JPH07220317A - Magneto-optical recording/reproducing device and magneto-optical recording medium - Google Patents

Magneto-optical recording/reproducing device and magneto-optical recording medium

Info

Publication number
JPH07220317A
JPH07220317A JP693294A JP693294A JPH07220317A JP H07220317 A JPH07220317 A JP H07220317A JP 693294 A JP693294 A JP 693294A JP 693294 A JP693294 A JP 693294A JP H07220317 A JPH07220317 A JP H07220317A
Authority
JP
Japan
Prior art keywords
recording
magneto
optical recording
optical
recorded
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
JP693294A
Other languages
Japanese (ja)
Inventor
Yasuyuki Miyaoka
康之 宮岡
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 JP693294A priority Critical patent/JPH07220317A/en
Publication of JPH07220317A publication Critical patent/JPH07220317A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To perform at least the quadruple recording with high density by setting the least recording pit length of a recording pattern at or less than 1/4 diameter of a beam spot. CONSTITUTION:When the record signals 2, 1, -1 and -2 are recorded, a magneto-optical recording medium is irradiated by a laser beam of necessary and sufficient intensity PW. At the same time, a modulated magnetic field HW is impressed to the part irradiated by the laser beam. Under such conditions, the drive current used for generation of the field HW is turned into a modulated current waveform so that each record pit string is recorded. Therefore the modulated magnetic fields of different directions are impressed to the part of the recording medium to be irradiated by the laser beam in accordance with the pit pattern to be recorded with necessary and sufficient field intensity HV. In such a way, the information is recorded. Thus the quadruple optical signal levels 2, 1, -1 and -2 are obtained when the record pit strings 1111, 0110 and 0000 having the smallest record pit length set at or less than 1/4 diameter of a beam spot are recorded on the recording medium.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は光磁気記録再生装置及び
光磁気記録媒体に係り、特に光ビームを照射するととも
に光照射部位に記録信号に応じた変調磁界を印加するこ
とにより記録ピットを形成し、情報の記録を行なう磁界
変調方式の光磁気記録再生装置及び光磁気記録媒体に関
するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-optical recording / reproducing apparatus and a magneto-optical recording medium, and in particular, a recording pit is formed by irradiating a light beam and applying a modulation magnetic field according to a recording signal to a light irradiation portion. However, the present invention relates to a magneto-optical recording / reproducing apparatus and a magneto-optical recording medium of a magnetic field modulation system for recording information.

【0002】[0002]

【従来の技術】従来、磁界変調方式による光磁気記録再
生装置は例えば図6のタイミング図に示すような方法で
記録が行なわれていた。
2. Description of the Related Art Conventionally, in a magneto-optical recording / reproducing apparatus using a magnetic field modulation method, recording is performed by a method shown in a timing chart of FIG. 6, for example.

【0003】図6中(a)の記録信号は、記録を行なう
2値データを例えば2−7変調方式のような変調方式で
変換後、さらにNRZI化した記録信号であり、2値信
号の立上り、立下りの両エッジ情報を持たせたマーク長
記録の記録信号である。図6中(b)は前記記録信号を
記録する場合のレーザ光出力であり、記録動作中、必要
十分な記録レーザパワーPw を一定強度で出力する。図
6中(c)は記録動作中に前記レーザ光の照射部位に印
加する変調磁界を示すものであり、図6中(d)は記録
動作により形成された記録ピット列を示す概略図、図6
中(e)は該記録ピット列を再生した場合の再生信号波
形を示すものである。
A recording signal shown in FIG. 6A is a recording signal obtained by converting binary data to be recorded by a modulation method such as a 2-7 modulation method and further converting it into NRZI. , A recording signal of mark length recording having both trailing edge information. FIG. 6B shows a laser light output when the recording signal is recorded, and outputs a necessary and sufficient recording laser power P w at a constant intensity during the recording operation. 6C shows the modulation magnetic field applied to the laser light irradiation portion during the recording operation, and FIG. 6D is a schematic view showing a recording pit row formed by the recording operation. 6
The middle part (e) shows a reproduced signal waveform when the recording pit string is reproduced.

