JPS60179959A - Photomagnetic disk device - Google Patents

Photomagnetic disk device

Info

Publication number
JPS60179959A
JPS60179959A JP3371084A JP3371084A JPS60179959A JP S60179959 A JPS60179959 A JP S60179959A JP 3371084 A JP3371084 A JP 3371084A JP 3371084 A JP3371084 A JP 3371084A JP S60179959 A JPS60179959 A JP S60179959A
Authority
JP
Japan
Prior art keywords
light
servo
sensor
signal
magneto
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
JP3371084A
Other languages
Japanese (ja)
Inventor
Kenta Mikuriya
健太 御厨
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.)
Yokogawa Electric Corp
Original Assignee
Yokogawa Hokushin Electric 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 Yokogawa Hokushin Electric Corp filed Critical Yokogawa Hokushin Electric Corp
Priority to JP3371084A priority Critical patent/JPS60179959A/en
Publication of JPS60179959A publication Critical patent/JPS60179959A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording 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
    • G11B11/10Recording 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
    • G11B11/105Recording 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

Abstract

PURPOSE:To improve S/N of a data signal by rotating slightly the polarizing direction of the light projected to a photomagnetic disk from a light source toward the polarizing direction of the light going toward a servo sensor and therefore eliminating the interference between the data signal and the servo signal. CONSTITUTION:Laser light given from a laser light source 1 is projected to a photoelectric disk 6 through a half mirror 3, and this reflected light is rotated with its polarized surface by a Kerr revolving angle +thetak or -thetak according to the magnetizing direction of the disk 6. Then the reflected light is reflected by the mirror 3 and separated by a polarized beam splitter 13. Then the P polarized component is made incident on a data sensor 12 with the S polarized component projected to a servo sensor 10 respectively. In such a way, no interference occurs between the data and servo signals since both signals are separated from each other. Furthermore a large output is obtained for the servo signal.

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の書込、読出特
性の改善に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to improving the writing and reading characteristics of an optical head of a magneto-optical disk device.

〔従来例〕[Conventional example]

従来の光磁気ディスク装置においては、■フォカスとト
ラ、キングのサーボ信号を、検光子を゛通った後の光を
センサに入力して得ていた。このようなものでは、サー
ボ用信号の中にデータ信号が干渉してくることが問題で
あり、また、サーボ用の光強度が小さいという欠点があ
る。これの改良として、第1図に示す如く、ハーフミラ
−を用いて、データ用の光とサーボ用の光を分けた装置
がある。
In conventional magneto-optical disk drives, focus, track, and king servo signals are obtained by inputting light that has passed through an analyzer into a sensor. This type of device has a problem in that the data signal interferes with the servo signal, and also has the disadvantage that the servo light intensity is low. As an improvement on this, there is a device that uses a half mirror to separate data light and servo light, as shown in FIG.

図において、1はレーザー光源、2は偏光子、3はハー
フミラ−14はミラー、5はレンズ、6は光磁気ディス
ク、7はハーフミラ−18はコリメータレンズ、9はシ
リンドリカルレンズ、1oはサーボ用センサ、11は検
光子、12はデータ用センサである。
In the figure, 1 is a laser light source, 2 is a polarizer, 3 is a half mirror, 14 is a mirror, 5 is a lens, 6 is a magneto-optical disk, 7 is a half mirror, 18 is a collimator lens, 9 is a cylindrical lens, 1o is a servo sensor , 11 is an analyzer, and 12 is a data sensor.

このようなものにおいては、レーザー光#1がもの光は
偏光子2で′偏光され、ハーフミラ−3を透過し、ミラ
ー4で曲屈され、レンズ5で集光され、光磁気14スク
6に投射される。光磁気ディスク6からの反射光は、投
射光と同じ径路を戻った後、ハーフミラ−5で反射され
、ハーフミラ−7で光は二分される。二分された光の一
方は、コリメータレンズ8、シリンドリカルレンズ9を
通り、サーボ用センサ10に投射される。他方の光は、
検光子11を通り、データ用センサ121C投射される
In such a device, the laser beam #1 is polarized by a polarizer 2, transmitted through a half mirror 3, bent by a mirror 4, condensed by a lens 5, and then directed to a magneto-optical 14 disk 6. Projected. After the reflected light from the magneto-optical disk 6 returns along the same path as the projected light, it is reflected by the half mirror 5, and the light is split into two by the half mirror 7. One of the two halves of the light passes through a collimator lens 8 and a cylindrical lens 9, and is projected onto a servo sensor 10. The other light is
It passes through the analyzer 11 and is projected onto the data sensor 121C.

