JPH0247017B2 - JIKIKOGAKUHETSUDO - Google Patents

JIKIKOGAKUHETSUDO

Info

Publication number
JPH0247017B2
JPH0247017B2 JP16449282A JP16449282A JPH0247017B2 JP H0247017 B2 JPH0247017 B2 JP H0247017B2 JP 16449282 A JP16449282 A JP 16449282A JP 16449282 A JP16449282 A JP 16449282A JP H0247017 B2 JPH0247017 B2 JP H0247017B2
Authority
JP
Japan
Prior art keywords
light
photodetector
optical
magneto
reflected
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
JP16449282A
Other languages
Japanese (ja)
Other versions
JPS5954054A (en
Inventor
Toshihisa Deguchi
Yoshikazu Fujii
Tetsuya Inui
Hideyoshi Yamaoka
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.)
Sharp Corp
Original Assignee
Sharp 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 Sharp Corp filed Critical Sharp Corp
Priority to JP16449282A priority Critical patent/JPH0247017B2/en
Publication of JPS5954054A publication Critical patent/JPS5954054A/en
Publication of JPH0247017B2 publication Critical patent/JPH0247017B2/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
    • G11B11/10532Heads

Description

【発明の詳細な説明】 <技術分野> 本発明は磁性膜を記憶媒体としレーザ光等の光
ビームを記憶媒体に照射することにより情報の記
録・再生・消去を行う光記憶装置に関するもので
あり、特にその光学装置に関する。
[Detailed Description of the Invention] <Technical Field> The present invention relates to an optical storage device that uses a magnetic film as a storage medium and records, reproduces, and erases information by irradiating the storage medium with a light beam such as a laser beam. , particularly regarding its optical device.

<従来技術> 近年、光記憶装置は高密度化、大容量化、及び
高速アクセス化が可能なメモリ装置として広く研
究されている。このうち記憶媒体に微細なピツト
列を形成し、該ピツト部における光ビームの回折
現象を利用して光再生する装置、あるいは記憶媒
体に屈折率の異なる領域をビツト状に形成し、そ
の反射率あるいは透過率の変化を利用して光再生
する装置について一部実用化が計られている。し
かしながら上記装置は再生専用あるいは情報の追
加記録が可能であるという機能をもつに留まつて
おり、メモリ装置の一大特徴たるべき消去機能を
もたないという問題を残している。
<Prior Art> In recent years, optical storage devices have been widely studied as memory devices capable of higher density, larger capacity, and faster access. Among these, there is a device that forms a fine pit row on a storage medium and uses the diffraction phenomenon of a light beam at the pit portion to reproduce light, or a device that forms bit-shaped regions with different refractive indexes on the storage medium and Alternatively, some devices for reproducing light using changes in transmittance are being put into practical use. However, the above devices only have the function of being read-only or capable of additionally recording information, and there remains the problem that they do not have an erasing function, which is a major feature of memory devices.

ところで光記憶装置のうち磁性体を記憶媒体と
する光磁気記憶装置は記録・再生・消去の3機能
を持ち有用な光記憶装置となりうるものである。
しかしながらこの光磁気記憶装置は再生光学系が
他の光記憶装置に比べて複雑なこと、及び光再生
信号の品質が悪いなどの問題点がありその実用化
が遅れている。
Incidentally, among optical storage devices, a magneto-optical storage device using a magnetic material as a storage medium has three functions of recording, reproducing, and erasing, and can be a useful optical storage device.
However, this magneto-optical storage device has problems such as its reproducing optical system being more complicated than other optical storage devices and the quality of the optical reproduction signal being poor, and its practical application has been delayed.

<目的> 本発明は上記の様な現状に鑑み光磁気記憶装置
の再生光学系の簡略化と光再生信号の信頼性の向
上を目的とする。
<Objective> In view of the above-mentioned current situation, it is an object of the present invention to simplify the reproduction optical system of a magneto-optical storage device and improve the reliability of optical reproduction signals.

<実施例> 以下本発明に係わる磁気光学ヘツドの実施例を
図面をもとに説明する。
<Embodiments> Examples of the magneto-optical head according to the present invention will be described below with reference to the drawings.

