JPS60147948A - Photo-electro-magnetic recording device - Google Patents

Photo-electro-magnetic recording device

Info

Publication number
JPS60147948A
JPS60147948A JP271484A JP271484A JPS60147948A JP S60147948 A JPS60147948 A JP S60147948A JP 271484 A JP271484 A JP 271484A JP 271484 A JP271484 A JP 271484A JP S60147948 A JPS60147948 A JP S60147948A
Authority
JP
Japan
Prior art keywords
disc
disk
magnetic field
light beam
recording medium
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.)
Pending
Application number
JP271484A
Other languages
Japanese (ja)
Inventor
Kazuo Isaka
井阪 和夫
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP271484A priority Critical patent/JPS60147948A/en
Publication of JPS60147948A publication Critical patent/JPS60147948A/en
Pending 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

Abstract

PURPOSE:To record uniform bits and also to attain reproduction with high S/N by providing a magnetic field generating means where an optical beam irradiating of a magnetooptical recording medium of disc form corresponds and the strength of an auxiliary magnetic field is increased as the outer circumference. CONSTITUTION:A disc 2 as a disc form magnetooptical recording medium is turned by a motor at a prescribed angular velocity. The optical beam modulated based on the information generated from a laser light source 2 of an optical beam irradiating device 14 is collected via an optical head part 13 and a condenser lens 5 into a minute spot and irradiated on the disc 1. A permanent magnet 101 generates an almost uniform magnetic field at an equal interval and the distance between the magnet 101 and the disc 1 is arranged so that the inside of disc 1 is parted in comparison with the outside of the disc 1. Thus, the strength of the auxiliary magnetic field to the disc 1 is increased toward the outer circumference of the disc 1, the same bits are recorded at the inside and outside of the disc 1 and the S/N at reproduction is improved.

Description

【発明の詳細な説明】 本発明は、円盤状記録媒体に微少スポットに絞られた光
ビームにより磁気光学的に情報の記録を行なう光磁気記
録装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magneto-optical recording device that magneto-optically records information on a disc-shaped recording medium using a light beam narrowed to a minute spot.

特に、微少スポットに絞られた光ビームにより円盤状の
記録媒体に情報の記録を行なう光磁気記録装置は情報の
高密度な記録が可能である為近年注目されている。
In particular, magneto-optical recording devices that record information on a disc-shaped recording medium using a light beam focused on a minute spot have attracted attention in recent years because they are capable of recording information at high density.

上記光磁気記録装置においては、バイアス磁界のもとで
微少光ビームスポットに絞られた光ビームを回転する円
盤状の記録媒体に照射しながら光ビーム照射手段を円盤
状の記録媒体の径方向に連続的に或いはステップ状に除
々に移動させて情報記録を行なう。
In the above-mentioned magneto-optical recording device, the light beam irradiation means is directed in the radial direction of the disk-shaped recording medium while irradiating the rotating disk-shaped recording medium with a light beam that has been focused into a minute optical beam spot under a bias magnetic field. Information is recorded by moving continuously or gradually in steps.

記録は記録媒体の記録層に光ビームを照射し、照射した
微少部分をキュリ一温度或いは補償温度付近まで加熱し
バイアス磁界及び加熱部分周囲からの反磁界により冷却
時に記録媒体の磁化方向を反転させて記録を行なう。
Recording is performed by irradiating the recording layer of a recording medium with a light beam, heating the irradiated minute part to around the Curie temperature or compensation temperature, and reversing the magnetization direction of the recording medium when cooled by a bias magnetic field and a demagnetizing field from around the heated part. and record.

ここで円型状の記録媒体を一定角速度で回転させて記録
を行なうと、光ビームが円盤状記録媒体の外周を走査す
る場合と内周を走査する場合とで単位時間の光ビーム照
射に対する記録層の光エネルギー吸収量が異なり、光ビ
ームの強度を記録媒体外周走査時に適正となるようにす
れば、その内周では光ビームエネルギーが強すぎる為、
ピットのデユーティ比が50チより大きくなり、再生時
のSAJを著るしく低下させてしまう問題が生じる。
Here, when recording is performed by rotating a circular recording medium at a constant angular velocity, the recording for a unit time of light beam irradiation is performed depending on when the light beam scans the outer circumference of the disk-shaped recording medium and when it scans the inner circumference. The amount of light energy absorbed by the layers is different, and if the intensity of the light beam is set to be appropriate when scanning the outer circumference of the recording medium, the light beam energy will be too strong at the inner circumference.
A problem arises in that the duty ratio of the pit becomes larger than 50 inches, and the SAJ during reproduction is significantly reduced.

