JP2604702B2 - Magneto-optical recording / reproduction / erasing method and apparatus - Google Patents

Magneto-optical recording / reproduction / erasing method and apparatus

Info

Publication number
JP2604702B2
JP2604702B2 JP60019567A JP1956785A JP2604702B2 JP 2604702 B2 JP2604702 B2 JP 2604702B2 JP 60019567 A JP60019567 A JP 60019567A JP 1956785 A JP1956785 A JP 1956785A JP 2604702 B2 JP2604702 B2 JP 2604702B2
Authority
JP
Japan
Prior art keywords
recording
magnetic field
erasing
reproducing
magneto
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
JP60019567A
Other languages
Japanese (ja)
Other versions
JPS61178750A (en
Inventor
満哉 岡田
壮太郎 ▲え▼所
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 JP60019567A priority Critical patent/JP2604702B2/en
Publication of JPS61178750A publication Critical patent/JPS61178750A/en
Application granted granted Critical
Publication of JP2604702B2 publication Critical patent/JP2604702B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、レーザ光と印加磁界のスイッチングによっ
て情報の記録再生消去をおこなう光磁気記録再生消去方
法及び装置に関する。
The present invention relates to a magneto-optical recording / reproducing / erasing method and apparatus for recording / reproducing / erasing information by switching between a laser beam and an applied magnetic field.

(従来技術とその問題点) 光記録方式、特に光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ファイルメモリの一つとして
近年注目を集めている。その中でも記録媒体としてMnB
i,MnCuBi,MnTiBi,MnAlGeなどの結晶性磁性薄膜あるいは
Tb,Gd,Dy,Hoなどの希土類金属とFe,Co,Ni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。
(Prior art and its problems) The optical recording method, especially the optical disk memory method,
In recent years, it has attracted attention as one of large-capacity file memories because it can perform large-capacity recording and can also perform non-contact and high-speed access. Among them, MnB as a recording medium
crystalline magnetic thin films such as i, MnCuBi, MnTiBi, MnAlGe or
Magneto-optical disk memory using an amorphous magnetic thin film made by combining rare earth metals such as Tb, Gd, Dy, Ho and transition metals such as Fe, Co, Ni, etc. Due to its advantages, it is being actively studied in various places.

従来、公知の光磁気記録再生消去方法においては、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。
Conventionally, in a known magneto-optical recording / reproducing / erasing method, the following operations are performed for recording / reproducing / erasing information.

記録には、レーザ光により発生する熱を利用する。レ
ーザ光ビームを1〜2μmφ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。キューリ温度
記録をおこなう場合には、記録媒体をキューリ温度以上
に上昇させ、外部印加磁界あるい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
光ビーム照射によってある温度まで昇温させ、媒体の保
磁力低下を利用し、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「1」「0」を記
録媒体の反転磁区の有無に対応した形で記録できる。
For recording, heat generated by a laser beam is used. The laser light beam is narrowed down to a minute spot of 1 to 2 μmφ and irradiated on the recording medium to raise the medium temperature. When performing Curie temperature recording, the recording medium is raised to a Curie temperature or higher, and a reversal magnetic domain is formed by an externally applied magnetic field or a demagnetizing field of the recording medium. When performing compensation temperature recording, set the compensation temperature of the recording medium to around room temperature, raise the temperature to a certain temperature by irradiating a laser light beam, and form a reversal magnetic domain by an externally applied magnetic field using the decrease in the coercive force of the medium. . By the means described above, the recording binary signals "1" and "0" can be recorded in a form corresponding to the presence or absence of the reversal magnetic domain of the recording medium.

再生は磁気光学効果(Kerr効果あるいはFaraday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は透過光の
偏光面が回転することを利用し、記録媒体から情報を読
み出す。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 performed using a magneto-optical effect (Kerr effect or Faraday effect). That is, information is read from the recording medium by utilizing the fact that the polarization plane of reflected light or transmitted light from the medium is rotated according to the presence or absence of the reversal magnetic domain of the recording medium. The recording medium is irradiated with a laser beam having a lower power level than during recording, and a signal is reproduced from the reflected light or transmitted light.

