレーザパワーの制御を、一般に、レーザ光
をモニタして系にフイードバツク制御を施し、記
録媒体の半径方向の位置に応じて制御目標を調整
することによつて行つている。
Conventionally, the solution to this problem is to gradually reduce the recording laser power from the outer track to the inner track and record on the recording medium. A method for correcting recording pits has been proposed. Such laser power control is generally performed by monitoring the laser light, applying feedback control to the system, and adjusting the control target according to the radial position of the recording medium.

しかしながら、このような従来の光磁気記録装
置の記録方式においては、制御系の構成が複雑で
あるために装置自体が高価とならざるを得ず、特
に、レーザダイオードを用いた装置においては、
レーザダイオードの波長および変換効率の相違等
によつてフイードバツクゲインがそれぞれ異な
り、従つて、安定した制御を行うことができる装
置を廉価に提供できない問題点があつた。
However, in the recording method of such a conventional magneto-optical recording device, the configuration of the control system is complicated, so the device itself has to be expensive, especially in a device using a laser diode.
The feedback gain varies depending on the wavelength and conversion efficiency of the laser diode, and therefore, there is a problem in that it is not possible to provide a device that can perform stable control at a low cost.

目 的 本発明は、かかる従来の問題点に鑑みてなされ
たもので、その目的は、レーザパワーを変えるこ
となく、記録時に形成する補助磁界の強さを制御
することによつて、記録媒体の全面にわたつて安
定した記録を行えるようになした光磁気記録方法
を提供することにある。
Purpose The present invention was made in view of such conventional problems, and its purpose is to control the strength of the auxiliary magnetic field formed during recording without changing the laser power. It is an object of the present invention to provide a magneto-optical recording method that allows stable recording over the entire surface.

実施例 以下、図面を参照して本発明を詳細に説明す
る。
EXAMPLES Hereinafter, the present invention will be described in detail with reference to the drawings.

光磁気記録において、記録補助磁界は記録媒体
クに用いる光磁気材料によつては照射する光ビー
ムとともに記録ピツト形成にとつて重要な要素で
あり、例えば、GaTbFe、GaTbCoFe等の材料で
は記録ピツト面積は記録用補助磁界の強さに応じ
て変化する。
In magneto-optical recording, depending on the magneto-optical material used for the recording medium, the recording auxiliary magnetic field is an important element for forming recording pits along with the irradiated light beam.For example, for materials such as GaTbFe and GaTbCoFe, the recording pit area varies depending on the strength of the recording auxiliary magnetic field.

そこで、記録媒体外周部では光ビームのエネル
ギ密度の不足によるピツト形成面積の不足を記録
用補助磁界の強度を強くすることによつて補償
し、内周部に向けて磁界強度を漸減することによ
つて記録媒体全面にわたつて安定なピツト記録面
積を形成することができる。ここで、記録補助磁
界の強さが過大であると、光ビームとは関わりな
く垂直磁化が反転してしまうので、その磁界の強
度より使用する補助磁界の強度を十分小さくす
る。
Therefore, we compensated for the lack of pit formation area due to insufficient energy density of the light beam at the outer periphery of the recording medium by increasing the strength of the recording auxiliary magnetic field, and gradually decreased the magnetic field strength toward the inner periphery. Therefore, a stable pit recording area can be formed over the entire surface of the recording medium. Here, if the strength of the recording auxiliary magnetic field is excessive, the perpendicular magnetization will be reversed regardless of the light beam, so the strength of the auxiliary magnetic field used is made sufficiently smaller than the strength of the magnetic field.

