JPS6150235A - System and apparatus for erasing and reproducing optomagnetic recording - Google Patents

System and apparatus for erasing and reproducing optomagnetic recording

Info

Publication number
JPS6150235A
JPS6150235A JP17109484A JP17109484A JPS6150235A JP S6150235 A JPS6150235 A JP S6150235A JP 17109484 A JP17109484 A JP 17109484A JP 17109484 A JP17109484 A JP 17109484A JP S6150235 A JPS6150235 A JP S6150235A
Authority
JP
Japan
Prior art keywords
recording
laser light
erasing
magnetic field
light source
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.)
Granted
Application number
JP17109484A
Other languages
Japanese (ja)
Other versions
JP2591729B2 (en
Inventor
Mitsuya Okada
満哉 岡田
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.)
NEC Corp
Original Assignee
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP59171094A priority Critical patent/JP2591729B2/en
Publication of JPS6150235A publication Critical patent/JPS6150235A/en
Application granted granted Critical
Publication of JP2591729B2 publication Critical patent/JP2591729B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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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
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B13/00Recording simultaneously or selectively by methods covered by different main groups among G11B3/00, G11B5/00, G11B7/00 and G11B9/00; Record carriers therefor not otherwise provided for; Reproducing therefrom not otherwise provided for
    • G11B13/04Recording simultaneously or selectively by methods covered by different main groups among G11B3/00, G11B5/00, G11B7/00 and G11B9/00; Record carriers therefor not otherwise provided for; Reproducing therefrom not otherwise provided for magnetically or by magnetisation and optically or by radiation, for changing or sensing optical properties
    • G11B13/045Recording simultaneously or selectively by methods covered by different main groups among G11B3/00, G11B5/00, G11B7/00 and G11B9/00; Record carriers therefor not otherwise provided for; Reproducing therefrom not otherwise provided for magnetically or by magnetisation and optically or by radiation, for changing or sensing optical properties combined recording by magnetic and optic means

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  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To attain rewrite of recording information with simple device constitution without switching application direction of an external magnetic field by changing an oscillated laser light intensity of a laser light source corresponding to recording/reproduction/erasure. CONSTITUTION:A laser light source modulating circuit 20 is used for the modulation of the laser light source 6 of an optical head 5 to modulate power of the laser light source 6 in matching with recording/reproduction/erasure. In desiring recording information recorded already on an optomagnetic disc 1, the power level of the laser light irradiated to a magnetic thin film 3 is adjusted to a power level PE at which the magnetizing direction of the already recorded part restores to the initial state. in recording the new signal information succeedingly, the adjustment is performed that the laser light power absorbed in the magnetic film 3 reaches a sufficient level PW to form the magnetization inverting part. A constant magnetic field is applied to the magnetic thin film 3 by a magnetic field generating means 12 in a series of erasure/recording processes as above and the field is not required to be changed throughout recording/reproduction/erasure.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明はレーザ光を用いて元磁気記分再生消去をおこな
う光磁気記録再生消去方式及びその装置に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a magneto-optical recording, reproducing and erasing method and apparatus for reproducing and erasing original magnetic recording using laser light.

(従来技術とその問題点〕 光記録方式、特に元ディスクメモリ方式は、高密度・大
容量記録が可能であり、かつ非接触・高速アクセスもで
きるという点から大容量ンアイルメモリの一つとして近
年注目を集めている。その中でも記e、媒体として〜I
nJ3i、  hincuBi、MnTiB1 。
(Prior art and its problems) Optical recording systems, especially original disk memory systems, have been used as a type of large-capacity alley memory because they enable high-density, large-capacity recording, as well as non-contact and high-speed access. It has been attracting attention in recent years.Among them, as a medium
nJ3i, hincuBi, MnTiB1.

MnAA!()eなどの結晶性磁性薄膜あるいはTb、
 Gd。
MnAA! ()e or other crystalline magnetic thin films or Tb,
Gd.