又逆に記録媒体内周走査時に適正となるように光ビーム
強度を調整すると外周では充分な記録が行なわれないと
いう問題が生じてしまう。
Conversely, if the light beam intensity is adjusted to be appropriate when scanning the inner circumference of the recording medium, a problem arises in that sufficient recording is not performed on the outer circumference.

その為に従来から記録媒体上の半径方向の光ビーム照射
位置に応じて光ビームの強度を変化させる案が報告され
ている。(例えば特開昭51−23902号公報、特開
昭52−69807号公報)しかし、上記記録方法によ
ると光ビームの強度が一定でない為、オートトラッキン
グ、オートフォーカシング操作時に記録媒体の外側と内
側で実質ゲインが異なり上記操作が不安定になってしま
うという欠点があった。又、光ビームの強度を変化させ
る為の電気回路が必要となり光ビーム発生回路を複雑に
してしまうという欠点が生じていtも本発明は上記欠点
に鑑み、提案されたものであり、安定したトラッキング
信号やフォーカシング信号を得、光ビームの安定したト
ラッキングやフォーカシングを得ると共に、再生時の再
生信号のS/N比が良好なビット列を形成する光磁気記
録装置を提供することを目的とする。
To this end, a proposal has been reported in which the intensity of the light beam is varied depending on the radial position of the light beam on the recording medium. (For example, JP-A No. 51-23902, JP-A No. 52-69807) However, according to the above recording method, the intensity of the light beam is not constant. There was a drawback that the actual gain was different and the above operation became unstable. In addition, an electric circuit is required to change the intensity of the light beam, which complicates the light beam generation circuit. It is an object of the present invention to provide a magneto-optical recording device which obtains signals and focusing signals, obtains stable tracking and focusing of a light beam, and forms a bit string with a good S/N ratio of a reproduced signal during reproduction.

即ち、本発明は円盤状の磁気光学的記録媒体を回転させ
、前記磁気光学的記録媒体に光ビーム発生装置から発生
した変調光ビームを微小スポットに収゛束すると共に補
助磁界を加えて記録する光磁気記録装置に於て、前記磁
気光学的記録媒体の光ビーム照射部位に対応し且つその
外周にいくに従って前記補助磁界の強度を増すようにし
て前記磁気光学的記録媒体の外周、内周を問わず同等の
ビットを形成することにより上記目的を達成することが
できた。
That is, the present invention rotates a disk-shaped magneto-optical recording medium, focuses a modulated light beam generated from a light beam generator on the magneto-optic recording medium into a minute spot, and records data by applying an auxiliary magnetic field to the magneto-optical recording medium. In the magneto-optical recording device, the outer periphery and inner periphery of the magneto-optical recording medium are arranged such that the intensity of the auxiliary magnetic field increases as it goes toward the outer periphery of the magneto-optical recording medium, corresponding to the light beam irradiation area of the magneto-optical recording medium. The above objective could be achieved by forming equivalent bits regardless of the type of bit.

以下、本発明の実施例を図面に従って説明する。Embodiments of the present invention will be described below with reference to the drawings.

本発明に関する光磁気記録装置の原理を第1図を参照し
ながら説明する。
The principle of the magneto-optical recording device according to the present invention will be explained with reference to FIG.

第1図において、円盤状の磁気光学的記録媒体(以下、
ディスクと称す。)1は例えばガラス円板にGd、Tb
、Fe 或いはMn 、 B i等の組成から成る磁性
膜をスパッタリング等により蒸着したものである。記録
時にはレーザ光源2から発した情報に基いて変調された
光ビームをコリメータレンズ3によって平行光となし、
偏光子6.ビームスプリッタ4を経て集光レンズ5を用
いてモータ12により回転しているディスクlの表面に
直径約1μmの光ビームスポットとして集光する。
In FIG. 1, a disc-shaped magneto-optical recording medium (hereinafter referred to as
It is called a disk. ) 1 is, for example, Gd, Tb on a glass disk.
, Fe, Mn, Bi, or the like is deposited by sputtering or the like. During recording, a light beam modulated based on information emitted from a laser light source 2 is made into parallel light by a collimator lens 3,
Polarizer 6. After passing through the beam splitter 4, the light beam is focused using a condensing lens 5 onto the surface of the disk 1 being rotated by the motor 12 as a light beam spot having a diameter of about 1 μm.

