JPS63282946A - Magneto-optical recording method - Google Patents

Magneto-optical recording method

Info

Publication number
JPS63282946A
JPS63282946A JP11864387A JP11864387A JPS63282946A JP S63282946 A JPS63282946 A JP S63282946A JP 11864387 A JP11864387 A JP 11864387A JP 11864387 A JP11864387 A JP 11864387A JP S63282946 A JPS63282946 A JP S63282946A
Authority
JP
Japan
Prior art keywords
recording
magneto
track
magnetic field
optical recording
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
JP11864387A
Other languages
Japanese (ja)
Inventor
Atsuyuki Watada
篤行 和多田
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP11864387A priority Critical patent/JPS63282946A/en
Publication of JPS63282946A publication Critical patent/JPS63282946A/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

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 技術分野 本発明は磁界変調方式による光磁気記録方法の改良に関
する。
DETAILED DESCRIPTION OF THE INVENTION Technical Field The present invention relates to an improvement in a magneto-optical recording method using a magnetic field modulation method.

従来技術 光磁気記録方法には光磁気記録媒体(基本的にはガイド
トラック用微小溝付き透明基板上に磁性体記録層を設け
たもの)に対し一定方向の磁界を印加しながら、レーザ
ー光の点滅信号を印加する光変調方式と記録媒体にレー
ザー光を連続照射しながら、磁界信号を印加する磁界変
調方式の2種類がある。現在、光変調方式が主流になっ
ているが、オーバーライド(消去後、直ちに記録するこ
と)の点からは磁界変調方式%式% 磁界変調方式では情報の記録時の磁界の方向だけで行な
うため、1の信号についても0の信号についても同等の
条件で記録される。記録層の記録トラックと記録トラッ
クとの間の部分が一様に(一方向にだけ)磁化されてい
る場合は読出し時にこれらトラック間の情報もある程度
、読出されるために、再生信号はDCバイアスがかかっ
た状態になり、エラー率を高める原因となる。また記録
時も記録磁界は1の信号及びOの信号を同等に反転させ
ても、記録トラック間の部分の記録層の磁化が作り出す
磁界が記録部分にかかり、記録トラック間の磁化の方向
と同じ方向に記録する場合と反対方向に記録する場合と
では実際の記録部分にかかる磁界に差が生じ、その結果
、各信号の記録にアンバランスが生じ、これもエラー率
を高める原因となる。
The conventional magneto-optical recording method involves applying a magnetic field in a fixed direction to a magneto-optical recording medium (basically a transparent substrate with micro grooves for guide tracks and a magnetic recording layer), while applying a laser beam. There are two types: an optical modulation method that applies a blinking signal, and a magnetic field modulation method that applies a magnetic field signal while continuously irradiating the recording medium with laser light. Currently, the optical modulation method is the mainstream, but from the point of view of override (immediately recording after erasing), the magnetic field modulation method% method%. Both the 1 signal and the 0 signal are recorded under the same conditions. If the areas between the recording tracks of the recording layer are magnetized uniformly (only in one direction), a certain amount of information between these tracks is also read out during reading, so the reproduced signal is biased to a DC bias. This can lead to a high error rate. Also, during recording, even if the 1 signal and the O signal are equally reversed, the magnetic field created by the magnetization of the recording layer between the recording tracks is applied to the recording area, and the direction of the magnetization is the same as the direction of the magnetization between the recording tracks. There is a difference in the magnetic field applied to the actual recorded portion when recording in one direction and when recording in the opposite direction, and as a result, an imbalance occurs in the recording of each signal, which also causes an increase in the error rate.

目     的 本発明の目的は記録層の記録トラック間部分の磁化方向
による信号への影響を除去することによりエラー率を低
減した磁界変調方式の光磁気記録方法を提供することで
ある。
Object The object of the present invention is to provide a magneto-optical recording method using a magnetic field modulation method, which reduces the error rate by eliminating the influence on the signal due to the magnetization direction of the portion between recording tracks of the recording layer.

構   成 本発明の光磁気記録方法はガイドトラック用微小溝付き
透明基板上に磁性体記録層を設けた光磁気記録媒体にレ
ーザー光を連続照射しながら、磁界信号を印加する光磁
気記録方法において、第1図(図中、1は記録層、2は
透明基板、3は記録トラック、4はガイドトラック、5
゜6は記録トラック間の部分)に示すように予め記録層
1の記録トラック3と記録トラック3との間の部分5,
6の磁化方向(矢印で示す)をトラック毎に互いに逆転
させておくことを特徴とするものである。なお記録トラ
ックが同心円状の場合は問題はないが、渦巻状の場合は
「トラック毎に」とは「トラック1周毎にJを意味する
Structure The magneto-optical recording method of the present invention is a magneto-optical recording method in which a magnetic field signal is applied while continuously irradiating a laser beam to a magneto-optical recording medium in which a magnetic recording layer is provided on a transparent substrate with micro grooves for guide tracks. Figure 1 (In the figure, 1 is a recording layer, 2 is a transparent substrate, 3 is a recording track, 4 is a guide track, 5 is a recording layer, 2 is a transparent substrate, 3 is a recording track, 4 is a guide track,
゜6 is a portion between recording tracks) As shown in FIG.
This is characterized in that the magnetization directions (indicated by arrows) of No. 6 are reversed for each track. There is no problem if the recording tracks are concentric, but if they are spiral, "for each track" means "J for each round of the track."