Dy・HOなどの希土類金属とPe、 Co、 Ni 
 などの遭移金門との組み合わせによって作成される非
晶質磁性薄膜を用いた光磁気ディスクメモリは、記録情
報の書き替えが可能であるという利点を持っていること
から、各所で盛んに研究されている。
Rare earth metals such as Dy/HO and Pe, Co, Ni
Magneto-optical disk memory using an amorphous magnetic thin film, which is created by combining it with a ferromagnet, has the advantage of being able to rewrite the recorded information, so it is being actively researched in various places. ing.

従来、公知の光磁気記録再生消去方式及び装置において
は、情報の記録・再生・消去に対してそれぞれ次のよう
な動作がとられる。
In conventionally known magneto-optical recording/reproducing/erasing systems and devices, the following operations are performed for recording, reproducing, and erasing information, respectively.

記録VcFi、レーザ光により発生する熱を利用する。Recording VcFi uses heat generated by laser light.

レーザ光ビームを1〜2μmψの微小スポットに絞り、
記録媒体に照射し、媒体温度を上昇させる。キューり温
度記録をおこなう場合には、記録媒体をキューり温度以
上に上昇させ、外部印加磁界あろ込は記録媒体の反磁界
によって反転磁区を形成する。補償温度記録をおこなう
場合には記録媒体の補償温度を室温付近に設定し、レー
ザ元ビーム照射によっである温度まで昇温させ、媒体の
保磁力低下全利用し、外部印加磁界によって反転磁区を
形成する前記手段により記録2値信号[JroJを記5
R:媒体の反転磁区の有無に対応しt形で記録できる。
Focus the laser beam to a minute spot of 1 to 2 μmψ,
The recording medium is irradiated to raise the medium temperature. When recording the temperature of the recording medium, the temperature of the recording medium is raised to a temperature above the temperature of the recording medium, and an externally applied magnetic field is used to form reversed magnetic domains due to the demagnetizing field of the recording medium. When performing compensated temperature recording, the compensation temperature of the recording medium is set near room temperature, the temperature is raised to a certain temperature by laser beam irradiation, the coercive force of the medium is fully utilized, and the reversed magnetic domain is created by an externally applied magnetic field. By the means for forming a recorded binary signal [JroJ
R: Can be recorded in a t-shape depending on the presence or absence of reversed magnetic domains in the medium.

再生は磁気光学効果(Kerr効果あるいはparad
By効果)を用いておこなわれる。すなわち記録媒体の
反転磁区の有無に対応して媒体からの反射光あるいけ透
過光の偏光面が回転するとと金利用し、記録媒体から情
報を読み出1゜記録媒体には記録時にくらべ低パワレベ
ルのレーザ光が照射され、その反射光または透過光から
信号を再生する。
Reproduction is based on the magneto-optical effect (Kerr effect or parad
By effect). In other words, when the plane of polarization of reflected light or transmitted light from the medium rotates in response to the presence or absence of reversed magnetic domains in the recording medium, information is read from the recording medium by utilizing the rotation of the plane of polarization. is irradiated with laser light, and a signal is reproduced from the reflected or transmitted light.

ここで、再生に用いるレーザ光の強度レベルは記録媒体
の磁化状態に変化を与えないレベルに設定される。
Here, the intensity level of the laser beam used for reproduction is set to a level that does not change the magnetization state of the recording medium.

記録情報を消去する場合には、外部磁界を記録時とは逆
極性に印加し、レーザ光ビームを記録時と同等の強度で
記録媒体に一様に照射する。外部磁界印加により記録媒
体の磁化状態は配分前の初期状態に戻る。
When erasing recorded information, an external magnetic field is applied with a polarity opposite to that during recording, and a laser beam is uniformly irradiated onto the recording medium with the same intensity as during recording. By applying an external magnetic field, the magnetization state of the recording medium returns to the initial state before distribution.