【0004】以下、図6のタイミング図を用いて、記録
動作を説明する。図6中(a)に示すような記録信号が
入力された場合、記録レーザパワー強度を記録に必要か
つ十分な値Pw を一定強度で出力する。同時に記録に必
要かつ十分な磁界強度Hw で記録信号に応じて、印加す
る向きの異なる変調磁界(図6の(c))がレーザ光照
射によりキュリー点以上に温度が上がった光磁気記録媒
体のレーザ光照射部位に印加され、記録が行なわれる。
この記録動作により図6の(d)に示すような記録ピッ
ト列が形成され、情報が記録される。ここで斜線部は磁
化の向きが上向きの記録ピットを示し、白抜き部は磁化
の向きが下向きの記録ピットを示している。
The recording operation will be described below with reference to the timing chart of FIG. When a recording signal as shown in (a) of FIG. 6 is input, a value P w necessary and sufficient for recording the recording laser power intensity is output at a constant intensity. At the same time, according to a recording signal with a magnetic field strength H w that is necessary and sufficient for recording, a magneto-optical recording medium in which a modulating magnetic field (FIG. 6C) applied in different directions increases its temperature above the Curie point by laser light irradiation. Is applied to the portion irradiated with the laser beam, and recording is performed.
By this recording operation, a recording pit string as shown in FIG. 6D is formed and information is recorded. Here, the shaded portions indicate the recording pits whose magnetization direction is upward, and the open portions indicate the recording pits whose magnetization direction is downward.

【0005】図6の(e)はこの記録ピットパターン
(図6の(d))を再生した場合に得られる光磁気信号
であり、図6の(e)中の“0”に示すレベルと再生波
形の交点に情報を持っており、例えば、コンパレータ等
で2値化を行なうことにより記録情報を再生することが
できる。
FIG. 6 (e) shows a magneto-optical signal obtained when this recording pit pattern ((d) in FIG. 6) is reproduced, and has a level indicated by "0" in FIG. 6 (e). Information is held at the intersection of the reproduced waveform, and the recorded information can be reproduced by performing binarization with a comparator or the like, for example.

【0006】[0006]

【発明が解決しようとする課題】しかしながら、上記従
来例において、光磁気記録媒体が記録によって取り得る
磁化の向きは、図6の(e)に示すように上向き、下向
きの2つの状態であり、再生信号も2値情報として処理
されており、さらに高密度化を図った場合2値記録では
高密度化に限界があるという問題があった。
However, in the above-mentioned conventional example, the directions of magnetization that the magneto-optical recording medium can take by recording are two states of upward and downward as shown in (e) of FIG. The reproduced signal is also processed as binary information, and there has been a problem that there is a limit to high density in binary recording when higher density is intended.

【0007】[0007]

【課題を解決するための手段】本発明の光磁気記録再生
装置は、光磁気記録媒体に光ビームを照射するとともに
光照射部位に記録信号に応じ変調磁界を印加すること
で、記録ピットを形成して情報の記録を行なう光磁気記
録再生装置において、最小記録ピット長がビームスポッ
ト径の1/4以下となるように前記変調磁界を印加する
手段を有することを特徴とする。
A magneto-optical recording / reproducing apparatus of the present invention forms a recording pit by irradiating a magneto-optical recording medium with a light beam and applying a modulation magnetic field to a light-irradiated portion according to a recording signal. The magneto-optical recording / reproducing apparatus for recording information is characterized in that it has means for applying the modulating magnetic field so that the minimum recording pit length becomes ¼ or less of the beam spot diameter.

