JPH01124132A - Recording method - Google Patents

Recording method

Info

Publication number
JPH01124132A
JPH01124132A JP28113487A JP28113487A JPH01124132A JP H01124132 A JPH01124132 A JP H01124132A JP 28113487 A JP28113487 A JP 28113487A JP 28113487 A JP28113487 A JP 28113487A JP H01124132 A JPH01124132 A JP H01124132A
Authority
JP
Japan
Prior art keywords
information
recording medium
magnetic field
recording
written
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
JP28113487A
Other languages
Japanese (ja)
Inventor
Mineo Moribe
峰生 守部
Kenichi Ito
健一 伊藤
Fuminori Imamura
今村 文則
Shuichi Hashimoto
修一 橋本
Yasumasa Iwamura
康正 岩村
Kazunori Naito
一紀 内藤
Miyozo Maeda
巳代三 前田
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP28113487A priority Critical patent/JPH01124132A/en
Publication of JPH01124132A publication Critical patent/JPH01124132A/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
    • G11B11/10502Recording 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 characterised by the transducing operation to be executed
    • G11B11/10517Overwriting or erasing
    • G11B11/10519Direct overwriting, i.e. performing erasing and recording using the same transducing means
    • 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

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To perform the rewrite of information in a short time by performing overwrite by forming two kinds of magnetic fields whose magnetizing directions are set oppositely to each other in the advancing direction of a recording medium, projecting two kinds of laser beams whose strength are different, and enabling a point less a Curie temperature or a compensation temperature to appear on respective magnetic field as advancing the recording medium. CONSTITUTION:The recording of information is performed by forming the two kinds of magnetic fields whose magnetizing directions are set oppositely to each other in the advancing direction of the recording medium 10, and projecting the two kinds of laser beams 5 whose strength are different on the recording medium 10, and enabling the point less than the Curie temperature or the compensation temperature to appear on respective magnetic field as advancing the recording medium 10. The method is performed by utilizing the fact that a time difference based on the strength of a laser power exists until the recording medium 10 is cooled. In such a way, it is possible to perform the overwrite of new information on old information without erasing the old information, and to shorten a time required for the rewrite of the information remarkably.

Description

【発明の詳細な説明】 〔概 要〕 光磁気ディスクにおいて情報の記録を重ね書きで行う方
法に関し、 情報の書き換えを、重ね書きで、容易かつ短時間に行い
得る方法を提供することを目的とし、記録媒体の進行方
向に、磁化方向が互いに反対である2種類の磁界を形成
しておき、この記録媒体に2種類の強度を異にするレー
ザビームを照射して、該記録媒体が進行するにつれて、
そのキュリー温度又は補償温度以下になる点が前記磁界
のそれぞれにおいてあらわれるようにして情報の記録を
行うように構成する。
[Detailed Description of the Invention] [Summary] Regarding a method of recording information on a magneto-optical disk by overwriting, the present invention aims to provide a method that allows information to be easily and quickly rewritten by overwriting. , two types of magnetic fields with opposite magnetization directions are formed in the traveling direction of the recording medium, and the recording medium is irradiated with two types of laser beams with different intensities, so that the recording medium advances. As time goes on,
Information is recorded so that a point below the Curie temperature or compensation temperature appears in each of the magnetic fields.

C産業上の利用分野〕 本発明は記録方法に関し、さらに詳しく述べると、光磁
気ディスクにおいて情報の記録を重ね書きで行う方法に
関する。
C. Industrial Application Field] The present invention relates to a recording method, and more specifically, to a method for recording information on a magneto-optical disk by overwriting.

〔従来の技術〕[Conventional technology]

従来の光磁気ディスクでは、通常、次のようにして情報
の記録、再生及び消去が行われている:記録・・・磁化
の方向が一方向にそろえられた光磁気ディスクの記録媒
体に高出力のレーザビーム(例えばφ1廂)を照射して
キュリー温度又は補償温度以上に加熱し、外部磁界によ
って、レーザ照射部だけの磁化方向を外部磁界の方向と
同じとする。
On conventional magneto-optical disks, information is normally recorded, reproduced, and erased in the following manner: Recording...High output is applied to the recording medium of a magneto-optical disk in which the direction of magnetization is aligned in one direction. is irradiated with a laser beam (for example, φ1 square) to heat it above the Curie temperature or compensation temperature, and an external magnetic field is used to make the magnetization direction of only the laser irradiated part the same as the direction of the external magnetic field.

なお、この情報記録はレーザ強度を変調して行う。Note that this information recording is performed by modulating the laser intensity.

再生・・・低出力のレーザビームを記録媒体に照射して
、磁気的カー効果による反射光の偏光面の回転方向で、
記録符号“O”。
Reproduction: A low-power laser beam is irradiated onto the recording medium, and the polarization plane of the reflected light is rotated by the magnetic Kerr effect.
Record code “O”.

“1”を読み取る。Read “1”.