前記従来の元磁気記り再生消去方式及び装置において、
記録情報の書き替えをおこなうには、まず、既記録情報
を前記消去動作に従って消去し、次に新しい記録情報を
前記記録動作に従って記録するという二段階の操作をお
こなう。このとき、消去時と、記録時では記録媒体に印
加する外部磁界の方向が逆であるために、消去時、記録
時では外部印加磁界の方向を切り替える手段を設けなけ
ればならない。
In the conventional original magnetic recording reproducing erasing method and device,
To rewrite the recorded information, a two-step operation is performed: first, the previously recorded information is erased according to the erasing operation, and then new recorded information is recorded according to the recording operation. At this time, since the direction of the external magnetic field applied to the recording medium is opposite during erasing and recording, means must be provided to switch the direction of the externally applied magnetic field during erasing and recording.

たとえば、コイル(よって外部磁界を印加する場合、第
4図に示すように、光磁気ディスクIK対して記録、消
去を行なうに雌元ヘッド5からのレーザ光の記録動作と
消去動作に同期させて、コイル21に流す電流の向きを
コイル@流極性切替手段22によって切)替える方式か
知られている。
For example, when applying an external magnetic field to the coil (therefore, as shown in FIG. 4), recording and erasing is performed on the magneto-optical disk IK in synchronization with the recording and erasing operations of the laser beam from the female head 5. A method is known in which the direction of the current flowing through the coil 21 is switched by the coil @flow polarity switching means 22.

また、第5図〈示すように永久磁石23によって外部磁
界を印加する場合には、磁石駆動機構を用いる方式及び
装置が知られている(0開昭57−ように外部磁界の印
加方向は逆転する。いずれの方式及び装置においても装
置構成がaJAになるという欠点かちる。
Furthermore, when applying an external magnetic field using a permanent magnet 23 as shown in FIG. Both methods and devices have the disadvantage that the device configuration is aJA.

(発明の目的) 本発明の目的は、前記従来の光磁気記録再生消去方式及
び装置の欠点を解決し、外部磁界の印加方向を切り替え
ることなく、簡単な装置構成により、記録情報の誉き替
えが可能な新規な光磁気記録再生消去方式及び装WLを
提供することにある。
(Objective of the Invention) An object of the present invention is to solve the drawbacks of the conventional magneto-optical recording/erasing method and device, and to change the quality of recorded information using a simple device configuration without changing the direction of application of an external magnetic field. The object of the present invention is to provide a new magneto-optical recording/reproducing/erasing method and WL that can perform the following.

(発明の構成) 本発明(よれば、垂直磁気異方性を有する磁性薄膜を記
録媒体とし、レーザ光によって情報を記録・再生・消去
する光磁気記録再生消去方式であって、前記記録媒体に
照射するレーザ光の強度を変化させて情報を記録する記
録過程と、前記記録媒体に一定の強度のレーザ光を照射
して記録情報を再生する再生過程と、一定の強度のレー
ザ光を照射して記りに情報を消去する消去過程から成り
、記録再生消去過程とを通じて一定の磁界を外部から記
録媒体に印加することを特徴とする光侮気記録再生消去
方式が得られ、さらには記録媒体と、記録媒体に一定の
磁界を印加する磁界発生手段と、記録媒体にレーザ光を
照射する光ヘッドと、記録時、再生時、消去時に対応し
てレーザ光源の見損レーザ光強度を変化させるレーザ光
源変調用回路とを具備することを特徴とする光磁気記録
再生消去装置が得られる。
(Structure of the Invention) According to the present invention, there is provided a magneto-optical recording/reproducing/erasing method in which a magnetic thin film having perpendicular magnetic anisotropy is used as a recording medium, and information is recorded, reproduced, and erased using a laser beam. There is a recording process in which information is recorded by changing the intensity of the irradiated laser light, a reproduction process in which the recorded information is reproduced by irradiating the recording medium with a laser beam of a constant intensity, and a reproduction process in which the recorded information is reproduced by irradiating the recording medium with a laser beam of a constant intensity. An optical recording/reproducing/erasing method is obtained, which consists of an erasing process in which information is erased as described above, and a constant magnetic field is externally applied to the recording medium through the recording/reproducing/erasing process. , a magnetic field generating means that applies a constant magnetic field to the recording medium, an optical head that irradiates the recording medium with laser light, and a laser light source that changes the intensity of the lost laser light corresponding to the time of recording, reproduction, and erasing. A magneto-optical recording, reproducing and erasing device is obtained, which is characterized in that it is equipped with a laser light source modulation circuit.

