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JPS59215046A - Method for recording and reproducing optomagnetism - Google Patents

Method for recording and reproducing optomagnetism

Info

Publication number
JPS59215046A
JPS59215046A JP8886683A JP8886683A JPS59215046A JP S59215046 A JPS59215046 A JP S59215046A JP 8886683 A JP8886683 A JP 8886683A JP 8886683 A JP8886683 A JP 8886683A JP S59215046 A JPS59215046 A JP S59215046A
Authority
JP
Japan
Prior art keywords
recording
magneto
optical recording
pit
laser light
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
JP8886683A
Other languages
Japanese (ja)
Other versions
JPH0546021B2 (en
Inventor
Nobuhiko Sakai
酒井 順彦
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.)
Dai Nippon Printing Co Ltd
Original Assignee
Dai Nippon Printing Co Ltd
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 Dai Nippon Printing Co Ltd filed Critical Dai Nippon Printing Co Ltd
Priority to JP8886683A priority Critical patent/JPS59215046A/en
Publication of JPS59215046A publication Critical patent/JPS59215046A/en
Publication of JPH0546021B2 publication Critical patent/JPH0546021B2/ja
Granted legal-status Critical Current

Links

Classifications

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

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To attain ease of reproduction of information by scanning a laser light while vibrating the light in the direction orthogonal to the scanning direction. CONSTITUTION:The laser light from a laser light source 1 and a photomagnetic recording medium 5 are moved relatively and linearly to record the data and the recording width is expanded by vibrating mechanically a fixed mirror 3 or the like. In reproducing the laser light while vibrating the light, the laser light scans on a pit 13 and at the outside of the pit of the photomagnetic medium 5 along a scanning line 14. In eliminating a signal twice the mirror vibrating number from an output signal by means of a filter, a signal shown in the figure is obtained. Even if the pit has a minute defect, when the width of defect is narrower than the pit width, the reproduction is made possible. The detection of a recording track and the tracking of the reproducing head to the recording track are attained easily and sure reproduction is attained even with variation in the manufacture of recording media.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は光磁気記録材料の記録位置精度のばらつきをレ
ーザー光の走査方式により補なう光磁気記録再生方法に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a magneto-optical recording and reproducing method that compensates for variations in recording position accuracy of magneto-optical recording materials using a laser beam scanning method.

(従来技術) 光磁気記録材料の光磁気記録層に一定磁場を作用させつ
つ集光されたレーザー光を照射し、照射部の光磁気記録
層の磁気モーメントを反転させることにより記録を行な
い、又、このようにして記録された光磁気記録材料の光
磁気記録層にレーザー光を照射し、得られる反射光の偏
光面の回転を検出することにより記録された情報を再生
する光磁気記録再生方法自体は既に知られている。光磁
気記録再生方法自体は非接触で情報の再生が出来、しか
も記録密度が他の記録再生方法にくらべて高い利点を有
している。
(Prior art) Recording is performed by irradiating a magneto-optical recording layer of a magneto-optical recording material with a focused laser beam while applying a constant magnetic field, and reversing the magnetic moment of the magneto-optical recording layer in the irradiated area. , a magneto-optical recording and reproducing method for reproducing recorded information by irradiating the magneto-optical recording layer of the magneto-optical recording material recorded in this way with a laser beam and detecting the rotation of the polarization plane of the resulting reflected light. itself is already known. The magneto-optical recording and reproducing method itself allows information to be reproduced without contact, and has the advantage of higher recording density than other recording and reproducing methods.

しかし々がら光学記録再生方法においては情報はせいぜ
い1μ巾程度のトラックに収まるため、情報の記録位置
を正確に検出し、トラックから外れないように走査して
再生する必要がある。
However, in the optical recording and reproducing method, information is stored in a track with a width of about 1 μm at most, so it is necessary to accurately detect the recording position of the information and scan and reproduce the information so as not to deviate from the track.

