JPH04298836A - Magneto-optical recording and reproducing device - Google Patents

Magneto-optical recording and reproducing device

Info

Publication number
JPH04298836A
JPH04298836A JP6346191A JP6346191A JPH04298836A JP H04298836 A JPH04298836 A JP H04298836A JP 6346191 A JP6346191 A JP 6346191A JP 6346191 A JP6346191 A JP 6346191A JP H04298836 A JPH04298836 A JP H04298836A
Authority
JP
Japan
Prior art keywords
magneto
birefringence
optical recording
optical
information
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
JP6346191A
Other languages
Japanese (ja)
Inventor
Hideyoshi Horigome
秀嘉 堀米
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP6346191A priority Critical patent/JPH04298836A/en
Publication of JPH04298836A publication Critical patent/JPH04298836A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To improve the C/N of reproducing information and to simplify the structure of an optical pickup by electrically correcting double refractivity on the transparent base board of the magneto-optical disk. CONSTITUTION:A luminous flux from the magneto-optical disk 1 is distributed between a pair of optical detectors 19a, 19b. A pair of level control circuits 24, 25 to obtain the double refractivity information in relation with the transparent base board 1b of the magneto-optical disk based on respective low range components of detected outputs from the optical detectors, and simultaneously, to control differentially the levels of respective high range components with the detected outputs from both optical detectors is provided. By controlling the level control curcuits with the double refractivity information, the reproducing information correcting the double refractivity on the transparent base board electrically is obtained.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】この発明は光磁気記録再生装置に
関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-optical recording and reproducing apparatus.

【0002】0002

【従来の技術】従来、光磁気記録装置においては、例え
ば遷移金属のような、適宜の光磁気記録材料を垂直方向
に磁化し、外部磁界の下で、この光磁気記録材料にレー
ザ光を照射して、磁化の方向を反転させることにより情
報を記録している。この記録情報は、垂直磁化に比例し
て直線偏光の偏光面が回転する現象(反射光の場合は磁
気カー効果)を利用して光学的に読み出される。通常、
記録媒体は円盤状に形成され、光磁気記録層を支持する
担体としては、デジタル・オーディオ・ディスクの場合
と同様に、耐熱性・耐湿性がよく透明な合成樹脂、例え
ば、ポリカーボネート樹脂が一般的に用いられる。
Conventionally, in a magneto-optical recording device, a suitable magneto-optical recording material such as a transition metal is magnetized in the perpendicular direction, and the magneto-optical recording material is irradiated with laser light under an external magnetic field. Information is recorded by reversing the direction of magnetization. This recorded information is optically read out using a phenomenon in which the plane of polarization of linearly polarized light rotates in proportion to perpendicular magnetization (magnetic Kerr effect in the case of reflected light). usually,
The recording medium is formed into a disk shape, and the carrier that supports the magneto-optical recording layer is generally made of transparent synthetic resin with good heat and moisture resistance, such as polycarbonate resin, as in the case of digital audio discs. used for.

【0003】0003

【発明が解決しようとする課題】ところが、ポリカーボ
ネート樹脂は、光学的異方性(複屈折性)が比較的大き
く、光磁気記録を再生する場合、読出し光が担体を透過
する際に偏光面の不要な回転が生じ、この不要な回転に
よるノイズが発生して、再生情報のC/Nが劣化すると
いう問題があった。もっとも、ディスクの成形工程にお
いては、樹脂及び金型の温度、インジェクション圧力な
どが細かく管理され、複屈折量を所定の基準値内に抑え
たディスクが出荷されてはいるが、ディスク内での複屈
折を一様にすることは極めて困難である。
However, polycarbonate resin has a relatively large optical anisotropy (birefringence), and when reproducing magneto-optical recording, the plane of polarization changes when the readout light passes through the carrier. There is a problem in that unnecessary rotation occurs, noise is generated due to this unnecessary rotation, and the C/N of reproduced information deteriorates. However, in the disc molding process, the temperature of the resin and mold, the injection pressure, etc. are carefully controlled, and although discs are shipped with the amount of birefringence kept within a predetermined standard value, It is extremely difficult to make refraction uniform.

