JPS6342055A - Magneto-optical recording method - Google Patents

Magneto-optical recording method

Info

Publication number
JPS6342055A
JPS6342055A JP18414686A JP18414686A JPS6342055A JP S6342055 A JPS6342055 A JP S6342055A JP 18414686 A JP18414686 A JP 18414686A JP 18414686 A JP18414686 A JP 18414686A JP S6342055 A JPS6342055 A JP S6342055A
Authority
JP
Japan
Prior art keywords
recording
magneto
magnetization
signal
magnetized
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
JP18414686A
Other languages
Japanese (ja)
Inventor
Yoshihiro Kobata
芳裕 古場田
Hisatoshi Baba
久年 馬場
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 JP18414686A priority Critical patent/JPS6342055A/en
Publication of JPS6342055A publication Critical patent/JPS6342055A/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

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To perform what is called overwrite by making the recording magnetic field opposite between the N-th recording and the (N+1)th recording. CONSTITUTION:Upward magnetized bits are indicated by oblique lines, and downward magnetized bits are indicated with white frames. Two bits are used to record one signal '1' or '0'. In case of the N-th recording, the recording magnetic field is preliminarily applied upward and only pertinent bits are magnetized downward in accordance with signals '1-1-0-0' to be recorded. Then, in case of the (N+1)th recording, the recording field is preliminarily applied downward and only pertinent bits are magnetized downward in accordance with signals '1-0-1-0' to be recorded. Thus, it is unnecessary to erase recorded signals before signals are recorded, and only 1/32 rotation of the disc is required for recording of signals on one sector, and therefore, the erasing and recording time is shortened.

Description

【発明の詳細な説明】 [産業上の利用分野] 本9.11は光磁気ディスク装置においてオーバライド
なn(能にする光磁気記録方法に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] This article 9.11 relates to a magneto-optical recording method that enables override n in a magneto-optical disk device.

〔従来の技術] 光磁気記録は、集光されたレーザービームによる記録媒
体上の局部的な加熱と該部分に存在する磁場との相互作
用を利用して情報を記録するものである。
[Prior Art] Magneto-optical recording records information by utilizing the interaction between local heating of a recording medium by a focused laser beam and a magnetic field existing in the area.

第7図(a)、(b) 、第8図はそれぞれ光磁気記録
の記録、消去、再生の原理を模式的に示した図である。
FIGS. 7(a) and 8(b) and FIG. 8 are diagrams schematically showing the principles of recording, erasing, and reproducing magneto-optical recording, respectively.

記録においては、光磁気ディスクの膜面に対し垂直方向
に容易に磁化する磁性膜lをあらかじめ同一方向に磁化
しておき、膜の保持力Hc以下の記録磁場H7中でレー
ザ光2により局部加熱を行い、キュリ一温度まで上昇さ
せて磁化消失させ、冷却過程における磁化回復時に記録
磁場H,により反転させる(第7図(a))、消去では
記録と同様レーザ光2による加熱と磁場印加により行う
が消去磁場H2の印加方向の向きは記録磁場H7の向き
とは逆にする(第7図(b))。
During recording, the magnetic film l, which is easily magnetized in the direction perpendicular to the film surface of the magneto-optical disk, is magnetized in advance in the same direction, and local heating is performed using a laser beam 2 in a recording magnetic field H7 having a coercive force Hc or less of the film. The magnetization is then raised to one Curie temperature to cause the magnetization to disappear, and when the magnetization is recovered during the cooling process, it is reversed by the recording magnetic field H (Fig. 7 (a)). For erasing, as with recording, heating with the laser beam 2 and application of the magnetic field are performed. However, the direction in which the erasing magnetic field H2 is applied is opposite to the direction of the recording magnetic field H7 (FIG. 7(b)).

再生は記録した磁化の方向を記録、消去よりも弱く連続
したレーザ光で読み出す、その際、光と磁気の相互作用
である磁気カー効果を利用する。
For reproduction, the direction of recorded magnetization is read out using a continuous laser beam that is weaker than for recording and erasing, and in this case, the magnetic Kerr effect, which is the interaction between light and magnetism, is used.

光も電波の一種で尤の進行方向に垂直な面で電界と磁界
か振動する。レーザ光はその電界(5a界)が一方向に
振動している。その光が記録媒体lの表面に照射されて
反射する際に振動方向が媒体の磁化の向きに依存して互
いに逆方向に回転する。
Light is also a type of radio wave, with electric and magnetic fields vibrating in a plane perpendicular to its direction of propagation. The electric field (5a field) of the laser beam oscillates in one direction. When the light is irradiated onto the surface of the recording medium l and reflected, the vibration directions rotate in opposite directions depending on the direction of magnetization of the medium.