【0008】また本発明の光磁気記録再生装置は、最小
記録ピット長がビームスポット径の1/4以下となるよ
うに記録パターンが記録された光磁気記録媒体からの再
生信号のレベルとそれぞれ設定された所定の基準電圧と
を比較する複数の比較手段と、該比較手段からの信号に
基づき、少なくとも4値の再生信号を得る手段とを有す
ることを特徴とする。
Further, in the magneto-optical recording / reproducing apparatus of the present invention, the level of the reproduction signal from the magneto-optical recording medium on which the recording pattern is recorded is set so that the minimum recording pit length becomes ¼ or less of the beam spot diameter. It is characterized in that it has a plurality of comparing means for comparing the generated predetermined reference voltage with each other, and means for obtaining at least a quaternary reproduced signal based on the signals from the comparing means.

【0009】本発明の光磁気記録媒体は、光ビームを照
射するとともに光照射部位に記録信号に応じた変調磁界
を印加することで、記録ピットを形成してなる光磁気記
録媒体において、記録パターンの最小記録ピット長をビ
ームスポット径の1/4以下としたことを特徴とする。
The magneto-optical recording medium of the present invention is a magneto-optical recording medium in which recording pits are formed by irradiating a light beam and applying a modulation magnetic field according to a recording signal to a light irradiation portion. The minimum recording pit length of is less than 1/4 of the beam spot diameter.

【0010】[0010]

【作用】本発明は、光ビームを照射するとともに光照射
部位に記録信号に応じた変調磁界を印加して記録ピット
を形成する磁界変調方式の光磁気記録再生装置又は磁界
変調方式の光磁気記録媒体において、記録パターンの最
小記録ピット長をビームスポット径の1/4以下とする
ことで、少なくとも4値の記録を可能とするものであ
る。また、本発明は最小記録ピット長がビームスポット
径の1/4以下の記録パターンから4値の再生信号出力
を得ることを可能とするものである。
According to the present invention, a magnetic field modulation type magneto-optical recording / reproducing apparatus or a magnetic field modulation type magneto-optical recording which irradiates a light beam and applies a modulation magnetic field according to a recording signal to a light irradiation portion to form a recording pit. In the medium, at least four-value recording is possible by setting the minimum recording pit length of the recording pattern to be ¼ or less of the beam spot diameter. Further, the present invention makes it possible to obtain a 4-level reproduction signal output from a recording pattern having a minimum recording pit length of ¼ or less of the beam spot diameter.

【0011】[0011]

【実施例】以下、本発明の実施例について図面を用いて
詳細に説明する。
Embodiments of the present invention will be described in detail below with reference to the drawings.

【0012】図1は本発明に係る光磁気記録再生装置に
おける光磁気記録方式を示すタイミング図であり、図1
の(a)は記録信号、図1の(b)は記録レーザパワ
ー、図1の(c)は変調磁界を発生させるための駆動電
流、図1の(d)は変調磁界、図1の(e)は記録ピッ
ト列、図1の(f)は記録ピット列を再生した場合の光
磁気信号である。なお、ここでは再生信号との対応を解
り易くするために図1の(a)の記録信号を4値レベル
で表現している。例えば、2値入力信号の“11”,
“10”,“01”,“00”を図1中(a)の記録信
号“2”,“1”,“−1”,“−2”にそれぞれ対応
させることができる。
FIG. 1 is a timing chart showing a magneto-optical recording system in a magneto-optical recording / reproducing apparatus according to the present invention.
1A is a recording signal, FIG. 1B is a recording laser power, FIG. 1C is a drive current for generating a modulation magnetic field, FIG. 1D is a modulation magnetic field, and FIG. FIG. 1F shows a magneto-optical signal when the recording pit string is reproduced. Note that, here, the recording signal of FIG. 1A is expressed by a four-value level in order to make it easy to understand the correspondence with the reproduction signal. For example, the binary input signal “11”,
"10", "01", "00" can be made to correspond to the recording signals "2", "1", "-1", "-2" of FIG.