【0004】前述のような、担体の光学的異方性に起因
する、再生情報のC/N劣化の問題を解消するため、本
出願人は、特開平2−260255号公報(特願平1−
83079号)において、複屈折を光学的に補正する複
屈折補正子を再生光学系に介挿すると共に、媒体からの
読出し光に基づいて複屈折情報を形成する複屈折情報形
成回路を設け、この複屈折情報に応じて、複屈折補正子
を制御するようにした光磁気記録再生装置を既に提案し
ている。
In order to solve the above-mentioned problem of C/N deterioration of reproduced information due to the optical anisotropy of the carrier, the present applicant has published Japanese Patent Application Laid-Open No. 2-260255 (Japanese Patent Application No. −
No. 83079), a birefringence corrector for optically correcting birefringence is inserted in the reproduction optical system, and a birefringence information forming circuit is provided for forming birefringence information based on light read from the medium. A magneto-optical recording and reproducing device has already been proposed in which a birefringence corrector is controlled according to birefringence information.

【0005】まず、図2〜図5を参照しながら、既提案
による光磁気記録再生装置について説明する。
First, a previously proposed magneto-optical recording/reproducing device will be described with reference to FIGS. 2 to 5.

【0006】図2において、1は光磁気ディスクであっ
て、光磁気記録層1aがポリカーボネート樹脂からなる
担体(基板)1b上に形成される。10は光学ピックア
ップであって、レーザダイオード11から射出された光
束が、コリメータレンズ12,ビームスプリッタ13,
対物レンズ14を経て、光磁気ディスク1の記録層1a
に入射する。
In FIG. 2, reference numeral 1 denotes a magneto-optical disk, in which a magneto-optical recording layer 1a is formed on a carrier (substrate) 1b made of polycarbonate resin. Reference numeral 10 denotes an optical pickup, in which the light beam emitted from the laser diode 11 is transmitted through a collimator lens 12, a beam splitter 13,
After passing through the objective lens 14, the recording layer 1a of the magneto-optical disk 1 is
incident on .

【0007】記録層1aからの反射光束は、対物レンズ
14を経て、ビームスプリッタ13に再び入射し、この
ビームスプリッタ13からの反射光束が、λ/2板(複
屈折補正子)15により、偏光面を45゜回転されて、
偏光ビームスプリッタ16に入射し、入射面に平行に振
動するp偏光の光束Lpと、入射面に垂直に振動するs
偏光の光束Lsとに分離される。ビームスプリッタ16
において分離された各光束Lp,Lsの光量は、光磁気
ディスク1の記録層1aによる正規の偏光面回転量と、
基板1bの複屈折による不要な偏光面回転量との和にそ
れぞれ対応し、かつ、差動的に変化する。
The reflected light flux from the recording layer 1a passes through the objective lens 14 and enters the beam splitter 13 again, and the reflected light flux from the beam splitter 13 is polarized by a λ/2 plate (birefringence corrector) 15. The plane is rotated 45 degrees,
A p-polarized light beam Lp enters the polarizing beam splitter 16 and vibrates parallel to the plane of incidence, and s vibrates perpendicular to the plane of incidence.
It is separated into a polarized light beam Ls. Beam splitter 16
The amount of light of each of the light beams Lp and Ls separated at
They each correspond to the sum of the amount of unnecessary rotation of the plane of polarization due to birefringence of the substrate 1b, and change differentially.