消去・・・高出力のレーザビームを記録媒体に照射して
、記録とは逆方向の外部磁界によって、磁化の方向をも
とに戻す。
Erasing: A high-power laser beam is irradiated onto the recording medium, and an external magnetic field in the opposite direction to the recording direction is used to return the magnetization direction to the original direction.

この従来の記録方法は、さらに具体的に説明すると、例
えば第5図に図示するような手法でもって実施されてい
る。光磁気ディスク10は、基板1と、その基板上の記
録媒体層2とからなっている。
To explain this conventional recording method more specifically, it is carried out, for example, by a method as shown in FIG. The magneto-optical disk 10 consists of a substrate 1 and a recording medium layer 2 on the substrate.

記録媒体の進行方向は矢印Aで示される。光学ヘッドは
、光学系4と、それによって集束せしめられるレーザビ
ーム5とからなっている。記録媒体の光学へ・ノドと対
向する側には、外部磁界形成のための磁石8が配置され
ている。磁石8は、情報の記録及び消去のたびごとに外
部磁化の方向を反転することができる。
The traveling direction of the recording medium is indicated by arrow A. The optical head consists of an optical system 4 and a laser beam 5 that is focused thereby. A magnet 8 for forming an external magnetic field is arranged on the side of the recording medium facing the optical node. The magnet 8 can reverse the direction of external magnetization each time information is recorded or erased.

第5図の記録方法は、例えば、第6図に図示するような
書き換えパルスでもって実施されている。
The recording method shown in FIG. 5 is implemented, for example, using a rewriting pulse as shown in FIG.

光ディスクの回転の1周目で情報の消去を行う。Information is erased during the first revolution of the optical disc.

これは、以下に述べる書き込みとは逆の外部磁界の存在
の下で高出力のレーザビームを記録媒体に照射すること
によって可能である。2周目にはいって情報の書き込み
を開始する。これは、外部磁界を前記消去とは反対の方
向にしたうえで、2つの異なるパワーレベルのレーザビ
ームを照射して、情報を2つの記録符号“0”、“1”
に変換して書き込むことによって、行うことができる。
This is possible by irradiating the recording medium with a high power laser beam in the presence of an external magnetic field opposite to the writing described below. Enter the second round and start writing information. This is done by setting the external magnetic field in the opposite direction to the erasing process and then irradiating the laser beam with two different power levels to convert the information into two recording codes "0" and "1".
This can be done by converting and writing.

図示の場合、符号“0”、“1”を交互に組み合わせて
連続したパルスとした。
In the illustrated case, the codes "0" and "1" are alternately combined to form continuous pulses.

上記した説明から明らかなように、この従来の情報記録
方法では、高出力のレーザビームを照射した部分のみに
おいて記録媒体の磁化の方向が変化するので、−度記録
された情報を新たな情報に書き換えるには、−旦旧情報
を消去してから新情報を書き込まなければならない。し
たがって、情報の書き換えにはディスクを最低2回転さ
せることが必要であり、そのふんだけ情報書き込み速度
が遅くなる。
As is clear from the above explanation, in this conventional information recording method, the direction of magnetization of the recording medium changes only in the area irradiated with a high-power laser beam, so information recorded at -degrees can be converted into new information. To rewrite, the old information must be erased and then the new information must be written. Therefore, it is necessary to rotate the disk at least twice in order to rewrite the information, and the information writing speed becomes slower accordingly.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

本発明の目的は、従来の技術の項において明らかにした
ような欠点を解消すること、換言すると、光磁気ディス
クにおける情報の書き換えを、重ね書きで、容易かつ短
時間に行い得る方法を提供することにある。
An object of the present invention is to eliminate the drawbacks as clarified in the section of the prior art, in other words, to provide a method for rewriting information on a magneto-optical disk easily and in a short time by overwriting. There is a particular thing.

〔問題点を解決するための手段〕[Means for solving problems]

本発明者らは、上記した目的を達成すべく鋭意研究の結
果、レーザビームを記録媒体に照射して加熱した場合に
、その記録媒体が冷えはじめてそのキュリー温度又は補
償温度を切る(すなわち、その温度以下になる)時間は
レーザパワーによっているいろに変化するということを
利用して、いちいち情報の消去を行わなくても符号“0
”。
As a result of intensive research to achieve the above object, the present inventors have discovered that when a recording medium is heated by irradiating it with a laser beam, the recording medium begins to cool down and falls below its Curie temperature or compensation temperature (i.e., its Curie temperature or compensation temperature). By using the fact that the time (below the temperature) changes in various ways depending on the laser power, the code “0” can be obtained without erasing information each time.
”.

“1”の分別記録を行うことが可能であることを見い出
した。
It has been found that it is possible to perform separate recording of "1".

