JPH04132031A - Method and device for reproducing magneto-optical information - Google Patents

Method and device for reproducing magneto-optical information

Info

Publication number
JPH04132031A
JPH04132031A JP25240690A JP25240690A JPH04132031A JP H04132031 A JPH04132031 A JP H04132031A JP 25240690 A JP25240690 A JP 25240690A JP 25240690 A JP25240690 A JP 25240690A JP H04132031 A JPH04132031 A JP H04132031A
Authority
JP
Japan
Prior art keywords
magneto
differential amplifier
signal
optical
light
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
JP25240690A
Other languages
Japanese (ja)
Inventor
Yukinori Okazaki
之則 岡崎
Toshiya Akagi
俊哉 赤木
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP25240690A priority Critical patent/JPH04132031A/en
Publication of JPH04132031A publication Critical patent/JPH04132031A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To realize the magneto-optical information reproduction of few noises, large signal reproducing margin and high reliability by controlling a differential input signal at the time of differential detection with the difference of the quantities of light of two polarized components intersecting almost orthogonally with the light reflected or transmitted from/ through a magneto-optical recording medium. CONSTITUTION:The light emitted from a laser beam source 1 is reflected by a magneto-optical disk 2, and the polarized state or reflected light 6 is changed by an information signal recorded on a magneto-optical recording film 3. This reflected light 6 is separated into two polarized components intersecting almost orthogonally with each other by using a polarizing beam splitter 7, and they are received by different photodetectors 8, 9. The output difference of signal amplifiers 10 to amplify the outputs of these photodetectors 8, 9 is detected by a DC differential amplifier 11, and one of the signal amplifiers 10 operates so as to increase an amplification factor higher than a reference amplification factor, and the other side operates so as to reduce the amplification factor lower than the reference amplification factor. Thus, the output becomes 0, and the noise of an AC differential amplifier 12 to generate a regenerative signal is canceled by the differential amplifier 12, and regenerative output 13 whose signal amplitude is uniform can be obtained.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、光磁気ディスク等の光磁気記憶媒体を用いた
光情報再生方法および光磁気情報再生装置に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an optical information reproducing method and a magneto-optical information reproducing apparatus using a magneto-optical storage medium such as a magneto-optical disk.

従来の技術 近年、光磁気ディスク装置に代表される、光磁気効果を
用いた情報記録装置が実用化されるようになってきた。
BACKGROUND OF THE INVENTION In recent years, information recording devices using magneto-optical effects, typified by magneto-optical disk devices, have come into practical use.

この装置は従来の光ディスクと同様に、情報の高密度記
録が可能で、さらに情報の追記、消去書換えが可能であ
り、磁気ディスク装置に代わる情報再生装置として有望
視されている。
Like conventional optical disks, this device is capable of high-density recording of information, as well as additional writing, erasing and rewriting of information, and is seen as a promising information reproducing device to replace magnetic disk devices.

以下、従来の光磁気情報再生装置の構成を第2図により
説明する。
The configuration of a conventional magneto-optical information reproducing device will be explained below with reference to FIG.

第2図において、51はレーザ光源、52は光磁気ディ
スク、53は光磁気ディスク52上の光磁気記録膜、5
4はレンズ、55はビームスプリッタ、56は反射光、
57は偏光ビームスプリッタ、58.59は光検出器、
60は信号増幅器、61は差動増幅器、62は再生信号
出力である。
In FIG. 2, 51 is a laser light source, 52 is a magneto-optical disk, 53 is a magneto-optical recording film on the magneto-optical disk 52, and 5
4 is a lens, 55 is a beam splitter, 56 is reflected light,
57 is a polarizing beam splitter, 58.59 is a photodetector,
60 is a signal amplifier, 61 is a differential amplifier, and 62 is a reproduced signal output.

上記の構成において、レーザ光源51より出射した光は
、光磁気ディスク52で反射され、光磁気ディスク52
上の光磁気記録膜53に記録された情報信号によって反
射光56の偏光状態が変化する。この情報信号によって
偏光状態が変化した反射光56は、偏光ビームスプリッ
タ57を用いて、互いに略直行した2つの偏光成分に分
離され、各々別の光検出器58.59に受光される。
In the above configuration, the light emitted from the laser light source 51 is reflected by the magneto-optical disk 52.
The polarization state of the reflected light 56 changes depending on the information signal recorded on the upper magneto-optical recording film 53. The reflected light 56 whose polarization state has been changed by this information signal is separated into two polarization components substantially perpendicular to each other using a polarization beam splitter 57, and each is received by a separate photodetector 58, 59.