第2図は本発明方法を実施する光磁気記録装置
の構成の一例を示し、ここで、1は記録媒体であ
り、基板1Aとその基板1A上に設けた光磁気薄
膜1Bとから成り、スピンドルモータ3によつて
一定角速度にて回転駆動される。4は光学記録ヘ
ツドであり、光磁気薄膜1Bと対向して配設し、
光磁気薄膜1Bに光ビームを照射する。5は記録
媒体1をはさんで光学記録ヘツド4とは反対側に
設ける補助磁界発生器であり、例えばDCコイル
を用いる。6は光学記録ヘツド4と補助磁界発生
器5とを一対として矢印で示す記録媒体1の半径
方向Rに移動させるモータである。7はヘツドア
クセスコントローラであり、光学記録ヘツド4お
よび補助磁界発生器5の位置制御を行う。また、
8は、例えば、コントローラ7の制御の下に補助
磁界発生器4を駆動して磁界の強さを切換えるプ
ログラム可能なDC可変電源である。
FIG. 2 shows an example of the configuration of a magneto-optical recording device for carrying out the method of the present invention, in which 1 is a recording medium, consisting of a substrate 1A and a magneto-optical thin film 1B provided on the substrate 1A, and a spindle. It is rotated by a motor 3 at a constant angular velocity. 4 is an optical recording head, which is disposed facing the magneto-optical thin film 1B;
A light beam is irradiated onto the magneto-optical thin film 1B. Reference numeral 5 designates an auxiliary magnetic field generator provided on the opposite side of the optical recording head 4 across the recording medium 1, and uses, for example, a DC coil. Reference numeral 6 denotes a motor that moves the optical recording head 4 and the auxiliary magnetic field generator 5 as a pair in the radial direction R of the recording medium 1 shown by the arrow. A head access controller 7 controls the positions of the optical recording head 4 and the auxiliary magnetic field generator 5. Also,
8 is a programmable DC variable power supply that drives the auxiliary magnetic field generator 4 to change the strength of the magnetic field under the control of the controller 7, for example.

かかる構成の光磁気記録装置において、その記
録動作を説明するに、まず、記録媒体1を一定角
速度で回転するようにスピンドルモータ3を起動
する。記録媒体1が設定した回転速度に達した
ら、ヘツドアクセスコントローラ7によりモータ
6を作動させて光学記録ヘツド4および補助磁界
発生器5を記録媒体1上の指定した記録トラツク
の位置へ向けて移動させる。同時に、ヘツドアク
セスコントローラ7は電源8に指令を与えて、補
助磁界発生器5の記録媒体1の半径方向上の位置
に応じた強さの磁界を発生させる。
To explain the recording operation of the magneto-optical recording device having such a configuration, first, the spindle motor 3 is activated so as to rotate the recording medium 1 at a constant angular velocity. When the recording medium 1 reaches the set rotational speed, the head access controller 7 operates the motor 6 to move the optical recording head 4 and the auxiliary magnetic field generator 5 toward the specified recording track position on the recording medium 1. . At the same time, the head access controller 7 gives a command to the power supply 8 to generate a magnetic field with a strength corresponding to the position of the auxiliary magnetic field generator 5 on the recording medium 1 in the radial direction.

すなわち、光学記録ヘツド4と補助磁界発生器
5とは記録媒体1を介して、記録媒体1の記録領
域上をR方向に一対として移動し、このとき補助
磁界発生器5は記録媒体1の半径方向上の位置に
応じてその磁界強度を変え、光学記録ヘツド4が
照射する記録光ビームと共働して、記録媒体1の
全面にわたつて安定したピツト記録を行う。
That is, the optical recording head 4 and the auxiliary magnetic field generator 5 move as a pair in the R direction on the recording area of the recording medium 1 via the recording medium 1, and at this time, the auxiliary magnetic field generator 5 moves along the radius of the recording medium 1. The magnetic field strength is changed according to the position in the direction, and in cooperation with the recording light beam irradiated by the optical recording head 4, stable pit recording is performed over the entire surface of the recording medium 1.