【0008】ビームスプリッタ16において分離された
一方の光束Lpが、集光レンズ17a,円筒レンズ18
aを経て、一方の光検出器19aに入射すると共に、他
方の光束Lsが、集光レンズ17b,円筒レンズ18b
を経て、他方の光検出器19bに入射する。光検出器1
9a,19bは、図3に示すように、それぞれ4分割検
出素子A〜Dを備えており、光検出器19a,19bか
らは、p偏光の光束Lp,s偏光の光束Lsにそれぞれ
対応して、全検出素子の検出出力の和の検出信号Sp,
Ssが出力される。
One of the light beams Lp separated by the beam splitter 16 passes through the condensing lens 17a and the cylindrical lens 18.
a, the light beam Ls enters one photodetector 19a, and the other light beam Ls passes through the condenser lens 17b and the cylindrical lens 18b.
The light then enters the other photodetector 19b. Photodetector 1
As shown in FIG. 3, the photodetectors 9a and 19b are each equipped with four-split detection elements A to D, and from the photodetectors 19a and 19b, light beams Lp of p-polarized light and light beams Ls of s-polarized light are detected, respectively. , a detection signal Sp of the sum of detection outputs of all detection elements,
Ss is output.

【0009】20は記録情報再生回路、30は複屈折検
出回路であって、それぞれ差動増幅器21,31を備え
、光検出器19a,19bからの検出信号Sp,Ssが
、高域フィルタ22,23を介して、差動増幅器21に
供給されると共に、低域フィルタ32,33を介して、
差動増幅器31に供給される。記録情報の再生信号が差
動増幅器21から導出されると共に、差動増幅器31の
出力は、サーボ回路34を経て、複屈折補正子15の駆
動コイル15cに供給される。
Reference numeral 20 denotes a recorded information reproducing circuit, and 30 denotes a birefringence detection circuit, each of which is equipped with differential amplifiers 21 and 31. 23, to the differential amplifier 21, and through low-pass filters 32, 33.
The signal is supplied to the differential amplifier 31. A reproduction signal of recorded information is derived from the differential amplifier 21, and the output of the differential amplifier 31 is supplied to the drive coil 15c of the birefringence corrector 15 via the servo circuit 34.

【0010】図4Aに示すように、光磁気ディスク1上
の記録トラックTKをピックアップ10からの光束が走
査する際に、角度位置(……θ1 ,θ2 ,θ3 ,
θ4 ……)をピックアップ光束が照射したとき、各角
度位置(……θ1 ,θ2 ,θ3 ,θ4 ……)に
おける基板1bの複屈折は、同図Bに示すように、3次
元の屈折率楕円体ベクトル(……n1 ,n2 ,n3
 ,n4 ……)により表され、しかも、使用されてい
るポリカーボネイト固有の特性として、種々の方向に変
動する。
As shown in FIG. 4A, when the light beam from the pickup 10 scans the recording track TK on the magneto-optical disk 1, the angular positions (...θ1, θ2, θ3,
When the pickup light beam illuminates θ4...), the birefringence of the substrate 1b at each angular position (...θ1, θ2, θ3, θ4...) is a three-dimensional refractive index ellipse, as shown in Figure B. field vector (...n1 , n2 , n3
, n4...), and varies in various directions as a characteristic specific to the polycarbonate used.

【0011】この複屈折の変動は、複屈折補正子15を
回転させずに固定した状態で、各光検出器19a、19
bにおいて検出した場合には、記録トラックの1周分に
ついて、図5に示す曲線Kのようになる。
This variation in birefringence can be observed when the birefringence corrector 15 is fixed without being rotated, and each photodetector 19a, 19
When detected at point b, a curve K shown in FIG. 5 is obtained for one round of the recording track.

【0012】このような基板1aの複屈折による検出信
号の変動成分は、300kHz程度までの比較的低い周
波数帯域に存在する。一方、ディスク1の光磁気記録層
1aの記録情報成分は、300kHz程度から数MHz
までの比較的高い周波数帯域に存在する。
Such a fluctuation component of the detection signal due to the birefringence of the substrate 1a exists in a relatively low frequency band up to about 300 kHz. On the other hand, the recorded information component of the magneto-optical recording layer 1a of the disk 1 ranges from about 300 kHz to several MHz.
It exists in a relatively high frequency band up to.