一般的な光磁気記録再生方式におけるようにトラックが
らせん状若しくは同心円状であるときは中心の位置精度
が成る程度維持されていれば光磁気ディスクの周辺部か
ら中心部に向かってほぼ直線状に走査を行なえばトラッ
クの検出、及び追随は比較的容易に行なえ光磁気ディス
クの駆動の偏りは周期的であって対応が可能である。こ
のよう外光磁気ディスクは記録容重が大きく、ランダム
アクセスも可能なため画像、オーディオ、電子計算機の
記憶媒体の分野に利用されている。一方、光磁気記録再
生方法は記録密度が高いだめ、小型の携帯可能な記録媒
体としても利用可能であり、例えば、現在、磁気カード
、情報カード、商品タグ、英会話カード等の磁気方式が
利用されている分野に利用すると同じ大きさの記録媒体
により多くの情報を記録再生することが可能である。し
かし、これらの記録媒体を商業的に利用する際には記録
媒体の寸法精度、記録位置の精度に加えて記録媒体の走
行精度のばらつきがあり、又、これらの記録媒体におけ
る記録は直線状になされているため記録部分の検出及び
追随には精密な走行のだめの駆動装置を要し、しかも駆
動の偏りはランダムであり、光磁気ディスクにくらべる
と特に再生」二の困ガ1さを有している。例えば磁気カ
ードを光磁気記録再生方式のカードに置き換えたものを
例にとるとその寸法精度は±50μ〜±100μ程度で
あり、レーザービームの径が1μ程度であることを考慮
すると再生時には記録部の検出とその追随のだめの手段
を講じなければならない。記録部の検出と追随のため、
光学記録による線や、機械的加工による溝を予め案内用
に設けておき、光学的、機械的にこれらの案内用の線や
溝を検出して追随する一方、本来の情報記録はこれらの
線や溝と平行なある間隔を保った位置に行なっておき、
再生を容易に行々おうとする試みが提案されている。し
かしこのように案内用の溝や線を設ける事及びこれらの
検出のだめの手段が記録再生の手段以外に必要であり煩
雑さが避けられないものである。
When the track is spiral or concentric as in a general magneto-optical recording/reproducing system, if the positional accuracy of the center is maintained to a certain degree, the track will be approximately straight from the periphery to the center of the magneto-optical disk. If scanning is performed, it is relatively easy to detect and follow the track, and deviations in the driving of the magneto-optical disk are periodic and can be dealt with. Such external optical magnetic disks have a large recording capacity and can be randomly accessed, so they are used in the fields of image, audio, and computer storage media. On the other hand, the magneto-optical recording and reproducing method has a high recording density and can also be used as a small, portable recording medium.For example, the magnetic method is currently used for magnetic cards, information cards, product tags, English conversation cards, etc. When used in the field of technology, it is possible to record and reproduce more information on a recording medium of the same size. However, when these recording media are used commercially, there are variations in the dimensional accuracy of the recording media, the accuracy of the recording position, and the running accuracy of the recording media, and the recording on these recording media is not linear. Because of this, a precise drive device is required to detect and track the recorded portion, and the drive bias is random, making playback particularly difficult compared to magneto-optical disks. ing. For example, if a magnetic card is replaced with a magneto-optical recording and reproducing card, its dimensional accuracy is approximately ±50μ to ±100μ, and considering that the diameter of the laser beam is approximately 1μ, the recording area during playback is Measures must be taken to detect this and prevent it from being followed. For detection and tracking of recording section,
Lines created by optical recording or grooves created by mechanical processing are prepared in advance for guidance purposes, and while these guidance lines and grooves are detected and followed optically and mechanically, original information recording is based on these lines. Do this at a position parallel to the groove and at a certain distance.
Attempts have been made to facilitate regeneration. However, provision of such guide grooves and lines and means for detecting these are necessary in addition to recording and reproducing means, and complexity is unavoidable.

(発明の目的) 本発明者は上記の従来技術における欠点を解消するため
種々研究の結果、」−記のような直線状に情報を記録す
る記録媒体においては、その直線方向の記録密度が高い
ことが要求されるが、反面、中方向の記録密度は叱較的
問題にならないことが多く、このため、中方向に拡大し
て記録を行なえば、直線方向の記録密度、ひいては記録
媒体自体の記録密度は低下せず、却って再生時の走行精
度のばらつきを吸収しうろことを見い出し、しかもこの
ように記録されている記録媒体を再生する際のレーザー
光をその走査方向に直角に振動させることにより情報の
再生が容易になることをも見い出して本発明に到達した
ものである。
(Objective of the Invention) As a result of various studies to eliminate the drawbacks of the above-mentioned prior art, the present inventor has found that a recording medium that records information in a straight line, such as the one shown in the figure, has a high recording density in the straight direction. However, on the other hand, the recording density in the middle direction is often not a critical issue, so if you enlarge the recording in the middle direction, the recording density in the straight direction, and by extension the recording medium itself, will be reduced. We found a way to absorb variations in running accuracy during playback without reducing the recording density, and to vibrate the laser beam perpendicular to the scanning direction when playing back a recording medium recorded in this way. The present invention was also achieved by discovering that information can be easily reproduced.

