JP2604700B2 - Magneto-optical recording / reproduction / erasing method and apparatus - Google Patents

Magneto-optical recording / reproduction / erasing method and apparatus

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Publication number
JP2604700B2
JP2604700B2 JP59225236A JP22523684A JP2604700B2 JP 2604700 B2 JP2604700 B2 JP 2604700B2 JP 59225236 A JP59225236 A JP 59225236A JP 22523684 A JP22523684 A JP 22523684A JP 2604700 B2 JP2604700 B2 JP 2604700B2
Authority
JP
Japan
Prior art keywords
recording
reproducing
thin film
magnetic
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
JP59225236A
Other languages
Japanese (ja)
Other versions
JPS61104444A (en
Inventor
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
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Filing date
Publication date
Application filed by NEC Corp filed Critical NEC Corp
Priority to JP59225236A priority Critical patent/JP2604700B2/en
Publication of JPS61104444A publication Critical patent/JPS61104444A/en
Application granted granted Critical
Publication of JP2604700B2 publication Critical patent/JP2604700B2/en
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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

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及びその装置に関する。
Description: TECHNICAL FIELD The present invention relates to a magneto-optical recording / reproducing / erasing system for recording / reproducing / erasing information by using a laser beam and an apparatus therefor.

(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式においては、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。記録媒体はあらかじめ媒体の保磁力以上の
外部磁界により一方向に着磁される。
Conventionally, in the known magneto-optical recording / reproducing / erasing method, the following operations are performed for recording / reproducing / erasing information. The recording medium is preliminarily magnetized in one direction by an external magnetic field greater than the coercive force of the medium.

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 reversed 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.

しかしながら、記録時と消去時では通常300Oe以上印
加磁界に差があるために空心コイルを用いる場合にはコ
イルが大型化するとともに記録媒体とコイルとの距離を
十分に接近させないと所要印加磁界が得られないという
欠点がある。また、電磁石を用いる場合にも、磁界印加
手段は大型化し、磁界切替えが遅いという欠点も生じ
る。永久磁石を用いる場合は、機械的な駆動手段を用い
て磁界を切替えるため、複雑な機構が必要であるという
欠点を持つ。
However, there is a difference in applied magnetic field of 300 Oe or more between recording and erasing.Therefore, when using an air-core coil, the coil becomes large and the required applied magnetic field cannot be obtained unless the distance between the recording medium and the coil is sufficiently close. There is a disadvantage that it cannot be done. Also, when an electromagnet is used, there is a disadvantage that the magnetic field applying means becomes large and the magnetic field switching is slow. When a permanent magnet is used, the magnetic field is switched using mechanical driving means, and thus has a disadvantage that a complicated mechanism is required.

従来のいずれの方式においても記録時、消去時の動作
モードでは第4図(a),(b),(c),(d)に示
したように記録時(第4図(a),(b))印加磁界Hw
と消去時(第4図(c),(d))の印加磁界HEの差が
大きいという欠点は解消されない。
In any of the conventional systems, the recording mode and the erasing operation mode are as shown in FIGS. 4 (a), (b), (c) and (d) during recording (FIGS. 4 (a) and (d)). b)) Applied magnetic field Hw
And erasing (Fig. 4 (c), (d)) is not eliminated disadvantage large difference of the applied magnetic field H E of.

(発明の目的) 本発明の目的はこのような従来の欠点を除去せしめ
て、小型でかつ容易な磁界印加手段を用い、容易に記録
・再生・消去をおこなうことのできる新規な光磁気記録
再生消去方式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 eliminate such a conventional drawback, and to use a small and easy magnetic field applying means, and to provide a novel magneto-optical recording / reproducing apparatus capable of easily performing recording / reproducing / erasing. An erasing method and apparatus are provided.