【0013】図2は光磁気記録媒体に記録された記録パ
ターンを再生する場合の原理を示す図であり、ビームス
ポット内光量分布、記録ピットパターン、光磁気信号レ
ベルの関係を示すものである。図2中(a)は4値入力
の“1”を再生する場合、図2中(b)は4値入力の
“−1”を再生する場合を示している。ここで図1の
(e)及び図2の斜線部は磁化の向きが上向きの磁区
を、白抜き部は磁化の向きが下向きの磁区をそれぞれ意
味している。
FIG. 2 is a diagram showing the principle of reproducing the recording pattern recorded on the magneto-optical recording medium, and shows the relationship among the light quantity distribution in the beam spot, the recording pit pattern, and the magneto-optical signal level. 2A shows the case of reproducing a four-value input "1", and FIG. 2B shows the case of reproducing a four-value input "-1". Here, the shaded portions in (e) and FIG. 2 in FIG. 1 indicate magnetic domains whose magnetization direction is upward, and the white portions indicate magnetic domains whose magnetization direction is downward.

【0014】まず、光磁気記録媒体に4値記録を行なう
原理について図2を用いて説明する。
First, the principle of 4-value recording on a magneto-optical recording medium will be described with reference to FIG.

【0015】本発明は、例えば図2(a)(b)の記録
ピットパターンに示すように、1つの光ビームスポット
内に磁化の向きが異なる複数の記録ピットが存在する場
合に、光磁気信号が干渉を起こし再生信号レベルに変化
が現れること、及び図2(a)(b)のビームスポット
光量分布に示されるように、光ビームスポットの光量分
布がガウス分布になっていて、スポット中心付近の光量
が大きいことを利用して、少なくとも4値の記録を行う
ものである。
According to the present invention, when a plurality of recording pits having different magnetization directions are present in one light beam spot, for example, as shown in the recording pit pattern of FIGS. Cause a change in the reproduction signal level, and as shown in the beam spot light quantity distributions of FIGS. 2A and 2B, the light quantity distribution of the light beam spot is a Gaussian distribution and is near the center of the spot. The recording of at least four values is performed by utilizing the large amount of light.

【0016】即ち、最短記録ピット長がビームスポット
径の1/4以下であるような記録ピット列“0110”
からなる図2(a)の記録ピットパターンに、光量分布
がガウス分布の光ビームが照射されると、光スポットの
中心付近の、磁化の向きが上向きの磁区を有する斜線部
には光量が多く、光スポットの周囲部付近の、磁化の向
きが下向きの磁区を有する白抜き部には光量が少なくな
るため、光磁気信号が干渉を起こし4値の光磁気信号レ
ベルの“1”が再生信号レベルとして得られる。また、
最短記録ピット長がビームスポット径の1/4以下であ
るような記録ピット列“1001”からなる図2(b)
の記録ピットパターンに、光量分布がガウス分布の光ビ
ームが照射されると、光スポットの中心付近の、磁化の
向きが下向きの磁区を有する白抜き部には光量が多く、
光スポットの周囲部付近の、磁化の向きが上向きの磁区
を有する斜線部には光量が少なくなるため、光磁気信号
が干渉を起こし4値の光磁気信号レベルの“−1”が再
生信号レベルとして得られる。
That is, the recording pit string "0110" whose shortest recording pit length is ¼ or less of the beam spot diameter.
2A is irradiated with a light beam having a Gaussian distribution, the amount of light is large in the shaded area near the center of the light spot, which has a magnetic domain with an upward magnetization direction. Since the amount of light is small in the white part near the periphery of the light spot, which has a magnetic domain with a downward magnetization direction, the magneto-optical signal causes interference and the 4-valued magneto-optical signal level "1" is the reproduction signal. Obtained as a level. Also,
FIG. 2B, which is composed of a recording pit string “1001” whose shortest recording pit length is ¼ or less of the beam spot diameter.
When the recording pit pattern of is irradiated with a light beam having a Gaussian distribution of light quantity, a large amount of light is present in the white part near the center of the light spot, which has a magnetic domain with a downward magnetization direction.
Since the amount of light is small in the shaded area near the periphery of the light spot that has a magnetic domain with an upward magnetization direction, the magneto-optical signal causes interference and the 4-level magneto-optical signal level “−1” is the reproduction signal level. Obtained as.