ここでディスクlの磁性膜は、予め垂直方向に向きをそ
ろえて磁化されており、バイアス磁極装置IOの発生す
るそれとは反対方向の磁界のもとで前記レーザ光を照射
することでそのキューリ一温度以上に熱せられてその冷
却時にノ(イアス磁極装置10の磁界により磁化方向が
反転し、画像情報を第2図のビット15のようにディス
ク上に記録するものである。
Here, the magnetic film of the disk l has been magnetized in advance with its orientation aligned in the vertical direction, and its cue is aligned by irradiating the laser beam under a magnetic field in the opposite direction to that generated by the bias magnetic pole device IO. When the magnet is heated above the temperature and cooled down, the direction of magnetization is reversed by the magnetic field of the magnetic pole device 10, and image information is recorded on the disk as shown in bit 15 in FIG.

なお、ここでバイアス磁極装置10の発生する磁界は、
ディスク1上の光ビームスポットのその半径方向の軌跡
に対応して発生するようになっており、その強さはディ
スクlの中心から外周方向に行(に従って増すようにな
っている。これによって、ディスク1の半径位置に応じ
て適当な強度のバイアス磁界が発生し、光ビームスポッ
トによりディスクlの記録層に与える光ビームエネルギ
ーとバイアス磁界の強度とのバランスがとれて適当な大
きさのビットの列がディスク1の内周、外周を問わずに
形成される。
Note that the magnetic field generated by the bias magnetic pole device 10 is as follows:
It is generated in accordance with the radial trajectory of the light beam spot on the disk 1, and its intensity increases from the center of the disk 1 to the outer circumference. A bias magnetic field of appropriate strength is generated depending on the radial position of the disk 1, and the light beam energy given to the recording layer of the disk 1 by the light beam spot is balanced with the strength of the bias magnetic field, so that bits of an appropriate size are generated. The rows are formed regardless of the inner or outer circumference of the disk 1.

一方、再生の際にはレーザ光源2により一定強度の光ビ
ームを発射し、ディスクlに形成されたビット列に照射
する。そして磁気カー効果によって記録情報に応じて偏
光面の回転されたディスクlからの反射光なビー介スプ
リツタキで方向転換し、集光レンズ11及び検光子7を
通して受光素子8に導き、信号を検出して信号処理回路
9により前記記録された情報を再生する。
On the other hand, during reproduction, a laser light source 2 emits a light beam of constant intensity and irradiates the bit string formed on the disk l. Then, the direction of the reflected light from the disk 1, whose plane of polarization has been rotated according to the recorded information due to the magnetic Kerr effect, is changed by beam splitting, and guided to the light receiving element 8 through the condenser lens 11 and the analyzer 7, where the signal is detected. The recorded information is reproduced by the signal processing circuit 9.

なお、上記記録及び再生の両方に於て、周知の手段によ
りフォーカシング信号やトラッキング信号を得、それに
応じて、たとえば対物レンズ5を光軸方向に移動させた
り、又はそれを半径方向に移動させたりしてフォーカシ
ング及びトラッキングを行なっている。又、18はコリ
メータレンズ3、偏光子6.ビームスプリッタ4.集光
レンズ11、検光子7.受光素子8.信号処理回路9か
らなる光学ヘッド部分、14は光学ヘッド部分18゜半
導体レーザー2.対物レンズ5から構成される光ビーム
照射装置で、不図示の周知の手段によりディスク1の径
方向に記録時もしくは再生時、連続的に或いはステップ
状に除々に移動させて情報の記録もしくは情報の再生を
行なう。
In addition, in both the above-mentioned recording and reproduction, focusing signals and tracking signals are obtained by well-known means, and accordingly, for example, the objective lens 5 is moved in the optical axis direction or it is moved in the radial direction. focusing and tracking. Further, reference numeral 18 indicates a collimator lens 3, a polarizer 6. Beam splitter 4. Condensing lens 11, analyzer 7. Light receiving element 8. An optical head section 14 consists of a signal processing circuit 9; an optical head section 18; and a semiconductor laser 2. A light beam irradiation device consisting of an objective lens 5, which is moved continuously or gradually in a stepwise manner in the radial direction of the disk 1 by a well-known means (not shown) during recording or reproduction, to record or record information. Perform playback.