この本発明の方法は、光磁気ディスクにおいて情報の記
録を重ね書きで行う方法であって、記録媒体の進行方向
に、磁化方向が互いに反対である2種類の磁界を形成し
ておき、この記録媒体に2種類の強度を異にするレーザ
ビームを照射して、該記録媒体が進行するにつれて、そ
のキュリー温度又は補償温度以下になる点が前記磁界の
それぞれにおいてあらわれるようにして情報の記録を行
うことを特徴とする。
The method of the present invention is a method of recording information on a magneto-optical disk by overwriting, and in which two types of magnetic fields with opposite magnetization directions are formed in the traveling direction of the recording medium. Information is recorded by irradiating the medium with two types of laser beams with different intensities so that as the recording medium advances, a point below its Curie temperature or compensation temperature appears in each of the magnetic fields. It is characterized by

本発明の方法は、上記したように、レーザパワーの大小
によって記録媒体が冷えるまでの時間に差があることを
利用したものである。したがって、本発明の方法を実施
するに当って、好ましくは、記録媒体に、その媒体をそ
の媒体のキュリー温度又は補償温度よりもわずかに高い
温度まで加熱可能な強度を有するレーザビームを照射し
て、レーザビーム照射部かもしくはその近傍で媒体進行
方向のある位置で第1の情報を書き込み、また、前記第
1の情報の書き込み時よりもさらに高い温度まで記録媒
体を加熱可能な強度を有するレーザビームを照射して、
前記第1の情報の書き込み位置よりもさらに媒体進行方
向に遠方のある位置において第2の情報を書き込む。な
お、これらの第1及び第2の情報の書き込みであるが、
これは、常法にしたがって、例えば2つのパワーレベル
を異にする記録符号、例えば“O”、′″1”への変換
によって行うのが好ましい。例えば、第1の情報を符号
“1”に、そして第2の情報を符号“0”にそれぞれ対
応させて情報の書き込みを行うことができる。本発明の
方法では、これらの情報の書き込みを、すでに書き込ま
れている情報を消去しないで、符号“O”、”l”の組
み合わせによりディスクの1回転のうちに連続して行う
ことができる。
The method of the present invention utilizes the fact that, as described above, there is a difference in the time required for the recording medium to cool down depending on the magnitude of the laser power. Therefore, in carrying out the method of the present invention, the recording medium is preferably irradiated with a laser beam having an intensity capable of heating the medium to a temperature slightly higher than the Curie temperature or compensation temperature of the medium. , a laser that writes the first information at a certain position in the medium traveling direction at or near the laser beam irradiation part, and has an intensity that can heat the recording medium to a higher temperature than when writing the first information. Irradiate the beam,
The second information is written at a position further away in the medium traveling direction than the writing position of the first information. In addition, regarding writing of these first and second information,
This is preferably done in a conventional manner, for example by converting the recording codes to two different power levels, eg "O", ``1''. For example, information can be written in such a manner that the first information corresponds to the code "1" and the second information corresponds to the code "0". In the method of the present invention, these pieces of information can be written continuously within one revolution of the disk using a combination of symbols "O" and "l" without erasing the information that has already been written.

本発明の方法は、好ましい1態様に従えば、記録媒体の
光学ヘッドと対向する側のある位置かもしくはその近傍
で媒体進行方向のある位置(第1位置)と、その第1位
置よりもさらに媒体進行方向に遠方のある位置(第2位
置)とに、それぞれ磁界方向が互いに反対である2個の
磁石を配置し、前記第1位置で第1の情報を書き込みか
つ前記第2位置で第2の情報を書き込むことによって実
施することができる。
According to a preferred embodiment, the method of the present invention includes a position (first position) in the medium traveling direction at or near a position on the side of the recording medium facing the optical head; Two magnets whose magnetic field directions are opposite to each other are arranged at a certain position (second position) far away in the medium traveling direction, and the first information is written at the first position and the second information is written at the second position. This can be implemented by writing the information in step 2.

また、本発明の方法は、もう1つの好ましい態様に従え
ば、記録媒体の光学ヘッドと対向する側のある位置かも
しくはその近傍で媒体進行方向のある位置に1個の永久
磁石を配置するとともに、前記記録媒体上に、該記録媒
体よりもキュリー温度が高く、記録時の最高温度におけ
る保磁力が前記永久磁石による外部磁界よりも大きく、
かつ記録媒体のキュリー温度における磁界が外部磁界よ
りも小さい垂直磁化膜からなる磁界形成層を設け、該磁
界形成層は予め記録時の外部磁界とは反対方向に磁化し
ておき、前記外部磁界にならわせて第1の情報を書き込
みかつ前記磁界形成層の磁界にならわせて第2の情報を
書き込むことによって実施することができる。
According to another preferred embodiment, the method of the present invention includes arranging one permanent magnet at a certain position in the medium traveling direction at or near a certain position on the side of the recording medium facing the optical head; , on the recording medium, the Curie temperature is higher than that of the recording medium, and the coercive force at the highest temperature during recording is larger than the external magnetic field caused by the permanent magnet,
In addition, a magnetic field forming layer made of a perpendicularly magnetized film whose magnetic field at the Curie temperature of the recording medium is smaller than the external magnetic field is provided, and the magnetic field forming layer is magnetized in advance in the opposite direction to the external magnetic field during recording. This can be carried out by writing the first information along with the magnetic field of the magnetic field forming layer and writing the second information along with the magnetic field of the magnetic field forming layer.