【0017】さらに、不図示であるが、最短記録ピット
長がビームスポット径の1/4以下であるような記録ピ
ット列“1111”からなる記録ピットパターンからは
4値の光磁気信号レベルの“2”が得られ、最短記録ピ
ット長がビームスポット径の1/4以下であるような記
録ピット列“0000”からなる記録ピットパターンか
らは4値の光磁気信号レベルの“−2”が得られる。
Further, although not shown, from the recording pit pattern consisting of the recording pit string "1111" whose shortest recording pit length is 1/4 or less of the beam spot diameter, a 4-level magneto-optical signal level "" is obtained. 2 "is obtained, and a 4-level magneto-optical signal level of" -2 "is obtained from a recording pit pattern consisting of a recording pit row" 0000 "in which the shortest recording pit length is 1/4 or less of the beam spot diameter. To be

【0018】このように、最短記録ピット長がビームス
ポット径の1/4以下であるような記録ピット列“11
11”、“0110”、“1001”、“0000”を
光磁気記録媒体に記録すれば、4値の光磁気信号レベル
の“2”、“1”、“−1”、“−2”を得ることがで
きる。
As described above, the recording pit row "11" whose shortest recording pit length is ¼ or less of the beam spot diameter is used.
If 11 "," 0110 "," 1001 ", and" 0000 "are recorded on the magneto-optical recording medium, four levels of magneto-optical signal levels of" 2 "," 1 "," -1 ", and" -2 "are obtained. Obtainable.

【0019】次に、光磁気記録媒体に4値記録を行い、
再生信号を得る方式について図1を用いて説明する。
Next, four-value recording is performed on the magneto-optical recording medium,
A method of obtaining a reproduction signal will be described with reference to FIG.

【0020】図1(a)に示すような記録信号“2”、
“1”、“−1”、“−2”を記録する場合、記録レー
ザ光強度として必要かつ十分なレーザ光強度Pw (図1
(b))のレーザビームを光磁気記録媒体に照射し、こ
れと同時に変調磁界HW をレーザ光照射部位に印加する
(図1(d))。この場合、変調磁界を発生させるため
の駆動電流はそれぞれの記録ピット列を記録するために
図1の(c)に示すような電流波形になる。このように
して、光磁気記録媒体の記録レーザ光照射部位には、記
録するために必要かつ十分な磁界強度Hw で記録するピ
ットパターンに応じて向きの異なる変調磁界が印加さ
れ、情報の記録が行なわれる。その結果、光磁気記録媒
体には図1の(e)に示すような記録磁区ピット列が形
成される。
The recording signal "2" as shown in FIG.
When “1”, “−1”, and “-2” are recorded, the laser light intensity P w that is necessary and sufficient as the recording laser light intensity (see FIG.
The magneto-optical recording medium is irradiated with the laser beam of (b)), and at the same time, the modulation magnetic field H W is applied to the laser light irradiation site (FIG. 1D). In this case, the driving current for generating the modulation magnetic field has a current waveform as shown in FIG. 1C for recording each recording pit row. In this way, a modulation magnetic field whose direction is different depending on the pit pattern to be recorded with a magnetic field intensity H w necessary and sufficient for recording is applied to the recording laser light irradiation portion of the magneto-optical recording medium, thereby recording information. Is performed. As a result, a recording magnetic domain pit train as shown in FIG. 1E is formed on the magneto-optical recording medium.