この現象を磁気カー効果というか、第8図 (a)に示
すようにそれぞれ±θ、たけ回転したとすると互いの角
度は2θ、となる0反射後の光を検光子10(ある方向
に振動する光のみ通過させる素子)に通すと、例えばそ
の通過軸5を下向き磁化て反射した光3の振動方向と直
交させておくと、光は検光子10を通過せず(第8図(
b))、またL向き磁化で反射した光4はsin 2θ
、の通過成分を持つこととなり光検出素子11により光
量が検出される(第8図(C) ) 、よって記録面の
磁化方向による光の振動面の回転はそれに対応する光の
強弱に変換され、記録された情報を検出することかてき
る。
This phenomenon is called the magnetic Kerr effect, and as shown in Figure 8 (a), if each rotates by ±θ, the angle between them will be 2θ. For example, if the passing axis 5 is magnetized downward and perpendicular to the vibration direction of the reflected light 3, the light will not pass through the analyzer 10 (see Fig. 8).
b)), and the light 4 reflected by the magnetization in the L direction is sin 2θ
, and the amount of light is detected by the photodetecting element 11 (Fig. 8 (C)). Therefore, the rotation of the light vibration plane due to the magnetization direction of the recording surface is converted into the corresponding intensity of light. , it is possible to detect the recorded information.

第9図は前述のような光磁気記録方法を採用した光磁気
ディスク装置の一例を示す図であり、(a)は模式側面
図、(b)はディスクの平面図である0回l′4におい
て、21はレーザ光を出射し、光磁気ディスク22から
の反射光を読取る、つまり情報の消去・記録・再生を行
う光学ヘット、23は記録磁界を形成するためのコイル
、24はディスク22を回転させるモータである。光学
ヘウト21とコイル23は不図示の駆動装置により、デ
ィスク22の半径方向へ移動し、ディスク22上の全ト
ラックの消去・記録・再生を行う。
FIG. 9 is a diagram showing an example of a magneto-optical disk device employing the above-mentioned magneto-optical recording method, in which (a) is a schematic side view and (b) is a plan view of the disk. , 21 is an optical head that emits a laser beam and reads reflected light from the magneto-optical disk 22, that is, erases, records, and reproduces information; 23 is a coil for forming a recording magnetic field; 24 is an optical head that reads the reflected light from the magneto-optical disk 22; It is a motor that rotates. The optical system 21 and the coil 23 are moved in the radial direction of the disk 22 by a drive device (not shown), and erase, record, and reproduce all tracks on the disk 22.

通常、ディスク21hのトラック25はらせん状または
同心円状(第9図(b)は同心円状を示す)てあり、デ
ィスク22の1回転分がいくつかのセクタに等分割され
ている。今、仮にその分割か32分割されているとする
と、あるlセクタ、例えばセクタS、に情報を記録する
場合、まず該セクタS1に既に記録された信号を消去す
るため、ディスク22は消去用レーザ光を該セクタ部分
に受けながら1/32回転する。この時、第7図(b)
に示すように下向き5a場Hアかかけられているため、
すべて下向きに磁化されることにより信号は消去される
。ディスク22はモーター24により一方向に高速回転
させられているため逆転はできないので、その後、同一
方向に31/:12回転し、再び該セクタの最初の部分
にレーザ光かあたる位シまでもってこなければならない
、ここからディスク22を1/32回転する間に第7図
(a)に示すように上向きに記録磁場Hllをかけてお
き、記録信号に応じて変調されたレーザ光をあて上向き
に磁化させる部分を作ることによりデジタル信号(1−
〇信号)を記録する。
Usually, the track 25 of the disk 21h is spiral or concentric (FIG. 9(b) shows a concentric circle), and one rotation of the disk 22 is equally divided into several sectors. Now, if we assume that the division is divided into 32, when information is to be recorded in a certain l sector, for example, sector S, the disk 22 must be operated by an erasing laser to first erase the signal already recorded in sector S1. It rotates 1/32 while receiving light in the sector portion. At this time, Fig. 7(b)
As shown in the figure, the downward 5a field H is applied, so
The signal is erased by magnetizing everything downward. Since the disk 22 is rotated at high speed in one direction by the motor 24, it cannot be reversed, so it is then rotated 31/:12 in the same direction until the laser beam hits the first part of the sector again. From here, while the disk 22 rotates 1/32, a recording magnetic field Hll is applied upward as shown in FIG. By creating a magnetized part, a digital signal (1-
〇signal).

[発明が解決しようとする問題点] しかしながら、上記の記録方法は、ディスク22を1/
:32回転分の領域を記録するのに、ディスク22を3
3/32回転もしなければならないことになる。
[Problems to be Solved by the Invention] However, in the above recording method, the disk 22 is
: To record the area for 32 revolutions, the disc 22 is
This means that you will have to complete 3/32 rotations.

つまり、lセクタ分信号を消去、記録するのに、実際の
1セクタ分の記録時111よりははるかに大きい33倍
の時間を要し、記録速度か8いという問題点を有してい
たのである。
In other words, it took 33 times as long to erase and record one sector's worth of signals, which is much longer than the actual recording time of one sector, and the recording speed was 8 times slower. be.