光検出器58.59の出力は信号増幅器60.60で増
幅され、差動アンプ61で差動検出されて光磁気記録膜
上の情報信号が再生信号出力62として再生される。
The outputs of the photodetectors 58 and 59 are amplified by signal amplifiers 60 and 60, differentially detected by a differential amplifier 61, and the information signal on the magneto-optical recording film is reproduced as a reproduction signal output 62.

しかしながら、実際の光磁気ディスクではポリカーボネ
ート等の樹脂材料で構成されたディスク基板の複屈折や
、レンズ、ビームスプリッタ等の光学系の偏光特性によ
って、上記光検出器58゜59の出力が変化する。光学
系の偏光特性は、使用部品の特性ばらつきや、光学系の
組立精度のばらつきによるが、この場合、再生信号への
影響は光検出器58.59の出力間に一定の振幅差があ
る状態になり、差動検出によるノイズの相殺と信号振幅
の拡大が充分行われない状態になる。
However, in an actual magneto-optical disk, the output of the photodetectors 58 and 59 changes depending on the birefringence of the disk substrate made of a resin material such as polycarbonate and the polarization characteristics of optical systems such as lenses and beam splitters. The polarization characteristics of the optical system depend on variations in the characteristics of the parts used and variations in the assembly precision of the optical system, but in this case, the influence on the reproduced signal is due to the state where there is a certain amplitude difference between the outputs of the photodetectors 58 and 59. As a result, noise cancellation and signal amplitude expansion by differential detection are not performed sufficiently.

方、ディスク基板の複屈折の場合は、ディスクの場所に
よって複屈折特性が変化するため、ディスクの回転に伴
って前記光検出器58.59の出力が変動を受け、これ
に伴って再生される信号の振幅が変調を受け、またノイ
ズの相殺効果も減少する。また、このディスク基板の複
屈折は基板の温度でも大きく変化するため、出荷検査時
ある温度で複屈折の小さい光磁気ディスク基板であって
も、実使用状態で光磁気ディスクドライブの中で使用し
た場合、基板温度が上昇するため実際の信号再生では、
複屈折の影響が出て、信号が変調を受けることになる。
On the other hand, in the case of birefringence of the disk substrate, since the birefringence characteristics change depending on the location of the disk, the output of the photodetectors 58 and 59 changes as the disk rotates, and the output of the photodetector 58 and 59 is accordingly reproduced. The amplitude of the signal is modulated and the noise cancellation effect is also reduced. In addition, the birefringence of this disk substrate changes greatly depending on the temperature of the substrate, so even if a magneto-optical disk substrate has low birefringence at a certain temperature during shipping inspection, it may not be possible to use it in a magneto-optical disk drive under actual conditions. In actual signal regeneration, the board temperature increases.
The signal will be modulated due to the effects of birefringence.

発明が解決しようとする課題 このように従来の光磁気ディスクでは、ディスク基板の
複屈折や光学系の偏光特性、特に温度変化に伴うディス
ク基板の複屈折の変化によって、光検出器の出力が変調
を受け、常に最適な状態で差動検出によって情報信号を
得るのが難しいという課題を有している。
Problems to be Solved by the Invention As described above, in conventional magneto-optical disks, the output of the photodetector is modulated by the birefringence of the disk substrate and the polarization characteristics of the optical system, especially changes in the birefringence of the disk substrate due to temperature changes. Therefore, there is a problem in that it is difficult to always obtain information signals by differential detection in an optimal state.

本発明は上記従来の課題を解決するもので、上記種々の
原因により光検出器が変調を受けた場合にも、再生され
る信号の振幅に変動がなく、ノイズの除去効果が大きく
、かつ信号再生マージンの大きな、信頼性の高い光磁気
情報再生方法および光磁気情報再生装置を提供すること
を目的とする。
The present invention solves the above-mentioned conventional problems, and even when the photodetector is modulated due to the various causes mentioned above, there is no fluctuation in the amplitude of the reproduced signal, the noise removal effect is large, and the signal It is an object of the present invention to provide a highly reliable magneto-optical information reproducing method and a magneto-optical information reproducing device with a large reproduction margin.