以上の如くして、データ用信号とサーボ用信号が分離し
−て得られ、サーボ用信号中にデータ信号が干渉してく
るおそれはない。
As described above, the data signal and the servo signal are obtained separately, and there is no possibility that the data signal will interfere with the servo signal.

しかしながら、このようなものにおいては、光は二倍さ
れるため、データ用信号が小さくなりSN比が悪くなる
。また、光学系が複雑になるという欠点がある。
However, in such a device, since the light is doubled, the data signal becomes smaller and the S/N ratio deteriorates. Another disadvantage is that the optical system becomes complicated.

本発明は、この問題点を解決するものである。The present invention solves this problem.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、簡潔な光学系の構成によ抄、データ信
号と干渉のないサーボ信号が得られ、かつSN比の良好
なデータ信号が得られる光磁気ディスク装置を提供する
Kある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a magneto-optical disk device that can obtain a servo signal that does not interfere with a data signal and a data signal with a simple optical system configuration, and can also provide a data signal with a good signal-to-noise ratio.

〔発明の構成〕[Structure of the invention]

この目的を達成するためくい光源からの袖先が投射され
る光磁気ディスクと、該光磁気ディスクからの光をサー
ボ用センサに向う光とデータ用センサに向う光とに分離
する偏光ビームスグリ、ターとを具備し、前記光源から
前記光磁気デスクに投射する光の偏光方向をサーボ用セ
ンサに向う光の偏光方向かられずかに回転させてなる光
磁気ディスク装置を構成したものである。
To achieve this purpose, we use a magneto-optical disk whose tip is projected from a sharp light source, a polarized beam currant that separates the light from the magneto-optical disk into light directed to the servo sensor and light directed to the data sensor. A magneto-optical disk device is constructed in which the polarization direction of light projected from the light source onto the magneto-optical disk is slightly rotated from the polarization direction of light directed toward the servo sensor.

以下、実施例について説明する。Examples will be described below.

〔実施例〕〔Example〕

第2図は、本発明の一実施例の構成説明図である。 FIG. 2 is an explanatory diagram of the configuration of an embodiment of the present invention.

図において、第1図と同一記号は同一機能を示す。In the figure, the same symbols as in FIG. 1 indicate the same functions.

以下、第1図を相違部分のみ説明する。Hereinafter, only the different parts of FIG. 1 will be explained.

13は、ハーフミラ−3がもの光をサーボ用センサ10
とデータ用センサ12に二倍する偏光ビームスプリッタ
である。14はサーボ用センサの信号を増幅するサーボ
アンプで、増幅された信号は、集光レンズ5に取付けら
れた7オカスアク(%−タ15とトラッキングアクチュ
エータ16に送られる。17はデータ用センサ9の信号
を増幅するデータ用プリアンプである。而して、レーザ
ー光源1のレーザー先位、偏光ビームスプリ、り130
反射面に対し、S−偏光方向からΔθ8だけ回転した偏
光方向をもつ平行光で構成されている。
13 is a servo sensor 10 that detects the light from the half mirror 3.
and a polarizing beam splitter that doubles the data sensor 12. 14 is a servo amplifier that amplifies the signal of the servo sensor, and the amplified signal is sent to the tracking actuator 15 and the tracking actuator 16 attached to the condenser lens 5. This is a data preamplifier that amplifies the signal.The laser tip of the laser light source 1, the polarized beam splitter, and the
It is composed of parallel light having a polarization direction rotated by Δθ8 from the S-polarization direction with respect to the reflecting surface.