(構成の詳細な説明) 本発明は上述の構成をとることにより、従来技術の問題
点全解決した。
(Detailed explanation of the structure) The present invention has solved all the problems of the prior art by adopting the above-mentioned structure.

以下、本発明の詳細について図面を用いて説明する。N
g1図は、本発明が適用された光磁気記録再生消去装置
の構成例を示したものである。第1図において光磁気デ
ィスク1は有機物樹脂基板あるいけガラス基板あるいは
金属基板より成る円板2の一方もしくは両面K、基板面
の垂直方向に磁化容易軸を有する磁性薄膜3を作成しt
ものである。
Hereinafter, details of the present invention will be explained using the drawings. N
Figure g1 shows an example of the configuration of a magneto-optical recording/reproducing/erasing device to which the present invention is applied. In FIG. 1, a magneto-optical disk 1 is formed by forming a magnetic thin film 3 having an axis of easy magnetization perpendicular to the substrate surface on one or both surfaces of a disk 2 made of an organic resin substrate, a glass substrate, or a metal substrate.
It is something.

前記母性薄膜3は、結晶性あるいは非晶質磁性薄膓であ
り、たとえば1MnB1. MnCuB1. MnTi
B1゜MnAlGeなどの結晶性磁性薄膜、あるいはS
m。
The mother thin film 3 is a crystalline or amorphous magnetic thin film, for example, 1MnB1. MnCuB1. MnTi
B1゜Crystalline magnetic thin film such as MnAlGe, or S
m.

Tb、 Gd、 Dy、 Ho  などの希土類金属と
F e + C0rNiなどの遷移金属との組み合わせ
によって作成される非晶質破性簿膜である。前記光磁気
ディス1     り1けディスク駆動用モータ4によ
って所定の速度で回転される。光へラド5は光母気記録
再生消去用の光学系、光検出機構を具備している。光ヘ
ッド5自体は、図中に矢印で示したように光磁気ディス
ク10半径方向に所定の速度によV移動可能である。
It is an amorphous fracture film created by a combination of rare earth metals such as Tb, Gd, Dy, and Ho and transition metals such as Fe + COrNi. The magneto-optical disk 1 is rotated at a predetermined speed by a single disk drive motor 4. The optical disc 5 is equipped with an optical system for reproducing and erasing optical recording, and a light detection mechanism. The optical head 5 itself is movable at a predetermined speed in the radial direction of the magneto-optical disk 10, as indicated by the arrow in the figure.

前記光ヘッド5において、6は直線偏光のレーザ光源で
あり、たとえば半導体レーザが使用される。7,8.9
はビームスプリッタである。
In the optical head 5, 6 is a linearly polarized laser light source, for example, a semiconductor laser is used. 7,8.9
is a beam splitter.

レーザ光ビーム集光用レンズ10はアクチュエータ11
により支持されている。磁界発生手段J2は光磁気ディ
スクを介してレーザ光ビームf%元用レンズと反対側も
しくは同じ側に設置され、永久磁石あるいけコイルと直
流電源の組み合わせが用いられる。フォーカスエラーな
らびにトラッキングエラー信号はそれぞれフォーカスエ
ラー検出用量v:IL子13、トラッキングエラー検出
用受光素子14によって検出されサーボ制御回路15.
16に入力され、サーボ信号となり、前記アクチーエー
タ11にフィードバックされる。再生信号は偏光フィル
タ17を通過後、再生信号検出用受光素子18によって
検出され、再生信号増幅回路19によって増幅される。
The laser beam focusing lens 10 is an actuator 11
Supported by The magnetic field generating means J2 is installed on the opposite side or on the same side as the laser beam f% source lens via the magneto-optical disk, and uses a combination of a permanent magnet or a coil and a DC power source. The focus error and tracking error signals are detected by the focus error detection amount v: IL element 13 and the tracking error detection light receiving element 14, respectively, and are sent to the servo control circuit 15.
16, becomes a servo signal, and is fed back to the actuator 11. After passing through the polarizing filter 17 , the reproduced signal is detected by the reproduced signal detection light receiving element 18 and amplified by the reproduced signal amplification circuit 19 .