【0013】図2の従来例では、複屈折検出回路30の
出力により、光学ピックアップ10内に配設された複屈
折補正子15が集光レンズ17aの光軸を中心として回
動されて、光磁気ディスク1の基板1aの複屈折による
偏光面の不要な回転が光学的に補正されて、所定のC/
Nの再生情報が得られる。このため、図2の従来例では
、光学ピックアップの構成が複雑になると共に、価格が
上昇するという問題があった。
In the conventional example shown in FIG. 2, the birefringence corrector 15 disposed in the optical pickup 10 is rotated about the optical axis of the condensing lens 17a by the output of the birefringence detection circuit 30, and the birefringence corrector 15 is rotated about the optical axis of the condensing lens 17a. Unnecessary rotation of the plane of polarization due to birefringence of the substrate 1a of the magnetic disk 1 is optically corrected to achieve a predetermined C//
N playback information is obtained. Therefore, in the conventional example shown in FIG. 2, there were problems in that the configuration of the optical pickup became complicated and the price increased.

【0014】かかる点に鑑み、この発明の目的は、光磁
気ディスクの透明基板における複屈折を光学的に補正す
る必要がなく、再生情報のC/Nを向上させ、光学ピッ
クアップの構成が簡単で価格が低減される、光磁気記録
再生装置を提供するところにある。
In view of the above, an object of the present invention is to improve the C/N of reproduced information without the need to optically correct birefringence in the transparent substrate of a magneto-optical disk, and to simplify the structure of an optical pickup. An object of the present invention is to provide a magneto-optical recording and reproducing device whose cost is reduced.

【0015】[0015]

【課題を解決するための手段】この発明は、ピックアッ
プ光束を光磁気記録媒体1に照射し、この光磁気記録媒
体からの光束を1対の光検出器19a,19bに分配す
る光学ピックアップと、1対の光検出器の検出出力の各
高域成分に基づいて、光磁気記録媒体に記録された情報
を再生する再生回路と、1対の光検出器の検出出力の各
低域成分に基づいて、光磁気記録媒体の担体に関する複
屈折情報を形成する複屈折情報形成回路30とを備える
光磁気記録再生装置において、1対の光検出器の検出出
力の各高域成分のレベルを差動的に制御するレベル制御
回路24,25を設けると共に、このレベル制御回路を
複屈折情報形成回路の出力により制御するようにした光
磁気記録再生装置である。
[Means for Solving the Problems] The present invention provides an optical pickup that irradiates a pickup light beam onto a magneto-optical recording medium 1 and distributes the light beam from the magneto-optical recording medium to a pair of photodetectors 19a and 19b; A reproduction circuit that reproduces information recorded on the magneto-optical recording medium based on each high-frequency component of the detection output of the pair of photodetectors, and a reproduction circuit that reproduces information recorded on the magneto-optical recording medium based on each low-frequency component of the detection output of the pair of photodetectors. In a magneto-optical recording and reproducing apparatus including a birefringence information forming circuit 30 that forms birefringence information regarding a carrier of a magneto-optical recording medium, the level of each high-frequency component of the detection output of a pair of photodetectors is differentiated. This is a magneto-optical recording and reproducing apparatus which is provided with level control circuits 24 and 25 for controlling the birefringence information, and which is controlled by the output of a birefringence information forming circuit.

【0016】[0016]

【作用】この発明によれば、光磁気ディスクの透明基板
における複屈折を光学的に補正する必要がなく、再生情
報のC/Nを向上させることができて、光学ピックアッ
プの構成が簡単になり、価格が低減される。
[Operation] According to the present invention, there is no need to optically correct birefringence in the transparent substrate of the magneto-optical disk, the C/N of reproduced information can be improved, and the structure of the optical pickup can be simplified. , the price is reduced.

【0017】[0017]

【実施例】以下、図1を参照しながら、この発明による
光磁気記録再生装置の一実施例について説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the magneto-optical recording and reproducing apparatus according to the present invention will be described below with reference to FIG.

【0018】この発明の一実施例の構成を図1に示す。 この図1において、前出図2に対応する部分には同一の
符号を付して重複説明を省略する。
FIG. 1 shows the configuration of an embodiment of the present invention. In FIG. 1, parts corresponding to those in FIG. 2 are given the same reference numerals and redundant explanation will be omitted.