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
媒体の磁化状態は記録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 the recording medium is uniformly irradiated with a laser beam at 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 recording.

ここで、公知の外部磁界印加手段は、たとえば空心コ
イルを用いる方法、電磁石を用いる方法、あるいは永久
磁石を用いる方法である。
Here, the known external magnetic field applying means is, for example, a method using an air core coil, a method using an electromagnet, or a method using a permanent magnet.

従来の光磁気記録再生消去方法及び装置において、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なければならない。たと
えば、空心コイルあるいは電磁石によって外部磁界を印
加する場合、第4図に示すように、記録時と消去時には
レーザ光の記録動作、消去動作に同期させてコイルに流
す電流の向きを切り替える方式及び装置が知られてい
る。ここでは光磁気ディスク、22は磁界発生手段、23は
電流源、Sは光ヘッドである。従来の方式では記録時と
消去時では300Oe以上の外部印加磁界の可変が必要であ
る。そのために空心コイルあるいは電磁石が大型化して
しまうという欠点がある。
In the conventional magneto-optical recording / reproducing erasing method and apparatus, rewriting of recorded information is performed in two steps of first erasing recorded information according to the erasing operation, and then recording new recorded information according to the recording operation. Perform the operation of. At this time, the direction of the external magnetic field applied to the recording medium is opposite between the time of erasing and the time of recording. Therefore, the direction of the externally applied magnetic field must be switched between the time of erasing and the time of recording. For example, when an external magnetic field is applied by an air-core coil or an electromagnet, as shown in FIG. 4, during recording and erasing, a method and apparatus for switching the direction of a current flowing through a coil in synchronization with a recording operation and an erasing operation of a laser beam. It has been known. Here, a magneto-optical disk, 22 is a magnetic field generating means, 23 is a current source, and S is an optical head. In the conventional method, it is necessary to vary the externally applied magnetic field of 300 Oe or more during recording and erasing. Therefore, there is a disadvantage that the air-core coil or the electromagnet is enlarged.

また、磁界発生手段24として永久磁石を用い外部磁界
を印加する場合には、第5図に示すように磁石駆動機構
が用いられるが装置構成が複雑になるという欠点を有し
ている。
When an external magnetic field is applied using a permanent magnet as the magnetic field generating means 24, a magnet driving mechanism is used as shown in FIG. 5, but there is a disadvantage that the device configuration becomes complicated.

(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法及
び装置の欠点を解決し、簡単な装置構成により情報の記
録・再生・消去ができる新規な光磁気記録再生消去方法
及び装置を提供することにある。
(Object of the Invention) An object of the present invention is to solve the drawbacks of the conventional magneto-optical recording / reproducing / erasing method and apparatus, and to provide a novel magneto-optical recording / reproducing / erasing method capable of recording / reproducing / erasing information with a simple apparatus configuration. It is to provide a device.