偏光フィルタとしてはたとえばグラ/トムソンプリズム
が用いられる。再生信号検出用受光素子としてはたとえ
ばPIN7.)ダイオード、アバランシェ・7オトダイ
オードが使用される。レーザ光源6の変調(はレーザ光
源変調用回路2oが使用され、記録時、・消去時、再生
時に合わせてレーザ光源6のパワーをf調する。
For example, a Grass/Thomson prism is used as the polarizing filter. As a light receiving element for detecting a reproduced signal, for example, PIN7. ) diode, avalanche 7 otodiode is used. A laser light source modulation circuit 2o is used to modulate the laser light source 6, and adjusts the power of the laser light source 6 according to recording, erasing, and reproducing.

次に上記構成の光磁気記録再生消去装置の動作方式、特
(従来方式と異なる消去方式について第2図によ、り説
明する。
Next, the operating method of the magneto-optical recording/reproducing/erasing apparatus having the above structure, particularly an erasing method different from the conventional method, will be explained with reference to FIG.

前記光磁気ディスク1上にはすでに第2図(8区示す2
値化号情報がディスクトラックに沿って記録されている
。このとき光磁気ディスク1の磁性薄M3の磁化状態は
第2図市中にR線にて表示した部分け「1」信号に対応
して磁化方向が周v!AK対して反転している。
On the magneto-optical disk 1, there are already 2 sections shown in FIG.
Value code information is recorded along the disc tracks. At this time, the magnetization state of the magnetic thin layer M3 of the magneto-optical disk 1 corresponds to the partial "1" signal indicated by the R line in FIG. It is reversed to AK.

次に記録情報を消去しfcい場合、磁性薄膜3に照射す
るレーザ光のパワーレベル’&第2図fC)Oように一
定パワーレベルPmVCIJIA整する。 これはレー
ザ光源V調用回路2oにて調整可能である。
Next, when the recorded information is to be erased, the power level of the laser beam irradiated onto the magnetic thin film 3 is adjusted to a constant power level PmVCIJIA as shown in FIG. This can be adjusted by the laser light source V adjustment circuit 2o.

Px#′i、  既記fk部分の磁化状態(すなわち磁
化反転の有無)にかかわらず、磁化方向が初期状態(「
0」信号レベル)に戻るレーザ光パワーである。
Px#'i, regardless of the magnetization state of the fk section described above (i.e., presence or absence of magnetization reversal), the magnetization direction is in the initial state ("
0'' signal level).

第2図(C)に示しtレーザ光パワー照射によって磁性
薄J[3の磁化は第2図fd)の状態になり、既記録情
報は消去される。
As shown in FIG. 2(C), by irradiation with the t laser beam power, the magnetic thin film J [the magnetization of 3 is fd in FIG. 2] is brought into the state, and the recorded information is erased.

続いて、新規の2値信号情報比とえば第2図telに示
したような信号情報を記録する場合には、磁性薄膜3に
吸収されるレーザ光パワーが第2図(0に示すレベルr
Cなるよう(レーザ光源変調用回路20を調整する。第
2図(f)においてレーザ光パワーレベルPw m化反
転部分(「1」信畳)を形成するに十分なレーザ光パワ
ーを示している。
Next, when recording a new binary signal information ratio, for example, signal information as shown in FIG.
(The laser light source modulation circuit 20 is adjusted so that the laser light source modulation circuit 20 is adjusted so that the laser light source modulation circuit 20 becomes C. FIG. .

PRI−i記録時のフォーカスエラー、 トラッキング
エラーを検出するために必要なレーザ光バク−を示して
いる。PRは再生時のレーザ光パワーと同レベルである
It shows the laser beam backlash required to detect focus errors and tracking errors during PRI-i recording. PR is at the same level as the laser light power during reproduction.