[問題点を解決するための手段] 未発IJ1の目的は、上述従来例の情報記録時間か長い
という欠点を解決し、いわゆるオーバライドをiT鮨に
する光磁気記録方法を提供することにあるゆ 以上のような目的は、光磁気記録媒体に光を照射し、情
報を記録する光磁気記録方法において、N回目記録時(
N=1,2.3・・・)と(N+ 1 )2回目記録時
とで記録磁場の向きを逆にすることを特徴とする光磁気
記録方法によって達成される。
[Means for Solving the Problems] The purpose of the unreleased IJ1 is to provide a magneto-optical recording method that solves the disadvantage of the long information recording time of the conventional example described above and makes so-called override an iT sushi. The above purpose is to use a magneto-optical recording method that records information by irradiating light onto a magneto-optical recording medium.
This is achieved by a magneto-optical recording method characterized by reversing the direction of the recording magnetic field between (N=1, 2.3, . . . ) and (N+ 1 ) second recording.

なお、上記本発明において、第1、第2の磁化の向きを
有する光磁気記録媒体に2値化信号を記録するに際し、
第1.第2の記Q磁場の向きそれぞれにおいて前記2値
化信号にそれぞれ対応する2種別の磁化パターンを用い
て情報を記録することによりさらに種々の利点を有する
ことかできる。
In the present invention, when recording a binary signal on a magneto-optical recording medium having the first and second magnetization directions,
1st. By recording information using two types of magnetization patterns corresponding to the binary signals in each direction of the second Q magnetic field, various advantages can be obtained.

[実施例] 以下、本発明に係る光磁気記録方法について具体的実施
例に基づき詳細に説明する。
[Examples] Hereinafter, the magneto-optical recording method according to the present invention will be described in detail based on specific examples.

第1図は本発明の第1実施例を示す図であり、以下の説
明においては、第1図(a)に示すように上向きに磁化
されたビットは斜線で示しく第7図(a)に相当)、下
向きに磁化されたビットは白い枠で示す(第7図(b)
に相当)、また、本実施例ではディスク上に(l−0個
号)を記録する時は、1つの信号″“1”又は“0″を
記録するために2ビットを使用する。これに対し、従来
例では、例えば上向き磁化ビットを“l”信号とすれば
下向き磁化ビット“0”信号としていた。
FIG. 1 is a diagram showing a first embodiment of the present invention, and in the following description, bits magnetized upward as shown in FIG. 1(a) are indicated by diagonal lines, and FIG. 7(a) (equivalent to ), and the downwardly magnetized bit is indicated by a white frame (Fig. 7(b)).
In addition, in this embodiment, when recording (1-0 numbers) on the disk, 2 bits are used to record one signal "1" or "0". On the other hand, in the conventional example, for example, if the upward magnetization bit is an "l" signal, the downward magnetization bit is a "0" signal.

本実施例では第1図(b)に示すように、記録磁場か玉
向き磁化時には“0”信号を上向き磁化ビット2個で表
わし、′1”信号を上向き磁化ビット1個の次に下向き
磁化ビット1個を続けることにより表わす、また、下向
き磁化時には“0”信号を下向き磁化ビット2個で表わ
し、“l”信号をヒ向き磁化ビット1個の次に下向き磁
化ビット1個を続けることにより表わす。
In this embodiment, as shown in FIG. 1(b), when the recording magnetic field is magnetized in the magnetic field, a "0" signal is represented by two upwardly magnetized bits, and a '1' signal is represented by one upwardly magnetized bit, followed by a downwardly magnetized bit. In addition, when downward magnetization is performed, a “0” signal is expressed by two downward magnetized bits, and an “L” signal is expressed by one downward magnetized bit followed by one downward magnetized bit. represent.