(発明の構成) 本発明によれば、垂直磁気異方性を有する磁性薄膜を
記録媒体とし、レーザ光と磁界の印加によって情報の記
録再生消去をおこなう光磁気記録再生消去方式におい
て、前記磁性薄膜の消磁状態を初期状態とし、一定強度
のレーザ光を照射し、記録情報に応じて印加磁界を高速
スイッチングして前記記録媒体に磁区を形成する記録過
程と、前記記録媒体の磁区の磁化方向に対応したレーザ
反射光の偏光面回転から情報を再生する再生過程と、磁
界印加とレーザ光照射によって前記記録薄膜の磁化状態
を消磁状態に戻す消去過程とを備えたことを特徴とする
光磁気記録再生消去方法が得られ、さらには前記光磁気
記録再生消去方法を用いた光磁気記録再生消去装置であ
って、磁性薄膜の消磁状態を初期状態とする記録媒体
と、記録媒体に一定強度のレーザ光を照射する光ヘッド
と、記録相対に磁界を印加する磁界発生手段と、記録時
に磁界発生手段の発生磁界強度を記録情報に応じて変化
させることができ、かつ消去時に磁界発生手段の発生磁
界強度を一定にして、前記磁性薄膜の磁化状態を消磁状
態に戻す磁界変調手段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。
(Constitution of the Invention) According to the present invention, in 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 / erased by applying a laser beam and a magnetic field, The demagnetization state as an initial state, irradiating a laser beam of a constant intensity, a high-speed switching of an applied magnetic field according to recording information to form a magnetic domain in the recording medium, and a recording direction of the magnetic domain of the recording medium. Magneto-optical recording, comprising: a reproducing step of reproducing information from a corresponding rotation of the plane of polarization of reflected laser light; and an erasing step of returning the magnetization state of the recording thin film to a demagnetized state by applying a magnetic field and irradiating a laser beam. A magneto-optical recording / reproducing / erasing apparatus using the magneto-optical recording / reproducing / erasing method, wherein the recording medium has a demagnetized state of a magnetic thin film as an initial state, An optical head for irradiating a medium with laser light of a constant intensity, a magnetic field generating means for applying a magnetic field relative to recording, and a magnetic field intensity generated by the magnetic field generating means during recording can be changed according to recording information; A magneto-optical recording / reproducing and erasing apparatus characterized by comprising a magnetic field modulating means for returning the magnetization state of the magnetic thin film to a demagnetized state while keeping the intensity of the magnetic field generated by the magnetic field generating means constant.

(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
題点を解決した。以下、本発明の詳細について図面を用
いて説明する。第1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はガラス
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
面に、基板面の垂直方向に磁化容易軸を有する磁性薄膜
3を形成したものである。
(Detailed Description of Configuration) The present invention has solved the problems of the prior art by adopting the above configuration. Hereinafter, details of the present invention will be described with reference to the drawings. FIG. 1 shows a configuration of a magneto-optical recording / reproducing / erasing apparatus to which the present invention is applied. In FIG. 1, a magneto-optical disk 1 has a magnetic thin film 3 having an axis of easy magnetization in a direction perpendicular to the substrate surface formed on one or both surfaces of a disk 2 made of an organic resin substrate, a glass substrate, or a metal substrate.

前記磁性薄膜3は、結晶性あるいは非晶質磁性薄膜で
あり、たとえば、MnBi,MnCuBi,MnTiBi,MnAlGeなどの結
晶性磁性薄膜あるいはSm,Tb,Gd,Dy,Hoなどの希土類金属
とFe,Co,Niなどの遷移金属との組み合わせによって作成
される非晶質磁性薄膜である。前記光磁気ディスク1は
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。光ヘッド5は光磁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1の半径方向に所定の速度
により移動可能である。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。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12は光磁気ディスク1を介し
て光ヘッド5と反対側もしくは同じ側に設置され、空心
コイルが望ましい。
The magnetic thin film 3 is a crystalline or amorphous magnetic thin film. And an amorphous magnetic thin film formed by a combination with a transition metal such as Ni. The magneto-optical disk 1 is rotated at a predetermined speed by a disk drive motor 4. The optical head 5 has an optical system for magneto-optical recording / reproduction and erasing, and a light detecting mechanism. The optical head 5 itself is movable at a predetermined speed in the radial direction of the magneto-optical disk 1 as indicated by an arrow in the figure. In the optical head 5, reference numeral 6 denotes a linearly polarized laser light source, for example, a semiconductor laser. 7, 8, and 9 are beam splitters. The laser light beam focusing lens 10 is supported by an actuator 11. The magnetic field generating means 12 is provided on the opposite side or the same side as the optical head 5 via the magneto-optical disk 1, and is preferably an air-core coil.