第2図(f)に示したレーザ光パワーによって記録をお
こなうと、その結果磁性R膜3の磁化状態は第2図(釦
釦なる。
When recording is performed with the laser light power shown in FIG. 2(f), the magnetization state of the magnetic R film 3 becomes as shown in FIG. 2 (button).

以上、一連の消去過程、記録過程においては、母性薄膜
3には磁界印加用コイルあるいは永久磁石から成る磁界
発生手段12により一定の磁界Haが印加されており、
記録再生消去全通して変える必要がない。すなわち、低
記録情報を印加磁界を貰えることなく、レーザ党パワー
を調整することにより消去でき、また新規な情報を記録
できる。
As described above, in the series of erasing and recording processes, a constant magnetic field Ha is applied to the mother thin film 3 by the magnetic field generating means 12 consisting of a magnetic field applying coil or a permanent magnet.
There is no need to change it throughout recording, playback, and erasure. That is, low recorded information can be erased by adjusting the laser power without receiving an applied magnetic field, and new information can be recorded.

(実施例1) 第1図に示した光磁気記録再生消去装置を用いて、光磁
気ディスクへの情報記録、再生、消去をおこなった。光
磁気ディスクとして、120Mψのポリカーボネート樹
脂基板上にスノくツタ法によりTbFe膜を700Al
l!!に形成したディスクを使用した。基板はあらかじ
め@0.8μm、ピッチ2.5μm、深さ7QOAの溝
が形成されているいわゆるプリグループ基板を用いた。
(Example 1) Information was recorded, reproduced, and erased on a magneto-optical disk using the magneto-optical recording, reproducing and erasing device shown in FIG. As a magneto-optical disk, a TbFe film of 700Al was coated on a 120Mψ polycarbonate resin substrate by the snot-vine method.
l! ! A disk formed in the following manner was used. The substrate used was a so-called pre-group substrate in which grooves of @0.8 μm, pitch of 2.5 μm, and depth of 7QOA were formed in advance.

TbFe膜上には保護膜として5if2 が真空蒸着法
によ!1112QOA形成されている。
5if2 is applied as a protective film on the TbFe film by vacuum evaporation! 1112QOA has been formed.

第3図は、消去特性の測定結果である。ディスクの後方
に置かれたコイルによって光磁気ディスクにTb Fe
の磁化と同方向に175Q6の一足磁界ヲ印加シ、線、
% g 111 /sst:の条件でIMHzの1g号
tレーザ光パワーpwにて記録したのち、消去用ノ一定
レーザブレ4ワーpg を歳記録トラックVC照射した
ときの結果である。Aの領域では既記録信号すなわちl
 Ml−I Zの信号は完全に消去された。−万Bの領
域では消去用レーザパワーP8では完全消失けされなか
った。また、Cの領域けPw が記録しきい値以下であ
るため信号記録ができない領域である。
FIG. 3 shows the measurement results of erasing characteristics. Tb Fe is applied to the magneto-optical disk by a coil placed behind the disk.
A magnetic field of 175Q6 is applied in the same direction as the magnetization of the wire,
% g 111 /sst: After recording with a laser beam power pw of 1 g of IMHz, the recording track VC was irradiated with a constant laser blur of 4 pg for erasing. In the area A, the recorded signal, that is, l
The Ml-IZ signal was completely erased. - In the region of 10,000 B, the erasing laser power P8 did not completely erase it. Further, since the area Pw of area C is less than the recording threshold value, it is an area where no signal recording is possible.

(実施例2) 実施例1に示し几光磁気配分再生消去装置と光a%fイ
スクf用い、Pw = 9.5mW、 Pn= 9.5
”WW PR=1.0  、線速9 m / sec、 磁界を
Tb Feの磁化と同方向に175Qe印加した条件で
、l fvll(Z、の信号の記録、消去を繰り返した
。記録消去を105回繰り返しても記E、消去特性には
変化がみられなかった。
(Example 2) Using the photomagnetic distribution reproducing and erasing device shown in Example 1 and the optical a%f disk f, Pw = 9.5 mW, Pn = 9.5
"WW PR = 1.0, linear velocity 9 m/sec, and a magnetic field of 175 Qe was applied in the same direction as the magnetization of Tb Fe. Recording and erasing of the signal l fvll (Z) were repeated. Recording and erasing was performed at 105 Qe. No change was observed in the erasing characteristics even after repeating the test several times.