第1[j6(c)は本実施例の記録方法を複数回繰り返
す時の説明図である。今、N回目の記録を行う時、記録
磁場を第7図(a)と同様に上向きにかけておき、記録
すべき信号“l−1−0−0“に応じ、図のように上向
き磁化ビット部にすべき部分のみにレーザ光をあてるの
で該当部のみL向き磁化ビット部となる。なお、ディス
クを最初に使用する時は例えば工場からディスクを出荷
する時に全ビットを下向きに磁化しておくこととする0
次に(N+1)回目の記録を行う時は、記録磁場を第7
+2(b)と同様に下向きにかけておき、記録すべき信
号”l−0−1−0″に応し図のように下向き磁化ビッ
トにすべき部分のみにレーザ光か照射されるので該当部
のみ下向き磁化ビット部となる。上向き磁化ビットとな
るべき部分はN回目記録時にと向き磁化ビットとなった
部分をそのまま使えるため問題はない0次に(N+2)
回目の記録を行なう時は、記録磁場をN回目の記録時同
様り向きにかけておき、記録すべき信号“0−1−1−
0”に応し図のようにt向き磁化ビ・ントにすべき部分
のみにレーザ光を照射するので、該ち部のみ上向き磁化
ビット部となる。下向き磁化ビットとなるべき部分は(
N+ 11回[1記録時に下向き磁化ビットとなった部
分をそのまま使える為、問題はない0以上の様に記録回
数か1回進むごとに記録磁場の向きを逆にしながら、信
号(第1図(C)のように4個のみでなく個数に制限は
ない)を記録してゆく。
The first [j6(c) is an explanatory diagram when the recording method of this embodiment is repeated a plurality of times. Now, when performing the Nth recording, the recording magnetic field is applied upward as in FIG. 7(a), and the upward magnetized bit portion is Since the laser beam is irradiated only on the part to be magnetized, only the corresponding part becomes the L-direction magnetized bit part. When using the disk for the first time, for example, when shipping the disk from the factory, all bits should be magnetized downward.
When performing the next (N+1)th recording, the recording magnetic field is
As with +2(b), apply the laser beam downward, and according to the signal "l-0-1-0" to be recorded, the laser beam is irradiated only on the part that should be the downward magnetized bit as shown in the figure, so only the corresponding part is irradiated. This becomes the downward magnetized bit part. There is no problem because the part that should become the upward magnetized bit can be used as is during the Nth recording.0th order (N+2)
When recording for the th time, the recording magnetic field is applied in the same direction as the Nth recording, and the signal to be recorded is “0-1-1-
As shown in the figure, the laser beam is irradiated only on the part that should be magnetized in the t-direction as shown in the figure, so that only that part becomes the upwardly magnetized bit part.The part that should be the downwardly magnetized bit part is (
N+ 11 times [There is no problem because the part that becomes the downward magnetized bit during one recording can be used as is.Reverse the direction of the recording magnetic field every time the number of recordings exceeds 0, and write the signal (see Figure 1) There is no limit to the number of items (not just four as shown in C)).

前記の説明において、上向き又は下向き磁化ビットにす
べき部分のみにレーザ光を照射するためには、その位置
を予め知る必要があるか、その−F段については後述す
る。しかし、本実施例は記録の3き換え時において、対
応する磁化ビットのみに照射するということを制限しな
ければ、記録された記録パターンを知らなくてもSき換
えを行うことができる0例えば、第2図に示すように、
上向き磁場で情報が記録されていた場合、記録磁場をr
向きとし、次に記録するデータか“0”てあれば2ビッ
ト分レーザを照射し、”t”てあれば2ビット中後の1
ビット分に対しレーザな照射すれば、たとえ前回記録の
データか“0”あるいは“l”てあっても古き換えが行
なえる(第2図(a)、(b)参照)、下向き磁場で記
録された情報も同様に磁場を上向きとし、次に記録する
データか′O″であれば2ビット分レーザを照射し、=
1″であれば2ビット中前の1ビット分に対しレーザを
照射することにより書き換えか行なえる(第2図(C)
、(d)参!!I1.)。
In the above description, in order to irradiate a laser beam only to a portion to be an upwardly or downwardly magnetized bit, it is necessary to know the position in advance, and the -F step will be described later. However, in this embodiment, if the irradiation is not limited to only the corresponding magnetized bits during the three-switching of recording, S switching can be performed without knowing the recorded recording pattern. , as shown in Figure 2,
If information is recorded with an upward magnetic field, the recording magnetic field is r
If the data to be recorded next is "0", the laser is irradiated for 2 bits, and if it is "t", the laser is irradiated for the last 1 of the 2 bits.
By irradiating a bit with a laser, even if the previous recorded data is "0" or "l", it can be replaced (see Figure 2 (a) and (b)). Recording is performed using a downward magnetic field. Similarly, for the recorded information, the magnetic field is directed upward, and if the next data to be recorded is 'O', the laser is irradiated for 2 bits, =
If it is 1", rewriting can be performed by irradiating the previous 1 bit of the 2 bits with a laser (Figure 2 (C)
, (d) See! ! I1. ).

ここで、本発明の記録速度を、従来例同様ディスク1回
転分か32分割されたうちの1セクタに信号を記録する
場合を例にとり考えると、本発明では信号を記録する前
に記録された信号を消去する必要はないため、lセクタ
に信号を記録するにはディスクはl/32回転するだけ
でよく、従来例に比較して大幅な消去記録時間の短縮を
達成できる。
Here, if we consider the recording speed of the present invention by taking as an example the case where a signal is recorded in one sector out of 32 divisions corresponding to one revolution of the disk, as in the conventional example, in the present invention, the recording speed is recorded before recording the signal. Since it is not necessary to erase the signal, the disk only needs to rotate 1/32 times to record the signal in 1 sector, and the erasing and recording time can be significantly shortened compared to the conventional example.