以上の構成において、レー古源1かものレーザー光は、
ハーフミラ−3を通り集光レンズ5で集光され、光磁気
デスク6に投射される。光磁気ディスク6から反射され
戻って来る光は、光磁気ディスクの磁化の向き(第2図
の左向き、あるいは、右向き)Kよりて、その偏波面は
カー回転内子〇、又は−θK(たとえば0.3°)回転
している。反射光は、ハーフミラ−3で反射され、偏光
ビームスプリッタ13に投射される。偏光ビームスプリ
ッタ13においてはP−偏光は、はとんど透過し、S−
偏光は反射されるので、データ用センサ12にはP−偏
光成分が入射され、サーボ用センサIOKはS−偏光成
分が投射される。レーザー光源1かものレーザー光及び
偏光ビームスプリ、り13へ入射される光の電界方向は
、@3図に示す如くなる。
In the above configuration, the laser beam of Le Kogen 1 is as follows:
The light passes through the half mirror 3, is focused by the condenser lens 5, and is projected onto the magneto-optical desk 6. The light reflected and returned from the magneto-optical disk 6 has a plane of polarization of Kerr rotator 〇 or -θK (for example, 0) depending on the magnetization direction K of the magneto-optical disk (leftward or rightward in FIG. .3°) is rotating. The reflected light is reflected by the half mirror 3 and projected onto the polarizing beam splitter 13. In the polarizing beam splitter 13, most of the P-polarized light is transmitted and the S-polarized light is transmitted.
Since the polarized light is reflected, the P-polarized light component is incident on the data sensor 12, and the S-polarized light component is projected on the servo sensor IOK. The electric field directions of the laser light from the laser light source 1 and the light incident on the polarized beam splitter 13 are as shown in Figure 3.

第3図から分る如く、サーボ用センサ10にはS方向成
分の光が送られ、■カー回転角十〇え、−〇えの違いは
#1とんどなく、■大きな信号が送られる。
As can be seen from Fig. 3, the light of the S direction component is sent to the servo sensor 10, and the difference between the car rotation angles of 10 and -0 is negligible, and ■ a large signal is sent. .

一方、データ用センサ12に社カー回転内子〇え及び−
〇えに対して、その振幅が大きく変化するP方向成分の
光が送られる。サーボ用センサ1oに向う光は、コリメ
ータレンズ8や、シリンドリカルレンズ9を通って、こ
の場合は、多分割センサよりなるサーボ用センサ1oで
受光され、サーボアンプ14で増幅され焦点誤差信号や
トラッキング誤差信号となり、フォカスアクチェエータ
15やトラッキングアクチェエータ16を動作させ、集
光レンズ5を制御する。
On the other hand, the data sensor 12 is connected to the company car rotating inner
In contrast, light of the P-direction component whose amplitude changes greatly is sent. The light directed toward the servo sensor 1o passes through the collimator lens 8 and the cylindrical lens 9, and in this case is received by the servo sensor 1o, which is a multi-segment sensor, and is amplified by the servo amplifier 14 to generate a focus error signal and a tracking error. This becomes a signal, operates the focus actuator 15 and the tracking actuator 16, and controls the condenser lens 5.

以上の結果、■データ用信号とサーボ用信号とが分離し
て得られるので、サーボ信号中にデータ信号が干渉して
くるおそれはない。■而も、サーボ用信号として出力の
大なるものが得られる。■偏光ビームスプリッター13
が用いられているので、検光子を必要とせず、光学系の
構成が簡単になる。
As a result of the above, (1) the data signal and the servo signal are obtained separately, so there is no possibility that the data signal will interfere with the servo signal. (2) Also, a large output can be obtained as a servo signal. ■Polarizing beam splitter 13
Since this is used, an analyzer is not required and the configuration of the optical system is simplified.

■サーボ用信号として、光が分離使用されても、データ
用信号SN比の悪化がないものが得られる。
(2) Even if the light is used separately as a servo signal, a signal without deterioration of the signal-to-noise ratio of the data signal can be obtained.