効 果 以上説明してきたように、本発明によれば、C.
A.V回転方式による光磁気記録装置において、記
録用補助磁界の強度を記録媒体の半径方向の外周
部から内周部に向けて漸減して記録してゆくよう
にしたので、記録媒体の全面にわたつて安定した
記録を行うことができる効果が得られる。
Effects As explained above, according to the present invention, C.
In a magneto-optical recording device using the AV rotation method, the strength of the auxiliary magnetic field for recording is gradually decreased from the outer circumference to the inner circumference in the radial direction of the recording medium. The effect is that stable recording can be performed.

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

第1図はC.A.V回転方式によつて光磁気記録を
行う際の記録媒体上の情報記録面積を説明する説
明図、第2図は本発明方法を実施する光磁気記録
装置の構成の一例を示すブロツク図である。 Δt……露光時間、T1,T2……トラツク、
ΔS1,ΔS2……ピツト記録面積、1……記録媒
体、1A……基板、1B……光磁気薄膜、3……
スピンドルモータ、4……光学ヘツド、5……補
助磁界発生器、6……モータ、7……ヘツドアク
セスコントローラ、8……電源。
Fig. 1 is an explanatory diagram illustrating the information recording area on a recording medium when magneto-optical recording is performed by the CAV rotation method, and Fig. 2 shows an example of the configuration of a magneto-optical recording device that implements the method of the present invention. It is a block diagram. Δt...exposure time, T1, T2...track,
ΔS1, ΔS2... Pit recording area, 1... Recording medium, 1A... Substrate, 1B... Magneto-optical thin film, 3...
Spindle motor, 4... Optical head, 5... Auxiliary magnetic field generator, 6... Motor, 7... Head access controller, 8... Power supply.

Claims (1)

【特許請求の範囲】 1 デイスク状記録媒体を等角速度で回転させ、
該記録媒体に磁界を印加しつつ一定強度の光ビー
ムを照射することによつて情報を光磁気的に記録
する光磁気記録方法において、 前記デイスク状記録媒体の外周部から内周部に
向つて、前記印加する磁界の強度を減少させるこ
とを特徴とする光磁気記録方法。
[Claims] 1. Rotating a disk-shaped recording medium at a constant angular velocity,
In a magneto-optical recording method in which information is recorded magneto-optically by irradiating a light beam of constant intensity while applying a magnetic field to the recording medium, . A magneto-optical recording method, characterized in that the intensity of the applied magnetic field is reduced.
JP1265883A 1983-01-31 1983-01-31 Recording system of photomagnetic recorder Granted JPS59140604A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1265883A JPS59140604A (en) 1983-01-31 1983-01-31 Recording system of photomagnetic recorder

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1265883A JPS59140604A (en) 1983-01-31 1983-01-31 Recording system of photomagnetic recorder

Publications (2)

Publication Number Publication Date
JPS59140604A JPS59140604A (en) 1984-08-13
JPH053044B2 true JPH053044B2 (en) 1993-01-13

Family

ID=11811454

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1265883A Granted JPS59140604A (en) 1983-01-31 1983-01-31 Recording system of photomagnetic recorder

Country Status (1)

Country Link
JP (1) JPS59140604A (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0687323B2 (en) * 1986-04-10 1994-11-02 キヤノン株式会社 Magneto-optical recording / reproducing device
JPH06150423A (en) * 1993-01-07 1994-05-31 Ricoh Co Ltd Magneto-optical recorder
JPH07262638A (en) * 1995-02-03 1995-10-13 Hitachi Ltd Magneto-optical disk device
US9394706B2 (en) 2013-10-08 2016-07-19 Simpson Strong-Tie Company, Inc. Concrete anchor
US9163655B2 (en) 2014-01-14 2015-10-20 Kaoru Taneichi Thrust nut

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5216208A (en) * 1975-07-29 1977-02-07 Mitsubishi Electric Corp Information recorder

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5216208A (en) * 1975-07-29 1977-02-07 Mitsubishi Electric Corp Information recorder

Also Published As

Publication number Publication date
JPS59140604A (en) 1984-08-13

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