課題を解決するための手段 上記目的を達成するために本発明においては、光磁気記
憶媒体より信号再生を行なう際に、前記光磁気記憶媒体
より反射または透過した光の互いに略直行する2つの偏
光成分の光量差を検出し、前記光量差によって前記2つ
の偏光成分の差動検出時の差動入力信号を制御するもの
である。
Means for Solving the Problems In order to achieve the above object, in the present invention, when a signal is reproduced from a magneto-optical storage medium, two polarized lights of light reflected or transmitted from the magneto-optical storage medium, which are substantially orthogonal to each other, are used. The light amount difference between the components is detected, and the differential input signal at the time of differential detection of the two polarization components is controlled based on the light amount difference.

さらに本発明においては上記方法を具体化する手段とし
て、レーザー等の光源と、前記光源より出射する光ビー
ムを導く第1の光学系と、光磁気記憶媒体と、前記光磁
気記憶媒体より反射または透過した前記光ビームを互い
に略直行する2つの偏光成分に分離する第2の光学系と
、前記第2の光学系によって分離された前記2つの偏光
成分の光強度を各々検出する2つの光検出器と、前記2
つの光検出器によって得られた光電流信号の差を求める
DC差動増幅器と、同じく前記2つの光検出器によって
得られた光電流信号の差を求めるAC差動増幅器とから
成り、前記DC差動増幅器の出力によって前記AC差動
増幅器に入力される2つの光検出器の出力信号を制御す
るものである。
Furthermore, in the present invention, as a means for embodying the above method, a light source such as a laser, a first optical system that guides a light beam emitted from the light source, a magneto-optical storage medium, and a light beam reflected or reflected from the magneto-optical storage medium are provided. a second optical system that separates the transmitted light beam into two polarized components substantially perpendicular to each other; and two photodetectors that respectively detect the light intensities of the two polarized components separated by the second optical system. vessel and the above 2
It consists of a DC differential amplifier for calculating the difference between the photocurrent signals obtained by the two photodetectors, and an AC differential amplifier for calculating the difference between the photocurrent signals obtained by the two photodetectors. The output signals of the two photodetectors input to the AC differential amplifier are controlled by the output of the dynamic amplifier.

さらに上記手段において、前記DC差動増幅器の高域遮
断周波数を前記AC差動増幅器の低域遮断周波数と略一
致させ、またAC差動増幅器に入力される2つの光検出
器の出力信号を制御する手段として、前記2つの光検出
器の出力信号の振幅を前記DC差動増幅器の出力によっ
て変化させる可変増幅率増幅器を用い、また前記AC差
動増幅器に入力される2つの光検出器の出力信号を制御
する方法として、前記DC差動増幅器の出力によって前
記2つの光検出器の出力信号の内、一方の光検出器の信
号の出力振幅を増加させ、同時に他方の光検出器の信号
の出力振幅を減少させることにより、前記DC差動増幅
器の出力がOになるように制御するものである。
Furthermore, in the above means, the high cut-off frequency of the DC differential amplifier is substantially matched with the low cut-off frequency of the AC differential amplifier, and output signals of the two photodetectors input to the AC differential amplifier are controlled. A variable gain amplifier is used as a means for changing the amplitude of the output signals of the two photodetectors according to the output of the DC differential amplifier, and the outputs of the two photodetectors are input to the AC differential amplifier. As a method of controlling the signal, the output amplitude of the signal of one of the two photodetectors is increased by the output of the DC differential amplifier, and at the same time, the output amplitude of the signal of the other photodetector is increased. By reducing the output amplitude, the output of the DC differential amplifier is controlled to become O.

作用 上記の構成による本発明によると、光学系の偏光特性や
、温度変化に伴うディスク基板の複屈折の変化によって
、光検出器の出力が変調を受けた場合でも、常に最適な
状態で差動検出によって情報信号を得ることがでと、光
学系の偏光特性の調整が不要になり、同時に、大きな信
号再生マージンを得ることがでと、信頼性の高い光磁気
情報再生装置が実現できる。
Effects According to the present invention having the above configuration, even if the output of the photodetector is modulated by the polarization characteristics of the optical system or changes in the birefringence of the disk substrate due to temperature changes, the differential signal is always maintained in an optimal state. By obtaining information signals through detection, there is no need to adjust the polarization characteristics of the optical system, and at the same time, a large signal reproduction margin can be obtained, making it possible to realize a highly reliable magneto-optical information reproducing device.