本発明方法では光磁気記録媒体に対し磁界変調方式で記
録する際、前述のように予め記録層の各記録トラック間
部分の磁化方向を互いに逆転させることにより、各記録
トラックの右側部分及び左側部分の磁化方向が逆になり
、デジタル記録の信号1,0を上向き、下向きのどちら
の磁化に対応させても記録後、両者は常に同等の条件に
あることになる(第2図参照)。
In the method of the present invention, when recording on a magneto-optical recording medium using the magnetic field modulation method, as described above, by reversing the magnetization direction of the portion between each recording track of the recording layer, the right side and left side of each recording track are The direction of magnetization is reversed, and regardless of whether digitally recorded signals 1 and 0 correspond to upward or downward magnetization, both will always be under the same conditions after recording (see Figure 2).

光磁気記録媒体において各記録トラック間部分の磁化方
向を互いに逆転させるには例えば第3図(図中7はレー
ザー光源、8はミラー、9は偏光ビームスプリッタ−1
10は174波長板、11は対物レンズ、12はハーフ
ミラ−113はナイフェツジ、14.16は2分割フォ
トダイオード、15はフォーカスエラー用アンプ、17
はトラッキングエラー用アンプ、18は磁石、19はガ
イドトラック付き光磁気ディスク、20はモーター)に
示すような通常の光磁気記録装置を用いて次のように操
作すればよい。即ちまず光磁気ディスク19の記録トラ
ックと記録トラックとの中間部分にレーザービームが照
射されるように調整する。なおレーザービームはレーザ
ー光源7からミラー8によって直角に反射され、偏向ビ
ームスプリッタ−9及び波長板10を通り、更にレンズ
11により集束されたものである。このレーザービーム
を光磁気ディスク19の前記中間部分に通常の記録用パ
ワーで連続照射すると同時に、照射部分に光磁気ディス
ク19の背面からトラック毎に磁石18によって磁界の
方向を逆転させながら、磁化を行なう。
In order to mutually reverse the magnetization direction of the portion between each recording track in a magneto-optical recording medium, for example, as shown in FIG.
10 is a 174 wavelength plate, 11 is an objective lens, 12 is a half mirror, 113 is a knife lens, 14.16 is a two-split photodiode, 15 is an amplifier for focus error, 17
An ordinary magneto-optical recording device (denoted as a tracking error amplifier, 18 as a magnet, 19 as a magneto-optical disk with a guide track, and 20 as a motor) may be operated as follows. That is, first, adjustment is made so that the laser beam is irradiated onto the intermediate portion between the recording tracks of the magneto-optical disk 19. Note that the laser beam is reflected from the laser light source 7 at right angles by the mirror 8, passes through the polarizing beam splitter 9 and the wave plate 10, and is further focused by the lens 11. This laser beam is continuously irradiated to the intermediate portion of the magneto-optical disk 19 with normal recording power, and at the same time, the irradiated portion is magnetized while reversing the direction of the magnetic field from the back of the magneto-optical disk 19 for each track. Let's do it.

次にこうして各記録トラック間部分の磁化方向を互いに
逆転させた光磁気ディスクに記録を行なうには、まず記
録トラック上にレーザービームが照射されるように調整
した後、従来と同様、レーザービームを光磁気ディスク
19の記録トラック上に通常の記録用パワーで連続照射
すると同時にこの照射部分に磁石18によって磁界信号
を印加して信号に応じた磁化を行なえばよい。なお再生
方法は従来と全く同じである。
Next, in order to record on a magneto-optical disk in which the magnetization direction of the portion between each recording track is reversed, first, the laser beam is adjusted so that it is irradiated onto the recording track, and then the laser beam is irradiated as before. It is sufficient to continuously irradiate the recording track of the magneto-optical disk 19 with a normal recording power and at the same time apply a magnetic field signal to the irradiated portion using the magnet 18 to perform magnetization in accordance with the signal. Note that the reproduction method is exactly the same as before.