第4図は本発明の他の実施例の構成説明図である。FIG. 4 is a configuration explanatory diagram of another embodiment of the present invention.

本実施例においては、集光レンズ5を、光磁気デスク6
をLさんで二個設け、透過形の構成としたものである。
In this embodiment, the condenser lens 5 is replaced with the magneto-optical disk 6.
Mr. L installed two of these, and they were configured to be of a transparent type.

なお、前述の実施例においては、レーザー光源1のレー
ザー光の偏光方向をS−偏光方向からΔθ8だけ回転し
た偏光方向を有する平行光で構成されていると説明した
が、レーザー光の偏光方向をP−偏光からΔθSだけ回
転した偏光方向を有する平行光で構成されてもよい。こ
の場合は、偏光ビームスプリッタ−13の透過光をサー
ボ用センサ10に、反射光をデーター用センサ12に投
射するようKすればよい。
In the above embodiment, it was explained that the polarization direction of the laser light from the laser light source 1 is composed of parallel light having a polarization direction rotated by Δθ8 from the S-polarization direction. It may be composed of parallel light having a polarization direction rotated by ΔθS from P-polarized light. In this case, it is sufficient to project the transmitted light of the polarizing beam splitter 13 onto the servo sensor 10 and the reflected light onto the data sensor 12.

また、シー4源1のレーザー光の偏光を、・・−7ミラ
ー3や光磁気ディスク60面に対して、正確にトラ、夕
方向又は半径方向に向け、偏光ビームスプリッタ−13
をこれに対してΔθ8だけ回転させたものであってもよ
い。
In addition, the polarization of the laser beam from the source 1 of the sea 4 is directed accurately toward the direction of the mirror 3 and the magneto-optical disk 60, toward the direction of the sky, or in the radial direction, and the polarizing beam splitter 13
may be rotated by Δθ8 with respect to this.

また、ハーフミラ−70代りに、センナ10.12に向
う光に消光比のやや悪い特性を有する偏光ビームスプリ
ッタ−13を用いてもよく、この場合は、書込時の光効
率の改善、データ用光の効率の改善また、ハーフミラ−
7等のP−偏光波やS−偏光波に対する位相ずれを補正
するために1偏光ビλ −ムスプリッター13に入る光に一板のような位相調整
素子を入れてもよい。
Furthermore, instead of the half mirror 70, a polarizing beam splitter 13 may be used which has a slightly poor extinction ratio for the light directed toward the sensor 10 and 12. Improved light efficiency and half mirror
In order to correct the phase shift with respect to the P-polarized light wave or the S-polarized light wave such as 7, etc., a phase adjustment element such as a plate may be inserted into the light entering the 1-polarized beam λ-splitter 13.

によるトラッキング誤差検出法では、データー用センサ
部10を多分割されたものを用いるととKなる。
In the tracking error detection method according to the above, when the data sensor section 10 is multi-divided, the result is K.

また、偏光子2は、レーザー光源1が半導体レザー等で
、レーザー光自体が偏光性を有するものである場合は、
なくてもよいことは勿論である。
In addition, when the laser light source 1 is a semiconductor laser or the like and the laser light itself has polarization, the polarizer 2 is
Of course, it is not necessary.

〔発明の作用、効果〕[Action and effect of the invention]

以上説明したように、本発明は、光磁気ディスクからの
光をサーボ用センナに向う光とデーター用センサに向う
光とに分離する偏光ビームスプリッタ−を具備し、光源
から光磁気ディスクに投射する光の偏光方向をサーボ用
センサに向う光の偏光方向かられずかに回転させた光磁
気ディスク装置を構成した。
As explained above, the present invention includes a polarizing beam splitter that separates light from a magneto-optical disk into light directed to a servo sensor and light directed to a data sensor, and projects the light from a light source onto the magneto-optical disk. A magneto-optical disk device was constructed in which the polarization direction of light was slightly rotated from the polarization direction of light directed toward a servo sensor.