本発明の方法において使用する磁界形成層は、それが上
記したような条件を満たす限りにおいて特に限定される
ものではない。例えば、記録媒体としてTbFeCoを
使用する場合には磁界形成層にも同じ(TbFeCoを
使用することができる。この場合、キュリー温度を上昇
させるためにCo11を増量するだけですみ、また、同
一の材料であるので積層も容易である。その他の有用な
磁界形成層材料としては、例えば、GdCo 、 Gd
FeCo 、 TbCo 、 SmCoなどをあげるこ
とができる。磁界形成層は、通常、記録媒体層の基板と
は反対の側に設けるのが好ましいけれども、必要に応じ
て、記録媒体層の基板と同じ側に設けてもよい。但し、
この場合には、磁界形成層がレーザによって加熱され、
それが記録媒体層に伝わるという形になるので、記録感
度や磁界形成層の材料選択の点で不利にならないように
配慮することが必要である。
The magnetic field forming layer used in the method of the present invention is not particularly limited as long as it satisfies the above conditions. For example, when TbFeCo is used as the recording medium, the magnetic field forming layer can also be made of TbFeCo. In this case, it is only necessary to increase the amount of Co11 to increase the Curie temperature, and Therefore, lamination is easy.Other useful magnetic field forming layer materials include, for example, GdCo, Gd
Examples include FeCo, TbCo, and SmCo. Although it is usually preferable to provide the magnetic field forming layer on the side of the recording medium layer opposite to the substrate, it may be provided on the same side of the recording medium layer as the substrate, if necessary. however,
In this case, the magnetic field forming layer is heated by a laser,
Since this is transmitted to the recording medium layer, it is necessary to take care not to be disadvantageous in terms of recording sensitivity and material selection for the magnetic field forming layer.

〔作 用〕[For production]

本発明の作用は、添付の図面に示される記録方法を参照
することによって十分に理解することができるであろう
The operation of the present invention can be fully understood by referring to the recording method shown in the accompanying drawings.

第1図は、基板1上に記録媒体層2を有する光磁気ディ
スクの光学ヘッドと対向する側に2個の磁石6及び7を
配置した記録方法を示す例である。
FIG. 1 shows an example of a recording method in which two magnets 6 and 7 are arranged on the side facing an optical head of a magneto-optical disk having a recording medium layer 2 on a substrate 1.

磁石6及び7は、それぞれ、磁界方向が互いに反対であ
り、したがって、ディスク10の記録媒体層2は、矢印
Aの方向に進行するに際して2つの外部磁界にさらされ
ることとなる。磁石6は第1の位置(ここでは、レーザ
ビーム照射部の近傍で少し媒体進行方向にずれた位置)
に配置され、また、磁石7は第2の位置(第1の位置よ
りもさらに媒体進行方向にずれた位置)に配置される。
The magnetic field directions of the magnets 6 and 7 are opposite to each other, so that the recording medium layer 2 of the disk 10 is exposed to two external magnetic fields as it moves in the direction of arrow A. The magnet 6 is in the first position (here, a position slightly shifted in the medium traveling direction near the laser beam irradiation part)
Further, the magnet 7 is arranged at a second position (a position further shifted in the medium traveling direction from the first position).

磁石6及び7の間隔は所望とする結果に応じて任意に変
更することができる。記録に用いられるレーザビーム5
は、光学系4によって集束せしめられた後に記録媒体層
2上に照射される。
The spacing between the magnets 6 and 7 can be arbitrarily changed depending on the desired result. Laser beam 5 used for recording
is focused by the optical system 4 and then irradiated onto the recording medium layer 2.

記録媒体層2にレーザビーム5を照射してその記録媒体
をキュリー温度又は補償温度よりや\高い温度に加熱す
ると(この時のレーザパワーをMとする;第2図参照)
、記録媒体はすぐ冷えてそのキュリー温度又は補償温度
をきり、結果として、磁化の方向は磁石6による外部磁
界にならう。次いで、先に用いたMより高いレーザパワ
ー(Hとする)を有するレーザビームの照射により記録
媒体をキュリー温度又は補償温度よりはるかに高い温度
に加熱すると、記録媒体が冷えるのに時間がかかるため
、キュリー温度又は補償温度をきる時には記録媒体はす
でに磁石7による外部磁界上に達している。この時の記
録媒体の磁化の方向は、したがって、磁石7による外部
磁界にならう。
When the recording medium layer 2 is irradiated with a laser beam 5 and the recording medium is heated to a temperature slightly higher than the Curie temperature or the compensation temperature (the laser power at this time is M; see Figure 2).
, the recording medium quickly cools down to its Curie or compensation temperature, so that the direction of magnetization follows the external magnetic field by the magnet 6. Next, if the recording medium is heated to a temperature much higher than the Curie temperature or the compensation temperature by irradiation with a laser beam having a higher laser power (denoted as H) than the previously used M, it will take a long time for the recording medium to cool down. , the recording medium has already reached the external magnetic field generated by the magnet 7 when the Curie temperature or compensation temperature is reached. The direction of magnetization of the recording medium at this time therefore follows the external magnetic field generated by the magnet 7.