本発明方法で使用される光磁記録媒体としては基本的に
は同心円状又は渦巻状ガイドトラック用微小溝を有する
プラスチック又はガラス板のような透明基板上に希土類
遷移金属非晶質合金、マグネトプラムバイトフェライト
、Co−スピネルフェライト、Bi置換ガーネット等の
磁性体からなる記録層を設けた通常のものが使用できる
The magneto-optical recording medium used in the method of the present invention is basically a rare earth transition metal amorphous alloy, magnetoplum, on a transparent substrate such as a plastic or glass plate having micro grooves for concentric or spiral guide tracks. Ordinary materials provided with a recording layer made of a magnetic material such as bite ferrite, Co-spinel ferrite, Bi-substituted garnet, etc. can be used.

以下に本発明を実施例によって説明する。The present invention will be explained below by way of examples.

実施例 第3図の装置に光磁気ディスク19(渦巻状ガイドトラ
ック用微小溝を有するガラス基板上にTbFcCo非晶
質合金膜からなる記録層とSi3N、保護層とを設けた
もの)をセットし、ディスクの記録トラックと記録トラ
ックとの中間部分にレーザービームが照射されるように
調整した後、前記中間部分にディスク線速度25m1秒
において20mWのレーザービームを連続照射すると同
時にこの照射部分に光磁気ディスク19の背面からトラ
ック毎に磁石18を用いて磁界強度2000 eで磁界
の方向を逆転させながら磁化を行なった。
EXAMPLE A magneto-optical disk 19 (a recording layer made of a TbFcCo amorphous alloy film and a protective layer made of Si3N on a glass substrate having a microgroove for a spiral guide track) was set in the apparatus shown in FIG. After adjusting the laser beam to be irradiated to the intermediate portion between the recording tracks of the disk, the intermediate portion is continuously irradiated with a 20 mW laser beam at a disk linear velocity of 25 m1 second, and at the same time, this irradiated portion is magneto-optically applied. Magnetization was performed for each track from the back of the disk 19 using a magnet 18 at a magnetic field strength of 2000 e while reversing the direction of the magnetic field.

次にこうして各記録トラック間部分の磁化方向を互いに
逆転させた光磁化ディスクを第4図の記録再生装置(図
中、21は半導体レーザー、22はコリメータレンズ、
23はミラー、24 、26 、27はハーフミラ−1
25は対物レンズ、28.32は2分割フォトダイオー
ド、29はトラックエラー用アンプ、30はスポットレ
ンズ、31はナイフェツジ、33はフォーカスエラー用
アンプ、34は172波長板、35は偏光ビームスプリ
ッタ−136a。
Next, the magneto-optical disk with the magnetization direction of the portion between each recording track reversed is used in the recording/reproducing apparatus shown in FIG. 4 (in the figure, 21 is a semiconductor laser, 22 is a collimator lens,
23 is a mirror, 24, 26, 27 are half mirrors 1
25 is an objective lens, 28.32 is a two-split photodiode, 29 is a track error amplifier, 30 is a spot lens, 31 is a knife lens, 33 is a focus error amplifier, 34 is a 172 wavelength plate, and 35 is a polarizing beam splitter 136a. .

36bはフォトダイオード、37はRF信号用アンプ、
38は電磁石、40はスピンドルモーター、41a。
36b is a photodiode, 37 is an RF signal amplifier,
38 is an electromagnet, 40 is a spindle motor, and 41a.

41bはスポットレンズ)にセットし、このディスク1
9の記録トラックにレーザービームが照射されるように
調整した後、記録トラック部分にディスク線速度3m/
秒において5IIIlllのレーザービームを連続照射
しながら、電磁石38からの磁界信号を印加することに
より記録を行なった。
41b is a spot lens), and this disc 1
After adjusting so that the laser beam is irradiated onto the recording track No. 9, the recording track portion is heated at a disc linear velocity of 3 m/min.
Recording was performed by applying a magnetic field signal from the electromagnet 38 while continuously irradiating a laser beam of 5IIIll per second.

次にこうして記録された光磁気ディスク19に1mWの
レーザービームを照射することにより再生を行なったと
ころ、エラー率は10−S%であった。
Next, when the thus recorded magneto-optical disk 19 was reproduced by irradiating a laser beam of 1 mW, the error rate was 10-S%.

一方、比較のため前記中間部分の磁化方向をトラック毎
に逆転する操作を行なわなかった他は同じ方法で記録及
び再生を行なったところ、エラー率は10−4%であっ
た。
On the other hand, for comparison, recording and reproduction were performed in the same manner except that the direction of magnetization of the intermediate portion was not reversed for each track, and the error rate was 10-4%.