【0019】図1において、10Fは光学ピックアップ
であって、この実施例では、前出図2の従来例で用いら
れた可動複屈折補正子15に代えて、固定のλ/2板1
5fが両ビームスプリッタ13,16間に配設される。 20Cは記録情報再生回路であって、この実施例では、
差動増幅器21の入力端子と高域フィルタ22,23と
の間に、1対の電圧制御係数器24,25が介挿される
。この電圧制御係数器24,25には、複屈折検出回路
30の出力が供給される。その余の構成は前出図2と同
様である。
In FIG. 1, 10F is an optical pickup, and in this embodiment, a fixed λ/2 plate 1 is used instead of the movable birefringence corrector 15 used in the conventional example shown in FIG.
5f is arranged between both beam splitters 13 and 16. 20C is a recorded information reproducing circuit, and in this embodiment,
A pair of voltage control coefficient multipliers 24 and 25 are inserted between the input terminal of the differential amplifier 21 and the high-pass filters 22 and 23. The voltage control coefficient multipliers 24 and 25 are supplied with the output of the birefringence detection circuit 30. The rest of the configuration is the same as that shown in FIG. 2 above.

【0020】この発明の一実施例の動作は次のとおりで
ある。図1に示すように、電圧制御係数器24,25の
係数は、k(0<k<1),1−kとされて、複屈折検
出回路30の出力により、両係数k,1−kが互いに差
動的に制御され、各係数器24,25の出力の和が一定
値とされる。
The operation of one embodiment of the present invention is as follows. As shown in FIG. 1, the coefficients of the voltage control coefficient multipliers 24 and 25 are set to k (0<k<1), 1-k, and both coefficients k, 1-k are determined by the output of the birefringence detection circuit 30. are controlled differentially with respect to each other, and the sum of the outputs of each coefficient multiplier 24 and 25 is made a constant value.

【0021】前述のように、ビームスプリッタ16にお
いて分離された各光束Lp,Lsの光量は、ディスク1
の光磁気記録層1aによる正規の偏光面回転量と、基板
1bの複屈折による不要な偏光面回転量との和にそれぞ
れ対応し、かつ、差動的に変化する。基板1bの複屈折
の変動によって、偏光面の正方向回転量が増加した場合
、例えば、一方の光束Lpの光量が増加すると共に、他
方の光束Lsの光量が減少する。この光量の増減に対応
して、一方の光検出器19aの出力Spのレベルが上昇
し、他方の光検出器19bの出力Ssのレベルが下降し
て、複屈折検出回路30の出力のレベルが下降する。
As described above, the amount of light beams Lp and Ls separated by the beam splitter 16 is
They correspond to the sum of the normal rotation amount of the polarization plane by the magneto-optical recording layer 1a and the unnecessary rotation amount of the polarization plane due to the birefringence of the substrate 1b, and change differentially. When the amount of positive rotation of the plane of polarization increases due to a change in the birefringence of the substrate 1b, for example, the amount of light of one light beam Lp increases and the amount of light of the other light beam Ls decreases. Corresponding to this increase/decrease in the amount of light, the level of the output Sp of one photodetector 19a increases, the level of the output Ss of the other photodetector 19b decreases, and the level of the output of the birefringence detection circuit 30 increases. descend.

【0022】この検出回路30の出力のレベル下降は、
一方の電圧制御係数器24の係数kを減少させると共に
、他方の電圧制御係数器25の係数1−kを増大させる
。これにより、一方の係数器24において、高域フィル
タ22を介して供給される、光検出器19aの出力Sp
のレベル上昇が相殺されると共に、他方の係数器25に
おいては、高域フィルタ23を介して供給される、光検
出器19bの出力Ssのレベル下降が相殺される。
The level drop of the output of the detection circuit 30 is as follows:
The coefficient k of one voltage control coefficient multiplier 24 is decreased, and the coefficient 1-k of the other voltage control coefficient multiplier 25 is increased. As a result, in one coefficient unit 24, the output Sp of the photodetector 19a is supplied via the high-pass filter 22.
At the same time, in the other coefficient multiplier 25, a decrease in the level of the output Ss of the photodetector 19b, which is supplied via the high-pass filter 23, is canceled out.