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受光素子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
チュエータ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、
偏光フィルタ17としてはたとえばグラントムソンプリズ
ムが用いられる。再生信号検出用受光素子18としてはた
とえばPINフォトダイオード,アバランシェ・フォトダ
イオードが使用される。
The focus error signal and the tracking error signal are detected by the focus error detecting light receiving element 13 and the tracking error detecting light receiving element 14, respectively, input to the servo control circuits 15 and 16, become servo signals, and are fed back to the actuator 11. After passing through the polarization filter 17, the reproduction signal is detected by the reproduction signal detection light-receiving element 18 and amplified by the reproduction signal amplifier circuit 19.
As the polarization filter 17, for example, a Glan-Thompson prism is used. As the reproduction signal detecting light receiving element 18, for example, a PIN photodiode or an avalanche photodiode is used.

磁界発生手段12を記録情報に応じて変調するには電流
源20が使用でき、記録情報に応じて記録時に空心コイル
に供給する電流を可変する。一方、消去時には消去に必
要な磁界が得られるよう磁界発生手段12に電流を供給す
る。
The current source 20 can be used to modulate the magnetic field generating means 12 according to the recording information, and the current supplied to the air-core coil during recording is varied according to the recording information. On the other hand, at the time of erasing, a current is supplied to the magnetic field generating means 12 so that a magnetic field necessary for erasing is obtained.

レーザ光源6への電流供給レーザ用電流源21が用いら
れ、記録時、再生時及び消去時にはそれぞれ一定出力の
レーザパワーが光磁気ディスク1に照射できるように調
整される。
A current source 21 for supplying a current to the laser light source 6 is adjusted so that a constant output laser power can be applied to the magneto-optical disk 1 during recording, reproduction, and erasing.

次に上記構成の光磁気記録再生消去装置の動作方式に
ついて、特に従来方式と異なる記録方式,消去方式につ
いて第2図により説明する。前記光磁気ディスク1のト
ラックの磁化状態はすでに第2図(a)に示すように消
磁状態になっている。
Next, the operation method of the magneto-optical recording / reproducing / erasing apparatus having the above-described configuration, particularly a recording method and an erasing method different from the conventional method will be described with reference to FIG. The magnetization state of the track of the magneto-optical disk 1 has already been demagnetized as shown in FIG. 2 (a).

第2図(b)に示す記録情報を光磁気ディスク1に記
録する場合、記録するディスクトラックに第2図(c)
に示す一定レベルのレーザパワー(Pw)を照射すると同
時に第2図(d)に示すような記録情報で変調された磁
界(振幅±Hw、バイアスHB)を供する。これは、電流源
20にて調整可能である。このときディスクトラックには
第2図(e)に示すような±θのKerr回転角を持つ記
録情報に応じた磁区が形成される。続いて消去をおこな
う場合、ディスクの既記録トラックに一定レベルのレー
ザパワー(PE)を照射するとともに、一定レベルの磁界
(HE)を供給する。このとき、ディスクトラックは第2
図(a)に示す磁化状態に戻る。
When recording information shown in FIG. 2 (b) is recorded on the magneto-optical disk 1, a disk track to be recorded is shown in FIG. 2 (c).
When irradiating the laser power (Pw) of a constant level shown in modulated with recorded information as shown in FIG. 2 (d) at the same time magnetic field (amplitude ± Hw, bias H B) subjecting the. This is the current source
Adjustable at 20. At this time, magnetic domains are formed in the disk track according to the recording information having a Kerr rotation angle of ± θ k as shown in FIG. 2 (e). Subsequently, when erasing is performed, a predetermined level of laser power (P E ) is applied to the already-recorded tracks of the disk, and a certain level of magnetic field (H E ) is supplied. At this time, the disc track is
The state returns to the magnetized state shown in FIG.