【0021】このように記録された記録ピット列を図1
中(e)に示すようなスポット径の光ビームで再生した
場合、前述した本発明の原理に従って、記録ピット列が
“1111”の場合は再生光磁気信号レベルは“2”に
なり、記録ピット列が“0110”の場合はビームスポ
ット内の光磁気信号の干渉により“1”になり、記録ピ
ット列が“1001”の場合は同様にビームスポット内
の光磁気信号の干渉により“−1”になり、記録ピット
列が“0000”の場合は光磁気信号レベルは“−2”
になり、その結果、図1の(f)に示すような4値のレ
ベルを取る再生光磁気信号が得られる。この信号を4値
のレベル検知することにより、記録情報を再生すること
が可能となり、より高密度に記録することが可能な光磁
気記録装置を提供することが可能となる。
FIG. 1 shows a row of recording pits thus recorded.
When reproducing with a light beam having a spot diameter as shown in the middle (e), the reproducing magneto-optical signal level becomes "2" when the recording pit row is "1111" according to the principle of the present invention described above, and the recording pit When the row is “0110”, it becomes “1” due to the interference of the magneto-optical signal in the beam spot, and when the row of recording pits is “1001”, similarly it is “−1” due to the interference of the magneto-optical signal in the beam spot. When the recording pit row is "0000", the magneto-optical signal level is "-2".
As a result, a reproduced magneto-optical signal having four levels as shown in FIG. 1 (f) is obtained. By detecting the four-valued level of this signal, it becomes possible to reproduce the recorded information, and it is possible to provide a magneto-optical recording device capable of recording at a higher density.

【0022】図3は本発明に係る磁気変調方式の光磁気
記録再生装置の概略的な構成を示す図であり、同図にお
いて、10は光磁気ディスク、11は光磁気ディスク1
0を回転させるスピンドルモータ、12はレーザ光をデ
ィスクにスポット状に合焦させ、ディスクからの反射光
を検出する光ヘッドである。光ヘッド12は各種レン
ズ,PBS等で構成されている。13は半導体レーザ駆
動回路、14は浮上磁気ヘッド、15は浮上磁気ヘッド
14を駆動する浮上磁気ヘッド駆動回路である。情報の
記録は光ヘッド12からレーザ光を光磁気ディスク10
に照射しつつ、浮上磁気ヘッド14によって変調磁界を
光磁気ディスク10に印加することによって行い、記録
された情報の再生は光ヘッド12からレーザ光を光磁気
ディスク10に照射し、媒体のカー効果による偏光面の
回転を光の強弱として検知することで行う。
FIG. 3 is a diagram showing a schematic structure of a magneto-optical recording / reproducing apparatus of the magnetic modulation type according to the present invention. In FIG. 3, 10 is a magneto-optical disk and 11 is a magneto-optical disk 1.
A spindle motor that rotates 0, and 12 is an optical head that focuses laser light on a disk in a spot shape and detects light reflected from the disk. The optical head 12 is composed of various lenses, PBS and the like. Reference numeral 13 is a semiconductor laser drive circuit, 14 is a floating magnetic head, and 15 is a floating magnetic head drive circuit for driving the floating magnetic head 14. Information is recorded by applying laser light from the optical head 12 to the magneto-optical disk 10.
The magnetic field is applied to the magneto-optical disk 10 by the levitation magnetic head 14 while irradiating the optical disk, and the recorded information is reproduced by irradiating the magneto-optical disk 10 with the laser beam from the optical head 12 to reproduce the Kerr effect of the medium. The rotation of the polarization plane due to is detected as the intensity of light.

【0023】図4は4値のレベル検知を行う信号処理回
路を示す図であり、図5は再生信号波形と検出同期クロ
ックとのタイミング図である。
FIG. 4 is a diagram showing a signal processing circuit for detecting four-valued levels, and FIG. 5 is a timing diagram of a reproduced signal waveform and a detection synchronization clock.