本発明では本実施例に限らない一般的な記録パターンを
用いたとき信号を記録するのに前回の記録時に記録磁場
(換言すれば、すでに記録された情報の“O”、“1”
を判断するのに基準となるトラック上の磁化の向き)が
上向き下向きいずれの向きであったか光磁気ディスク装
置が判別しなければならない、この判別方法としては、
−例として前回記録時の記録磁場の向きの情報をディス
クとのある領域、例えばセクタ等を管理する管理情報と
共に記録する方法か考えられる。他には、lトラックに
つき該トラック上の記録セクタの磁場方向の情報を記録
しておく管理セクタを設けることも可使である0例えば
セクタごとに情報を記録する時には、管理領域を読み取
り、情報セクタの前回記録のm*方向を知り、今回記録
の磁場方向を書き込んだ上で該セクタの情報を書き換え
ることになる。よって、この場合はセクタごとに記録磁
場の向きがまらまちになることになる。なお、該管理情
報の取り扱いには、前記方法たけに限らず各種の方法に
よって時間の短縮が可使である。
In the present invention, when a general recording pattern not limited to this embodiment is used, the recording magnetic field (in other words, "O", "1" of already recorded information) is used for recording a signal.
The magneto-optical disk device must determine whether the direction of magnetization on the track (which is used as a reference for determining the direction of magnetization) is upward or downward.The method for this determination is as follows:
- For example, a method may be considered in which information about the direction of the recording magnetic field at the time of previous recording is recorded together with management information for managing a certain area of the disk, such as a sector. Alternatively, it is also possible to provide a management sector for each track in which information about the magnetic field direction of the recording sector on the track is recorded.For example, when recording information for each sector, the management area is read and the information is The m* direction of the previous recording of the sector is known, the magnetic field direction of the current recording is written, and the information of the sector is rewritten. Therefore, in this case, the direction of the recording magnetic field will vary from sector to sector. Note that in handling the management information, it is possible to shorten the time by using not only the above-mentioned method but also various methods.

以北、述べた本発明の実施例は、光磁気ディスク玉に記
録する磁化パターンについて述べており、従来の変調方
式によりデータを変調後、本発明の記録方法を用いるこ
とかできる。このようにすると、“O′″信号が連続す
ることかなくなり、ビット同期あるいはクロック同期を
必ずとることかてきる0例えば2−7変換後、本発明の
記録方法を用いれば、O”の連続か7以内なので、ビッ
ト同期あるいはクロック同期がとれる。他の変調方式の
場合も同様に最小反転間隔か規潤されているものであれ
ばよい。
The embodiments of the present invention described above describe magnetization patterns recorded on magneto-optical disk balls, and the recording method of the present invention can be used after data is modulated by a conventional modulation method. By doing this, the "O'" signal will not be continuous, and bit synchronization or clock synchronization will be ensured. Since it is within 7, bit synchronization or clock synchronization can be achieved.In the case of other modulation methods, it is sufficient as long as the minimum inversion interval is kept regular.

また、各種変調方式を用いず、直接データを未完11の
記録方法で記録する場合も“0”およびl″に対応する
磁化パターン内に少なくとも1つの磁化反転をもたせる
ことでビット同期をとることかてきる。この場合の記録
パターンの一例を第3図に示す。
Furthermore, even when directly recording data using the recording method described in Incomplete 11 without using various modulation methods, bit synchronization can be achieved by providing at least one magnetization reversal in the magnetization patterns corresponding to "0" and "1". An example of a recording pattern in this case is shown in FIG.

ビット同期をとる為には、他に第4図に示す様にデータ
ビウド対応の記録パターンを連続記録する時、ビット同
期あるいはクロック同期の為の磁化反転を有する記録パ
ターン30(回期パターン)を挿入することか考えられ
る。こうした同期パターンを挿入し、該同期パターンを
特殊なパターンとすることにより、データの同期をとる
ことかできる。もちろん、第5図に示すようにデータ同
期用の特殊パターン31を別に設けてもデータの同期を
とることができる。
In addition, in order to achieve bit synchronization, as shown in Figure 4, when recording patterns compatible with data video are continuously recorded, a recording pattern 30 (periodic pattern) having magnetization reversal for bit synchronization or clock synchronization is inserted. I can think of something to do. By inserting such a synchronization pattern and making the synchronization pattern a special pattern, data can be synchronized. Of course, as shown in FIG. 5, data synchronization can also be achieved by separately providing a special pattern 31 for data synchronization.