第3図を基に本発明に係る磁性層の記録特性の一例を示
す。第3図は出力1− Omwのレーザービーム光をデ
ィスク上で上述のように1μInφに絞り、Gd 、 
Tb 、 Fe よりなる11000rpで回転するデ
ィスク上の磁性面に03μ秒間照射した場合の磁化反転
によって得られるディスク上のビット径を示している。
An example of the recording characteristics of the magnetic layer according to the present invention is shown based on FIG. Figure 3 shows that a laser beam with an output of 1-Omw is focused on the disk to 1 μInφ as described above, and Gd,
It shows the bit diameter on the disk obtained by magnetization reversal when the magnetic surface on the disk made of Tb, Fe and rotating at 11,000 rpm is irradiated for 03 μs.

X軸方向には光ビーム照射の際に印加したバイアス磁界
の強度を示しており、バイアス磁界の強度によってビッ
ト径が変化する様子を示している。一般にこのような記
録においては光ビームにより照射された磁性層がキュリ
一温度まで加熱されなくても、まわりの磁性層からの反
磁界により磁化反転が生じるが、バイアス磁界はこの反
磁界を補助するものである。実線はディスク上半径r 
= 100 (nun)、点線はディスク上半径r=5
0(nun )の点における測定値である。
The X-axis direction shows the intensity of the bias magnetic field applied during light beam irradiation, and shows how the bit diameter changes depending on the intensity of the bias magnetic field. Generally, in such recording, magnetization reversal occurs due to the demagnetizing field from the surrounding magnetic layer even if the magnetic layer irradiated by the light beam is not heated to one Curie temperature, but the bias magnetic field assists this demagnetizing field. It is something. The solid line is the radius r on the disk
= 100 (nun), the dotted line is the radius on the disk r = 5
This is the measured value at the point 0 (nun).

たとえば、ここで上記条件と同じにし、第1図に示した
バイアス磁極装置10がディスク1の記録層に及ぼす磁
界をディスク10半径50調の位置で約110 (Oe
)とし、その半径100mの位置で約350 (Oe)
になるようにすれば、ディスク1の半径50m及び10
0wnの位置で1.0μmのビットが形成される。そこ
で、これと同じようにディスク1の半径50岨からxo
ommの間で110 (Oe)から350 (Oe)迄
連続的に増加するようにして、適当なバイアス磁界を加
えるようにバイアス磁極装置10を構成すれば、常に1
.(1μmのビット径のビットをディスク1上に形成す
ることが可能となる。
For example, under the same conditions as above, the magnetic field exerted by the bias magnetic pole device 10 shown in FIG. 1 on the recording layer of the disk 1 is approximately 110 (Oe
), and approximately 350 (Oe) at a radius of 100 m.
If the radius of disk 1 is 50 m and 10
A 1.0 μm bit is formed at the 0wn position. So, in the same way as this, from the radius of disk 1 xo
If the bias magnetic pole device 10 is configured to apply an appropriate bias magnetic field so that it increases continuously from 110 (Oe) to 350 (Oe) between
.. (It becomes possible to form bits with a bit diameter of 1 μm on the disk 1.

なお、ここで、このディスクの半径方向の光ビームスポ
ットの位置とバイアス磁界強度の関係は一般的には比例
関係となるが磁性薄膜媒体の保磁力Hcの温度特性によ
りその曲線はそれとは異なる関係を示す。
Note that the relationship between the position of the optical beam spot in the radial direction of the disk and the bias magnetic field strength is generally a proportional relationship, but the curve may have a different relationship due to the temperature characteristics of the coercive force Hc of the magnetic thin film medium. shows.

第4図は本発明に係る光磁気記録装置の具体的な一実施
例を示す説明図である。図において、14は光ビーム照
射装置で、第1図に示した同構成のものであり、■はデ
ィスク、1o1は第1図のバイアス磁極装置10として
の永久磁石で、等距離でほぼ一様な磁界を発生し、永久
磁石101とディスク1の距離をディスク1の外側に比
較してディスクlの内側を遠くすることにより、そのバ
イアス磁界効果を異ならしめ、ディスクlの内側、外側
において同等のビットが形成されるようにするものであ
る。
FIG. 4 is an explanatory diagram showing a specific embodiment of the magneto-optical recording device according to the present invention. In the figure, 14 is a light beam irradiation device with the same configuration as shown in FIG. 1, ■ is a disk, and 1o1 is a permanent magnet as the bias magnetic pole device 10 in FIG. By generating a magnetic field and making the distance between the permanent magnet 101 and the disk 1 farther on the inside of the disk 1 compared to the outside of the disk 1, the bias magnetic field effect is made different, and the same effect is generated on the inside and outside of the disk 1. This allows bits to be formed.