【0024】図4において、20は再生信号を増幅する
アンプ、21〜23は各非反転入力端子にアンプからの
信号が入力され、各反転入力端子にそれぞれ基準電圧源
1,V2 ,V3 が接続されるコンパレータ、24はコ
ンパレータ21〜23の出力が入力される4値判定回路
である。4値判定回路24は“2”、“1”、“−
1”、“−2”の判定を行い、2値化して(1,1)、
(1,0)、(0、1)、(0,0)の信号を出力す
る。図5に示すように、再生信号は所定のスライスレベ
ル(V1 ,V2 ,V3 )で、4値に分けられて検知され
る。
In FIG. 4, reference numeral 20 denotes an amplifier for amplifying a reproduction signal, and reference numerals 21 to 23 denote non-inverting input terminals to which signals from the amplifier are input, and reference terminals V 1 , V 2 and V, respectively, to the inverting input terminals. Reference numeral 24 is a comparator to which 3 is connected, and reference numeral 24 is a four-value determination circuit to which the outputs of the comparators 21 to 23 are input. The four-value determination circuit 24 is "2", "1", "-".
1 "," -2 "is determined, binarized (1, 1),
The signals (1,0), (0,1), and (0,0) are output. As shown in FIG. 5, the reproduced signal is detected by being divided into four values at a predetermined slice level (V 1 , V 2 , V 3 ).

【0025】[0025]

【発明の効果】以上説明したように、本発明によれば、
光ビームを照射するとともに光照射部位に記録信号に応
じた変調磁界を印加して記録ピットを形成する磁界変調
方式の光磁気記録媒体又は磁界変調方式の光磁気記録再
生装置において、記録パターンの最小記録ピット長をビ
ームスポット径の1/4以下とすることで、少なくとも
4値の記録が可能となり、高密度記録が可能となる。ま
た、本発明によれば最小記録ピット長がビームスポット
径の1/4以下の記録パターンから4値の再生信号出力
を得ることが可能となる。
As described above, according to the present invention,
In a magnetic field modulation type magneto-optical recording medium or a magnetic field modulation type magneto-optical recording / reproducing apparatus that irradiates a light beam and applies a modulation magnetic field according to a recording signal to a light irradiation portion to form a recording pit, a minimum recording pattern By setting the recording pit length to be ¼ or less of the beam spot diameter, at least four-value recording becomes possible and high density recording becomes possible. Further, according to the present invention, it is possible to obtain a 4-level reproduction signal output from a recording pattern whose minimum recording pit length is ¼ or less of the beam spot diameter.

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

【図1】本発明に係る光磁気記録再生装置における光磁
気記録方式を示すタイミング図である。
FIG. 1 is a timing diagram showing a magneto-optical recording system in a magneto-optical recording / reproducing apparatus according to the present invention.

【図2】光磁気記録媒体に記録された記録パターンを再
生する場合の原理を示す図である。
FIG. 2 is a diagram showing the principle of reproducing a recording pattern recorded on a magneto-optical recording medium.

【図3】本発明に係る磁気変調方式の光磁気記録再生装
置の概略的な構成を示す図である。
FIG. 3 is a diagram showing a schematic configuration of a magnetic modulation type magneto-optical recording / reproducing apparatus according to the present invention.

【図4】4値のレベル検知を行う信号処理回路を示す図
である。
FIG. 4 is a diagram showing a signal processing circuit for performing 4-level detection.

【図5】再生信号波形と検出同期クロックとのタイミン
グ図である。
FIG. 5 is a timing diagram of a reproduced signal waveform and a detection synchronization clock.

【図6】従来の磁界変調方式による光磁気記録再生装置
の記録方法を示すタイミング図である。
FIG. 6 is a timing chart showing a recording method of a magneto-optical recording / reproducing apparatus according to a conventional magnetic field modulation method.