したがって、例えば磁石6による外部磁界を情報“1”
の磁界としかつ磁石7による外部磁界を情報“0”の磁
界としておけば、第2図に示されるように、ディスクの
第1同月から、以前の書き込み状態によらず(したがっ
て、旧情報の消去の必要なしに)、パワーMのレーザビ
ームで11を書き込み、パワーHのレーザビームで“0
”を書き込むことができる。
Therefore, for example, the external magnetic field caused by the magnet 6 becomes information "1".
If the magnetic field is set to 1 and the external magnetic field by the magnet 7 is set to the magnetic field of information "0", as shown in FIG. ), write 11 with a laser beam of power M, and write “0” with a laser beam of power H.
” can be written.

第3図は、光磁気ディスクの記録媒体層上で磁界形成層
を使用した記録方法を示す例である。光磁気ディスク1
0は、図示の通り、基板l上に記録媒体層2及び磁界形
成層3を有し、そして矢印Aの方向に進行可能である。
FIG. 3 is an example showing a recording method using a magnetic field forming layer on the recording medium layer of a magneto-optical disk. magneto-optical disk 1
0 has a recording medium layer 2 and a magnetic field forming layer 3 on a substrate l, and can move in the direction of arrow A.

本記録方法では、第1図の方法のように2個の磁石を使
用する代りに、この磁界形成層3を追加しかつディスク
を境にして光学ヘッドと対向する側の位置に外部磁界形
成のための永久磁石8を配置している。磁界形成層3は
、記録媒体よりもキュリー温度が高(、記録時の最高温
度における保磁力が永久磁石による外部磁界よりも太き
く(シたがって、外部磁界によって磁界の方向が反転さ
れない)、かつ記録媒体のキュリー温度における磁界が
外部磁界よりも小さい(したがって、外部磁界の下で記
録を行う場合に、この媒体の磁界が妨げとなることはな
い)垂直磁化膜であり、また、この膜は、予め外部磁界
とは反対の方向に磁化されている。
In this recording method, instead of using two magnets as in the method shown in Fig. 1, this magnetic field forming layer 3 is added and an external magnetic field forming layer is provided at a position facing the optical head with the disk as the boundary. A permanent magnet 8 is arranged for this purpose. The magnetic field forming layer 3 has a Curie temperature higher than that of the recording medium (and the coercive force at the highest temperature during recording is thicker than the external magnetic field of the permanent magnet (therefore, the direction of the magnetic field is not reversed by the external magnetic field). The magnetic field at the Curie temperature of the recording medium is smaller than the external magnetic field (therefore, when recording under an external magnetic field, the magnetic field of this medium does not interfere). is previously magnetized in the direction opposite to the external magnetic field.

記録媒体層2に光学系4で集束せしめられたレーザビー
ム5を照射してその記録媒体をキュリー温度又は補償温
度よりや\高い温度に加熱すると(この時のレーザパワ
ーをMとする;第4図参照)、記録媒体はすぐ冷えるの
で、キュリー温度又は補償温度をきる時にはまた永久磁
石8による外部磁界の影響下にあり、したがって、記録
媒体の磁化の方向は外部磁界にならう。次いで、先に用
いたMより高いレーザパワー(Hとする;但し、このパ
ワーで磁界形成層がキュリー温度以上にならないこと)
を有するレーザビームの照射により記録媒体をキュリー
温度又は補償温度よりはるかに高い温度に加熱すると、
記録媒体が冷えるのに時間がかかるため、キュリー温度
又は補償温度に達する時には記録媒体は外部磁界の外に
出てしまい、したがって、記録媒体の磁化の方向は磁界
形成層にならう。
When the recording medium layer 2 is irradiated with the laser beam 5 focused by the optical system 4 and the recording medium is heated to a temperature slightly higher than the Curie temperature or the compensation temperature (the laser power at this time is M; the fourth Since the recording medium cools down quickly, it is also under the influence of the external magnetic field from the permanent magnet 8 when it reaches the Curie temperature or the compensation temperature, and therefore the direction of magnetization of the recording medium follows the external magnetic field. Next, use a laser power higher than the previously used M (referred to as H; however, this power should not cause the magnetic field forming layer to exceed the Curie temperature).
When the recording medium is heated to a temperature much higher than the Curie temperature or the compensation temperature by irradiation with a laser beam having
Since it takes time for the recording medium to cool down, when the Curie temperature or compensation temperature is reached, the recording medium is outside the external magnetic field, and therefore the direction of magnetization of the recording medium follows the magnetic field forming layer.

したがって、例えば外部磁界の方向を情報“1”としか
つ磁界形成層の方向を情報“0”とすれば、第4図に示
されるように、ディスクの第1周回から、以前の書き込
み状態によらず(したがって、旧情報の消去の必要なし
に)、パワーMのレーザビームで“1”を書き込み、パ
ワーHのレーザビームで0”を書き込むことができる。
Therefore, for example, if the direction of the external magnetic field is set as information "1" and the direction of the magnetic field forming layer is set as information "0", as shown in FIG. "1" can be written with a laser beam of power M, and "0" can be written with a laser beam of power H (therefore, without the need to erase old information).