(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
含む記録媒体に対しレーザ光によって情報の記録再生消
去を行う光磁気記録再生消去方法において、前記磁性薄
膜の磁化方向が再生用レーザ光のスポットサイズ内にお
いてランダムな消磁状態を初期状態とし、一定磁界印加
と情報により変調されたレーザ光照射によって前記磁性
薄膜に磁区を形成する記録過程と、前記記録薄膜の磁区
の有無に対応したレーザ反射光の偏光回転から情報を再
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から
なる光磁気記録再生消去方法が得られ、さらには垂直磁
気異方性を有する磁性薄膜を含む記録媒体に対しレーザ
光によって情報の記録再生消去を行う光磁気記録再生消
去装置において、磁化方向が再生用レーザ光のスポット
サイズ内においてランダムな消磁状態を初期状態とする
磁性薄膜から成る記録媒体と、該記録媒体に磁界を印加
する磁界発生手段と、記録媒体にレーザ光を照射する光
磁気記録用ヘッドと、記録・消去に対して磁界発生手段
に供給する電流を変化させることができる電流供給源と
を備え、記録は、一定磁界印加と情報により変調された
レーザ光照射によって前記磁性薄膜に磁化方向が媒体面
に対して上向き又は下向きの磁区を形成することにより
行い、再生は、前記記録薄膜の磁区の有無に対応したレ
ーザ反射光の偏光面回転を信号として取り出すことによ
り行い、消去は、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ことにより行うこ
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 for recording / reproducing / erasing information on a recording medium including a magnetic thin film having perpendicular magnetic anisotropy with a laser beam, the magnetization direction of the magnetic thin film The recording process of forming a magnetic domain in the magnetic thin film by applying a constant magnetic field and irradiating a laser beam modulated by information with a random demagnetized state as an initial state within the spot size of the reproducing laser light, A magneto-optical recording / reproducing / erasing method comprising a reproducing process of reproducing information from the polarization rotation of the laser reflected light corresponding to the presence / absence and an erasing process of returning the magnetization state of the recording thin film to a demagnetized state by applying a magnetic field and irradiating a laser beam is obtained. A magneto-optical recording / reproducing / erasing apparatus for recording / reproducing / erasing information on a recording medium including a magnetic thin film having perpendicular magnetic anisotropy by using a laser beam A recording medium comprising a magnetic thin film whose magnetization direction is initially set to a random demagnetized state within a spot size of a reproducing laser beam; a magnetic field generating means for applying a magnetic field to the recording medium; A magneto-optical recording head for irradiating a laser beam, and a current supply source for changing a current supplied to a magnetic field generating means for recording and erasing. The irradiation is performed by forming magnetic domains in the magnetic thin film whose magnetization direction is upward or downward with respect to the medium surface by irradiation, and reproduction is performed by extracting the polarization plane rotation of laser reflected light corresponding to the presence or absence of the magnetic domains of the recording thin film as a signal. And erasing is performed by returning the magnetization state of the recording thin film to a demagnetized state by applying a magnetic field and irradiating a laser beam. Recording and playback erasing device can be obtained.