即ち、本発明は、光磁気記録材料の光磁気記録層に磁場
を作用させつつレーザー光を集光して走査することによ
り記録再生を行なう光磁気記録再生方法において、レー
ザー光を走査方向に対して直角方向に振動させつつ走査
することを特徴とする光磁気記録再生方法をその主旨と
するものである。
That is, the present invention provides a magneto-optical recording and reproducing method in which recording and reproducing is performed by focusing and scanning a laser beam while applying a magnetic field to a magneto-optical recording layer of a magneto-optical recording material. The gist of this method is a magneto-optical recording and reproducing method characterized by scanning while vibrating in the perpendicular direction.

(発明の構成) 本発明において使用しうる光磁気記録材料としては平滑
で耐熱性のある基材上にスパッタリング等の方法で形成
したGd −Co 、Gd −Tb−C。
(Structure of the Invention) Magneto-optical recording materials that can be used in the present invention include Gd-Co and Gd-Tb-C formed on a smooth and heat-resistant base material by a method such as sputtering.

等のアモルファス(非晶質)磁性膜を有するものを挙げ
ることができるが、これら以外のものでも使用しうる。
Examples include those having an amorphous magnetic film such as, but materials other than these may also be used.

これらの光磁気記録材料に記録を行なうには通常の方法
を利用し、更に部分的に改変して行なう。例えば第1図
に示すごとくレーザー光源1より出射されたレーザー光
は偏光器2を介して固定ミラー3により反射され、集光
レンズ4を用いて集光させ、光磁気記録材料5の光磁気
記録層6に照射される。光磁気記録層6は垂直方向、即
ち層6の厚み方向に予め磁化配向されたものを使用する
。レーザー光を照射する際には集光レンズ4と光磁気記
録材料5との間に磁気コイル7を介して行なう。又、光
磁気記録材料に記録された情報を再生するには、上記と
はゾ同様にしてレーザー光を光磁気記録層に照射して得
られる反射光をコイル7、集光レンズ4を経て八−フミ
ラー8に導入し、分割された一方の光を検光子9及び光
検知器10を用いて、又、他方の光を検光子11及び光
検知器12を用いてそれぞれ電気信号に変換し読み取り
を行なうものである。検光子9及び1】は所定の方向の
光のみを通過させるものであるので、光磁気記録材料5
の磁気モーメントに応じて異なる偏光角を有する反射光
のうち、所定の偏光角を持つ反射光のみを通過させる。
To record on these magneto-optical recording materials, conventional methods are used, with some modifications made. For example, as shown in FIG. 1, a laser beam emitted from a laser light source 1 is reflected by a fixed mirror 3 via a polarizer 2, and is focused using a condensing lens 4 to record magneto-optical information on a magneto-optical recording material 5. Layer 6 is irradiated. The magneto-optical recording layer 6 used is one whose magnetization is previously oriented in the perpendicular direction, that is, in the thickness direction of the layer 6. Laser light is irradiated via a magnetic coil 7 between the condenser lens 4 and the magneto-optical recording material 5. Furthermore, in order to reproduce the information recorded on the magneto-optical recording material, the reflected light obtained by irradiating the magneto-optical recording layer with a laser beam is passed through the coil 7 and the condensing lens 4 in the same manner as described above. - One of the split lights is introduced into the fumirror 8, and the other split light is converted into an electrical signal using the analyzer 9 and the photodetector 10, and the other light is converted into an electrical signal and read using the analyzer 11 and the photodetector 12. This is what we do. Analyzers 9 and 1 allow only light in a predetermined direction to pass through, so the magneto-optical recording material 5
Of the reflected lights having different polarization angles depending on the magnetic moment of the magnet, only the reflected lights having a predetermined polarization angle are allowed to pass through.

なお、上記の記録・再生において光磁気記録材料5に入
射するレーザー光の出力がある一定限度以上であれば記
録が行なわれるものである。
In addition, in the above-mentioned recording and reproduction, recording is performed if the output of the laser light incident on the magneto-optical recording material 5 is above a certain limit.

