JPS6159605A - Information recording and reproducing device - Google Patents
Information recording and reproducing deviceInfo
- Publication number
- JPS6159605A JPS6159605A JP18080984A JP18080984A JPS6159605A JP S6159605 A JPS6159605 A JP S6159605A JP 18080984 A JP18080984 A JP 18080984A JP 18080984 A JP18080984 A JP 18080984A JP S6159605 A JPS6159605 A JP S6159605A
- Authority
- JP
- Japan
- Prior art keywords
- bias
- magnetic field
- signal
- disk
- duty cycle
- 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
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording 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
- G11B11/10—Recording 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
- G11B11/105—Recording 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
- Digital Magnetic Recording (AREA)
Abstract
Description
【発明の詳細な説明】
〔技術分野〕
本発明は、情報記録再生装置、特に、記録バイアスυ制
御装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to an information recording/reproducing device, and particularly to a recording bias υ control device.
光磁気記録は、記録媒体として、ガラス等の、円板状の
ものに磁性体をスパッタしたディスクを用い、この記録
媒体に垂直磁場をかけて、磁性体を一定方向に磁化させ
ておき、記録すべき情報信号により変調されたレーザー
ビームをディスクに照射する事により、その照射部位の
磁性体の温度を磁気転移温度(キューリ一温度)以上に
して照射部位の磁化を反転させ、これによって情報をデ
ィスクに記録し、再生時には磁気カー効果、ファラデー
効果等を利用して、レーザービームを用いてディスクに
記録された情報信号を再生する。Magneto-optical recording uses a disc made of glass or other disc-shaped material sputtered with magnetic material as a recording medium. A perpendicular magnetic field is applied to this recording medium to magnetize the magnetic material in a certain direction. By irradiating the disk with a laser beam modulated by the information signal to be transmitted, the temperature of the magnetic material in the irradiated area is raised to above the magnetic transition temperature (Curie temperature), and the magnetization of the irradiated area is reversed, thereby transmitting information. Information signals are recorded on a disk, and during reproduction, the magnetic Kerr effect, Faraday effect, etc. are used to reproduce the information signals recorded on the disk using a laser beam.
光磁気記録においては、記録媒体となる磁性体の感度、
レーザービームのパワーおよび垂直磁場の磁界の強さの
各々に関係して、記録されるビットの大きさが異なる。In magneto-optical recording, the sensitivity of the magnetic material that becomes the recording medium,
The size of the recorded bit differs depending on the power of the laser beam and the strength of the perpendicular magnetic field.
このため磁界およびレーザーパワー一定では、ディスク
交換においてディスク状記録媒体に感度差があった場合
等に、ピットの大きさが適正とならず、再生信号のレベ
ル低下とともに、信号のデユーティ−サイクルが変化し
て、MFM(Modified Frequency
+5adulation)などの変調方式で変調され
た信号などは正確な復調が不可能となる。Therefore, when the magnetic field and laser power are constant, if there is a sensitivity difference in the disk-shaped recording medium during disk replacement, the pit size will not be appropriate, and the signal duty cycle will change as the level of the reproduced signal decreases. Then, MFM (Modified Frequency)
Accurate demodulation of signals modulated by a modulation method such as +5 adulation is impossible.
また、ディスクの外周と内周とではピットの大きさが変
化し、レーザービームのエネルギー密度によってもピッ
トの大きさが変化するが、この場合も、従来は、一定率
位置検出により、ビームパワーを変えたり、バイアス(
Bias)磁界を変えたりしているが、ディスク状記録
媒体の感度差があると、正確な補正は不可能となる。In addition, the size of the pits changes between the outer and inner peripheries of the disk, and the pit size also changes depending on the energy density of the laser beam. change or bias (
(Bias) by changing the magnetic field, but if there is a difference in sensitivity between disk-shaped recording media, accurate correction is impossible.
ピットの大きさを変化させる手段として、ビームパワー
を変化させる方式も考えられているが。A method of changing the beam power has also been considered as a means of changing the size of the pit.