(発明の効果) 以上、説すしたように本発明によれば、従来例と比較し
て次のような効果がある。
(Effects of the Invention) As described above, the present invention has the following effects compared to the conventional example.

すなわち、外部磁界の印加方向を切!ll替えることな
く、一定の外部8界印加状態で、記録・消去が達成でき
るので、光磁気記録再生消去装置の構成を簡単化できる
。ま7t1本発明け、光磁気ディスクとして笑が一例で
示したTbFe膜に限られるものではなく、光磁気記録
用結晶性磁性薄膜、非晶質磁性薄膜に広く適用できる。
In other words, change the direction of external magnetic field application! Since recording and erasing can be achieved under a constant external field application state without changing the structure, the configuration of the magneto-optical recording/reproducing/erasing device can be simplified. The present invention is not limited to the TbFe film shown as an example as a magneto-optical disk, but can be widely applied to crystalline magnetic thin films and amorphous magnetic thin films for magneto-optical recording.

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

第1図は本発明の適用された光磁気記録再生消去装置の
構成例を示す図、第2図(al〜fg+は消去、記録時
の各部の動作モードならびに記録状態を示す模式図であ
る。また、@3図は本発明の一冥施は従来の元舒気記録
再生消去方式の各部の動作モードを示す模式図である。 図において、1け光磁気ディスク、  2は円板、3け
母性薄膜、  4Viデイスク駆動用モータ。 5は光ヘッド、  6けレーザ光源、  7.8.9は
ビームスプリッタ、  10はレーザ元ビーム集元ビー
ム集光用レンズ、11はアクチュエータ、12け磁界発
生手段、13はフォーカスエラー検出用受光素子、14
けトラスキングエラー検出用受元会子、 15.161
−t:サーボ制御回路、  17i!偏ブCフイルタ、
 18は再生信号検出用量f、、i子、19は再生信号
増幅回路、 20はレーザ光源変調用回路、21けコイ
ル、  22はコイル用電源及びコイル電流極性切替手
1グ、 23け永久磁石をてよる磁界発生手段である。 代理人 ヂ「π± 同 plt   刊71 図 1:光磁気ディスク  20:レーザ光源変調用回路5
:光ヘッド 12:磁界発生手段 72 図 (9)  磁化状態        。 73 図 記録パワ−Pw (mW) 74 図 1:光磁気ディスク 5:光ヘッド 21:コイル A−5図 1:光磁気ディスク 5:光ヘッド 23:磁界発生手段 オ6図 +01 記録時 (b)消去時 −17,1−
FIG. 1 is a diagram showing an example of the configuration of a magneto-optical recording/reproducing/erasing device to which the present invention is applied, and FIG. 2 (al to fg+ are schematic diagrams showing the operation mode and recording state of each part during erasing and recording. In addition, Figure @3 is a schematic diagram showing the operation mode of each part of the conventional original recording/reproducing/erasing system, which is one of the features of the present invention. Matrix thin film, 4Vi disk drive motor. 5 is an optical head, 6 laser light sources, 7, 8, 9 are beam splitters, 10 is a laser source beam focusing lens, 11 is an actuator, 12 is a magnetic field generating means , 13 is a light receiving element for focus error detection, 14
15.161 Receiving member for tracking error detection
-t: Servo control circuit, 17i! Unbalanced C filter,
Reference numeral 18 indicates a reproduction signal detection quantity f, i, 19 indicates a reproduction signal amplification circuit, 20 indicates a laser light source modulation circuit, 21 coils, 22 indicates a coil power supply and coil current polarity switching device, and 23 permanent magnets. This is a magnetic field generating means based on Agent もπ± Same plt publication 71 Figure 1: Magneto-optical disk 20: Laser light source modulation circuit 5
: Optical head 12 : Magnetic field generating means 72 Figure (9) Magnetization state. 73 Figure Recording power - Pw (mW) 74 Figure 1: Magneto-optical disk 5: Optical head 21: Coil A-5 Figure 1: Magneto-optical disk 5: Optical head 23: Magnetic field generating means O Figure 6 +01 During recording (b) When erasing -17,1-

