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JPH07105084B2 - Magneto-optical disk device - Google Patents

Magneto-optical disk device

Info

Publication number
JPH07105084B2
JPH07105084B2 JP61159609A JP15960986A JPH07105084B2 JP H07105084 B2 JPH07105084 B2 JP H07105084B2 JP 61159609 A JP61159609 A JP 61159609A JP 15960986 A JP15960986 A JP 15960986A JP H07105084 B2 JPH07105084 B2 JP H07105084B2
Authority
JP
Japan
Prior art keywords
photodetector
magneto
prism
signal
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.)
Expired - Lifetime
Application number
JP61159609A
Other languages
Japanese (ja)
Other versions
JPS6316449A (en
Inventor
敏光 賀来
正啓 尾島
裕史 助田
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP61159609A priority Critical patent/JPH07105084B2/en
Publication of JPS6316449A publication Critical patent/JPS6316449A/en
Publication of JPH07105084B2 publication Critical patent/JPH07105084B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

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装置の光ヘッドに係り、特に光
磁気信号再生用の光検出器とプリアンプを一体化するこ
とにより再生信号の信号対雑音化を向上するに好適な光
磁気ディスク装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical head of a magneto-optical disk device, and more particularly to a signal pair of a reproduced signal by integrating a photodetector for reproducing a magneto-optical signal and a preamplifier. The present invention relates to a magneto-optical disk device suitable for improving noise reduction.

〔従来の技術〕[Conventional technology]

従来の装置は、特開昭60-20340号に記載の様に、光磁気
信号の検出方式として差動検出を採用し、検光子として
ウォラストンプリズムやローションプリズムなど互いに
直交する偏光成分を別個に取り出すことのできる偏光プ
リズムを用い、これらのプリズムを入射偏光方向に対し
45°傾けるかあるいはプリズムの前にλ/2板(λ:使用
波長)を設置してこれをプリズムの入射偏光方向に対し
45°傾けてプリズムで2分された光束を2分割光検出器
で検出している。通常、2分割光検出器の出力を差動し
て光磁気信号を得るが、従来の装置ではその検出手段に
ついて明言されていない。
As described in JP-A-60-20340, the conventional device employs differential detection as a method for detecting a magneto-optical signal, and separates mutually orthogonal polarization components such as a Wollaston prism or a lotion prism as an analyzer. Use polarizing prisms that can be taken out, and use these prisms for the incident polarization direction.
Tilted at 45 °, or installed a λ / 2 plate (λ: wavelength used) in front of the prism, and set this to the incident polarization direction of the prism.
The light beam split by the prism while tilted at 45 ° is detected by the two-split photodetector. Usually, the output of the two-division photodetector is differentially obtained to obtain a magneto-optical signal, but in the conventional device, the detecting means is not specified.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

上記従来技術は光磁気信号の信号対雑音比向上に関し、
最適な光検出器からの信号検出手段について配慮されて
おらず、ただ電流−電圧変換用のプリアンプを設置した
だけでは配線による浮遊容量やノイズを受けて十分な信
号対雑音比が得られないという問題があった。
The above-mentioned prior art relates to improvement of a signal-to-noise ratio of a magneto-optical signal,
No consideration is given to the optimum signal detection method from the photodetector, and it is said that a sufficient signal-to-noise ratio cannot be obtained due to stray capacitance and noise due to wiring simply by installing a preamplifier for current-voltage conversion. There was a problem.

本発明の目的は信号検出用の光検出器とその出力を電気
信号に変換するプリアンプを一体化することにより、信
号対雑音比を向上し、プリアンプの占有面積を小さくす
ることにある。
An object of the present invention is to improve the signal-to-noise ratio and reduce the area occupied by the preamplifier by integrating a photodetector for signal detection and a preamplifier for converting its output into an electric signal.

〔問題点を解決するための手段〕[Means for solving problems]

上記目的は、2分割光検出器のパッケージ内に信号再生
用のプリアンプを内蔵することにより、達成される。
The above object is achieved by incorporating a preamplifier for signal reproduction in the package of the two-divided photodetector.