(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、従来の技術の
問題点を解決した。第1図に本発明に係る光磁気記録再
生消去方式の記録・消去動作モード図を示す。記録媒体
に用いる磁性薄膜の磁化状態を消磁状態とし、これを初
期状態とする。ここで消磁状態とは、磁性薄膜の磁化状
態が次のような状態をいう。磁性薄膜の磁化状態が、再
生用レーザ光のスポットサイズ内において、ランダムな
状態、すならち垂直磁化膜を用いている場合は、記録膜
のの膜厚方向に対して上向きと下向きの磁化がスポット
サイズに比べて十分小さく分割されて混在した状態であ
る。記録はこの消磁状態の磁性薄膜に磁区を形成するこ
とによりおこなわれる(第1図(a))。磁区の磁化方
向は媒体面に対して上向きでも下向きでもよい。第1図
(b)において印加磁界HwとHw′に相当する。従来の記
録が一方向に着磁された磁性薄膜に反転磁区を件成して
記録をおこなうのに対して、本発明に係る記録において
は、消磁状態の磁性薄膜に磁区を形成すればよいので、
記録に要する印加磁界は従来の記録よりも小さくてよ
い。再生は従来の再生と同じように、磁性薄膜から反射
されるレーザ光の偏光面回転を信号として取り出す。磁
区のある領域と消磁された領域では明らかにKerr効果に
よる偏光面の回転が異なるので、十分な再生信号が得ら
れる。消磁された領域を再生した場合、上下方向の個々
の磁化を判別することは困難であり、記録媒体からの再
生信号は、上方向の磁化からの再生信号と下方向の磁化
からの再生信号の中間レベルとなる。消去時には第1図
(c),(d)に示したように消去を要する領域に一定
強度のレーザ光PEと一定値の外部磁界HEが印加され、消
去後の磁化状態が初期状態と同じ消磁状態になる。
(Detailed Description of Configuration) The present invention has solved the problems of the conventional technology by adopting the above configuration. FIG. 1 shows a recording / erasing operation mode diagram of the magneto-optical recording / reproducing / erasing method according to the present invention. The magnetization state of the magnetic thin film used for the recording medium is set to a demagnetized state, and this is set to an initial state. Here, the demagnetized state refers to a state in which the magnetization state of the magnetic thin film is as follows. When the magnetization state of the magnetic thin film is in a random state within the spot size of the reproducing laser beam, that is, when a perpendicular magnetization film is used, the upward and downward magnetizations with respect to the thickness direction of the recording film. This is a state in which the image is divided into small portions that are sufficiently smaller than the spot size and are mixed. Recording is performed by forming magnetic domains in the magnetic thin film in the demagnetized state (FIG. 1A). The magnetization direction of the magnetic domain may be upward or downward with respect to the medium surface. In FIG. 1B, it corresponds to the applied magnetic fields Hw and Hw '. Whereas conventional recording performs recording by forming a reversal magnetic domain in a magnetic thin film magnetized in one direction, in the recording according to the present invention, it is sufficient to form a magnetic domain in a demagnetized magnetic thin film. ,
The applied magnetic field required for recording may be smaller than in conventional recording. In the reproduction, as in the conventional reproduction, the polarization plane rotation of the laser light reflected from the magnetic thin film is extracted as a signal. Clearly, the rotation of the polarization plane due to the Kerr effect is different between a region having a magnetic domain and a demagnetized region, so that a sufficient reproduction signal can be obtained. When reproducing the demagnetized area, it is difficult to determine the individual magnetization in the vertical direction, and the reproduction signal from the recording medium is composed of the reproduction signal from the upper magnetization and the reproduction signal from the lower magnetization. Intermediate level. Figure 1 is an erase (c), the external magnetic field H E is applied, the magnetization state initial state after erasing the predetermined value and the laser beam P E of constant intensity in a region requiring the erase as shown in (d) of It becomes the same demagnetized state.

以下、本発明の詳細について図面に従って説明する。
第2図は本発明に係る光磁気記録再生消去装置の構成の
例を示したものである。
Hereinafter, details of the present invention will be described with reference to the drawings.
FIG. 2 shows an example of the configuration of a magneto-optical recording / reproducing / erasing apparatus according to the present invention.

垂直磁気異方性を有する磁性薄膜2を記録媒体とする
光磁気ディスク1の上方に光磁気記録用ヘッド3を設
け、光磁気ディスク1と光磁気記録用ヘッド3との間に
磁界印加手段として空心コイル4を設けた構成である。
前記磁性薄膜2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F
e,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5によって所定の速度で回転され
る。光磁気記録用ヘッド3は光磁気記録再生消去用の光
学系及び光検出機構を具備している。光磁気記録用ヘッ
ド3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。
A magneto-optical recording head 3 is provided above a magneto-optical disk 1 using a magnetic thin film 2 having perpendicular magnetic anisotropy as a recording medium, and a magnetic field applying means is provided between the magneto-optical disk 1 and the magneto-optical recording head 3. This is a configuration in which an air core coil 4 is provided.
The magnetic thin film 2 is a crystalline or amorphous magnetic thin film, for example, a crystalline magnetic thin film such as MnBi, MnCuBi, MnTiBi, MnAlGe, or a rare earth metal such as Sm, Tb, Gd, Dy, Ho and F.
An amorphous magnetic thin film formed by a combination with a transition metal such as e, Co, and Ni. The magneto-optical disk 1 is rotated at a predetermined speed by a disk drive motor 5. The magneto-optical recording head 3 includes an optical system for magneto-optical recording / reproducing and erasing and a light detecting mechanism. The magneto-optical recording head 3 itself is a magneto-optical disk 1 as indicated by an arrow in the figure.
At a predetermined speed in the radial direction.