又、この他にも永久磁石の表面に磁性体を取付は磁性体
の厚みを変えることによっても良いし、勿論永久磁石の
残留磁化をディスクの半径方向で異ならしめても良い。
In addition, a magnetic material may be attached to the surface of the permanent magnet by changing the thickness of the magnetic material, and of course, the residual magnetization of the permanent magnet may be varied in the radial direction of the disk.

但し、この場合、永久磁石をディスクから等距離の位置
に配置することができる。
However, in this case, the permanent magnets can be placed equidistant from the disk.

第5図は、本発明の他の一実施例を示す説明図である。FIG. 5 is an explanatory diagram showing another embodiment of the present invention.

図に於て1はディスク、■4は第1図に示した構成の光
ビーム照射装置、1o2は摺動可変抵抗器で、ディスク
1の中心から外周方向に直線的に設けられた固定抵抗部
102aと光ビーム照射装置14と共に一体となってデ
ィスク10半径方向に移動し且つ固定抵抗部102a上
を摺動する摺動切片102bとからなる。103は光ビ
ーム照射装置14によりディスク1上に形成される光ビ
ームスポットの軌跡に対応してディスクlの直下に設け
られた磁性体、104はこの磁性体に巻かれたコイルで
、一端は摺動切片102bに接続され、他端は電源10
5を介してディスク1の最外周側の固定抵抗部102a
の一端に接続されている。
In the figure, 1 is a disk, 4 is a light beam irradiation device having the configuration shown in FIG. 102a, and a sliding section 102b that moves in the radial direction of the disk 10 together with the light beam irradiation device 14 and slides on the fixed resistance section 102a. 103 is a magnetic material provided directly under the disk l corresponding to the locus of the light beam spot formed on the disk 1 by the light beam irradiation device 14; 104 is a coil wound around this magnetic material; The other end is connected to the power supply 10.
Fixed resistance part 102a on the outermost circumference side of the disk 1 via 5
connected to one end of the

光ビーム照射装置14がディスクlの中心側から外周に
行くに従って、摺動切片102 +)もこれと同方向に
移動して摺動抵抗器102の抵抗値が減少する。この抵
抗値の減少に共ない電源105によりそれ及びコイル1
04に流れる電流は増加する。従って、この電流の増加
につれて磁性体103から発生ずる磁界の強さも増す。
As the light beam irradiation device 14 moves from the center to the outer periphery of the disk l, the sliding piece 102 +) also moves in the same direction, and the resistance value of the sliding resistor 102 decreases. As the resistance value decreases, the power supply 105 causes it and the coil 1 to
The current flowing through 04 increases. Therefore, as this current increases, the strength of the magnetic field generated from the magnetic body 103 also increases.

この磁界の方向はディスク1の記録層の初期に設定され
た磁化方向とは逆の方向で補助磁界として記録用に用い
るものである。
The direction of this magnetic field is opposite to the initially set magnetization direction of the recording layer of the disk 1, and is used as an auxiliary magnetic field for recording.

故に、光ビーム照射装置14がディスク1の外周に行く
程、即ち、光ビーム照射装置14による光ビームスポッ
トがディスク1の外周に行く程、それにつれて、摺動可
変抵抗器102.磁性体108゜コイル104.電源1
05から構成されるバイアス磁極装置IOによるディス
ク1の記録層に対する磁界が強くなる。これにより、デ
ィスクlの内周及び外周において同等のビットが形成さ
れる。
Therefore, the further the light beam irradiation device 14 goes to the outer periphery of the disk 1, that is, the farther the light beam spot by the light beam irradiation device 14 goes to the outer periphery of the disk 1, the more the sliding variable resistor 102. Magnetic material 108° coil 104. Power supply 1
The magnetic field applied to the recording layer of the disk 1 by the bias magnetic pole device IO composed of 05 becomes stronger. As a result, equivalent bits are formed on the inner and outer circumferences of the disk l.