実施例 以下、その実施例を図面を参照して説明する。Example Examples thereof will be described below with reference to the drawings.

第1図は本発明の光磁気再生装置の一実施例の構成を示
す。図において、1はレーザー光源、2は光磁気ディス
ク、3は光磁気ディスク2上の光磁気記録膜、4はレン
ズ、5はビームスプリッタ、6は反射光、7は偏光ビー
ムスプリッタ、8.9は光検出器、10は信号増幅器、
11はDC差動増幅器、12はAC差動増幅器、13は
再生信号出力である。
FIG. 1 shows the configuration of an embodiment of the magneto-optical reproducing apparatus of the present invention. In the figure, 1 is a laser light source, 2 is a magneto-optical disk, 3 is a magneto-optical recording film on the magneto-optical disk 2, 4 is a lens, 5 is a beam splitter, 6 is reflected light, 7 is a polarizing beam splitter, 8.9 is a photodetector, 10 is a signal amplifier,
11 is a DC differential amplifier, 12 is an AC differential amplifier, and 13 is a reproduction signal output.

第1図でレーザ光源1を出射した光は、光磁気ディスク
2で反射され、光磁気ディスク2上の光磁気記録膜3に
記録された情報信号によって反射光6の偏光状態が変化
する。この情報信号によって偏光状態が変化した反射光
6は、偏光ビームスプリッタ7を用いて、互いに略直行
した2つの偏光成分に分離され、各々別の光検出器8,
9に受光される。しかしこの時、光検出器8,9て検出
される信号の中には、光磁気記録膜3に記録された情報
信号だけでなく、多くはポリカーボネート等の樹脂材料
で作られた光磁気ディスクの基板の複屈折や、レンズ4
やビームスプリッタ5,7等の光学系の位相差による偏
光成分の変動が含まれている。特に光磁気ディスクの基
板の複屈折はディスク基板の温度によって大きく変化す
る。これらの変動は本来光磁気ディスクに記録された情
報信号に対し、信号振幅の変動やピークシフトとなって
影響を与える。本発明ではこの光検出器8.9の出力を
増幅する信号増幅器10.10の出力差を直流成分から
検出するDC差動増幅器11で検出し、この検出結果に
応じて制御信号増幅器10.10の増幅率を制御し、前
記DC差動増幅器11の出力がOになるように制御され
る。この時、信号増幅器10.10の基準増幅率、およ
びDC差動増幅器11のオフセット電圧はあらかじめ複
屈折が少ないディスクで校正されて基準位置が設定され
ている。このようにして、複屈折のあるディスクを再生
した場合、本発明では前記DC差動増幅器11の出力に
応じて、2つの前記信号増幅器10.10の一方は基準
増幅率に対して増幅率を上げ、他方は基準増幅率に対し
て増幅率を下げる働きをする。この結果、DC差動増幅
器11の出力は0になり、再生信号を作るAC差動増幅
器12の出力は、ノイズが差動増幅器12で相殺され、
信号振幅が揃った再生信号出力13を得ることができる
In FIG. 1, light emitted from a laser light source 1 is reflected by a magneto-optical disk 2, and the polarization state of the reflected light 6 is changed by an information signal recorded on a magneto-optical recording film 3 on the magneto-optical disk 2. The reflected light 6 whose polarization state has been changed by this information signal is separated into two polarization components that are substantially orthogonal to each other using a polarization beam splitter 7, and each is separated by a separate photodetector 8,
The light is received at 9. However, at this time, the signals detected by the photodetectors 8 and 9 include not only information signals recorded on the magneto-optical recording film 3, but also information signals from magneto-optical disks made of resin materials such as polycarbonate. Birefringence of the substrate and lens 4
This includes fluctuations in polarization components due to phase differences in optical systems such as the beam splitters 5 and 7, and the like. In particular, the birefringence of the substrate of a magneto-optical disk changes greatly depending on the temperature of the disk substrate. These fluctuations affect the information signals originally recorded on the magneto-optical disk by causing signal amplitude fluctuations and peak shifts. In the present invention, the output difference of the signal amplifier 10.10 that amplifies the output of the photodetector 8.9 is detected by the DC differential amplifier 11 that detects the DC component, and the control signal amplifier 10.10 is The amplification factor of the DC differential amplifier 11 is controlled such that the output of the DC differential amplifier 11 becomes O. At this time, the reference amplification factor of the signal amplifier 10.10 and the offset voltage of the DC differential amplifier 11 are calibrated in advance using a disk with little birefringence, and the reference position is set. In this way, when a disc with birefringence is reproduced, one of the two signal amplifiers 10.10 adjusts the amplification factor with respect to the reference amplification factor according to the output of the DC differential amplifier 11. The other serves to lower the amplification factor relative to the reference amplification factor. As a result, the output of the DC differential amplifier 11 becomes 0, and the noise of the output of the AC differential amplifier 12 that produces the reproduced signal is canceled by the differential amplifier 12.
A reproduced signal output 13 with uniform signal amplitude can be obtained.