前記光磁気記録用ヘッド3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。
In the magneto-optical recording head 3, 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.

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12トラッキン
グエラー検出用受光素子13によって検出されサーボ制御
回路14,15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16を通過後再生信号検出用受光素子17によって検
出され、再生信号増幅回路18によって増幅される。偏光
フィルタ16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17としてはたとえ
ばPINフォトダイオードまたはアバランシェ・フォトダ
イオードが使用される。レーザ光源6の変調にはレーザ
光源変調用回路19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のパワーを変調する。
The focus error and tracking error signals are respectively detected by the focus error detecting light receiving element 12 and the tracking error detecting light receiving element 13 and input to the servo control circuits 14 and 15 to become servo signals, which are fed back to the actuator 11. The reproduction signal is detected by the reproduction signal detecting light receiving element 17 after passing through the polarization filter 16 and is amplified by the reproduction signal amplifier circuit 18. As the polarizing filter 16, for example, a Glan-Thompson prism is used. As the reproduction signal detecting light receiving element 17, for example, a PIN photodiode or an avalanche photodiode is used. A laser light source modulation circuit 19 is used to modulate the laser light source 6, and modulates the power of the laser light source 6 at the time of recording, erasing, and reproducing.

前記空心コイル4は前記光磁気記録用ヘッド3と一体
化され電流供給源20から所望の印加磁界を得るための電
流が供給される。記録・消去に要する印加磁界は従来例
に比べて少なくてよいので、空心コイル4は従来より小
型のものでよい。
The air-core coil 4 is integrated with the magneto-optical recording head 3 and supplied with a current for obtaining a desired applied magnetic field from a current supply source 20. Since the applied magnetic field required for recording / erasing may be smaller than in the conventional example, the air-core coil 4 may be smaller than in the conventional example.

(実施例1) 第2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120mmφのプラスチック基板上に
スパッタ法によりTbFe膜を800Å厚に形成したディスク
を使用した。基板としてはあらかじめ幅0.8μm、ピッ
チ2.5μm深さ700Å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) Using the magneto-optical recording / reproducing / erasing apparatus shown in FIG. 2, information was recorded, reproduced, and erased on the magneto-optical disk.
As the magneto-optical disk, a disk in which a TbFe film was formed to a thickness of 800 mm by a sputtering method on a 120 mmφ plastic substrate was used. As the substrate, a so-called pre-group substrate in which a groove having a width of 0.8 μm and a pitch of 2.5 μm and a depth of 700 ° was formed in advance was used.

まず、光磁気ディスクを一方向に初期着磁したのち光
磁気ディスクに初期着磁方向に140Oeのバイアス磁界を
印加し、線速9m/secにてディスク面上4mWの一定強度レ
ーザ光を照射した。照射したディスクトラックの磁化状
態を偏光顕微鏡で観察した結果、一様に消磁されている
ことが確認された。
First, after the magnetized magneto-optical disk was initially magnetized in one direction, a bias magnetic field of 140 Oe was applied to the magneto-optical disk in the initial magnetized direction, and a constant intensity laser beam of 4 mW was irradiated on the disk surface at a linear velocity of 9 m / sec. . As a result of observing the magnetization state of the irradiated disk track with a polarizing microscope, it was confirmed that the disk track was uniformly demagnetized.

次に、消磁された光磁気ディスクに対して4mWのパワ
ーで印加磁界を変えて1MHzの信号の記録をおこなった。
再生C/Nは第3図に示すように磁化反転方向に0Oe以上な
らびに初期着磁方向に270Oe以上の範囲で飽和し、良好
な記録ができた。
Next, a 1 MHz signal was recorded on the demagnetized magneto-optical disk while changing the applied magnetic field at a power of 4 mW.
The reproduction C / N was saturated in the range of 0 Oe or more in the magnetization reversal direction and 270 Oe or more in the initial magnetization direction as shown in FIG. 3, and good recording was possible.

消去は初期着磁方向に140Oeの磁界を印加し4mWの一定
強度のレーザ光により実行された。記録信号の消え残り
はみられなかった。
The erasure was performed by applying a magnetic field of 140 Oe in the initial magnetization direction and using a laser beam having a constant intensity of 4 mW. No disappearance of the recorded signal was observed.