〔実施例〕〔Example〕

2つの外部磁界の使用(第1図) 基板としてのガラス円板上にフォトポリマ(三菱油化■
製のアクリレート5A1002  )を塗布し、フォト
ポリマー法(2P法)によりプリグループパターンを形
成した0次いで、このプリグループを形成した基板上に
Tb及びFeを主成分とする光磁気記録媒体をスパッタ
成膜した。得られた光磁気ディスクの記録媒体層の膜厚
は1100nであり、Tb1.Fe、、Co11からな
った。
Use of two external magnetic fields (Fig. 1) Photopolymer (Mitsubishi Yuka ■) on a glass disk as a substrate
A pre-group pattern was formed using the photopolymer method (2P method).Next, a magneto-optical recording medium containing Tb and Fe as main components was formed by sputtering on the substrate on which the pre-group was formed. It was filmed. The thickness of the recording medium layer of the obtained magneto-optical disk was 1100n, and Tb1. It consisted of Fe, Co11.

外部磁界形成用に、強度3000eの磁石2個を磁界の
方向が逆になるように貼り合わせた。磁石間距離は30
pmであった。貼り合わせた磁石を、光磁気ディスクに
関してみて、光学ヘッドの反対側にセットし、また、そ
の際、片方の磁石がレーザビームと対向し、他方の磁石
がディスクの進行方向側になるように配慮した。
To form an external magnetic field, two magnets with a strength of 3000e were bonded together so that the directions of the magnetic fields were opposite. The distance between magnets is 30
It was pm. Set the bonded magnets on the opposite side of the optical head with respect to the magneto-optical disk, making sure that one magnet faces the laser beam and the other magnet faces in the direction of disk travel. did.

最初に、光磁気ディスクを回転数90Orpmで回転さ
せ、周波数IMIIzの信号を記録した。照射したレー
ザビームのパワーは、高いほう(H)が81、低いはう
(M)が2a+Wであった。
First, the magneto-optical disk was rotated at a rotational speed of 90 rpm, and a signal with a frequency of IMIIz was recorded. The power of the irradiated laser beam was 81 on the high side (H) and 2a+W on the low side (M).

先に記録を行ったものと同じトラックに、同じ回転数で
ディスクを回転させながら、周波数0.5M Hzの信
号を記録した。照射したレーザビームのパワーは、高い
はう (H)が8mW、低いはう (M)が211IW
であった。信号の書き換えが確認された。
A signal with a frequency of 0.5 MHz was recorded on the same track as previously recorded while rotating the disk at the same rotation speed. The power of the irradiated laser beam is 8 mW for high crawl (H) and 211 IW for low crawl (M).
Met. Signal rewriting was confirmed.

なお、本発明者らの知見によれば、貼り合わせる2個の
磁石の磁石間距離や磁石の配置位置は記録媒体の熱容量
等によって任意に変更することができ、また、2個の磁
石は、そのうちの片方が必ずしもレーザビームに対向し
ていなくてもよく、記録媒体が加熱後に2つの磁界内を
通ればそれでよい。
According to the findings of the present inventors, the distance between the two magnets bonded together and the placement position of the magnets can be arbitrarily changed depending on the heat capacity of the recording medium, etc. One of the magnetic fields does not necessarily have to face the laser beam, as long as the recording medium passes through the two magnetic fields after being heated.

肛 磁界形成層の使用(第3図) 基板としてのガラス円板上にフォトポリマ(三菱油化領
製の5A1002)をスピンコードし、2P法によりプ
リグループパターンを形成した。次いで、このプリグル
ープを形成した基板上にTb  。
Use of magnetic field forming layer (FIG. 3) A photopolymer (5A1002 manufactured by Mitsubishi Yukaryo) was spin-coded on a glass disk as a substrate, and a pregroup pattern was formed by the 2P method. Next, Tb was deposited on the substrate on which this pregroup was formed.

Fe及びCoを主成分とする光磁気記録媒体をスパッタ
、成膜した。膜厚100nsのTbt4Feth*CO
sからなる記録媒体層が形成された。引き続いて、記録
媒体層の形成と同様にして、膜厚1100nのTb1.
Fe5yCoz4(キュリー温度を高めるためにG。
A magneto-optical recording medium containing Fe and Co as main components was formed by sputtering. Tbt4Feth*CO with a film thickness of 100 ns
A recording medium layer consisting of s was formed. Subsequently, in the same manner as in the formation of the recording medium layer, Tb1.
Fe5yCoz4 (G to increase the Curie temperature.

量を増量した)からなる磁界形成層をスパッタ成膜した
A magnetic field forming layer was formed by sputtering.