本来、本発明で用いたDC差動増増幅器1の制御帯域と
しては、複屈折変動の発生する全周波数範囲を設定する
べきである。しかし、実際に光磁気記憶媒体に記録され
る信号は信号の変調方式にもよるが、ある程度の低周波
成分を持っており、信号を再生するAC差動増幅器の周
波数帯域は通常、ある程度低域側に広く設定されている
。したがって、このAC差動増輻器12の低域遮断周波
数をfLとした時、本発明の光磁気再生装置で、基板の
複屈折の影響を検出するDC差動増幅器11の高域遮断
周波数をfLに取り、制御周波数帯域をDCからfLま
で取るのが最も効果的である。
Originally, the control band of the DC differential amplifier 1 used in the present invention should be set to cover the entire frequency range in which birefringence fluctuations occur. However, depending on the signal modulation method, the signals actually recorded on magneto-optical storage media have a certain degree of low frequency components, and the frequency band of the AC differential amplifier that reproduces the signal is usually a certain degree of low frequency. It is set wide on the side. Therefore, when the low cutoff frequency of this AC differential amplifier 12 is fL, the high cutoff frequency of the DC differential amplifier 11 that detects the influence of birefringence of the substrate in the magneto-optical reproducing apparatus of the present invention is It is most effective to set the control frequency band from DC to fL.

なお、上記実施例では、光磁気ディスク(光磁気記憶媒
体)が反射形のものについて説明したが、透過形のもの
であっても本発明は適用できるものである。
In the above embodiments, the magneto-optical disk (magneto-optical storage medium) is of a reflective type, but the present invention is also applicable to a transmissive type.

発明の効果 以上の説明からも明らかなように、本発明の方法および
装置を用いることにより、光学系の′偏光特性や、温度
変化に伴う光磁気ディスク基板における複屈折の変化に
よって、光検出器の出力が変調を受けた場合でも、常に
最適な状態で差動検出によって情報信号を再生すること
が可能で、再生された信号の振幅に変動がな(、ノイズ
の除去効果が太き(、かつ信号再生マージンの大きな、
信頼性の高い光磁気情報再生方法および装置が実現可能
で、同時に光学系の偏光特性の無調整化ができるという
効果も得られる。
Effects of the Invention As is clear from the above explanation, by using the method and apparatus of the present invention, the photodetector can be Even when the output of a and a large signal regeneration margin.
It is possible to realize a highly reliable magneto-optical information reproducing method and apparatus, and at the same time, it is possible to achieve the effect that the polarization characteristics of the optical system can be made unadjusted.

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

第1図は本発明の光磁気情報再生装置の一実施例を示す
構成図、第2図は同装置の従来例を示す構成図である。 1・・・・・・レーザー光源(光源)、2・・・・・・
光磁気ディスク(光磁気記憶媒体)、4・・・・・・レ
ンズ、5・・・・・・ビームスプリッタ、6・・・・・
・反射光、7・・・・・・偏光ビームスプリッタ、8,
9・・・・・・光検出器、10・・・・・・信号増幅機
器、11・・・・・・DC差動増幅器、12・・・・・
・AC差動増幅器、13・・・・・・再生信号出力。
FIG. 1 is a block diagram showing an embodiment of the magneto-optical information reproducing apparatus of the present invention, and FIG. 2 is a block diagram showing a conventional example of the same apparatus. 1... Laser light source (light source), 2...
Magneto-optical disk (magneto-optical storage medium), 4...lens, 5...beam splitter, 6...
・Reflected light, 7...Polarizing beam splitter, 8,
9...Photodetector, 10...Signal amplification equipment, 11...DC differential amplifier, 12...
- AC differential amplifier, 13... Reproduction signal output.