(実施例) 第1図に示した光磁気記録再生消去装置及び第2図に
示した動作方式に準じて、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12
0mmφの樹脂基板上にスパッタ法によりTbFe膜を800Å厚
に形成したディスクを用いた。基板にあらかじめ幅0.8
μm、ピッチ2.5μm、深さ700Åの溝が形成されている
プリグルーブ基板を用いた。TbFe膜上には保護膜として
SiO2が1200Å形成されている。
(Example) According to the magneto-optical recording / reproducing / erasing apparatus shown in FIG. 1 and the operation method shown in FIG. 2, information was recorded, reproduced and erased on the magneto-optical disk. 12 as a magneto-optical disk
A disk was used in which a TbFe film was formed to a thickness of 800 mm on a 0 mmφ resin substrate by a sputtering method. 0.8 width on board in advance
A pre-groove substrate in which a groove having a pitch of 2.5 μm and a depth of 700 ° was formed was used. As a protective film on TbFe film
SiO 2 is formed at 1200 °.

第1図中の磁界発生手段12としては一定バイアス磁界
発生用に線径0.1mmφの被覆銅線を用いた空心コイル
(外径6.0mmφ,内径2.0mmφ,コイル長0.5mm,巻数100
ターン)を用い、変調磁界発生用には同じく線径0.1mm
φの被覆銅線を用いた空心コイル(外径2.6mmφ,内径
1.0mmφ,コイル長0.7mm,巻数56ターン)を用いた。
An air-core coil (outer diameter 6.0 mmφ, inner diameter 2.0 mmφ, coil length 0.5 mm, number of turns 100) using a coated copper wire with a diameter of 0.1 mmφ as a magnetic field generating means 12 in FIG.
Turn), and a wire diameter of 0.1 mm for generating the modulated magnetic field
An air-core coil using a coated copper wire of φ (outer diameter 2.6mmφ, inner diameter
1.0mmφ, coil length 0.7mm, number of turns 56).

まず、ディスク全体を10KOeの磁場中で一方向に直磁
後、ディスクを線速9m/secで回転し、1トラックにわた
り4mWのレーザ光照射と同時に140Oeの磁界を着磁と同方
向に印加した。この操作により該トラックが消磁状態に
なっていることが偏光顕微鏡観察によって確認された。
First, after the whole disk was perpendicularly magnetized in one direction in a magnetic field of 10 KOe, the disk was rotated at a linear velocity of 9 m / sec, and a laser beam of 4 mW was irradiated over one track and a magnetic field of 140 Oe was applied in the same direction as the magnetization. . This operation confirmed that the track was in a demagnetized state by observation with a polarizing microscope.

次に、消磁状態のトラックに対してPW=4mW、HB=140
0eの条件で1MHzの周波数においてHWを変えて記録をおこ
なった。
Next, P W = 4 mW and H B = 140 for the track in the demagnetized state.
Recording was performed with the HW changed at a frequency of 1 MHz under the condition of 0e.

第3図は再生C/NとHWとの関係である。HWが100Oe以上
で再生C/Nは飽和し、良好な記録が達成された。
Figure 3 shows the relationship between the reproduction C / N and H W. H W playback C / N is saturated with more than 100 Oe, good recording is achieved.

記録トラックの消去は4mWのレーザ光照射と140Oeの磁
界印加(着磁と同方向)によりおこなった。1トラック
にわたり消え残りはなく、完全に消去できた。
The recording track was erased by irradiating a laser beam of 4 mW and applying a magnetic field of 140 Oe (in the same direction as the magnetization). There was no erasure over one track, and the track was completely erased.

(発明の効果) 以上説明したように、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, according to the present invention, the following effects are obtained as compared with the conventional example.

印加磁界の可変範囲が±100Oe程度と小さく、それ
により磁界発生手段を小型化,簡単化できる。
The variable range of the applied magnetic field is as small as about ± 100 Oe, so that the magnetic field generating means can be reduced in size and simplified.