第6図は本発明の他の一実施例を示す説明図である。第
1図に示した同符号のものは同構成となっているが、但
し、光ビーム照射装置14の信号処理回′I89は省略
し、その一部をバイアス磁極装置■0に用〜・ている。
FIG. 6 is an explanatory diagram showing another embodiment of the present invention. Components with the same reference numerals shown in FIG. There is.

103は磁性体、104は磁性体を巻いているコイルで
、その位置については、第5図において述べた位置と同
位置である−8106はディスクlからのアドレス信号
を受光素子8を介して入力しディスクlの位置であるア
ドレスを再生するアドレス再生回路、108は中央処理
装置で、アドレス再生回路106からのアドレス信号に
対応して可変電圧源109の出力を調整するための制御
量を格納している読取り専用メモリ(以下、ROMと略
称する。)107から制御量を読み出して可変電圧源1
09の出力調整する。可変電圧源109はコイル104
に通電するための電源である。
103 is a magnetic material, 104 is a coil wound with a magnetic material, and its position is the same as that described in FIG. 108 is a central processing unit that stores a control amount for adjusting the output of the variable voltage source 109 in response to an address signal from the address reproduction circuit 106. The control amount is read out from the read-only memory (hereinafter abbreviated as ROM) 107 and the variable voltage source 1
Adjust the output of 09. The variable voltage source 109 is connected to the coil 104
This is the power supply for energizing the.

ディスクlには予めアドレスナンバーが記録されており
、レーザ光源2がら射出した光ビームは対物レンズ5に
より上述のようにディスクlの記録層上に光ビームスポ
ットとして絞られ、ディスクl上に情報を記録すると共
に、その反射光はビームスプリッタ4を介して受光素子
8で検出され、アドレス再生回路106によって、アド
レスが読み取られる。このアドレス信号をアドレス再生
回路106から入力した中央処理装置108は、ROM
I、07からアドレス信号に応じた制御量を読み出し、
この制御量にもとづいて可変電圧源109の出力を制御
する。この可変電圧源109の出力はコイル104に与
えられ、コイル104はその出力に応じて通電し、磁性
体103がらディスク1の記録層にむけてその通電量に
応じた磁界が発生する。この磁界の強度は光ビームスポ
ットのディスク1上の位置がその外周程高くなるように
しており、これによってディスクl上の内周、外周を問
わず同一径のビットが形成されることになる。
An address number is recorded in advance on the disk l, and the light beam emitted from the laser light source 2 is focused as a light beam spot on the recording layer of the disk l by the objective lens 5 as described above, and information is transferred onto the disk l. While recording, the reflected light is detected by the light receiving element 8 via the beam splitter 4, and the address is read by the address reproducing circuit 106. The central processing unit 108 inputting this address signal from the address reproducing circuit 106 inputs the ROM
Read the control amount according to the address signal from I, 07,
The output of variable voltage source 109 is controlled based on this control amount. The output of the variable voltage source 109 is applied to the coil 104, which is energized in accordance with the output, and a magnetic field is generated from the magnetic body 103 toward the recording layer of the disk 1 in accordance with the amount of energization. The strength of this magnetic field is set so that the position of the light beam spot on the disk 1 becomes higher as the outer circumference increases, so that bits with the same diameter are formed on the disk 1 regardless of whether it is on the inner or outer circumference.

第7図は本発明の他の一実施例の説明図である。FIG. 7 is an explanatory diagram of another embodiment of the present invention.

110はガイドバーで、ディスクlの直下の中心側から
外周側の半径方向に傾斜して設けられ、その位置はディ
スク1の外周側程、ディスクlに近くなっている。11
1はガイドバー110に遊嵌し、ガイドバー110上を
摺動する摺動部拐、で、その側方に永久磁石1’ l 
2が取付けられている。
Reference numeral 110 denotes a guide bar, which is provided so as to be inclined in the radial direction from the center side directly below the disk 1 to the outer circumferential side, and its position is closer to the disk 1 as the outer circumferential side of the disk 1 approaches. 11
1 is a sliding part that loosely fits into the guide bar 110 and slides on the guide bar 110, and a permanent magnet 1'l is attached to the side thereof.
2 is installed.