【0023】上述とは逆に、基板1bの複屈折により偏
光面の正方向回転量が減少した場合は、一方の光束Lp
の光量が減少し、他方の光束Lsの光量が増大して、一
方の光検出器19aの出力Spのレベルが下降し、他方
の光検出器19bの出力Ssのレベルが上昇する。そし
て、複屈折検出回路30の出力のレベルが上昇して、一
方の電圧制御係数器24の係数kが増大すると共に、他
方の電圧制御係数器25の係数1−kが減少して、係数
器24,25においては、対応する光検出器19a、1
9bの出力Sp、Ssのレベル変動がそれぞれ相殺され
る。
Contrary to the above, when the amount of positive rotation of the plane of polarization decreases due to the birefringence of the substrate 1b, one of the light beams Lp
The amount of light of the other light beam Ls decreases, the amount of light of the other light beam Ls increases, the level of the output Sp of one photodetector 19a decreases, and the level of the output Ss of the other photodetector 19b increases. Then, the level of the output of the birefringence detection circuit 30 rises, and the coefficient k of one voltage control coefficient multiplier 24 increases, and the coefficient 1-k of the other voltage control coefficient multiplier 25 decreases. 24, 25, corresponding photodetectors 19a, 1
The level fluctuations of the outputs Sp and Ss of 9b are canceled out.

【0024】そして、差動増幅器21からは、上述のよ
うにして、ディスク1の基板1bの複屈折の変動が電気
的に補償された、所定の高C/Nの再生信号が得られる
。また、複屈折の変動が電気的に補償されるため、ディ
スクの成形工程における基板の複屈折量の出荷基準を緩
和することができて、各種の管理が容易となり、ディス
クのコストが低減される。
As described above, the differential amplifier 21 obtains a reproduced signal with a predetermined high C/N in which variations in the birefringence of the substrate 1b of the disk 1 are electrically compensated. In addition, since variations in birefringence are electrically compensated, shipping standards for the amount of birefringence of the substrate in the disk molding process can be relaxed, making various management easier and reducing disk costs. .

【0025】[0025]

【発明の効果】以上詳述のように、この発明によれば、
光磁気ディスク1からの光束を1対の光検出器19a,
19bに分配し、この光検出器の検出出力の各低域成分
に基づいて、光磁気ディスクの透明基板1bに関する複
屈折情報を得ると共に、両光検出器の検出出力の各高域
成分のレベルを差動的に制御する1対のレベル制御回路
24,25を設け、このレベル制御回路を複屈折情報に
より制御して、透明基板における複屈折を電気的に補正
した再生情報を得るようにしたので、再生情報のC/N
を向上させることができると共に、、光学ピックアップ
の構成を簡単にすることができる光磁気記録再生装置が
得られる。
[Effects of the Invention] As detailed above, according to the present invention,
A pair of photodetectors 19a,
19b, and based on each low frequency component of the detection output of this photodetector, birefringence information regarding the transparent substrate 1b of the magneto-optical disk is obtained, and the level of each high frequency component of the detection output of both photodetectors is obtained. A pair of level control circuits 24 and 25 are provided to differentially control the level control circuits 24 and 25, and this level control circuit is controlled by birefringence information to obtain reproduction information in which birefringence in the transparent substrate is electrically corrected. Therefore, the C/N of playback information
A magneto-optical recording/reproducing device is obtained in which the optical pickup can be improved and the structure of the optical pickup can be simplified.

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

【図1】  この発明による光磁気記録再生装置の一実
施例の構成を示すブロック図
[Fig. 1] A block diagram showing the configuration of an embodiment of a magneto-optical recording/reproducing device according to the present invention.