上記方tノEにおいて、本発明においては特にレーザー
光と光学記録再生とを相対的に直線的に移動させつつ直
線状に記録を行ない、なおかつ、直線の長さ方向とは直
角の方向に記録層を拡大させる。拡大は種々の方法で行
ない得るが、後述する再生と同一の方法で行なうとすれ
ばレーザー光をl]方向に振動させるのがよく、振動は
第1図中性号3で示す固定ミラーを機械的に振動させる
か、或いは固定ミラーを用いるかわりにT”c 02 
、 L IN+)05等の結晶(「音響光学偏光器」と
呼ばれる)を用い、該結晶内に超音波を発生させてレー
ザー光を回折させる方法によって行なうことができる。
In the above method, in the present invention, recording is performed in a straight line while moving the laser beam and the optical recording/reproducing device relatively linearly, and the recording is performed in a direction perpendicular to the length direction of the straight line. Expand the layers. Enlargement can be done in various ways, but if it is done in the same way as the reproduction described later, it is best to vibrate the laser beam in the l] direction. T”c 02 instead of vibrating or using a fixed mirror.
, LIN+) 05 (referred to as an "acousto-optic polarizer"), and generates ultrasonic waves in the crystal to diffract laser light.

振動の周波数、振l]等は光学記録材料の製作精度、レ
ーザービームの径等の条件によっても異々るので一概に
は言えないが、前記した記録媒体用であれば光磁気記録
材料の寸法精度は±50μ〜±100μであり、レーザ
ービームの集光状態での直径を1μ、光磁気記録材料の
走査速度を100 ytrm /see  とすれば、
振動の周波数は例えば10 Q kHz 、II上、振
[11は光学記録4′Aネエ1上で少くとも100μ〜
200μである。上記条件や振動については以上の数値
は一例であってこれらに拘束されるものではないが、レ
ーザービーム径は通常0.5μ〜1.5μ程度であり、
レーザービーム径を太くすると各ピットの形状の精度が
悪くなるため、細い方が好ましい。各ピットの直線走査
方向の長さは通常5μ〜50μ程度である。又、光磁気
記録材料の走査速度は現在の磁気カードの走査速度(8
0vm /5ee)を基亭とすればよいが、これに拘束
されるものではない。走査時のレーザービームの振動数
は光磁気記録材料の走査速度をレーザービーム径で除し
て得られる数値を目安とじ又、振巾は光学記録材料の寸
法のバラツキの範囲を充分カバーできればよい。
The frequency of vibration, vibration l] etc. vary depending on conditions such as the manufacturing precision of the optical recording material and the diameter of the laser beam, so it cannot be stated unconditionally, but if it is for the above-mentioned recording medium, the dimensions of the magneto-optical recording material. The accuracy is ±50μ to ±100μ, and if the diameter of the laser beam in the condensed state is 1μ and the scanning speed of the magneto-optical recording material is 100 ytrm/see,
The frequency of the vibration is, for example, 10 Q kHz, on II, the vibration [11 is at least 100 μ on optical recording 4'A
It is 200μ. Regarding the above conditions and vibrations, the above numerical values are just examples and are not restricted to these, but the laser beam diameter is usually about 0.5μ to 1.5μ,
If the diameter of the laser beam is increased, the accuracy of the shape of each pit will deteriorate, so a smaller diameter is preferable. The length of each pit in the linear scanning direction is usually about 5 to 50 microns. Furthermore, the scanning speed of magneto-optical recording materials is faster than the scanning speed of current magnetic cards (8.
0vm/5ee) may be used as the basic value, but it is not limited to this. The frequency of the laser beam during scanning is determined by dividing the scanning speed of the magneto-optical recording material by the diameter of the laser beam, and the amplitude should be sufficient to cover the range of variations in the dimensions of the optical recording material.

このように光磁気記録の施された光磁気記録材料を再生
する際にも第1図に示すような公知の方法を用い、但し
上記の記録とほぼ同様に集光されたレーザービームを前
記したような方法により走査方向とは直角方向に振動さ
せることを付加して行々えばよく、振動の周波数及び振
巾は記録の際と同様に、出来れば振1]についてはやや
大きめにして行なうとよい。
When reproducing the magneto-optical recording material that has been subjected to magneto-optical recording in this way, a known method as shown in FIG. It is sufficient to add vibration in a direction perpendicular to the scanning direction using a method such as this, and the frequency and amplitude of vibration should be the same as in recording, but if possible, vibration 1] should be slightly larger. good.