この永久磁石112が発生する磁界の方向はディスク1
の記録層においてディスク1の記録層が初期に設定され
た磁化の方向とは反対方向である。
The direction of the magnetic field generated by this permanent magnet 112 is
The direction of magnetization in the recording layer of the disk 1 is opposite to the initially set magnetization direction.

なJd、この永久磁石112の磁極は光ビーム照射装置
14によりディスク1上に形成される光ビームスポット
の真下に常に配置されることが望ましく・。ここで、永
久磁石112と摺動部組111とは不図示の手段により
ガイドバー110に沿って光ビーム照射装置14と一体
となって移動するものである。従って、光ビームスポッ
トがディスク1の外周にいくにつれて、永久磁石112
はガイドバー110に案内されてディスクlに近づき、
永久磁石112によるディスク1の記録層に対する磁界
の強さが増す。これによって、ディスクlの内周、外周
を問わず、同一径のビットが安定的にディスク1の記録
層に形成される。
Jd, it is desirable that the magnetic pole of this permanent magnet 112 is always placed directly below the light beam spot formed on the disk 1 by the light beam irradiation device 14. Here, the permanent magnet 112 and the sliding part assembly 111 move together with the light beam irradiation device 14 along the guide bar 110 by means not shown. Therefore, as the light beam spot moves toward the outer periphery of the disk 1, the permanent magnet 112
is guided by the guide bar 110 and approaches the disk l,
The strength of the magnetic field applied to the recording layer of the disk 1 by the permanent magnet 112 increases. As a result, bits of the same diameter are stably formed on the recording layer of the disc 1 regardless of whether it is on the inner or outer periphery of the disc 1.

本発明はこの他にも、第5図において光ビームスポット
の位置をアドレス信号で検出する代りに、光ビーム照射
装置の位置、即ち光ビームスポットの位置を、ポジショ
ンメータもしくは、マグネスケール等を利用して検出し
、その検出信号に応じて補助磁界の強度を調整するよう
にしてもよい。
In addition to this, the present invention uses a position meter, a magnet scale, etc. to detect the position of the light beam irradiation device, that is, the position of the light beam spot, instead of detecting the position of the light beam spot using an address signal as shown in FIG. Alternatively, the intensity of the auxiliary magnetic field may be adjusted according to the detected signal.

上記実施例ではいずれも、磁性体にコイルを巻いたが、
永久磁石にコイルを逆方向に巻き、永久磁石の磁力をコ
イルの通電により減少させるようにしてもよい。又、デ
ィスク半径方向に複数個の電磁石を並べ、ディスク1上
に応じてコイルの巻き数を増加させる等の装置もある。
In each of the above examples, a coil was wound around a magnetic material, but
A coil may be wound around the permanent magnet in the opposite direction, and the magnetic force of the permanent magnet may be reduced by energizing the coil. There is also a device in which a plurality of electromagnets are arranged in the radial direction of the disk and the number of turns of the coil is increased depending on the surface of the disk 1.

又、磁性体がディスクと対向する側を傾斜させて、この
磁性体に常時一定量の電流を通電させてもよいし、磁性
体の幅をディスクの外周にいくに従って細くしてもよい
Alternatively, the side of the magnetic body facing the disk may be inclined so that a constant amount of current is always applied to the magnetic body, or the width of the magnetic body may be made thinner toward the outer periphery of the disk.

す、上説明したように、磁気光学的記録媒体に光ビーム
を照射する手段と、光ビームを照射する記録媒体の径方
向の位置に対応した強度の磁界を発ノドさせる磁界発生
手段を設けることにより、安定したトラッキング検出信
号、フォーカシング検出伝号を得、光ビームの安定した
トラッキング、フォーカシングを得るとともに均一なビ
ットを3己録媒体1−に形成し、再生信号のS/N比が
非常に向上した。
As explained above, a means for irradiating the magneto-optical recording medium with a light beam and a magnetic field generating means for generating a magnetic field with an intensity corresponding to the radial position of the recording medium to which the light beam is irradiated are provided. As a result, stable tracking detection signals and focusing detection signals are obtained, stable tracking and focusing of the optical beam is obtained, and uniform bits are formed on the recording medium 1-, and the S/N ratio of the reproduced signal is extremely high. Improved.