【符号の説明】[Explanation of symbols]

10 光磁気ディスク 11 スピンドルモータ 12 光ヘッド 13 半導体レーザ駆動回路 14 浮上磁気ヘッド 15 浮上磁気ヘッド駆動回路 20 アンプ 21〜23 コンパレータ 24 4値判定回路 10 magneto-optical disk 11 spindle motor 12 optical head 13 semiconductor laser drive circuit 14 floating magnetic head 15 floating magnetic head drive circuit 20 amplifiers 21-23 comparator 24 four-value determination circuit

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 光磁気記録媒体に光ビームを照射すると
ともに光照射部位に記録信号に応じ変調磁界を印加する
ことで、記録ピットを形成して情報の記録を行なう光磁
気記録再生装置において、 最小記録ピット長がビームスポット径の1/4以下とな
るように前記変調磁界を印加する手段を有することを特
徴とする光磁気記録再生装置。
1. A magneto-optical recording / reproducing apparatus for recording information by forming a recording pit by irradiating a magneto-optical recording medium with a light beam and applying a modulation magnetic field to a light-irradiated portion according to a recording signal. A magneto-optical recording / reproducing apparatus comprising means for applying the modulating magnetic field so that the minimum recording pit length becomes ¼ or less of the beam spot diameter.
【請求項2】 最小記録ピット長がビームスポット径の
1/4以下となるように記録パターンが記録された光磁
気記録媒体からの再生信号のレベルとそれぞれ設定され
た所定の基準電圧とを比較する複数の比較手段と、該比
較手段からの信号に基づき、少なくとも4値の再生信号
を得る手段とを有する光磁気記録再生装置。
2. A level of a reproduction signal from a magneto-optical recording medium on which a recording pattern is recorded such that the minimum recording pit length is 1/4 or less of a beam spot diameter, and a predetermined reference voltage respectively set. A magneto-optical recording / reproducing apparatus having a plurality of comparing means and a means for obtaining a reproduced signal of at least four values based on signals from the comparing means.
【請求項3】 光ビームを照射するとともに光照射部位
に記録信号に応じた変調磁界を印加することで、記録ピ
ットを形成してなる光磁気記録媒体において、 記録パターンの最小記録ピット長をビームスポット径の
1/4以下としたことを特徴とする光磁気記録媒体。
3. A minimum recording pit length of a recording pattern in a magneto-optical recording medium having recording pits formed by irradiating a light beam and applying a modulation magnetic field according to a recording signal to a light irradiation portion. A magneto-optical recording medium having a spot diameter of 1/4 or less.
JP693294A 1994-01-26 1994-01-26 Magneto-optical recording/reproducing device and magneto-optical recording medium Pending JPH07220317A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP693294A JPH07220317A (en) 1994-01-26 1994-01-26 Magneto-optical recording/reproducing device and magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP693294A JPH07220317A (en) 1994-01-26 1994-01-26 Magneto-optical recording/reproducing device and magneto-optical recording medium

Publications (1)

Publication Number Publication Date
JPH07220317A true JPH07220317A (en) 1995-08-18

Family

ID=11652031

Family Applications (1)

Application Number Title Priority Date Filing Date
JP693294A Pending JPH07220317A (en) 1994-01-26 1994-01-26 Magneto-optical recording/reproducing device and magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JPH07220317A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1999063530A1 (en) * 1998-06-02 1999-12-09 Seagate Technology, Inc. A magneto-optical recording system employing linear recording and playback channels
US6208594B1 (en) 1998-06-02 2001-03-27 Seagate Technology Llc Efficient linearization of saturation channels
US6542443B1 (en) 1999-06-02 2003-04-01 Seagate Technology Llc Efficient linearization of saturation channels
US6687205B1 (en) 1998-06-09 2004-02-03 Seagate Technology Llc Parallel coded spread spectrum communication for data storage

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1999063530A1 (en) * 1998-06-02 1999-12-09 Seagate Technology, Inc. A magneto-optical recording system employing linear recording and playback channels
US6178144B1 (en) 1998-06-02 2001-01-23 Seagate Technology Llc Magneto-optical recording system employing linear recording and playback channels
US6208594B1 (en) 1998-06-02 2001-03-27 Seagate Technology Llc Efficient linearization of saturation channels
US6687205B1 (en) 1998-06-09 2004-02-03 Seagate Technology Llc Parallel coded spread spectrum communication for data storage
US6542443B1 (en) 1999-06-02 2003-04-01 Seagate Technology Llc Efficient linearization of saturation channels

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