第1図は本発明に係る一実施例を示す構成図で
ある。1はGdTbFe、GdDyFe、GdTbDyFe、
TbFe等の非晶質磁性薄膜を基板上にスパツタリ
ングによつて被覆してなる記憶デイスクであり、
上記磁性薄膜をトレース誤差情報を得るための図
示しない凹凸状のガイドトラツクの上に形成され
ている。2は所定の強度のレーザ光を射出できる
レーザ装置、3は偏光子、4は前記記憶デイスク
1からの反射情報光を検出系側に導くとともに、
前記記憶媒体の磁化状態に応じて生じる磁気光学
回転角を増大させる機能をもつハーフプリズムで
あり、一例としてRp=0.3、Tp=0.7、Rs=0.99、
Ts=0.01の偏光特性をもつ場合には磁気光学回
転角を約1.6倍に増大させうるものである。5は
磁性薄膜上に微小スポツトを結ばせる対物レン
ズ、6は反射情報光を後述する光検出器上に集光
させるスポツトレンズ、7は反射情報光を直角方
向に2分するハーフプリズム(ビームスプリツ
タ)であり、S波・P波の透過率及び反射率が
1:1に近く、P波及びS波の位相ズレが小さい
という光学特性をもつ。このハーフプリズム7と
してはプリズム斜面にAgをコートしたものが適
用できる。8,9は反射情報光の回転角変位を所
定の方向に変化することのできる1/2波長板(8
は第1の1/2波長板、9は第2の1/2波長板)であ
る。
FIG. 1 is a configuration diagram showing an embodiment according to the present invention. 1 is GdTbFe, GdDyFe, GdTbDyFe,
A storage disk formed by sputtering a substrate with an amorphous magnetic thin film such as TbFe.
The magnetic thin film is formed on an uneven guide track (not shown) for obtaining tracing error information. 2 is a laser device capable of emitting a laser beam of a predetermined intensity; 3 is a polarizer; 4 guides the reflected information light from the storage disk 1 to the detection system side;
It is a half prism that has a function of increasing the magneto-optical rotation angle that occurs depending on the magnetization state of the storage medium, and for example, Rp = 0.3, Tp = 0.7, Rs = 0.99,
When the polarization characteristic is Ts=0.01, the magneto-optic rotation angle can be increased by about 1.6 times. 5 is an objective lens that connects a minute spot on the magnetic thin film, 6 is a spot lens that focuses the reflected information light onto a photodetector, which will be described later, and 7 is a half prism (beam splitter) that divides the reflected information light into two at right angles. It has the optical properties that the transmittance and reflectance of S waves and P waves are close to 1:1, and the phase shift of P waves and S waves is small. As this half prism 7, a prism whose inclined surface is coated with Ag can be used. 8 and 9 are half-wave plates (8 and 9) that can change the rotation angle displacement of the reflected information light in a predetermined direction
is a first 1/2 wavelength plate, and 9 is a second 1/2 wavelength plate).

該1/2波長板の作用を第2図を用いて説明する。
第2図はハーフプリズム7を通過した後の反射情
報光の偏光状態をベクトルで示したものである。
但し記憶デイスク1に入射するレーザ光の偏光状
態はPの方向とする。第2図においてM+、M-
記憶デイスク1における磁化情報に対応した反射
情報光の偏光状態を示す。但し、同図のM+、M-
は光の記憶デイスク1で反射された光が磁気光学
効果を増大させる機能をもつハーフプリズム4で
磁気光学回転角が増大された結果の光である。こ
の反射情報光M+、M-はハーフプリズム7(この
ハーフプリズム7は前述したようにS波・P波の
透過率及び透過率が1:1に近く、P波・S波の
位相ズレが小さい。よつて磁気光学回転角を増大
させる機能はなく単に光を2分するだけである。)
によりほぼ2分されて後1/2波長板8,9に入射
する。該1/2波長板8,9の構造はその光学軸に
平行に切断され、所定の厚さに仕上げられた水晶
板あるいは雲母板であり、互いに直交する偏波面
をもつ偏光の位相を相対的に最大180゜ズラすこと
ができる。従つて、入射偏光の方位だけを変化さ
せることが可能である。
The action of the 1/2 wavelength plate will be explained using FIG. 2.
FIG. 2 shows the polarization state of the reflected information light after passing through the half prism 7 using vectors.
However, the polarization state of the laser beam incident on the storage disk 1 is assumed to be in the P direction. In FIG. 2, M + and M - indicate the polarization state of the reflected information light corresponding to the magnetization information on the storage disk 1. In FIG. However, M + and M - in the same figure
is the light that is the result of the magneto-optic rotation angle of the light reflected by the optical storage disk 1 being increased by the half prism 4 which has the function of increasing the magneto-optic effect. These reflected information beams M + and M - pass through the half prism 7 (as mentioned above, this half prism 7 has a transmittance of S and P waves close to 1:1, and a phase shift between P and S waves. It is small. Therefore, it does not have the function of increasing the magneto-optical rotation angle, but simply divides the light into two.)
The light is split into approximately two halves by the light beam and enters the rear half-wave plates 8 and 9. The structure of the 1/2 wavelength plates 8 and 9 is a quartz plate or a mica plate cut parallel to the optical axis and finished to a predetermined thickness. It can be shifted by up to 180°. Therefore, it is possible to change only the orientation of the incident polarized light.