〔作用〕[Action]

光検出器内にプリアンプ類を設けることにより浮遊容量
の問題、外乱の影響がなくなり、高S/Nの信号が得られ
ることになる。
By providing preamplifiers in the photodetector, the problem of stray capacitance and the influence of disturbance are eliminated, and a high S / N signal can be obtained.

〔実施例〕〔Example〕

以下、本発明の一実施例を第1図により説明する。半導
体レーザ1から出た光はカップリングレンズ2を通りビ
ーム整形プリズム3で円形の平行光となって第一ビーム
スプリッタ4にp偏向として入射する。第1ビームスプ
リッタ4を出射した光はトラッキング用のガルバノミラ
ー5および自動焦点合わせ用のボイスコイル6に取付け
られている絞り込みレンズ7を通って垂直磁化膜8が蒸
着またはスパッタリングにより形成されているディスク
9上に1μm程度のスポット状に絞り込まれる。ディス
ク9からの反射光は入射光と同一経路を通って第1ビー
ムスプリッタ4に入射し、第1ビームスプリッタで決ま
るp偏光反射率成分が反射し、光路を分離される。その
後第2ビームスプリッタ10で光は2分され、透過側は自
動焦点合わせ信号検出およびトラッキング信号検出用の
サーボ信号検出信号用光束として使用され、反射側は光
磁気信号検出用光束として使用される。透過した光束は
凸レンズ11を経て第3ビームスプリッタ12で2分され、
透過側はトラッキング信号検出用2分割光検出器13に導
かれ、反射側はシリンドリカルレンズ14、ナイフエッジ
15を通過後、自動焦点合わせ信号検出用2分割光検出器
16に導かれる。トラッキングは案内溝付ディスクからの
回折光を差動して誤差信号を得るPush-Pull方式を利用
し、差動増幅器17で差動した後、ガルバノミラー駆動回
路18を通ってガルバノミラー5を駆動することにより行
なう。自動焦点合わせは特開昭57-108811号に記載の像
回転方式を利用し、差動増幅器19で差動した後、ボイス
コイル駆動回路20を通ってボイスコイル6を駆動するこ
とにより行なう。
An embodiment of the present invention will be described below with reference to FIG. The light emitted from the semiconductor laser 1 passes through the coupling lens 2, becomes a circular parallel light at the beam shaping prism 3, and enters the first beam splitter 4 as p-polarized light. The light emitted from the first beam splitter 4 passes through a focusing lens 7 attached to a tracking galvano mirror 5 and a voice coil 6 for automatic focusing, and a perpendicular magnetic film 8 is formed on the disk by vapor deposition or sputtering. 9 is narrowed down to a spot shape of about 1 μm. The reflected light from the disk 9 enters the first beam splitter 4 through the same path as the incident light, the p-polarized reflectance component determined by the first beam splitter is reflected, and the optical path is separated. After that, the light is divided into two by the second beam splitter 10, the transmission side is used as a servo signal detection signal light beam for automatic focusing signal detection and tracking signal detection, and the reflection side is used as a magneto-optical signal detection light beam. . The transmitted light flux passes through the convex lens 11 and is split into two by the third beam splitter 12.
The transmission side is guided to the two-part photodetector 13 for tracking signal detection, and the reflection side is the cylindrical lens 14 and knife edge.
2-pass photodetector for automatic focusing signal detection after passing 15
Guided by 16. For tracking, a push-pull method is used for obtaining an error signal by differentially diffracting light from a disc with a guide groove. After being differentiated by a differential amplifier 17, the galvano mirror 5 is driven through a galvano mirror drive circuit 18. By doing. The automatic focusing is performed by driving the voice coil 6 through the voice coil drive circuit 20 after using the image rotation method described in Japanese Patent Application Laid-Open No. 57-108811, after being differentiated by the differential amplifier 19.