第1図の記録パターンを用いた場合、前回記録の記録パ
ターンを知ることなしに次の記録か行なえるか、別のパ
ターン、例えば第7図に承すようにL向き磁化記録時の
“0”を3ビットのL向き磁化、“l”を3ピツト中2
ビットを上向き磁化とした3つのパターンとし、また下
向き磁化記録時の“0′を3ヒツトの下向き磁化、′1
″を3ビット中2ビットを下向き磁化とした3つのパタ
ーンとすると、下向き磁場て“l”を記録する場合、前
回の記録である上向き磁化のパターンかどの様なパター
ンであるか判断か必要となる。そこで第7図のような記
録パターンを採用するときは、前回のデータを読み取る
為に、記録ビームに先行して読取りビームを設け、曲回
記録のデータを読み取った上て読み取ったデータ応して
レーザ光を照射してパターンを、I?き換えるようにす
る。
When the recording pattern shown in Figure 1 is used, is it possible to perform the next recording without knowing the recording pattern of the previous recording? ” is magnetized in the L direction of 3 bits, “l” is 2 out of 3 pits
There are 3 patterns in which the bit is magnetized upward, and 3 hits of "0" during downward magnetization recording, 3 hits of downward magnetization, '1
'' is three patterns in which 2 out of 3 bits are magnetized downward, and when recording "l" with a downward magnetic field, it is necessary to judge which pattern is the previous recording pattern of upward magnetization. Therefore, when adopting a recording pattern as shown in Figure 7, a reading beam is provided in advance of the recording beam in order to read the previous data, and after reading the data of the track record, the reading beam is Then, a laser beam is irradiated to change the pattern.

また、先行したビームて読み取る必要のない第1[′A
のパターンを用いた場合ても、先行した読み取りビーム
を設けることにより、レーザを照射して磁化を反転する
必要のないパターン(例えば、■−向きの“1″から下
向きのl”に3き換える場合等)に無駄なレーザ照射を
することか避けられる。このようにすれば、レーザの高
寿命化に効果かあり、また複数回にわたり、同一方向に
磁化することかなくなりパターンの変形等を防ぐことか
Cきる。
Also, the first ['A
Even if a pattern of (e.g.), unnecessary laser irradiation can be avoided.This will have the effect of extending the lifespan of the laser, and will also prevent pattern deformation since it will not be magnetized in the same direction multiple times. Kotoka C Kiruru.

さらに、記録ビームの後方に読み取りビームを配するこ
とにより、記録したデータのベリファイも”r tmと
する構成を取ることもてきる。
Furthermore, by arranging the reading beam behind the recording beam, it is also possible to verify the recorded data at "rtm".

[発明の効果] 以L、説明したように本発明に係る光磁気記録方法によ
れば、N回目記録時と(N+ 1 )四〇記録時として
記録磁場の向きを逆にすることにより、いわゆるオーバ
ライドを可涜とし、信号の消去記録時間を大幅に短縮す
ることができる。
[Effects of the Invention] As explained below, according to the magneto-optical recording method according to the present invention, by reversing the direction of the recording magnetic field at the time of Nth recording and at the time of (N+1)40th recording, so-called By making override unnecessary, signal erasure recording time can be significantly shortened.

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

第1図(a)、(b)、(C)、第2図(a)、(b)
、(c)、(d)はそれぞれ本発明の光磁気記録方法の
第1実施例を説11するための説明図、第3図はパター
ン中に少なくとも1つの磁化反転を有する実施例の説明
図、第4図、第5UAはそれぞれビット同期あるいはク
ロック回期をとる実施例の説明図、第6図は記録ビーム
に先行して読み取りビームを設ける実施例の説明図であ
る。 第7図(a)、(b)、第8図(a)、(b)、(c)
はそれぞれ光磁気2鎚の原理を説明するための図、第9
図(a)、(b)はそれデれ光磁気ディスク装置の側面
図、光磁気ディスクのモ面図である。 代理人 弁理士  山 下 橿 子 弟1図 (a)      (b) ロ下E1.魚7tビ・7ト  80 ロコ下幻5急/L
時(す 9  面上ヱj=  ”=   No1sZs′r(よ
I’fi’l :’A/c al )8B−ゴWコ  
 (N++3回目自InLH’t(j m 51a%I
rQ9%)@   ヒj−上”   ’     (N
+2)riJgmtt1時(Lfn3Kb、ttB*)
第2 前銹秋態 −二 (C) 下1幻S茄Iヒ日丹のイ灸 ゛0′!乙1乗 薊も乙衾豫杯Jミ・   口D[ を乙f朱ギk   ピエコ      山間 ゝ1°自乙″を粂 (d) 乙コ    ロコ 第3図 (エイ1A爆] 第41A (、)チータビ゛1.ト:寥衿5を乙を未へr−レを巳
づ第5 図 I 第6図 Oイi 号           1 イ剋号□ QD   □ [=ピコエコ     下friさ4泣にイヒ時□ 第7図 (0)盲乙値         (b)哨気第8図 (Cン                (bン第9図 (G)
Figure 1 (a), (b), (C), Figure 2 (a), (b)
, (c), and (d) are explanatory diagrams for explaining the first embodiment of the magneto-optical recording method of the present invention, respectively, and FIG. 3 is an explanatory diagram of an embodiment having at least one magnetization reversal in the pattern. , FIGS. 4 and 5 UA are explanatory diagrams of an embodiment in which bit synchronization or clock cycles are provided, respectively, and FIG. 6 is an explanatory diagram of an embodiment in which a reading beam is provided in advance of a recording beam. Figure 7 (a), (b), Figure 8 (a), (b), (c)
are diagrams for explaining the principle of magneto-optical two hammers, respectively.
Figures (a) and (b) are a side view of the magneto-optical disk device and a top view of the magneto-optical disk. Agent Patent Attorney Kashi Yamashita Children 1 (a) (b) Lower E1. Fish 7t Bi・7t 80 Loco Gen5 Rapid/L
Time (S9 上ヱj= ”= No1sZs'r(yoI'fi'l :'A/cal)8B-GoWko
(N++3rd selfInLH't(j m 51a%I
rQ9%) @ Hij-Up"' (N
+2) riJgmtt1 time (Lfn3Kb, ttB*)
2nd Mae-Seiju-2 (C) 2nd 1 Illusion S-I Hihitan's I moxibustion゛0'! Otsu 1st place 薊 also Otsu 衾 豫 Cup J Mi・口D [ を ト f 朱GI k pieko Yamama ゝ 1° ゝ ゝ'' を 粂 (d) Otsuko loco fig. 3 (Ei 1A bomb) 41A (,) Cheetah beat 1. To: 5th collar 5 to Otsu to R-re. 5th Figure I Figure 6 Oi No. 1 No. Figure 7 (0) Blind value (b) Wind alarm Figure 8 (Cn (b) Figure 9 (G)

