JPS6342040A - Optical head - Google Patents

Optical head

Info

Publication number
JPS6342040A
JPS6342040A JP18557486A JP18557486A JPS6342040A JP S6342040 A JPS6342040 A JP S6342040A JP 18557486 A JP18557486 A JP 18557486A JP 18557486 A JP18557486 A JP 18557486A JP S6342040 A JPS6342040 A JP S6342040A
Authority
JP
Japan
Prior art keywords
signal
magneto
tracking
focusing
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
JP18557486A
Other languages
Japanese (ja)
Inventor
Shigeru Kogure
小暮 茂
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson 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 Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP18557486A priority Critical patent/JPS6342040A/en
Publication of JPS6342040A publication Critical patent/JPS6342040A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To improve the S/N of an RF signal to increase the recording density and to reduce a read error by obtaining servo signals for focusing and tracking from the light reflected from a recording medium. CONSTITUTION:The output light of a semiconductor laser 1 is converted to parallel rays by a collimator lens 3 and is transmitted through a beam splitter 4 and is turned orthogonally by a mirror and is condensed on a magneto-optical disk 7 by an objective lens 6. The RF signal is obtained from the light transmitted through the disk by an analyzer 8 and a 4-divided PTN photodiode 9. The light reflected on the magneto-optical disk 7 passes a reverse path, and servo signals are obtained by a knife edge 10, a lens 11, and a PIN photodiode. The knife edge method is used for focusing, and the push-pull method is used for tracking. Since the differential detection method is used in the transmission-side optical system in such a manner, the S/N of a reproduced signal is improved to increase the recording density, and the read error is reduced.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、逃過型元ヘッドの構造に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to the structure of an escape type original head.

〔従来の技術〕[Conventional technology]

近年活発に実用化され、徐々に普及しつつある元ディス
ク装置においては、光ヘッドは記録再生を行う重要な要
素である1元ヘッドには記録媒体の反射光からRF倍信
号得る反射型光ヘッドと透過光から得る透過型光ヘッド
がある。透過型光ヘッドの従来例としては、グロシーデ
ィングズ、オプ、ニス・ピー拳アイ・イー(PROOF
!KD工NGS  OIF  5PIF1i)、382
巻、240〜244頁、1983年に記載されているも
のがある。これは光磁気記録用元ヘッドで、その構成図
を第3図に示す、半導体レーザ100の出力光をコリメ
ートレンズ101.対物レンズ102を用いて光磁気デ
ィスク103の上に集光する。透過光を検光子104を
通して4分割フォトダイオード105により受光し、サ
ーボ信号、RF倍信号得る構成となっている。106は
バイアス磁場を印加するだめの電磁石である。
In the original disk drive, which has been actively put into practical use in recent years and is gradually becoming popular, the optical head is an important element for recording and reproducing.The single head is a reflective optical head that obtains an RF multiplied signal from the reflected light of the recording medium. There is also a transmission type optical head that obtains light from transmitted light. Conventional examples of transmissive optical heads include PROOF, PROOF
! KD Engineering NGS OIF 5PIF1i), 382
Vol., pp. 240-244, 1983. This is a source head for magneto-optical recording, the configuration of which is shown in FIG. The objective lens 102 is used to focus the light onto the magneto-optical disk 103 . The transmitted light passes through an analyzer 104 and is received by a 4-split photodiode 105 to obtain a servo signal and an RF multiplied signal. 106 is an electromagnet for applying a bias magnetic field.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかし、前述の従来例では次のような問題点がある。即
ち、1つのセンサーでサーボ信号とR7信号を得るため
にRIF信号再生時に差動検出法を使えないことである
。第4図に差動検出系の例を示す、光磁気ディスク10
3を透過した光はレンズ107により概ね平行光とされ
、偏光ビームスプリッタ108により2分岐され、2つ
の光検出器109,110の出力を差動増幅器111に
より差をとり、R1’信号が得られる。第5図は簡略化
した差動検出法の例である。112は透過光の偏光面方
向を示す、透過光を検光子113を通し4分割光検出器
により受光する。113’、114′は検光子113.
4分割光検出器114を真上から見た図である。4分割
光検出器の出力の対角和を差動増幅器111により差を
とりRIF信号が得られる。尚、検光子113′の斜線
は透過軸の方向を示す。いずれの差動検出法においても
、レーザ雑音等の同相雑音が除去可能であり、R?倍信
号S / N比が数df3向上する。前述の従来例では
、この方法が採れないため、記録密度を上げられないと
か、再生信号の読み取シ誤りが生じ易くなる。
However, the conventional example described above has the following problems. That is, since the servo signal and the R7 signal are obtained using one sensor, the differential detection method cannot be used when reproducing the RIF signal. FIG. 4 shows an example of a differential detection system, a magneto-optical disk 10.
The light that has passed through 3 is made almost parallel by a lens 107, split into two by a polarizing beam splitter 108, and the difference between the outputs of the two photodetectors 109 and 110 is taken by a differential amplifier 111 to obtain an R1' signal. . FIG. 5 is an example of a simplified differential detection method. Reference numeral 112 indicates the direction of the polarization plane of the transmitted light, and the transmitted light is passed through an analyzer 113 and received by a four-split photodetector. 113' and 114' are analyzers 113.
4 is a diagram of the four-split photodetector 114 viewed from directly above. FIG. A differential amplifier 111 takes the difference between the diagonal sums of the outputs of the four-split photodetectors to obtain an RIF signal. Note that the diagonal line on the analyzer 113' indicates the direction of the transmission axis. In either differential detection method, common mode noise such as laser noise can be removed, and R? The signal S/N ratio is improved by several df3. In the conventional example described above, since this method cannot be adopted, the recording density cannot be increased, and errors in reading the reproduced signal are likely to occur.