なお、本発明においてレーザー光を振動させつつ再生を
行なうと、第2図fa)に示すよう外信号が出力される
。これは第3図に示すように蛇行した走査線14に沿っ
てレーザー光が光磁気記録材料5のピット(記録された
部分の凹み)13上及びピット上を外れた部分をも走査
するため、ピット上を走査している時間だけ出力信号が
変化するからである。第2図(a)に示すような出力信
号からミラー振動数の2倍の信号をフィルターで除くと
、第2図(b)で示すような信号が得られる。出力信号
にこのような操作を施こすことにより、例えばある一つ
のピットに微小な欠損があっても欠損箇所の巾がピット
中(走査方向と直角方向のピット中)よりも狭ければ再
生を可能とすることができる。
In the present invention, when reproduction is performed while the laser beam is vibrated, an external signal is output as shown in FIG. 2 fa). This is because, as shown in FIG. 3, the laser beam scans over the pits (indentations in recorded areas) 13 of the magneto-optical recording material 5 as well as over the areas outside the pits along the meandering scanning line 14. This is because the output signal changes during the time the pit is scanned. When a signal having twice the mirror frequency is removed from the output signal as shown in FIG. 2(a) by a filter, a signal as shown in FIG. 2(b) is obtained. By performing this kind of operation on the output signal, for example, even if there is a minute defect in one pit, if the width of the defective part is narrower than the width of the pit (in the pit in the direction perpendicular to the scanning direction), playback can be performed. It can be made possible.

本発明は以上のような構成からなるため、光学記録再生
の際に記録トラックの検出、及び記録トラックに対する
再生ヘッドの追随が容易であり、光学記録再生方式の記
録媒体の製造上のばらつきがあっても確実に再生が行な
え、しかもレーザービームを振動させる事自体は公知の
技術を利用して行なえるので容易であり、本発明の方法
により記録密度の高い記録媒体の利用時の確実さが確保
できる。
Since the present invention has the above configuration, it is easy to detect a recording track during optical recording and reproduction, and the reproduction head can easily follow the recording track, and there are no manufacturing variations in optical recording and reproduction type recording media. Furthermore, the method of the present invention ensures reliability when using a recording medium with a high recording density. can.

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

第1図は本発明の方法を示す説明図、第2国情)及び(
b)は本発明の方法によって得られる出力信号を示すだ
めのグラフ、第3図はレーザービームの走査線を示すだ
めの説明図である。 1・・・・・・・・レーサー光源 2・・・・・・・・・偏光器 3・・・・・・・・・固定ミラー 4・・・・・・・・・集光レンズ 5・・・・・・・・・光磁気記録材料 6・・・・・・・・・光磁気記録層 7・・・・・・・・・磁気コイル 8・・・・・・・・・ハーフミラ− 9,11・・・・・・・・・検光子 10 、1.2・・・・・・光検知器 13・・・・・・・・・・・・・・・ピット14・・・
・・・・・・・・・・・・走査線才1図 才2図to+ 才2図[bl 才8図 −29:
Figure 1 is an explanatory diagram showing the method of the present invention;
b) is a diagram showing the output signal obtained by the method of the invention, and FIG. 3 is a diagram showing the scanning line of the laser beam. 1... Racer light source 2... Polarizer 3... Fixed mirror 4... Condensing lens 5. ......Magneto-optical recording material 6...Magneto-optical recording layer 7...Magnetic coil 8...Half mirror 9, 11... Analyzer 10, 1.2... Photodetector 13... Pit 14...
・・・・・・・・・・・・Scanning line 1st figure 2nd figure to+ 2nd figure [bl 8th figure-29:

Claims (1)

【特許請求の範囲】[Claims] (1)光磁気記録材料の光磁気記録層に磁場を作用させ
つつレーザー光を集光して走査することにより記録再生
を行なう光磁気記録再生方法において、レーザー光を走
査方向に対して直角方向に振動させつつ走査することを
特徴とする光磁気記録再生方法。
(1) In a magneto-optical recording and reproducing method in which recording and reproduction is performed by focusing and scanning a laser beam while applying a magnetic field to the magneto-optical recording layer of a magneto-optical recording material, the laser beam is directed in a direction perpendicular to the scanning direction. A magneto-optical recording and reproducing method characterized by scanning while vibrating.
JP8886683A 1983-05-20 1983-05-20 Method for recording and reproducing optomagnetism Granted JPS59215046A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8886683A JPS59215046A (en) 1983-05-20 1983-05-20 Method for recording and reproducing optomagnetism

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8886683A JPS59215046A (en) 1983-05-20 1983-05-20 Method for recording and reproducing optomagnetism

Publications (2)

Publication Number Publication Date
JPS59215046A true JPS59215046A (en) 1984-12-04
JPH0546021B2 JPH0546021B2 (en) 1993-07-12

Family

ID=13954927

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8886683A Granted JPS59215046A (en) 1983-05-20 1983-05-20 Method for recording and reproducing optomagnetism

Country Status (1)

Country Link
JP (1) JPS59215046A (en)

Also Published As

Publication number Publication date
JPH0546021B2 (en) 1993-07-12

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