Claims (4)

【特許請求の範囲】[Claims] (1)光磁気記憶媒体より信号再生を行なう際に、前記
光磁気記憶媒体より反射または透過した光の互いに略直
行する2つの偏光成分の光量差を検出し、前記光量差に
よって前記2つの偏光成分の差動検出時の差動入力信号
を制御することを特徴とする光磁気情報再生方法。
(1) When reproducing a signal from a magneto-optical storage medium, the difference in the amount of light between two polarized components that are substantially perpendicular to each other in the light reflected or transmitted from the magneto-optical storage medium is detected, and the difference in the amount of polarized light is determined based on the difference in the amount of light. A magneto-optical information reproducing method characterized by controlling a differential input signal during differential detection of components.
(2)光源と、前記光源より出射する光ビームを導く第
1の光学系と、光磁気記憶媒体と、前記光磁気記憶媒体
より反射または透過した前記光ビームの互いに略直行す
る2つの偏光成分を分離する第2の光学系と、前記第2
の光学系によって分離された前記2つの偏光成分の光強
度を各々検出する2つの光検出器と、前記2つの光検出
器によって得られた光電流信号の差を求めるDC差動増
幅器と、同じく前記2つの光検出器によって得られた光
電流信号の差を求めるAC差動増幅器とから成り、前記
DC差動増幅器の出力によって前記AC差動増幅器に入
力される2つの光検出器の出力信号を制御するように構
成したことを特徴とする光磁気情報再生装置。
(2) a light source, a first optical system that guides a light beam emitted from the light source, a magneto-optical storage medium, and two mutually orthogonal polarization components of the light beam reflected or transmitted from the magneto-optical storage medium; a second optical system that separates the second optical system;
two photodetectors that respectively detect the light intensities of the two polarized components separated by the optical system; and a DC differential amplifier that calculates the difference between the photocurrent signals obtained by the two photodetectors. and an AC differential amplifier for determining the difference between the photocurrent signals obtained by the two photodetectors, and the output signals of the two photodetectors are input to the AC differential amplifier by the output of the DC differential amplifier. 1. A magneto-optical information reproducing device configured to control.
(3)DC差動増幅器の高域遮断周波数を、同じくAC
差動増幅器の低域遮断周波数と略一致させたことを特徴
とする請求項2記載の光磁気情報再生装置。
(3) Set the high cutoff frequency of the DC differential amplifier to
3. The magneto-optical information reproducing apparatus according to claim 2, wherein the low cutoff frequency of the differential amplifier is substantially the same as that of the differential amplifier.
(4)AC差動増幅器に入力される2つの光検出器の出
力信号を制御する手段として、その2つの光検出器の出
力信号の振幅を、DC差動増幅器の出力によって増幅率
を変化させる可変増幅率増幅器を経由して前記AC差動
増幅器に供給する手段を用いたことを特徴とする請求項
2記載の光磁気情報再生装置。
(4) As a means of controlling the output signals of the two photodetectors that are input to the AC differential amplifier, the amplification factor of the output signals of the two photodetectors is changed by the output of the DC differential amplifier. 3. The magneto-optical information reproducing apparatus according to claim 2, further comprising means for supplying the signal to said AC differential amplifier via a variable gain amplifier.
JP25240690A 1990-09-20 1990-09-20 Method and device for reproducing magneto-optical information Pending JPH04132031A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25240690A JPH04132031A (en) 1990-09-20 1990-09-20 Method and device for reproducing magneto-optical information

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25240690A JPH04132031A (en) 1990-09-20 1990-09-20 Method and device for reproducing magneto-optical information

Publications (1)

Publication Number Publication Date
JPH04132031A true JPH04132031A (en) 1992-05-06

Family

ID=17236901

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25240690A Pending JPH04132031A (en) 1990-09-20 1990-09-20 Method and device for reproducing magneto-optical information

Country Status (1)

Country Link
JP (1) JPH04132031A (en)

Cited By (2)

* 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

Cited By (2)

* 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

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