Claims (2)

【特許請求の範囲】[Claims] (1)垂直磁気異方性を有する磁性薄膜を記録媒体とし
、レーザ光によって情報を記録・再生・消去する光磁気
記録再生消去方式であって、前記記録媒体に照射するレ
ーザ光の強度を変化させて情報を記録する記録過程と、
前記記録媒体に一定の強度のレーザ光を照射して記録情
報を再生する再生過程と、一定の強度のレーザ光を照射
して記録情報を消去する消去過程とを通じて一定の磁界
を外部から記録媒体に印加することを特徴とする光磁気
記録再生消去方式。
(1) A magneto-optical recording, reproducing and erasing method in which a magnetic thin film with perpendicular magnetic anisotropy is used as a recording medium and information is recorded, reproduced and erased using a laser beam, and the intensity of the laser beam irradiated to the recording medium is varied. a recording process of recording information by
A constant magnetic field is applied to the recording medium from the outside through a reproduction process in which recorded information is reproduced by irradiating the recording medium with a laser beam of a constant intensity, and an erasing process in which the recorded information is erased by irradiating the recording medium with a laser beam of a constant intensity. A magneto-optical recording, reproducing and erasing method characterized by applying an electric current to the magnetic field.
(2)記録媒体と、該記録媒体に一定の磁界を印加する
磁界発生手段と、記録媒体にレーザ光を照射する光ヘッ
ドと、記録時、再生時、消去時に対応してレーザ光源の
発振レーザ光強度を変化させるレーザ光源変調用回路と
を具備することを特徴とする光磁気記録再生消去装置。
(2) A recording medium, a magnetic field generating means that applies a constant magnetic field to the recording medium, an optical head that irradiates the recording medium with a laser beam, and an oscillating laser of a laser light source during recording, reproduction, and erasing. 1. A magneto-optical recording/reproducing/erasing device comprising: a laser light source modulation circuit that changes light intensity;
JP59171094A 1984-08-17 1984-08-17 Magneto-optical recording / reproduction / erasing method and apparatus Expired - Lifetime JP2591729B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59171094A JP2591729B2 (en) 1984-08-17 1984-08-17 Magneto-optical recording / reproduction / erasing method and apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59171094A JP2591729B2 (en) 1984-08-17 1984-08-17 Magneto-optical recording / reproduction / erasing method and apparatus

Publications (2)

Publication Number Publication Date
JPS6150235A true JPS6150235A (en) 1986-03-12
JP2591729B2 JP2591729B2 (en) 1997-03-19

Family

ID=15916873

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Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP2591729B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5184335A (en) * 1986-03-07 1993-02-02 Movid Information Technology, Inc. Method and system for erasing previously recorded domains in a magneto-optic recording medium
US5528564A (en) * 1986-03-07 1996-06-18 Movid Information Technology, Inc. Direct overwrite magneto-optic system for strip erasing and recording elongated domains

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59113507A (en) * 1982-12-21 1984-06-30 Nec Corp System and device for photomagnetic recording, reproducing, and erasing
JPS59113506A (en) * 1982-12-21 1984-06-30 Nec Corp System and device for photomagnetic recording, reproducing, and erasing

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59113507A (en) * 1982-12-21 1984-06-30 Nec Corp System and device for photomagnetic recording, reproducing, and erasing
JPS59113506A (en) * 1982-12-21 1984-06-30 Nec Corp System and device for photomagnetic recording, reproducing, and erasing

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5184335A (en) * 1986-03-07 1993-02-02 Movid Information Technology, Inc. Method and system for erasing previously recorded domains in a magneto-optic recording medium
US5528564A (en) * 1986-03-07 1996-06-18 Movid Information Technology, Inc. Direct overwrite magneto-optic system for strip erasing and recording elongated domains

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