第2ビームスプリンタ10で反射した光磁気信号検出用光
束は1/2波長板21および凸レンズ22を通ってウォラスト
ンプリズムあるいはローションプリズム23に入射する。
これらはいずれも水晶のプリズムを組合わせたもので、
前者は境界面での複屈折によって常光線と異常光線がち
がった方向へ進むので二つの偏光を分離でき、後者も二
つの偏光が分離できるが、常光線は波長によらず直進す
るのでその分離角はウォラストンプリズムの方が大きく
なる。二つの偏光を分離する点で二つのプリズムは同じ
働きをするので、以下ウォラストンプリズムを代表して
説明する。
The magneto-optical signal detecting light beam reflected by the second beam sprinter 10 passes through the half-wave plate 21 and the convex lens 22 and enters the Wollaston prism or the lotion prism 23.
Each of these is a combination of crystal prisms,
The former can separate two polarized lights because the ordinary ray and the extraordinary ray go in different directions due to the birefringence at the boundary surface, and the latter can also separate the two polarized rays. The Wollaston prism has a larger angle. Since the two prisms have the same function in separating the two polarized lights, the Wollaston prism will be described below as a representative.

ストンプリズム23に入射する偏光方向を波長板21により
45°に設定すると分離される2光束の光量を等しくする
ことができる。また1/2波長板を用いずに、ウォラスト
ンプリズム自身を45°回転しても同様の効果が得られ
る。ウォラストンプリズム23で二分された光束は2分割
光検出器24にて独立に検出される。2分割光検出器24の
受光素子241,242は各々電流−電圧変換器251,252で光電
変換された後増幅器253,254を通り(但し、251,252の出
力が十分ある場合は不用)、差動増幅器26へ入力して光
磁気信号を得、また和動増幅器27へ入力されてディスク
9上にあらかじめ凹凸ピットの形成されているID信号
(セクタマーク、番地情報、CRC信号など)を得る。光
磁気信号は通常のID信号に比べて1〜2桁小さいために
使用するプリアンプのアンプノイズが問題となる。例え
ば、プリアンプ類(251,252,253,254)を光ヘッド上に
配置したプリアンプ基板に部品単体を組合わせ形成した
場合、光検出器から電流−電圧変換器251,252までの布
線による浮遊容量と帰還抵抗の浮遊容量のために周波数
特性を考慮すると帰還抵抗を大きくできない。そのため
に信号光量成分は小さくなりノイズ成分はアンプルノイ
ズが支配的となってしまい、信号対雑音比(SN比)が低
下してしまう。本発明ではその問題を解決するために、
プリアンプ類(251,252,253,254)と差動増幅器26、和
動増幅器27を1チップのICとして作製し(第1図に破線
で囲む部分)、2分割光検出器を収納するパッケージ内
に内蔵する。第2図にその様子を示す。パッケージ31は
TO−18あるいはTO−5という規格のケースを用い、ケー
スの中心に2分割光検出器241,242を配置し、その囲り
にプリアンプル類をIC化したチップ32を配置する(第2
図において簡略のため、ワイヤ、端子類は省略した)。
また、以上説明では2分割光検出器とプリアンプICをア
ッセンブルする方式をとったが、Si基板上にモノリシッ
クに2分割光検出器とプリアンプを形成することもでき
る。
The direction of polarization incident on the stone prism 23 is determined by the wave plate 21.
When the angle is set to 45 °, the light quantities of the two separated light beams can be made equal. The same effect can be obtained by rotating the Wollaston prism itself by 45 ° without using the half-wave plate. The light flux divided by the Wollaston prism 23 is independently detected by the two-split photodetector 24. The light receiving elements 241 and 242 of the two-divided photodetector 24 are photoelectrically converted by the current-voltage converters 251 and 252 and then pass through the amplifiers 253 and 254 (however, not necessary when the outputs of 251, 252 are sufficient) and input to the differential amplifier 26. A magneto-optical signal is obtained, and an ID signal (sector mark, address information, CRC signal, etc.) in which concave and convex pits are previously formed on the disk 9 by being input to the summing amplifier 27 is obtained. Since the magneto-optical signal is smaller than the ordinary ID signal by 1 to 2 digits, the amplifier noise of the preamplifier used becomes a problem. For example, when preamplifiers (251, 252, 253, 254) are formed on the preamplifier board that is placed on the optical head by combining components, the stray capacitance of the wiring from the photodetector to the current-voltage converter 251, 252 and the stray capacitance of the feedback resistor Therefore, considering the frequency characteristics, the feedback resistance cannot be increased. Therefore, the signal light amount component becomes small, and the ampule noise becomes dominant in the noise component, and the signal-to-noise ratio (SN ratio) decreases. In order to solve the problem in the present invention,
The preamplifiers (251, 252, 253, 254), the differential amplifier 26, and the summing amplifier 27 are manufactured as a one-chip IC (a portion surrounded by a broken line in FIG. 1) and incorporated in a package containing a two-divided photodetector. The situation is shown in FIG. Package 31
A case of the standard of TO-18 or TO-5 is used, two-divided photodetectors 241 and 242 are arranged at the center of the case, and a chip 32, which is an IC of preampules, is arranged around it.
For simplicity, the wires and terminals are omitted in the figure).
In the above description, the method of assembling the two-division photodetector and the preamplifier IC is adopted, but the two-division photodetector and the preamplifier can be formed monolithically on the Si substrate.