この結果、■データ用信号とサーボ用信号とが出力の大
なるものが得られる。■偏光ビームスプリ、ターが用い
られているので、検光子を必要とせず、光学系の構造が
簡単になる。■サーボ用信号として、光が分離使用され
てもデータ用信号のSN比の悪化がないものが得られる
As a result, large outputs of data signals and servo signals can be obtained. ■Since a polarized beam splitter is used, an analyzer is not required and the structure of the optical system is simplified. (2) A servo signal that does not deteriorate the S/N ratio of the data signal even if the light is used separately can be obtained.

したがって、本発明によれば、簡潔な光学系の構成によ
り、データ信号と干渉のないサーボ信号が得られ、かつ
、SN比の良好なデータ信号が得られる光磁気ディスク
装置を実現することができる。
Therefore, according to the present invention, it is possible to realize a magneto-optical disk device in which a servo signal that does not interfere with a data signal can be obtained and a data signal with a good S/N ratio can be obtained with a simple optical system configuration. .

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

第1図は従来より一般に使用されている従来例の構成説
明図、第2図り本発明の一実施例の構成説明図、第3図
は第2図の動作説明図、第4図は本発明の他の実施例の
構成説明図である。 1・・・レーザー光源、2・・・偏光子、3・・・ハー
フミラ−14・・・ミラー、5・・−レンズ、6・・・
光磁気デスク、8・・・コリメータレンズ、9・・・シ
リンドリカルレンズ、10・・・サーボ用センサ、12
・・・データ用センサ、13・・・備元ビームスプリッ
タ−114・・・サーボアンプ、15・・・フォカスア
クチュエーター、16・・・トラッキングアクチュエー
ター、17・・・データ用プリアンプ。
Fig. 1 is an explanatory diagram of the configuration of a conventional example commonly used in the past, Fig. 2 is an explanatory diagram of the configuration of an embodiment of the present invention, Fig. 3 is an explanatory diagram of the operation of Fig. 2, and Fig. 4 is an explanatory diagram of the present invention. FIG. 2 is a configuration explanatory diagram of another embodiment of the present invention. DESCRIPTION OF SYMBOLS 1...Laser light source, 2...Polarizer, 3...Half mirror-14...Mirror, 5...-Lens, 6...
Magneto-optical desk, 8... Collimator lens, 9... Cylindrical lens, 10... Servo sensor, 12
... Data sensor, 13... Beam splitter-114... Servo amplifier, 15... Focus actuator, 16... Tracking actuator, 17... Data preamplifier.

Claims (1)

【特許請求の範囲】[Claims] 光源からの偏光が投射される光磁気ディスクと、該光磁
気ディスクからの光をサーボ用センサに向う光とデータ
用センサに向う光とに分離する偏光ビームスプリッタ−
とを具備し、前記光源から前記光磁気ディスクに投射す
る光の偏光方向をサーボ用センサに向う光の偏光方向か
られずかに回転させてなる光磁気ディスク装置。
A magneto-optical disk onto which polarized light from a light source is projected, and a polarizing beam splitter that separates the light from the magneto-optical disk into light directed to a servo sensor and light directed to a data sensor.
A magneto-optical disk device comprising: a magneto-optical disk device in which the direction of polarization of light projected from the light source onto the magneto-optical disk is slightly rotated from the direction of polarization of light directed toward a servo sensor.
JP3371084A 1984-02-24 1984-02-24 Photomagnetic disk device Pending JPS60179959A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3371084A JPS60179959A (en) 1984-02-24 1984-02-24 Photomagnetic disk device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3371084A JPS60179959A (en) 1984-02-24 1984-02-24 Photomagnetic disk device

Publications (1)

Publication Number Publication Date
JPS60179959A true JPS60179959A (en) 1985-09-13

Family

ID=12393962

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3371084A Pending JPS60179959A (en) 1984-02-24 1984-02-24 Photomagnetic disk device

Country Status (1)

Country Link
JP (1) JPS60179959A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6063751A (en) * 1983-09-19 1985-04-12 Olympus Optical Co Ltd Photoelectro-magnetic pickup device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6063751A (en) * 1983-09-19 1985-04-12 Olympus Optical Co Ltd Photoelectro-magnetic pickup device

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