ビームパワーを大きくするために半導体レーザーを用い
る場合にはドライブ方法、および絶対パワーの面におい
て問題が多い。When using a semiconductor laser to increase beam power, there are many problems in terms of drive method and absolute power.
本発明の目的は、11u記従来例の欠点を除去し、比較
的簡単な構成で情報を正確に再生できる情報記録再生装
置を実現する事にある。An object of the present invention is to eliminate the drawbacks of the conventional example described in Section 11u and to realize an information recording and reproducing apparatus that can accurately reproduce information with a relatively simple configuration.
第1図は本発明一実施例のブロック図であり、1は光磁
気ディスク(記録媒体)9へ信号を記録再生するための
光学式ピックアップ、2は記録時にレーザービームを情
報信号により変調する変調器、3は記録時および再生時
にフォーカス、トラッキングをかけるための誤差信号お
よび情報信号を再生する前置1?j幅器、4は前置増幅
器3からのフォーカスエラーおよびトラッキングエラー
信号によりピックアップlにサーボをかける為のサーボ
回路、5は光学式ピックアップ1をディスクの直径方向
に移動させるためのコントローラー、6は前置増幅器3
からの情報信号を2値化するためのコンパレーター、7
はコンパレーター6の出力に接続されたローパスフィル
ター、および8はコントローラ5を介したローパスフィ
ルター7からの信号と、ディスク9上のピックアップ1
の位置とにより、ディスク9にかかるバイアス磁界を制
御するバイアス制御回路である。FIG. 1 is a block diagram of one embodiment of the present invention, in which 1 is an optical pickup for recording and reproducing signals on a magneto-optical disk (recording medium) 9, and 2 is a modulation system that modulates a laser beam with an information signal during recording. Prefix 1?3 reproduces error signals and information signals for focusing and tracking during recording and playback. 4 is a servo circuit for applying servo to the pickup L based on the focus error and tracking error signals from the preamplifier 3; 5 is a controller for moving the optical pickup 1 in the diametrical direction of the disk; Preamplifier 3
a comparator for binarizing the information signal from 7
is a low-pass filter connected to the output of comparator 6, and 8 is a signal from low-pass filter 7 via controller 5 and pickup 1 on disk 9.
This is a bias control circuit that controls the bias magnetic field applied to the disk 9 depending on the position of the disk 9.
以上のような構成の実施例の動作について以下に説明す
る。The operation of the embodiment configured as above will be explained below.
第1図において、変調器2は、ディスク9に情報を記録
する場合に肝阿等の変調をレーザービームにかけるが、
バイアスのyA整時には、再生信号が歪まない様にデユ
ーティ−サイクルが50%となる様にレーザービームを
変調する。デユーティ−サイクル50%でディスク9に
記録した場合、バイアス磁界の強弱により、ディスク上
のピット形状は第2図(a)、(b)および(C)のよ
うに変化する。In FIG. 1, the modulator 2 modulates the laser beam when recording information on the disk 9.
When adjusting the bias yA, the laser beam is modulated so that the duty cycle is 50% so that the reproduced signal is not distorted. When recording is performed on the disk 9 with a duty cycle of 50%, the shape of the pits on the disk changes as shown in FIGS. 2(a), (b) and (C) depending on the strength of the bias magnetic field.
第2図(a)はバイアス磁界が弱い場合であり、ピット
形状A1が小さく、信号用前置増幅器3の信号出力波形
は図中A2の様になり、その信号をコンパレーター6に
よりz値化したものは図中A3(7)様になり、ローパ
スフィルター7を通す事によりこの信−衿A3の直流(
pc)成分を検出すると、マイナス(負)の直流分を検
出する事が出来る。FIG. 2(a) shows a case where the bias magnetic field is weak, the pit shape A1 is small, and the signal output waveform of the signal preamplifier 3 becomes like A2 in the figure, and the signal is converted into a z-value by the comparator 6. The resulting signal looks like A3 (7) in the figure, and by passing it through the low-pass filter 7, the direct current (
By detecting the pc) component, it is possible to detect the minus (negative) DC component.