得られた光磁気ディスクを回転数600rpmで回転さ
せ、レーザパワー15mW及び外部磁界3000eで、
記録媒体層及び磁界形成層をともに一方向じO”の方向
)に磁化した。なお、この操作は、磁界形成層の磁化の
方向を“0”の方向にそろえるために行ったものであり
、この通りである必要はない。
The obtained magneto-optical disk was rotated at a rotation speed of 600 rpm, with a laser power of 15 mW and an external magnetic field of 3000 e.
Both the recording medium layer and the magnetic field forming layer were magnetized in one direction (O" direction). This operation was performed to align the magnetization direction of the magnetic field forming layer to the "0" direction. It doesn't have to be this way.

すなわち、例えば外部磁界の磁化が“0”の方向である
場合には、この磁界形成層の磁化の方向を“1″の方向
にそろえることができる。
That is, for example, when the magnetization of the external magnetic field is in the "0" direction, the magnetization direction of this magnetic field forming layer can be aligned in the "1" direction.

最初に、光磁気ディスクを回転数90Orpmで回転さ
せ、周波数IMHzの信号を記録した。照射したレーザ
ビームのパワーは、高いはう(H)が8mW、低いはう
(M)が2mWであった。
First, the magneto-optical disk was rotated at a rotational speed of 90 rpm, and a signal with a frequency of IMHz was recorded. The power of the irradiated laser beam was 8 mW for high crawl (H) and 2 mW for low crawl (M).

先に記録を行ったものと同じトラックに、同じ回転数で
ディスクを回転させながら、周波数0.5M llzの
信号を記録した。照射したレーザビームのパワーは、高
いはう(H)が8mW、低いはう(M)が2mWであっ
た。信号の書き換えが確認された。
A signal with a frequency of 0.5 Mllz was recorded on the same track as previously recorded while rotating the disk at the same rotation speed. The power of the irradiated laser beam was 8 mW for high crawl (H) and 2 mW for low crawl (M). Signal rewriting was confirmed.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、情報の書き換えを行うに当って、ディ
スクを1回転させるうちに、旧情報を消去しないでその
上に新たな情報を重ね書きすることができるので、書き
換えに要する時間を大幅に短縮することができる。また
、本発明によれば、この重ね書きを、複雑な装置を用い
ないで、容易に実施することができる。
According to the present invention, when rewriting information, it is possible to overwrite new information on top of the old information without erasing it while the disk rotates once, thereby significantly reducing the time required for rewriting. can be shortened to Further, according to the present invention, this overwriting can be easily performed without using a complicated device.

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

第1図は、本発明の記録方法の好ましい一例を示した略
示図、 第2図は、第2図の記録方法を実施するための書き換え
パルスの波形図、 第3図は、本発明の記録方法のもう1つの好ましい例を
示した略示図、 第4図は、第3図の記録方法を実施するための書き換え
パルスの波形図、 第5図は、従来の記録方法の一例を示した略示図、そし
て 第6図は、第5図の記録方法を実施するための書き換え
パルスの波形図である。 図中、1は基板、2は記録媒体層、3は磁界形成層、4
は光学系、5はレーザビーム、6及び7は磁石、そして
10は光磁気ディスクである。
FIG. 1 is a schematic diagram showing a preferred example of the recording method of the present invention, FIG. 2 is a waveform diagram of a rewriting pulse for carrying out the recording method of FIG. 2, and FIG. 3 is a diagram showing a preferred example of the recording method of the present invention. A schematic diagram showing another preferred example of the recording method, FIG. 4 is a waveform diagram of a rewriting pulse for carrying out the recording method of FIG. 3, and FIG. 5 shows an example of a conventional recording method. FIG. 6 is a waveform diagram of a rewriting pulse for carrying out the recording method of FIG. 5. In the figure, 1 is a substrate, 2 is a recording medium layer, 3 is a magnetic field forming layer, 4
5 is an optical system, 5 is a laser beam, 6 and 7 are magnets, and 10 is a magneto-optical disk.

Claims (1)