今、反射情報光M+、M-に対して1/2波長板8,
9の位相の遅れる軸の方位をそれぞれ第2図A,
Bのように設定すると、1/2波長板8,9を通過
してくる偏光は同図のM+A、M-A、M+B、M-B
様に表わされる。即ち、1/2波長板8では遅延軸
の方位がAに設定されており、A方位と(S)軸
のなす角の2倍だけM+、M-が反時計回りに変化
し、M+A、M-Aのベクトルとなる。又、1/2波長
板9では遅延軸の方位がBに設定されており、B
方位と(S)軸のなす角の2倍だけM+、M-が時
計回りに変化し、M+B、M-Bのベクトルになる。
この第2図から明らかなように1/2波長板を介す
ることで通過した光ビームの記憶媒体の磁化情報
に対応した偏光情報の差が強調される。尚、前記
1/2波長板8,9の遅延軸の方位A,Bは入射偏
光の方位に対して通常一方が(n/4π−π/8)、他 方が(n/4π+π/8)の値に設定にする。ここで、 nは0、1、2、…の整数である。これによつて
A方位とB方位の互いのなす角を45゜に設定して
いる。
Now, for the reflected information light M + and M - , the 1/2 wavelength plate 8,
The directions of the axes with delayed phase of 9 are shown in Fig. 2A and 9, respectively.
When set as shown in B, the polarized light passing through the half-wave plates 8 and 9 is expressed as M +A , M -A , M +B , and M -B in the figure. That is, in the half-wave plate 8, the direction of the delay axis is set to A, and M + and M - change counterclockwise by twice the angle between the A direction and the (S) axis, and M + A becomes a vector of M -A . In addition, the direction of the delay axis of the 1/2 wavelength plate 9 is set to B;
M + and M - change clockwise by twice the angle between the azimuth and the (S) axis, becoming vectors M +B and M -B .
As is clear from FIG. 2, the difference in polarization information corresponding to the magnetization information of the storage medium of the light beam passing through the half-wave plate is emphasized. Note that the orientations A and B of the delay axes of the half-wave plates 8 and 9 are usually one (n/4π-π/8) and the other (n/4π+π/8) with respect to the orientation of the incident polarized light. Set to value. Here, n is an integer of 0, 1, 2,... As a result, the angle between the A direction and the B direction is set to 45 degrees.

以上の設定により互いに直交する偏波面をもつ
光を2分する偏光ビームスプリツタ10,11
(10は第1の偏光ビームスプリツタ、11は第
2の偏光ビームスプリツタ)のそれぞれの偏光軸
を同図のS,P(Sの偏光方向の光は反射し、P
の偏光方向の光は透過する。)とすると該偏光ビ
ームスプリツタを経た光は、記憶デイスク1の磁
化状態に応じて強度変調されたものとなる。従つ
て該偏光ビームスプリツタの各々の反射側に設置
された光検出器12,13(12は第1の光検出
器、13は第2の光検出器)には互いに逆位相の
光が得られる。図示しない差動増巾器に上記光検
出器12,13の出力信号を入力することにより
偏波面の変化する情報(記録情報)のみを得るこ
とができる。
Polarizing beam splitters 10 and 11 that divide light having mutually orthogonal polarization planes into two with the above settings.
(10 is the first polarizing beam splitter, 11 is the second polarizing beam splitter).
Light with polarization direction is transmitted. ), the light passing through the polarizing beam splitter is intensity-modulated according to the magnetization state of the storage disk 1. Therefore, the photodetectors 12 and 13 (12 is the first photodetector, 13 is the second photodetector) installed on the reflective side of each of the polarizing beam splitters receive light with opposite phases to each other. It will be done. By inputting the output signals of the photodetectors 12 and 13 to a differential amplifier (not shown), only information (recorded information) whose plane of polarization changes can be obtained.