バイアス磁界の強さが適正の場合、第2図(b)に示す
様に、ディスク上の記録ピット形状はBlのようになり
、再生信号のデユーティ−サイクルは50%となり、ロ
ーパスフィルター7の出力の1α流分はほぼ0となる。When the strength of the bias magnetic field is appropriate, as shown in FIG. 2(b), the recording pit shape on the disk becomes Bl, the duty cycle of the reproduction signal becomes 50%, and the output of the low-pass filter 7 The 1α flow of is almost 0.
このときのピットの大きさは1.2〜1−3 p、mと
なっている0図中B2は増幅器3の出力、B3はコンパ
レーター6の出力を示す。The size of the pit at this time is 1.2 to 1-3 p, m. In the figure, B2 indicates the output of the amplifier 3, and B3 indicates the output of the comparator 6.
さらにバイアス磁界が強い場合、第2V!J(c)に示
すように、記録ピット形状はC1の様になり。If the bias magnetic field is even stronger, the second V! As shown in J(c), the recording pit shape becomes C1.
ローパスフィルター7の出力は、プラスのDC4分を検
出する0図中02は増幅器3の出力、C3はコンパレー
タ6の出力を示す。The output of the low-pass filter 7 detects the positive DC4 component. In the figure, 02 indicates the output of the amplifier 3, and C3 indicates the output of the comparator 6.
なお、磁界の強弱により記録ピットの大きさも変化する
ためコンパレータ7の出力としては、磁界の強さにほぼ
比例した出力が得られる。この事を利用して自動的に適
正バイアス磁界強度を設定する。この動作のフローチャ
ートを第3図および第4図に示して詳細に説明する。Note that since the size of the recording pit changes depending on the strength of the magnetic field, the output of the comparator 7 is approximately proportional to the strength of the magnetic field. Utilizing this fact, the appropriate bias magnetic field strength is automatically set. Flowcharts of this operation are shown in FIGS. 3 and 4 and will be explained in detail.
第3図に示すようにまずStにおいてピックアップlを
ディスク9の最外周(そのシステムで記録可能な)に移
動し、S2にすすんでサブルーチンを実行する。すなわ
ち、第4図に示すように、まずSllにおいてバイアス
をあらかじめ設定した標準値とし、S12においてディ
スク上にデユーティ−サイクル50%となる様に変調器
2により変調された信号を記録する。ついで513にお
いて今記録した信号を再生し、S14においてその時の
2値化した信号のDC成分をローパスフィルター7で検
出して、その値をバイアス制御回路8に送り、再生信号
の2値化信号のDC成分が許容値(−〇)以内かそれ以
上または以下かのいずれであるかを判定して、その直流
レベルが許容範囲より大きいときは515にすすみ、許
容範囲より小さいときは31Bにすすみ、許容範囲即ち
ほぼOのときはメインルーチンにもどる。S15におい
ては、変化させるバイアス量Δを−(マイナス)にして
Sl?にすすみ、318においては変化させるバイアス
措Δを+(プラス)にして517にすすむ。S17にお
いてはそれまでのバイアス値に変化させるバイアス量Δ
を加えたバイアス値によってディスク−ヒにデユーティ
−サイクル50%で変調された信号を記録し、518に
おいて再生する。そこでS14にもどって再び再生信号
にかかるDC成分を検出し、上記の処理を繰り返して、
S14における検出DCレベルが許容される範囲(#O
)に入ったなら、メインルーチンの53にもどり、そこ
でそのバイアス値をバイアス制御回路8の不図示の第1
メモリ8−1に記憶させる。As shown in FIG. 3, first, in St, the pickup 1 is moved to the outermost circumference of the disc 9 (recordable in that system), and the process proceeds to S2, where a subroutine is executed. That is, as shown in FIG. 4, first, the bias is set to a preset standard value in Sll, and in S12 a signal modulated by the modulator 2 is recorded on the disk so that the duty cycle is 50%. Next, in step 513, the signal just recorded is reproduced, and in step S14, the DC component of the binarized signal at that time is detected by the low-pass filter 7, and the value is sent to the bias control circuit 8, and the DC component of the binarized signal of the reproduced signal is detected. Determine whether the DC component is within the allowable value (-〇), above it, or below, and if the DC level is greater than the allowable range, proceed to 515, and if it is less than the allowable range, proceed to 31B, When the value is within the permissible range, that is, approximately O, the process returns to the main routine. In S15, the bias amount Δ to be changed is set to - (minus) and Sl? Then, in 318, the bias measure Δ to be changed is set to + (plus), and the process proceeds to 517. In S17, the bias amount Δ is changed to the previous bias value.