(実施例2) 実施例1に示した光磁気記録再生消去装置と光磁気デ
ィスクを用い、1MHzの信号の記録・消去の反復をおこな
った。
(Example 2) Using the magneto-optical recording / reproducing / erasing apparatus shown in Example 1 and a magneto-optical disk, recording / erasing of a 1 MHz signal was repeated.

記録パワー4mW、記録時印加磁界0Oe、消去パワー4m
W、消去時印加磁界140Oe(初期着磁方向)とした。105
回の反復によっても記録消去特性には変化がみられなか
った。
Recording power 4mW, recording applied magnetic field 0Oe, erase power 4m
W, the applied magnetic field at the time of erasing was 140 Oe (initial magnetization direction). 10 5
No change was observed in the recording / erasing characteristics even after the repetition.

(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.

磁性薄膜の消磁状態を初期状態としているので、従
来の記録再生消去方式に比べて、記録再生消去に要する
磁界変化量は1/2以下でよい。
Since the demagnetized state of the magnetic thin film is set to the initial state, the amount of change in magnetic field required for recording / reproducing / erasing may be 1/2 or less as compared with the conventional recording / reproducing / erasing method.

記録再生消去に要する磁界変化量が従来方式に比べ
て小さいので、磁界発生手段を小型化できそれに伴い光
磁気記録再生消去装置を軽量・小型化できる。
Since the amount of change in the magnetic field required for recording / reproducing / erasing is smaller than that of the conventional method, the magnetic field generating means can be reduced in size, and accordingly, the magneto-optical recording / reproducing / erasing device can be reduced in weight and size.

磁界発生手段の小型化により、磁界スイッチング速
度を速くすることができ、トラックのみならずセクター
単位の記録・消去が容易となる。
Due to the miniaturization of the magnetic field generating means, the magnetic field switching speed can be increased, and recording / erasing not only in tracks but also in sector units becomes easy.

また、本発明は光磁気ディスクとして実施例で示した
TbFe膜に限られるものではなく、光磁気記録用結晶性薄
膜あるいは非晶質磁性薄膜に広く適用できる。
Further, the present invention has been described in the embodiment as a magneto-optical disk.
The present invention is not limited to the TbFe film but can be widely applied to a crystalline thin film for magneto-optical recording or an amorphous magnetic thin film.