一方、前記偏光ビームスプリツタ10,11の
透過側に配した光検出器14,15(第3の光検
出器)のうち一方は前記記憶デイスク1と対物レ
ンズ5との相対距離の変化を検出する即ちフオー
カスサーボ用の光検出器(この光検出器として
は、例えば4分割検出器を用い、反射光の光軸中
心に対して、その光検出器の分割中心を一方の分
割線の方向に微少距離ずらすことで容易にフオー
カスサーボ用の信号を得ることができる。この構
成については先に出願した特願昭56−173975に明
記される。この構成とは異なる他の周知なフオー
カスサーボ用信号を得るための光学系を配置して
も無論構わない。)であり、他方は前記記憶デイ
スク1に設けられたガイドトラツクとレーザ光ス
ポツトの相対的な位置ズレを検出する即ちトラツ
クサーボ用の光検出器(この光検出器としては、
例えばトラツク方向に分割線を有する2分割検出
器を用いることで周知のプツシユプル法により容
易にトラツクサーボ用の信号を得ることができ
る。)である。該光検出器14,15によつて得
た誤差信号は図示しない増巾回路および位相補償
回路を経て図示しない駆動機構にフイードバツク
されて、フオーカス方向、トラツク方向に対物レ
ンズ5、もしくは光学ヘツド全体を駆動制御し
て、レーザ光スポツトを所定の位置に結ばせる様
に構成されている。
On the other hand, one of the photodetectors 14 and 15 (third photodetector) arranged on the transmission side of the polarizing beam splitters 10 and 11 detects a change in the relative distance between the storage disk 1 and the objective lens 5. In other words, a photodetector for focus servo (for example, a 4-split detector is used, and the splitting center of the photodetector is aligned in the direction of one dividing line with respect to the optical axis center of the reflected light. A focus servo signal can be easily obtained by shifting the focus servo by a small distance.This configuration is specified in the previously filed Japanese Patent Application No. 56-173975. (Of course, an optical system for obtaining servo signals may be provided.), and the other is a track servo system that detects the relative positional deviation between the guide track provided on the storage disk 1 and the laser beam spot. photodetector (this photodetector is
For example, by using a two-part detector having a dividing line in the track direction, a track servo signal can be easily obtained by the well-known push-pull method. ). The error signals obtained by the photodetectors 14 and 15 are fed back to a drive mechanism (not shown) via an amplification circuit and a phase compensation circuit (not shown), and drive the objective lens 5 or the entire optical head in the focus direction and track direction. It is configured to drive and control the laser beam spot to connect it to a predetermined position.

尚、前記光検出器14,15はフオーカス用、
トラツク用に必らずしも分離されなくとも、一個
の光検出器により両方の制御信号を得る様に構成
しても良く、例えば一方の光検出器よりフオーカ
ス及びトラツク誤差信号を得、他方の光検出器よ
り記憶デイスク1と光学ヘツドの傾斜を検出し、
制御信号にフイードバツクする様にすることもで
きる。
Note that the photodetectors 14 and 15 are for focus,
Although they are not necessarily separated for tracking, it may be configured to obtain both control signals using one photodetector. For example, one photodetector may be used to obtain focus and track error signals, while the other photodetector may be used to obtain focus and track error signals. The inclination of the storage disk 1 and the optical head is detected by a photodetector,
It is also possible to provide feedback to the control signal.

或いは前述した偏光ビームスプリツタ10,1
1の透過側に配した光検出器14,15にて得ら
れた信号から記録情報信号を得、偏光ビームスプ
リツタ10,11の反射側に配した光検出器1
2,13にて得られた信号からフオーカスサーボ
用信号或いはトラツクサーボ用信号等の制御信号
を得るようにした構成としてもよい。
Or the aforementioned polarizing beam splitter 10,1
The recording information signal is obtained from the signal obtained by the photodetectors 14 and 15 placed on the transmission side of the polarizing beam splitters 10 and 11.
A configuration may be adopted in which a control signal such as a focus servo signal or a track servo signal is obtained from the signals obtained in steps 2 and 13.

<効果> 以上詳細に説明した本発明によれば、反射情報
光の中で従来では検出後に廃棄されていたものを
積極的に制御信号用光として利用することが可能
であり、この事によつて光学系を簡略化できるも
のである。又反射情報光の偏光方位の設定に1/2
波長板を用いる事によつて、任意の偏光方位の反
射情報光が得られ、この事によつて差動光学系を
構成する光ヘツドとして極めて優れたものを得
る。
<Effects> According to the present invention described in detail above, it is possible to actively utilize the reflected information light, which was conventionally discarded after detection, as control signal light. Therefore, the optical system can be simplified. Also, 1/2 for setting the polarization direction of the reflected information light.
By using a wavelength plate, reflected information light of any polarization direction can be obtained, thereby providing an extremely excellent optical head constituting a differential optical system.