第3図にプリアンプ類をIC化して内蔵した場合とプリア
ンプをプリント基板上に部品単体で組立てた場合の周波
数特性について示す。図において、本発明の場合周波数
特性は20MHzまで劣化はなく、アンプノイズは計算によ
るショットノイズの値よりも小さくなり、理想的なアン
プとなっている。従来の場合は周波数特性は3dB低下で1
2MHzであるが、ノイズはアンプノイズが支配的となり本
発明の場合の値よりも10〜15dB低下している。以上説明
した様に本発明によれば、光磁気信号の信号対雑音比を
充分確保することができる。
Fig. 3 shows the frequency characteristics when the preamplifiers are integrated as an IC and when the preamplifier is assembled as a single component on a printed circuit board. In the figure, in the case of the present invention, the frequency characteristic does not deteriorate up to 20 MHz, and the amplifier noise becomes smaller than the calculated shot noise value, which is an ideal amplifier. In the conventional case, the frequency characteristic is 3 dB lower than 1
Although it is 2 MHz, the noise is 10 to 15 dB lower than the value in the present invention because the amplifier noise is dominant. As described above, according to the present invention, the signal-to-noise ratio of the magneto-optical signal can be sufficiently secured.

なお第1図において記録/消去動作時に垂直磁化膜の磁
化方向を決定する磁場発生器30は本発明に無関係なので
説明を割愛した。
The magnetic field generator 30 for determining the magnetization direction of the perpendicular magnetization film during the recording / erasing operation is not related to the present invention in FIG.

〔発明の効果〕〔The invention's effect〕

本発明によれば、光電変換部の光検出器とプリアンプ類
を光検出器の同一パッケージの中に収納したことにより
浮遊容量を大幅に低減できるので周波数特性が良好でア
ンプノイズが低減でき、光磁気信号の信号対雑音比を大
幅にに向上することができる。また、2分割光検出器、
プリアンプ類はペアで形成できるので特性が同一となり
差動すべき2つの信号のゲインバラツキがなくなるので
同相除去比も向上する効果がある。
According to the present invention, since the photodetector of the photoelectric conversion unit and the preamplifiers are housed in the same package of the photodetector, the stray capacitance can be significantly reduced, the frequency characteristics are good, and the amplifier noise can be reduced. The signal-to-noise ratio of magnetic signals can be significantly improved. Also, a two-part photodetector,
Since the preamplifiers can be formed in pairs, the characteristics are the same and the gain variation between the two signals to be differentiated is eliminated, so that the common mode rejection ratio is also improved.