【図2】  従来の光磁気記録再生装置の構成例を示す
ブロック図
[Figure 2] Block diagram showing a configuration example of a conventional magneto-optical recording/reproducing device

【図3】  従来例の要部の構成を示す略線平面図[Figure 3] Schematic plan view showing the configuration of the main parts of the conventional example

【図
4】  この発明を説明するための斜視図
[Fig. 4] Perspective view for explaining this invention

【図5】  
この発明を説明するための線図
[Figure 5]
Diagram for explaining this invention

【符号の説明】[Explanation of symbols]

10F  光学ピックアップ 11  レーザダイオード 16  偏光ビームスプリッタ 19a,19b  光検出器 20C  情報検出回路 24,25  電圧制御係数器(レベル制御回路)30
  複屈折検出回路
10F Optical pickup 11 Laser diode 16 Polarizing beam splitter 19a, 19b Photodetector 20C Information detection circuit 24, 25 Voltage control coefficient unit (level control circuit) 30
Birefringence detection circuit

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  ピックアップ光束を光磁気記録媒体に
照射し、この光磁気記録媒体からの光束を1対の光検出
器に分配する光学ピクアップと、上記1対の光検出器の
検出出力の各高域成分に基づいて、上記光磁気記録媒体
に記録された情報を再生する再生回路と、上記1対の光
検出器の検出出力の各低域成分に基づいて、上記光磁気
記録媒体の担体に関する複屈折情報を形成する複屈折情
報形成回路とを備える光磁気記録再生装置において、上
記1対の光検出器の検出出力の各高域成分のレベルを差
動的に制御するレベル制御回路を設けると共に、このレ
ベル制御回路を上記複屈折情報形成回路の出力により制
御するようにしたことを特徴とする光磁気記録再生装置
1. An optical pickup that irradiates a magneto-optical recording medium with a pickup light beam and distributes the light beam from the magneto-optical recording medium to a pair of photodetectors, and each detection output of the pair of photodetectors. a reproducing circuit that reproduces information recorded on the magneto-optical recording medium based on the high-frequency components; and a reproducing circuit that reproduces information recorded on the magneto-optical recording medium based on the high-frequency components; A magneto-optical recording/reproducing device comprising a birefringence information forming circuit for forming birefringence information regarding the above, and a level control circuit for differentially controlling the level of each high frequency component of the detection output of the pair of photodetectors. 1. A magneto-optical recording and reproducing apparatus, characterized in that the level control circuit is controlled by the output of the birefringence information forming circuit.
JP6346191A 1991-03-27 1991-03-27 Magneto-optical recording and reproducing device Pending JPH04298836A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6346191A JPH04298836A (en) 1991-03-27 1991-03-27 Magneto-optical recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6346191A JPH04298836A (en) 1991-03-27 1991-03-27 Magneto-optical recording and reproducing device

Publications (1)

Publication Number Publication Date
JPH04298836A true JPH04298836A (en) 1992-10-22

Family

ID=13229903

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6346191A Pending JPH04298836A (en) 1991-03-27 1991-03-27 Magneto-optical recording and reproducing device

Country Status (1)

Country Link
JP (1) JPH04298836A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5537383A (en) * 1995-03-01 1996-07-16 Eastman Kodak Company Optical data storage system with differential data detection and source noise subtraction for use with magneto-optic, write-once and other optical media
US5586101A (en) * 1995-03-01 1996-12-17 Eastman Kodak Company Magneto-optic data storage system with differential detection channels having separate gain control circuit
US5805536A (en) * 1996-11-07 1998-09-08 Eastman Kodak Company Method for bandwidth reduction in writeable optical data storage apparatus
US5809001A (en) * 1996-11-07 1998-09-15 Eastman Kodak Company Bandwidth reduction in writeable optical data storage apparatus

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5537383A (en) * 1995-03-01 1996-07-16 Eastman Kodak Company Optical data storage system with differential data detection and source noise subtraction for use with magneto-optic, write-once and other optical media
US5586101A (en) * 1995-03-01 1996-12-17 Eastman Kodak Company Magneto-optic data storage system with differential detection channels having separate gain control circuit
US5805536A (en) * 1996-11-07 1998-09-08 Eastman Kodak Company Method for bandwidth reduction in writeable optical data storage apparatus
US5809001A (en) * 1996-11-07 1998-09-15 Eastman Kodak Company Bandwidth reduction in writeable optical data storage apparatus

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