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

第1図は本発明に係る光磁気記録再生消去方式の動作モ
ード図、第2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3図は本発明の実施例で用いられた
光磁気ディスクの記録特性を示す図、第4図は従来の光
磁気記録再生消去方式の動作モード図である。 図中、1……光磁気ディスク、2……磁性薄膜、3……
光磁気記録用ヘッド、4……空心コイル、5……ディス
ク駆動用モーター、6……レーザ光源、7,8,9……ビー
ムスプリッタ、10……レーザビーム集光用レンズ、11…
…アクチュエータ、12,13……エラー検出用受光素子、1
4,15……サーボ制御回路、16……偏光フィルタ、17……
再生信号検出用受光素子、18……増幅回路、19……レー
ザ光源変調用回路、20……電流供給源である。
1 is an operation mode diagram of the magneto-optical recording / reproducing / erasing method according to the present invention, FIG. 2 is a configuration diagram of a magneto-optical recording / reproducing / erasing apparatus to which the present invention is applied, and FIG. 3 is used in an embodiment of the present invention. FIG. 4 is a diagram showing the recording characteristics of the magneto-optical disk obtained, and FIG. 4 is an operation mode diagram of a conventional magneto-optical recording / reproducing / erasing method. In the figure, 1 ... magneto-optical disk, 2 ... magnetic thin film, 3 ...
Magneto-optical recording head, 4 air-core coil, 5 disk drive motor, 6 laser light source, 7, 8, 9 beam splitter, 10 laser beam focusing lens, 11
… Actuator, 12, 13 …… Light receiving element for error detection, 1
4,15 ... servo control circuit, 16 ... polarizing filter, 17 ...
A light receiving element for detecting a reproduction signal, 18 an amplifier circuit, 19 a laser light source modulation circuit, and 20 a current supply 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含む記
録媒体に対しレーザ光によって情報の記録再生消去を行
う光磁気記録再生消去方法において、前記磁性薄膜の磁
化方向が再生用レーザ光のスポットサイズ内においてラ
ンダムな消磁状態を初期状態とし、一定磁界印加と情報
により変調されたレーザ光照射によって前記磁性薄膜に
磁区を形成する記録過程と、前記記録薄膜の磁区の有無
に対応したレーザ反射光の偏光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からなる光
磁気記録再生消去方法。
1. A magneto-optical recording / reproducing / erasing method for recording / reproducing / erasing information on a recording medium including a magnetic thin film having perpendicular magnetic anisotropy by using a laser beam, wherein the magnetization direction of the magnetic thin film is the same as that of the reproducing laser beam. A recording process of forming a magnetic domain in the magnetic thin film by applying a constant magnetic field and irradiating a laser beam modulated by information with a random demagnetized state as an initial state within the spot size, and a laser reflection corresponding to the presence or absence of a magnetic domain in the recording thin film A magneto-optical recording / reproducing / erasing method comprising: a reproducing process of reproducing information from a polarization rotation of light; and an erasing process 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】垂直磁気異方性を有する磁性薄膜を含む記
録媒体に対しレーザ光によって情報の記録再生消去を行
う光磁気記録再生消去装置において、磁化方向が再生用
レーザ光のスポットサイズ内においてランダムな消磁状
態を初期状態とする磁性薄膜から成る記録媒体と、該記
録媒体に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磁気記録用ヘッドと、記録・消去に
対して磁界発生手段に供給する電流を変化させることが
できる電流供給源とを備え、記録は、一定磁界印加と情
報により変調されたレーザ光照射によって前記磁性薄膜
に磁化方向が媒体面に対して上向き又は下向きの磁区を
形成することにより行い、再生は、前記記録薄膜の磁区
の有無に対応したレーザ反射光の偏光面回転を信号とし
て取り出すことにより行い、消去は、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
すことにより行うことを特徴とする光磁気記録再生消去
装置。
2. A magneto-optical recording / reproducing / erasing apparatus for recording / reproducing / erasing information on a recording medium including a magnetic thin film having perpendicular magnetic anisotropy by using a laser beam, wherein the magnetization direction is within the spot size of the reproducing laser beam. A recording medium comprising a magnetic thin film having a random demagnetized state as an initial state; a magnetic field generating means for applying a magnetic field to the recording medium; a magneto-optical recording head for irradiating the recording medium with laser light; And a current supply source capable of changing a current supplied to the magnetic field generating means. The recording is performed by applying a constant magnetic field and irradiating a laser beam modulated by information so that the magnetization direction of the magnetic thin film is directed upward with respect to the medium surface. Alternatively, the reproduction is performed by forming a downward magnetic domain, and the reproduction is performed by extracting the polarization plane rotation of the laser reflected light corresponding to the presence or absence of the magnetic domain of the recording thin film as a signal. Ri performed, erasing, magneto-optical recording and reproducing erasing apparatus which is characterized in that by returning the magnetization state of the recording thin film by a magnetic field applied and laser light irradiation demagnetized.
JP59225236A 1984-10-26 1984-10-26 Magneto-optical recording / reproduction / erasing method and apparatus Expired - Lifetime JP2604700B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59225236A JP2604700B2 (en) 1984-10-26 1984-10-26 Magneto-optical recording / reproduction / erasing method and apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59225236A JP2604700B2 (en) 1984-10-26 1984-10-26 Magneto-optical recording / reproduction / erasing method and apparatus

Publications (2)

Publication Number Publication Date
JPS61104444A JPS61104444A (en) 1986-05-22
JP2604700B2 true JP2604700B2 (en) 1997-04-30

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Country Link
JP (1) JP2604700B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2642639B2 (en) * 1987-09-14 1997-08-20 オリンパス光学工業株式会社 Magneto-optical recording method
US5014254A (en) * 1988-05-09 1991-05-07 U.S. Philips Corporation Magneto-optical recording method and magneto-optical recording apparatus

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59168951A (en) * 1983-03-16 1984-09-22 Sanyo Electric Co Ltd Optical magnetic disc device

Also Published As

Publication number Publication date
JPS61104444A (en) 1986-05-22

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