Claims (10)

【特許請求の範囲】[Claims] (1)光磁気記録媒体に光を照射し、情報を記録する光
磁気記録方法において、N回目記録時(N=1、2、3
・・・)と(N+1)回目記録時とで記録磁場の向きを
逆にすることを特徴とする光磁気記録方法。
(1) In a magneto-optical recording method in which information is recorded by irradiating light onto a magneto-optical recording medium, at the Nth recording (N=1, 2, 3
...) and the (N+1)th recording time, the direction of the recording magnetic field is reversed.
(2)第1、第2の磁化の向きを有する光磁気記録媒体
に2値化信号を記録するに際し、第1、第2の記録磁場
の向きそれぞれにおいて前記2値化信号にそれぞれ対応
する2種別の磁化パターンを用いて情報を記録すること
を特徴とする特許請求の範囲第1項記載の光磁気記録方
法。
(2) When recording a binary signal on a magneto-optical recording medium having first and second magnetization directions, two 2. The magneto-optical recording method according to claim 1, wherein information is recorded using different types of magnetization patterns.
(3)複数に分割された記録領域に対応して、該記録領
域の前記記録磁場の向きを光磁気記録媒体上に記録する
ことを特徴とする特許請求の範囲第1項記載の光磁気記
録方法。
(3) Magneto-optical recording according to claim 1, characterized in that the direction of the recording magnetic field of the recording area is recorded on a magneto-optical recording medium corresponding to a plurality of divided recording areas. Method.
(4)記録用光ビームに先行した再生用光ビームにより
、前回記録のデータを再生し、該再生データに基づき記
録用光ビームの変調を決めることを特徴とする特許請求
の範囲第1項記載の光磁気記録方法。
(4) A reproducing light beam that precedes a recording light beam reproduces previously recorded data, and modulation of the recording light beam is determined based on the reproduced data. magneto-optical recording method.
(5)記録用光ビームに後続する再生用光ビームにより
記録データを再生確認することを特徴とする特許請求の
範囲第1項記載の光磁気記録方法。
(5) The magneto-optical recording method according to claim 1, characterized in that reproduction of recorded data is confirmed by a reproduction light beam following a recording light beam.
(6)前記磁化パターン内に少なくとも1つの磁化反転
を有することを特徴とする特許請求の範囲第2項記載の
光磁気記録方法。
(6) The magneto-optical recording method according to claim 2, wherein the magnetization pattern has at least one magnetization reversal.
(7)前記2値化信号が記録情報を所定の変調方法によ
り変調された後の2値化信号であることを特徴とする特
許請求の範囲第2項記載の光磁気記録方法。
(7) The magneto-optical recording method according to claim 2, wherein the binary signal is a binary signal obtained by modulating recording information using a predetermined modulation method.
(8)1個又は複数の前記磁化パターンおきに同期パタ
ーンを挿入することを特徴とする特許請求の範囲第2項
記載の光磁気記録方法。
(8) The magneto-optical recording method according to claim 2, characterized in that a synchronization pattern is inserted every other one or more of the magnetization patterns.
(9)前記磁化パターンか前記記録媒体上において2ビ
ットで構成され、2値化信号(1−0信号)を記録する
に際し、媒体磁化の向きが第1の向きである場合には、
“0”信号を第1の向き磁化ビット2個で表わし、“1
”信号を第1の向き磁化ビット1個と第2の向き磁化ビ
ット1個とで表わし、また、媒体磁化の向きが第2の向
きである場合には、“0”信号を第2の向き磁化ビット
2個で表わし、“1”信号を第1の向き磁化ビット1個
と第2の向き磁化ビット1個とで表わすことを特徴とす
る特許請求の範囲第2項記載の光磁気記録方法。
(9) If the magnetization pattern is composed of 2 bits on the recording medium and the direction of medium magnetization is the first direction when recording a binary signal (1-0 signal),
A “0” signal is represented by two first direction magnetized bits, and a “1”
” signal is represented by one bit magnetized in the first direction and one bit magnetized in the second direction, and when the direction of medium magnetization is in the second direction, the “0” signal is expressed in the second direction. The magneto-optical recording method according to claim 2, characterized in that the "1" signal is represented by two magnetized bits, and the "1" signal is represented by one magnetized bit in the first direction and one magnetized bit in the second direction. .
(10)前記磁化パターンが前記記録媒体上において2
ビットで構成され、2値化信号(1−0信号)を記録す
るに際し、媒体磁化の向きが第1の向きである場合には
、“1”信号を第1の向き磁化ビット2個で表わし、“
0”信号を第1の向き磁化ビット1個と第2の向き磁化
ビット1個とで表わし、また、媒体磁化の向きか第2の
向きである場合には、“1”信号を第2の向き磁化ビッ
ト2個で表わし、“0”信号を第1の向き磁化ビット1
個と第2の向き磁化ビット1個とで表わすことを特徴と
する特許請求の範囲第2項記載の光磁気記録方法。
(10) The magnetization pattern is set to 2 on the recording medium.
When recording a binary signal (1-0 signal), if the direction of medium magnetization is the first direction, a "1" signal is represented by two bits magnetized in the first direction. ,“
A “0” signal is represented by one first direction magnetization bit and one second direction magnetization bit, and if the medium magnetization direction is the second direction, the “1” signal is represented by a second direction magnetization bit. It is represented by two direction magnetization bits, and the “0” signal is expressed as the first direction magnetization bit 1.
3. The magneto-optical recording method according to claim 2, wherein the magneto-optical recording method is represented by one bit and one bit magnetized in the second direction.
JP18414686A 1986-08-07 1986-08-07 Magneto-optical recording method Pending JPS6342055A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18414686A JPS6342055A (en) 1986-08-07 1986-08-07 Magneto-optical recording method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18414686A JPS6342055A (en) 1986-08-07 1986-08-07 Magneto-optical recording method