記録情報に応じた磁界変化によって記録をおこなう
ので、従来のようにレーザ光源を変調する必要がない。
Since recording is performed by a magnetic field change according to the recording information, there is no need to modulate the laser light source as in the related art.

記録時,消去時の印加磁界(HW,HB,HE)は独立に可
変できるので、種々の磁性薄膜を用いた光磁気ディスク
に本発明が適用できる。
During recording, the magnetic field applied during erasing (H W, H B, H E) so can be varied independently, the present invention can be applied to the magneto-optical disk using a variety of magnetic thin film.

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

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
構成図、第2図は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、第3図は本発明の一
実施例の測定結果を示す図である。第4図,第5図は従
来の光磁気記録再生消去装置の構成図である。 図において1は光磁気ディスク、2は円板、3は磁性薄
膜、4はディスク駆動用モータ、5は光ヘッド、6はレ
ーザ光源、7,8,9はビームスプリッタ、10はレーザ光ビ
ーム集光用レンズ、11はアクチュエータ、12,22,24は磁
界発生手段、13はフォーカスエラー検出用受光素子、14
はトラッキングエラー検出用受光素子、15,16はサーボ
制御回路、17は偏光フィルタ、18は再生信号検出用受光
素子、19は再生信号増幅回路、20,23は磁界発生手段用
電流源、21はレーザ用電流源である。
FIG. 1 is a configuration diagram of a magneto-optical recording / reproducing and erasing apparatus to which the present invention is applied, and FIG. 2 is a schematic diagram showing an operation mode and a recording state of each unit at the time of recording. FIG. 3 is a view showing a measurement result of one embodiment of the present invention. FIGS. 4 and 5 are block diagrams of a conventional magneto-optical recording / reproducing / erasing apparatus. In the figure, 1 is a magneto-optical disk, 2 is a disk, 3 is a magnetic thin film, 4 is a disk drive motor, 5 is an optical head, 6 is a laser light source, 7, 8, and 9 are beam splitters, and 10 is a laser light beam collector. Optical lens, 11 is an actuator, 12, 22, 24 are magnetic field generating means, 13 is a light receiving element for focus error detection, 14
Is a tracking error detecting light receiving element, 15 and 16 are servo control circuits, 17 is a polarization filter, 18 is a reproducing signal detecting light receiving element, 19 is a reproducing signal amplifying circuit, 20 and 23 are current sources for magnetic field generating means, 21 is This is a laser current source.