そこで本発明はこのような問題点を解決するもので、R
IF信号のS / N比が高く、高記録密度を達成でき
、読み取り誤りを減少させることのできる透過型光ヘッ
ドを提供することである。
Therefore, the present invention is intended to solve such problems.
It is an object of the present invention to provide a transmissive optical head that has a high S/N ratio of an IF signal, can achieve high recording density, and can reduce reading errors.

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

本発明になる元ヘッドは、記録媒体を透過した光からR
?倍信号再生する光ヘッドにおいて、α)7オーカシン
グ、トラックキングのためのサーボ信号を記録媒体によ
り反射された光から得ることと、 b)入射側光学系と透過側光学系をトラックキング方向
とフォーカシング方向へ一体駆動させるアクチュエータ
を備えていることを特徴とする。
The original head according to the present invention has an R
? In an optical head that reproduces double signals, α) servo signals for 7-focusing and tracking are obtained from the light reflected by the recording medium, and b) the incident side optical system and the transmission side optical system are aligned in the tracking direction and focusing. It is characterized by being equipped with an actuator that integrally drives it in the direction.

〔作用〕[Effect]

本発明の上記の構成によれば1.R?信号再生用センサ
ーとサーボ信号用センサーが異なるため差動検出法を使
うことができ、R?倍信号S/N比が向上する。
According to the above configuration of the present invention, 1. R? Since the sensor for signal reproduction and the sensor for servo signal are different, differential detection method can be used, and R? Double signal S/N ratio is improved.