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

第1図は本発明の原理を示す説明図、第2図はディスク
に記録されたビット列を示す説明図、第3図はバイアス
磁界とビット径との関係をディスクの半径をパラメータ
として示した一実施例の説明図、第4図乃至第7図は本
発明の各実施例を示す説明図である。 ■は(光磁気)ディスク、2は半導体レーザ。 5は対物レンズ、10はバイアス磁極装置、18は光学
〜ラド部分、14は光ビーム照射装置。 101は永久磁石、102は摺動可変抵抗器。 103は磁性体、104はコイル、105は電源。 106はアトl/ス再生回路、107はROM、 10
8は中央処理装置、109は可変電圧源、110はガイ
ドバー、111は摺動部祠、■12は永久磁石である。 特許出願人 キャノン株式会社 第4図 第5図 第6図 第7図
Fig. 1 is an explanatory diagram showing the principle of the present invention, Fig. 2 is an explanatory diagram showing a bit string recorded on a disk, and Fig. 3 is an explanatory diagram showing the relationship between bias magnetic field and bit diameter using the disk radius as a parameter. DESCRIPTION OF EMBODIMENTS FIGS. 4 to 7 are explanatory diagrams showing each embodiment of the present invention. ■ is a (magneto-optical) disk, and 2 is a semiconductor laser. 5 is an objective lens, 10 is a bias magnetic pole device, 18 is an optical to rad portion, and 14 is a light beam irradiation device. 101 is a permanent magnet, and 102 is a sliding variable resistor. 103 is a magnetic material, 104 is a coil, and 105 is a power source. 106 is an atlas regeneration circuit, 107 is a ROM, 10
8 is a central processing unit, 109 is a variable voltage source, 110 is a guide bar, 111 is a sliding part shrine, and 12 is a permanent magnet. Patent applicant Canon Co., Ltd. Figure 4 Figure 5 Figure 6 Figure 7

Claims (1)

【特許請求の範囲】[Claims] 円盤状の磁気光学的記録媒体を一定角速度で回転させ、
前記磁気光学的記録媒体に光ビーム発生装置から発生し
た変調光ビームを微小スポットに収束すると共に補助磁
界を加えて記録する光磁気記録装置に於て、前記磁気光
学的記録媒体の光ビーム照射部位に対応し且つその外周
にいくに従って前記補助磁界の強度を増すようにした磁
界発生手段を備えたことを特徴とする光磁気記録装置。
A disc-shaped magneto-optical recording medium is rotated at a constant angular velocity,
In the magneto-optical recording device that records on the magneto-optical recording medium by converging a modulated light beam generated from a light beam generator into a minute spot and applying an auxiliary magnetic field, the magneto-optical recording medium has a light beam irradiated portion. What is claimed is: 1. A magneto-optical recording device comprising magnetic field generating means that increases the intensity of the auxiliary magnetic field toward the outer periphery thereof.
JP271484A 1984-01-12 1984-01-12 Photo-electro-magnetic recording device Pending JPS60147948A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP271484A JPS60147948A (en) 1984-01-12 1984-01-12 Photo-electro-magnetic recording device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP271484A JPS60147948A (en) 1984-01-12 1984-01-12 Photo-electro-magnetic recording device

Publications (1)

Publication Number Publication Date
JPS60147948A true JPS60147948A (en) 1985-08-05

Family

ID=11536970

Family Applications (1)

Application Number Title Priority Date Filing Date
JP271484A Pending JPS60147948A (en) 1984-01-12 1984-01-12 Photo-electro-magnetic recording device

Country Status (1)

Country Link
JP (1) JPS60147948A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4803674A (en) * 1985-11-20 1989-02-07 Hitachi, Ltd. Magneto-optical recorder with small-sized, low-powered electromagnetic coil
EP0421768A2 (en) * 1989-10-04 1991-04-10 Nikon Corporation External magnetic field generating device for optical magnetic disk apparatus
JPH06150423A (en) * 1993-01-07 1994-05-31 Ricoh Co Ltd Magneto-optical recorder

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4803674A (en) * 1985-11-20 1989-02-07 Hitachi, Ltd. Magneto-optical recorder with small-sized, low-powered electromagnetic coil
EP0421768A2 (en) * 1989-10-04 1991-04-10 Nikon Corporation External magnetic field generating device for optical magnetic disk apparatus
US5126984A (en) * 1989-10-04 1992-06-30 Nikon Corporation External magnetic field generating device for optical magnetic disk apparatus
JPH06150423A (en) * 1993-01-07 1994-05-31 Ricoh Co Ltd Magneto-optical recorder

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