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

第1図は本発明に係る磁気光学ヘツドの一実施
例の構成図、第2図はその反射情報光の偏光状態
を示すベクトル図である。 図中、1:記憶デイスク、2:レーザ装置、
3:偏光子、4:ハーフプリズム、5:対物レン
ズ、6:スポツトレンズ、7:ハーフプリズム、
8,9:1/2波長板、10,11:偏光ビームス
プリツタ、12,13,14,15:光検出器。
FIG. 1 is a block diagram of an embodiment of a magneto-optical head according to the present invention, and FIG. 2 is a vector diagram showing the polarization state of reflected information light. In the figure, 1: storage disk, 2: laser device,
3: Polarizer, 4: Half prism, 5: Objective lens, 6: Spot lens, 7: Half prism,
8, 9: 1/2 wavelength plate, 10, 11: polarizing beam splitter, 12, 13, 14, 15: photodetector.

Claims (1)

【特許請求の範囲】 1 磁性薄膜を記憶媒体とし、該記憶媒体へのレ
ーザ光の照射により、情報の記録・再生・消去を
行う光磁気記憶装置の磁気光学ヘツドにおいて、 前記記憶媒体からの反射光ビームを2分するビ
ームスプリツタと、 該ビームスプリツタによつて分離された各光ビ
ームの光軸上に配置された第1及び第2の1/2波
長板とを備え、 該第1及び第2の1/2波長板の遅延軸の方位角
を、通過した光ビームの記憶媒体の磁化情報に対
応した偏光状態の差が強調されるように互いに異
ならせ、 該1/2波長板を通過した光の光軸上に互いに直
交する偏光面を有する第1及び第2の偏光ビーム
スプリツタと、 該第1及び第2の偏光ビームスプリツタによつ
て反射(若しくは透過)された光をそれぞれ検出
する第1及び第2の光検出器と、 前記2つの偏光ビームスプリツタによつて透過
(若しくは反射)された光を検出する少なくとも
1つの第3の光検出器と、 前記第1及び第2の光検出器の出力を差動する
ことにより記録情報を得る回路手段と、 前記第3の光検出器の出力からサーボ用の信号
を得る回路手段と、 を備えたことを特徴とする磁気光学ヘツド。
[Scope of Claims] 1. In a magneto-optical head of a magneto-optical storage device that uses a magnetic thin film as a storage medium and records, reproduces, and erases information by irradiating the storage medium with a laser beam, there is provided the following: comprising: a beam splitter that splits a light beam into two; and first and second half-wave plates disposed on the optical axis of each light beam separated by the beam splitter; and the azimuth angles of the delay axes of the second 1/2 wavelength plate are made different from each other so as to emphasize the difference in the polarization state corresponding to the magnetization information of the storage medium of the light beam that has passed through the 1/2 wavelength plate, first and second polarizing beam splitters having planes of polarization perpendicular to each other on the optical axis of the light that has passed therethrough; and light reflected (or transmitted) by the first and second polarizing beam splitters. at least one third photodetector that detects the light transmitted (or reflected) by the two polarizing beam splitters; and at least one third photodetector that detects the light transmitted (or reflected) by the two polarizing beam splitters. and circuit means for obtaining recorded information by differentially outputting the output of the second photodetector; and circuit means for obtaining a servo signal from the output of the third photodetector. magneto-optical head.
JP16449282A 1982-09-20 1982-09-20 JIKIKOGAKUHETSUDO Expired - Lifetime JPH0247017B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16449282A JPH0247017B2 (en) 1982-09-20 1982-09-20 JIKIKOGAKUHETSUDO

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16449282A JPH0247017B2 (en) 1982-09-20 1982-09-20 JIKIKOGAKUHETSUDO

Publications (2)

Publication Number Publication Date
JPS5954054A JPS5954054A (en) 1984-03-28
JPH0247017B2 true JPH0247017B2 (en) 1990-10-18

Family

ID=15794181

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16449282A Expired - Lifetime JPH0247017B2 (en) 1982-09-20 1982-09-20 JIKIKOGAKUHETSUDO

Country Status (1)

Country Link
JP (1) JPH0247017B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH07101523B2 (en) * 1986-09-12 1995-11-01 キヤノン株式会社 Magneto-optical signal reproducing device

Also Published As

Publication number Publication date
JPS5954054A (en) 1984-03-28

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