効   果 以上の如く本発明方法は磁界変調方式の光磁気記録にお
いて予め記録媒体の記録トラックと記録トラックとの間
の部分の磁化方向をトラック毎に互いに逆転させたので
、トラック間の記録層の磁化の方向による再生信号のD
Cバイアス、及び1,0信号記録時の磁界のアンバラン
スがなくなり、このためエラー率が従来よりも著しく少
なくなるという利点を有している。
Effects As described above, in the method of the present invention, in magneto-optical recording using the magnetic field modulation method, the magnetization directions of the portions of the recording medium between the recording tracks are reversed for each track in advance, so that the magnetic field of the recording layer between the tracks is D of the reproduced signal depending on the direction of magnetization
This method has the advantage that the C bias and the unbalance of the magnetic field when recording 1,0 signals are eliminated, and therefore the error rate is significantly lower than that of the conventional method.

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

第1図は、本発明方法における予備工程後の光磁気記録
媒体の各記録トラック間部分の磁化方向を示す斜視図、
第2図は第1図の光磁気配録媒体に磁界変調記録を行な
った時の状態図、第3図は光磁気記録媒体に第1図のよ
うな磁化方向を形成するための一例の装置図、第4図は
本発明方法に従って記録、再生を行なうための一例の装
置図である。 1・・・磁性体記録層 2・・・ガイドトラック用微小溝付き透明基板3・・・
記録トラック  4・・・ガイドトラック5.6・・・
記録トラックと記録トラックとの間の部分7・・・レー
ザー光源  18・・・磁  石19・・・光磁気ディ
スク
FIG. 1 is a perspective view showing the magnetization direction of the portion between each recording track of the magneto-optical recording medium after the preliminary step in the method of the present invention;
Fig. 2 is a state diagram when magnetic field modulation recording is performed on the magneto-optical recording medium shown in Fig. 1, and Fig. 3 is an example of an apparatus for forming the magnetization direction as shown in Fig. 1 on the magneto-optical recording medium. 4 are diagrams of an example of an apparatus for recording and reproducing according to the method of the present invention. 1... Magnetic recording layer 2... Transparent substrate with micro grooves for guide track 3...
Recording track 4... Guide track 5.6...
Portion between recording tracks 7... Laser light source 18... Magnet 19... Magneto-optical disk

Claims (1)

【特許請求の範囲】[Claims] 1、ガイドトラック用微小溝付き透明基板上に磁性体記
録層を設けた光磁気記録媒体にレーザー光を連続照射し
ながら、磁界信号を印加する光磁気記録方法において、
予め記録層の記録トラックと記録トラックとの間の部分
の磁化方向をトラック毎に互いに逆転させておくことを
特徴とする光磁気記録方法。
1. In a magneto-optical recording method in which a magnetic field signal is applied while continuously irradiating a laser beam to a magneto-optical recording medium in which a magnetic recording layer is provided on a transparent substrate with micro grooves for guide tracks,
A magneto-optical recording method characterized in that the magnetization directions of the portions of the recording layer between the recording tracks are reversed for each track in advance.
JP11864387A 1987-05-14 1987-05-14 Magneto-optical recording method Pending JPS63282946A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11864387A JPS63282946A (en) 1987-05-14 1987-05-14 Magneto-optical recording method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11864387A JPS63282946A (en) 1987-05-14 1987-05-14 Magneto-optical recording method

Publications (1)

Publication Number Publication Date
JPS63282946A true JPS63282946A (en) 1988-11-18

Family

ID=14741625

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11864387A Pending JPS63282946A (en) 1987-05-14 1987-05-14 Magneto-optical recording method

Country Status (1)

Country Link
JP (1) JPS63282946A (en)

Similar Documents

Publication Publication Date Title
JPS6259375B2 (en)
US5007039A (en) Optical information recording/reproducing apparatus
JPS605441A (en) Information processor
JPH0775042B2 (en) Magneto-optical recording / reproducing device
WO1991011806A1 (en) Magneto-optical recording/reproducing apparatus
JP2636957B2 (en) Magnetic recording / reproducing device
JPS61214256A (en) magneto-optical disk device
JPS63282946A (en) Magneto-optical recording method
JP2985213B2 (en) Magneto-optical recording / reproducing device
JPS61214266A (en) Magneto-optical recording/reproducing device
JP2604702B2 (en) Magneto-optical recording / reproduction / erasing method and apparatus
JPH0445134Y2 (en)
JP3361336B2 (en) Information recording and playback system
JPS60147950A (en) Information file which permits simultaneous erasing and recording
JP2636694B2 (en) Recording / reproducing method and recording / reproducing apparatus for magneto-optical recording medium
JPS6150235A (en) System and apparatus for erasing and reproducing optomagnetic recording
JPS6353619B2 (en)
JPS6360451B2 (en)
JPS58118047A (en) Photomagnetic recording medium
JPH03130951A (en) Magneto-optical pickup device
JPS6035303A (en) Rewritable optical information recording and reproducing device
JPH01191326A (en) optical information processing device
JPH02161641A (en) Magneto-optical recording system
JPS59142760A (en) Optical information recording device
JPH05342625A (en) Optical recording device