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】垂直磁気異方性を有する磁性薄膜を記録媒
体とし、レーザ光と磁界の印加によって情報の記録再生
消去をおこなう光磁気記録再生消去方法において、前記
磁性薄膜の消磁状態を初期状態とし、一定強度のレーザ
光を照射し、記録情報に応じて印加磁界を高速スイッチ
ングして前記記録媒体に磁区を形成する記録過程と、前
記記録媒体の磁区の磁化方向に対応したレーザ反射光の
偏光面回転から情報を再生する再生過程と、磁界印加と
レーザ光照射によって前記記録薄膜の磁化状態を消磁状
態に戻す消去過程とを備えたことを特徴とする光磁気記
録再生消去方法。
1. A magneto-optical recording / reproducing and erasing method for recording / reproducing / erasing information by applying a laser beam and a magnetic field to a magnetic thin film having perpendicular magnetic anisotropy as a recording medium. And irradiating a laser beam of a constant intensity, a recording process of forming a magnetic domain in the recording medium by rapidly switching an applied magnetic field according to recording information, and a laser reflected light corresponding to a magnetization direction of the magnetic domain of the recording medium. A magneto-optical recording / reproducing / erasing method comprising: a reproducing step of reproducing information from a polarization plane rotation; and an erasing step of returning a magnetization state of the recording thin film to a demagnetized state by applying a magnetic field and irradiating a laser beam.
【請求項2】磁性薄膜の消磁状態を初期状態とする記録
媒体と、記録媒体に一定強度のレーザ光を照射する光ヘ
ッドと、記録媒体に磁界を印加する磁界発生手段と、記
録時に磁界発生手段の発生磁界強度を記録情報に応じて
変化させることができ、かつ消去時に磁界発生手段の発
生磁界強度を一定にして、前記磁性薄膜の磁化状態を消
磁状態に戻す磁界変調手段とを具備したことを特徴とす
る光磁気記録再生消去装置。
2. A recording medium for initializing a demagnetized state of a magnetic thin film, an optical head for irradiating the recording medium with a laser beam having a constant intensity, a magnetic field generating means for applying a magnetic field to the recording medium, and a magnetic field generation during recording. Magnetic field modulating means for changing the intensity of the generated magnetic field of the means in accordance with the recorded information, and making the intensity of the generated magnetic field of the magnetic field generating means constant during erasing, and returning the magnetization state of the magnetic thin film to the demagnetized state. A magneto-optical recording / reproducing / erasing apparatus characterized by the above-mentioned.
JP60019567A 1985-02-04 1985-02-04 Magneto-optical recording / reproduction / erasing method and apparatus Expired - Lifetime JP2604702B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60019567A JP2604702B2 (en) 1985-02-04 1985-02-04 Magneto-optical recording / reproduction / erasing method and apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60019567A JP2604702B2 (en) 1985-02-04 1985-02-04 Magneto-optical recording / reproduction / erasing method and apparatus

Publications (2)

Publication Number Publication Date
JPS61178750A JPS61178750A (en) 1986-08-11
JP2604702B2 true JP2604702B2 (en) 1997-04-30

Family

ID=12002867

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60019567A Expired - Lifetime JP2604702B2 (en) 1985-02-04 1985-02-04 Magneto-optical recording / reproduction / erasing method and apparatus

Country Status (1)

Country Link
JP (1) JP2604702B2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6048806B2 (en) * 1978-01-11 1985-10-29 ケイディディ株式会社 Thermomagnetic recording method

Also Published As

Publication number Publication date
JPS61178750A (en) 1986-08-11

Similar Documents

Publication Publication Date Title
US4472748A (en) Method of processing information signal with respect to opto-magnetic record medium
JPS60236137A (en) Simultaneously erasing-recording type photomagnetic recording system and recording device and medium used for this system
JPS60170048A (en) Photomagnetic memory device
US4495530A (en) Method of processing information signal with respect to opto-magnetic record medium
JPH0630183B2 (en) Magneto-optical recording / reproducing method and device
JPH0721894B2 (en) Magneto-optical recording method
JPH0448406A (en) Magneto-optical recording and reproducing device and magnetic head
JPH0721892B2 (en) Magneto-optical recording method
JPS61214256A (en) Photomagnetic disc device
JPH0721895B2 (en) Magneto-optical recording method
JPH0551975B2 (en)
JPS6217282B2 (en)
EP0241222A1 (en) Opto-magnetic recording apparatus for sequentially driving optical head drive means and biasing magnetic field generation means
JP2604702B2 (en) Magneto-optical recording / reproduction / erasing method and apparatus
JP2604700B2 (en) Magneto-optical recording / reproduction / erasing method and apparatus
JP2591729B2 (en) Magneto-optical recording / reproduction / erasing method and apparatus
JPH0721896B2 (en) Magneto-optical recording method
JPH0721893B2 (en) Magneto-optical recording method
JPH0568763B2 (en)
JPS61214258A (en) Write and reproducing integrated magnetic head
JP2705598B2 (en) Magneto-optical storage method and apparatus
JP2744776B2 (en) Magneto-optical recording / reproducing device
JP3146614B2 (en) Recording method and recording apparatus for magneto-optical recording medium
JPH06150423A (en) Magneto-optical recorder
JPH0456362B2 (en)