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

第1図は本発明の1実施例を示す図、第2図,第3図は
実施例を捕捉する図である。 4,10,12……ビームスプリッタ、21……1/2波長板、23…
…ウォラストンプリズム、24……2分割光検出器、251,
252……電流−電圧変換器、253,254……増幅器、26……
差動増幅器、27……和動増幅器
FIG. 1 is a view showing an embodiment of the present invention, and FIGS. 2 and 3 are views for catching the embodiment. 4,10,12 …… Beam splitter, 21 …… 1/2 wave plate, 23…
… Wollaston prism, 24 …… 2 split photo detector, 251,
252 ... Current-voltage converter, 253,254 ... Amplifier, 26 ...
Differential amplifier, 27 ... Wadou amplifier

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】光源と、上記光源から出た光を垂直磁化膜
から成る情報記録媒体上に導く光学系と上記情報記録媒
体からの反射光に含まれる光磁気信号を差動的に検出す
る偏光プリズムと上記偏光プリズムで分離された光を受
光する光検出器と上記情報記録媒体に記録/消去動作時
に磁場を印加する磁場発生器とからなる光磁気ディスク
装置において、上記偏光プリズムとしてウォラストンプ
リズムまたはローションプリズムを用い、上記光検出器
として二分割光検出器を用いて上記光検出器のパッケー
ジの中に上記光検出器の出力を電気変換するプリアンプ
を内蔵する光検出器を設けたことを特徴とする光磁気デ
ィスク装置。
1. A light source, an optical system for guiding light emitted from the light source onto an information recording medium made of a perpendicularly magnetized film, and a magneto-optical signal contained in reflected light from the information recording medium are differentially detected. In a magneto-optical disk device comprising a polarizing prism, a photodetector for receiving the light separated by the polarizing prism, and a magnetic field generator for applying a magnetic field to the information recording medium at the time of recording / erasing operation, Wollaston is used as the polarizing prism. A photodetector having a preamplifier for electrically converting the output of the photodetector is provided in the package of the photodetector using a prism or a lotion prism and a two-divided photodetector as the photodetector. A magneto-optical disk device characterized by.
JP61159609A 1986-07-09 1986-07-09 Magneto-optical disk device Expired - Lifetime JPH07105084B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61159609A JPH07105084B2 (en) 1986-07-09 1986-07-09 Magneto-optical disk device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61159609A JPH07105084B2 (en) 1986-07-09 1986-07-09 Magneto-optical disk device

Related Child Applications (1)

Application Number Title Priority Date Filing Date
JP8280545A Division JP2795271B2 (en) 1996-10-23 1996-10-23 Optical disk drive

Publications (2)

Publication Number Publication Date
JPS6316449A JPS6316449A (en) 1988-01-23
JPH07105084B2 true JPH07105084B2 (en) 1995-11-13

Family

ID=15697451

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61159609A Expired - Lifetime JPH07105084B2 (en) 1986-07-09 1986-07-09 Magneto-optical disk device

Country Status (1)

Country Link
JP (1) JPH07105084B2 (en)

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0234718A (en) * 1988-07-25 1990-02-05 Daido Steel Co Ltd Induction hardening control method
JPH0234717A (en) * 1988-07-25 1990-02-05 Daido Steel Co Ltd Induction hardening control method
JPH0238517A (en) * 1988-07-27 1990-02-07 Daido Steel Co Ltd Method for controlling high frequency quenching
JPH0238521A (en) * 1988-07-27 1990-02-07 Daido Steel Co Ltd Induction hardening system
US5283712A (en) * 1988-10-27 1994-02-01 Mazda Motor Corporation Integrated circuit for vehicle
JPH02170597A (en) * 1988-12-23 1990-07-02 Mazda Motor Corp On-vehicle control unit structure
JP2690533B2 (en) * 1988-12-23 1997-12-10 三洋電機株式会社 Connector structure of hybrid integrated circuit
JPH02193344A (en) * 1989-01-20 1990-07-31 Matsushita Electric Ind Co Ltd Optical pickup

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6020340A (en) * 1983-07-14 1985-02-01 Matsushita Electric Ind Co Ltd Magneto-optical disk playback optical head

Also Published As

Publication number Publication date
JPS6316449A (en) 1988-01-23

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