A signal modulated with a duty cycle of 50% is recorded on the disk by a bias value in which . Therefore, the process returns to S14 and the DC component applied to the reproduced signal is detected again, and the above process is repeated.
The detection DC level in S14 is within the permissible range (#O
), the process returns to 53 of the main routine, where the bias value is input to the first bias control circuit 8 (not shown).
It is stored in the memory 8-1.
次に54においてピックアップをディスクの中央に進め
、S5にすすんで前記サブルーチンにすすんで上記と同
様の事を行い、S6において最終的なバイアス値を第2
メモリ8−2に記憶する。Next, in step 54, the pickup is advanced to the center of the disk, and the process proceeds to step S5, which proceeds to the aforementioned subroutine and performs the same thing as above, and in step S6, the final bias value is set to the second
It is stored in the memory 8-2.
さらに57においてピックアップをディスク最内周に送
り、S8にすすんで前記サブルーチンにすすんで上記同
様の事を行い、S9において最終的なバイアス値を第3
メモリ8−3に記憶する。Furthermore, in step 57, the pickup is sent to the innermost circumference of the disk, and the process proceeds to step S8, which proceeds to the aforementioned subroutine and performs the same thing as described above, and in step S9, the final bias value is set to the third
It is stored in the memory 8-3.
ついで510において、この外周、中央および内周の3
ポイントのバイアス値を基準として、バイアス制御回路
8内において外周および中央の値からその間のバイアス
値の傾きを演算して各位置におけるその場所(位置)に
合ったバイアス値を決定し、外周および中央間における
各位置においてこの決定したバイアス値になるようにバ
イアスを変更する。中央および外局間においても同様に
行う、また、3点から公知の演算方法で3点を通る曲線
(直線)を求め、任意の位置のバイアス値を求めること
もできる。Then, at 510, the outer circumference, the center, and the inner circumference are
Using the bias value at the point as a reference, the bias control circuit 8 calculates the slope of the bias value between the values at the outer periphery and the center, determines the bias value suitable for that location (position) at each position, and The bias is changed to the determined bias value at each position in between. The same process can be performed between the central and outer stations, or a bias value at an arbitrary position can be determined by calculating a curve (straight line) passing through the three points using a known calculation method.
このように、ディスクの3ポイントで適正バイアスを求
め、各ポイントの中間は求めた3ポイントの適正/ヘイ
アスから推測したバイアスを適用することによって、デ
ィスクの全体にわたって適正なバイアス磁界を比較的短
い時間で得ることができる。In this way, by determining the appropriate bias at three points on the disk, and applying the bias estimated from the determined appropriateness/heias at the three points in the middle of each point, an appropriate bias magnetic field can be applied over the entire disk in a relatively short period of time. You can get it at
以上の動作を、ディスクを装着した事をセンサ等で検出
l−、フォーカスサーボがかかった2ftをサーボ回路
4において検出してから自動的に開始する。The above operation is automatically started after the sensor etc. detects that the disk is mounted, and the servo circuit 4 detects 2ft where the focus servo is applied.
以上の実施例においては、記録バイアスを3ポイントで
測定したが、さらにこの数を増加する事 −も可能
である。In the above embodiment, the recording bias was measured at three points, but it is also possible to further increase this number.