Publications (1)

Publication Number Publication Date
JPS6342055A true JPS6342055A (en) 1988-02-23

Family

ID=16148170

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18414686A Pending JPS6342055A (en) 1986-08-07 1986-08-07 Magneto-optical recording method

Country Status (1)

Country Link
JP (1) JPS6342055A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0227549A (en) * 1988-07-15 1990-01-30 Pioneer Electron Corp Magneto-optical disk device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0227549A (en) * 1988-07-15 1990-01-30 Pioneer Electron Corp Magneto-optical disk device

Similar Documents

Publication Publication Date Title
JPH03183047A (en) Magneto-optical recorder
JPH04259941A (en) Method for recording sector management information of magneto-optical disk
JPS6342055A (en) Magneto-optical recording method
JPH0664767B2 (en) Optical information recording method and optical information recording device
JPS61240453A (en) Optical magnetic disk device
JPS61229247A (en) Photomagnetic medium
US6577560B2 (en) Magneto-optic recording medium in which magnetic partition tracks are removed for high track density
JPH0417142A (en) Magneto-optical recording and reproducing device
JP2783774B2 (en) Optical information recording device
JPS6265251A (en) Information recording and reproducing device
JPS59210530A (en) Writing system of servo signal
JP2855918B2 (en) Optical information recording method and device
JPH04177644A (en) Megnetooptical compact disk drive
JPS6334756A (en) Recording method for magneto-optical memory
JP3104913B2 (en) Optical recording method and apparatus for disk-shaped recording medium
JPS61175947A (en) Optical information recording and reproducing device
JPH01248341A (en) Method for recording on magneto-optical recording medium
JPS63225931A (en) Reloadable optical disk device
JPH0782706B2 (en) Disc recording / reproducing device
JPH0963143A (en) Optical disk device
JPS62165768A (en) Optical information recording and reproducing device
JPH10105972A (en) Optical recording method
JP2001084598A (en) Optical information recording medium
JPH08153349A (en) Digital data recording method, digital data recorder and digital data recording/reproducing device
JPS61261870A (en) Photo magnetic recording and reproducing device