【特許請求の範囲】 1、光磁気ディスクにおいて情報の記録を重ね書きで行
う方法であって、記録媒体の進行方向に、磁化方向が互
いに反対である2種類の磁界を形成しておき、この記録
媒体に2種類の強度を異にするレーザビームを照射して
、該記録媒体が進行するにつれて、そのキュリー温度又
は補償温度以下になる点が前記磁界のそれぞれにおいて
あらわれるようにして情報の記録を行うことを特徴とす
る記録方法。 2、記録媒体に、その媒体をその媒体のキュリー温度又
は補償温度よりもわずかに高い温度まで加熱可能な強度
を有するレーザビームを照射して、レーザビーム照射部
かもしくはその近傍で媒体進行方向のある位置で第1の
情報を書き込み、また、前記第1の情報を書き込み時よ
りもさらに高い温度まで記録媒体を加熱可能な強度を有
するレーザビームを照射して、前記第1の情報の書き込
み位置よりもさらに媒体進行方向に遠方のある位置にお
いて第2の情報を書き込む、特許請求の範囲第1項に記
載の記録方法。 3、前記第1及び第2の情報の書き込みを2つのパワー
レベルを異にする符号への変換によって行う、特許請求
の範囲第2項に記載の記録方法。 4、前記記録媒体の光学ヘッドと対向する側のある位置
かもしくはその近傍で媒体進行方向のある位置と、その
位置よりもさらに媒体進行方向に遠方のある位置とに、
それぞれ磁界方向が互いに反対である2個の磁石を配置
し、前者の位置で第1の情報を書き込みかつ後者の位置
で第2の情報を書き込む、特許請求の範囲第2項に記載
の記録方法。 5、前記情報が符号“0”、“1”に変換されて書き込
まれるべきものであり、その際、前記第1及び第2の情
報がそれぞれ符号“1”及び“0”に対応する、特許請
求の範囲第4項に記載の記録方法。 6、前記情報の書き込みを符号“0”、“1”の組み合
わせによりディスクの1回転のうちに連続して行う、特
許請求の範囲第5項に記載の記録方法。 7、前記記録媒体の光学ヘッドと対向する側のある位置
かもしくはその近傍で媒体進行方向のある位置に1個の
永久磁石を配置するとともに、前記記録媒体上に、該記
録媒体よりもキュリー温度が高く、記録時の最高温度に
おける保磁力が前記永久磁石による外部磁界よりも大き
く、かつ記録媒体のキュリー温度における磁界が外部磁
界よりも小さい垂直磁化膜からなる磁界形成層を設け、
該磁界形成層は予め記録時の外部磁界とは反対方向に磁
化しておき、前記外部磁界にならわせて第1の情報を書
き込みかつ前記磁界形成層の磁界にならわせて第2の情
報を書き込む、特許請求の範囲第2項に記載の記録方法
。 8、前記情報が符号“0”、“1”に変換されて書き込
まれるべきものであり、その際、前記第1及び第2の情
報がそれぞれ符号“1”及び“0”に対応する、特許請
求の範囲第7項に記載の記録方法。 9、前記情報の書き込みを符号“0”、“1”の組み合
わせによりディスクの1回転のうちに連続して行う、特
許請求の範囲第8項に記載の記録方法。
[Claims] 1. A method for recording information on a magneto-optical disk by overwriting, in which two types of magnetic fields with opposite magnetization directions are formed in the traveling direction of the recording medium, and Information is recorded by irradiating a recording medium with two types of laser beams with different intensities so that as the recording medium advances, a point below its Curie temperature or compensation temperature appears in each of the magnetic fields. A recording method characterized by: 2. Irradiate the recording medium with a laser beam that has an intensity that can heat the medium to a temperature slightly higher than the Curie temperature or compensation temperature of the medium, and then Write first information at a certain position, and irradiate the recording medium with a laser beam having an intensity that can heat the recording medium to a higher temperature than when writing the first information, and write the first information at the writing position. 2. The recording method according to claim 1, wherein the second information is written at a certain position further away in the direction of travel of the medium. 3. The recording method according to claim 2, wherein the first and second information are written by converting into codes having two different power levels. 4. At or near a certain position on the side of the recording medium facing the optical head in the medium traveling direction, and at a position further away from that position in the medium traveling direction,
The recording method according to claim 2, wherein two magnets are arranged with magnetic field directions opposite to each other, and first information is written at the former position and second information is written at the latter position. . 5. A patent in which the information is to be converted into codes "0" and "1" and written, and in this case, the first and second information correspond to the codes "1" and "0", respectively. A recording method according to claim 4. 6. The recording method according to claim 5, wherein the information is written continuously during one rotation of the disk by a combination of codes "0" and "1". 7. A permanent magnet is disposed at or near a certain position on the side of the recording medium facing the optical head in the medium traveling direction, and a permanent magnet is placed on the recording medium at a Curie temperature lower than that of the recording medium. a magnetic field forming layer made of a perpendicularly magnetized film, which has a high coercive force at the highest temperature during recording than the external magnetic field by the permanent magnet, and whose magnetic field at the Curie temperature of the recording medium is smaller than the external magnetic field,
The magnetic field forming layer is magnetized in advance in a direction opposite to the external magnetic field during recording, and first information is written in accordance with the external magnetic field, and second information is written in accordance with the magnetic field of the magnetic field forming layer. 3. The recording method according to claim 2, wherein the recording method is written. 8. A patent in which the information is to be converted into codes "0" and "1" and written, and in this case, the first and second information correspond to the codes "1" and "0", respectively. A recording method according to claim 7. 9. The recording method according to claim 8, wherein the information is written continuously in one revolution of the disk by a combination of codes "0" and "1".
JP28113487A 1987-11-09 1987-11-09 Recording method Pending JPH01124132A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28113487A JPH01124132A (en) 1987-11-09 1987-11-09 Recording method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28113487A JPH01124132A (en) 1987-11-09 1987-11-09 Recording method

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JPH01124132A true JPH01124132A (en) 1989-05-17

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JP28113487A Pending JPH01124132A (en) 1987-11-09 1987-11-09 Recording method

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