デユーティ−サイクルをローパスフィルターを用いて検
出したが、クロックによりz値化信号のパルス巾を検出
する帛によって検出しても同様の効果が得られる。Although the duty cycle is detected using a low-pass filter, the same effect can be obtained by detecting it using a device that detects the pulse width of the z-valued signal using a clock.
以上説明した様に本発明によれば、記録媒体を交換した
場合でも簡単に正確な情報信号の再生をすることができ
る。As described above, according to the present invention, it is possible to easily and accurately reproduce information signals even when the recording medium is replaced.
第1図は本発明の一実施例のブロック図。
ff52図はディスク上のピット及び再生信号の説明図
。
第3図および第4図は本発明の一実施例の処理フローチ
ャートである。
1・・・光学式ピックアップ。
2・・・変調器、
3・・・前置増幅器、
4・・・サーボ回路。
5・・・コントローラ、
6・・・ コンパレータ、
7・・・ローパスフィルター、
8・・・バイアス制御回路、
9・・・ディスク。FIG. 1 is a block diagram of an embodiment of the present invention. Figure ff52 is an explanatory diagram of pits on the disc and reproduction signals. 3 and 4 are processing flowcharts of one embodiment of the present invention. 1...Optical pickup. 2...Modulator, 3...Preamplifier, 4...Servo circuit. 5... Controller, 6... Comparator, 7... Low pass filter, 8... Bias control circuit, 9... Disk.
Claims (1)
イアス磁界を制御する手段とを備えたことを特徴とする
情報記録再生装置。[Claims] Means for detecting a duty cycle of a reproduced signal; means for changing the strength of a bias magnetic field during information recording; and controlling the bias magnetic field based on the signal detected by the detection means. An information recording/reproducing device comprising: means.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18080984A JPS6159605A (en) | 1984-08-31 | 1984-08-31 | Information recording and reproducing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18080984A JPS6159605A (en) | 1984-08-31 | 1984-08-31 | Information recording and reproducing device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6159605A true JPS6159605A (en) | 1986-03-27 |
Family
ID=16089730
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP18080984A Pending JPS6159605A (en) | 1984-08-31 | 1984-08-31 | Information recording and reproducing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6159605A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0411934A2 (en) * | 1989-08-02 | 1991-02-06 | Sharp Kabushiki Kaisha | Video signal recording/reproducing device |
WO1992014245A1 (en) * | 1991-02-05 | 1992-08-20 | Sony Corporation | Method for reproducing signal in optically recording medium |
WO1992015093A1 (en) * | 1991-02-13 | 1992-09-03 | Sony Corporation | Method for reproducing signal in optically recording medium |
EP0576245A2 (en) * | 1992-06-23 | 1993-12-29 | Canon Kabushiki Kaisha | Magneto-optic recording apparatus and method therefor |
-
1984
- 1984-08-31 JP JP18080984A patent/JPS6159605A/en active Pending
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0411934A2 (en) * | 1989-08-02 | 1991-02-06 | Sharp Kabushiki Kaisha | Video signal recording/reproducing device |
US5315402A (en) * | 1989-08-02 | 1994-05-24 | Sharp Kabushiki Kaisha | Video signal recording/reproducing system for increasing recording density of a frequency modulated signal |
WO1992014245A1 (en) * | 1991-02-05 | 1992-08-20 | Sony Corporation | Method for reproducing signal in optically recording medium |
US5390162A (en) * | 1991-02-05 | 1995-02-14 | Sony Corporation | Method for reproducing signals recorded on optical recording medium |
WO1992015093A1 (en) * | 1991-02-13 | 1992-09-03 | Sony Corporation | Method for reproducing signal in optically recording medium |
US5335213A (en) * | 1991-02-13 | 1994-08-02 | Sony Corporation | Positional detection of a magneto-optic recording medium for controlling irradiation of a relief region |
EP0576245A2 (en) * | 1992-06-23 | 1993-12-29 | Canon Kabushiki Kaisha | Magneto-optic recording apparatus and method therefor |
EP0576245A3 (en) * | 1992-06-23 | 1994-02-16 | Canon Kk | Magneto-optic recording apparatus and method therefor |
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