〔実施例〕〔Example〕

第1図は、本実施例のアクチュエータを除く光学系の構
成図である。本実施例は光磁気ディスク用の元ヘッドで
ある。光学系を説明する。半導体レーザ1の出力光をコ
リメートレンズ3により平行光とし、ビームスプリッタ
4を透過させた後、ミラーで光路を直角に曲げて対物レ
ンズ6により光磁気ディスク7の上に集光する。これを
透過した光は検光子8.4分割Pl”Nフォトダイオー
ド9によりR?倍信号得られる。尚、透過側光学系は第
5図に示されているものである。光磁気ディスク7で反
射された光は、逆経路をたどりナイフェツジ10.レン
ズ11.4分割P工Nフォトダイオードによりサーボ信
号が得られる。本実施例では、フォーカシングはナイフ
ェツジ法、トラッキングはプッシユ・プル法で行ってい
る。尚、ナイフェツジ10.レンズ11.4分割P工N
フォトダイオード12は実際には紙面に垂直な側に配置
されており、より薄をヘッドになっている本実施例の如
く、透過側光学系において第5図に示された差動検出法
が使用できるため、再生信号のS/N比が向上し、記録
密度が向上し、読み取り誤りが減少する。
FIG. 1 is a configuration diagram of the optical system excluding the actuator of this embodiment. This embodiment is an original head for a magneto-optical disk. The optical system will be explained. The output light of the semiconductor laser 1 is made into parallel light by a collimator lens 3, transmitted through a beam splitter 4, the optical path is bent at right angles by a mirror, and the light is focused onto a magneto-optical disk 7 by an objective lens 6. The light transmitted through this is subjected to an analyzer 8.4-divided Pl''N photodiode 9 to obtain an R? times signal.The optical system on the transmission side is shown in FIG. The reflected light follows the reverse path and a servo signal is obtained by the Naifetsu 10. Lens 11. 4-split P/N photodiode.In this example, focusing is performed by the Naifetsu method and tracking is performed by the push-pull method. .In addition, Naifetsuji 10. Lens 11. 4 division P work N
The photodiode 12 is actually placed on the side perpendicular to the plane of the paper, and the differential detection method shown in FIG. 5 is used in the transmission side optical system, as in this embodiment, which has a thinner head. As a result, the S/N ratio of the reproduced signal is improved, the recording density is improved, and reading errors are reduced.

第2図(α)、(b)は、トラッキング及びフォーカシ
ングを行うためのアクチュエータの構成図を示す、14
は光磁気ディスク、15は第1図の光学系の部分である
。16は7オーカシング用の板バネであり、17は磁石
である。19はトラッキング用の板バネであり、18は
磁石である。
FIGS. 2(α) and (b) show a configuration diagram of an actuator for tracking and focusing, 14
1 is a magneto-optical disk, and 15 is the optical system shown in FIG. 16 is a leaf spring for 7 orcasing, and 17 is a magnet. 19 is a leaf spring for tracking, and 18 is a magnet.

磁石17.18には凹部が設けられており、その中に電
磁コイルが配置されている。電磁コイルに電流を流すこ
とにより磁石17.18との間に引力9反発力が作用し
、光学系15がフォーカシング方向、トラッキング方向
に駆動される。このアクチェエータを含めた光学系は、
リニアモータもしくはスピップモータ等の上に載置され
て、トラッキングに関して2段す−ボ方式(又は、2段
アクセス方式)がとられることがある。
The magnets 17, 18 are provided with a recess in which an electromagnetic coil is arranged. By passing a current through the electromagnetic coil, attractive force 9 and repulsive force act between the electromagnetic coil and the magnets 17 and 18, and the optical system 15 is driven in the focusing direction and the tracking direction. The optical system including this actuator is
It may be placed on a linear motor, a spin motor, or the like, and a two-stage turbo system (or two-stage access system) may be used for tracking.

〔発明の効果〕 以上述べたように本発明によれば、差動検出法が採用で
きろためR?倍信号S / N比が向上する。その結果
、記録波長を短くすることができ、記録密度を向上させ
ることができる。更にノイズジッタが減少するため読み
取シ誤りが減少オ・ろと一つ効果がある。
[Effects of the Invention] As described above, according to the present invention, since the differential detection method can be adopted, R? Double signal S/N ratio is improved. As a result, the recording wavelength can be shortened and the recording density can be improved. Furthermore, since noise jitter is reduced, reading errors are reduced, which has one effect.

本発明は上記実施例に限定されることなく、幾多の変更
を加えうろことは勿論である1例えば、記録媒体は光磁
気記録媒体でなくてもよく、形状もディスク形でなくカ
ード形でもよい。
It goes without saying that the present invention is not limited to the embodiments described above, and may be modified in many ways. For example, the recording medium may not be a magneto-optical recording medium, and the shape may be card-shaped instead of disk-shaped. .

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

第1図は、本発明の実施例の光学系構成図。 第2図(α>、Cb>は、本発明の実施例のアクチュエ
ータ構成図。 @3図は、従来の透過型光ヘッドの構成図。 第4図は、差動検出系の構成図。 第5図は、簡略化した差動検出系の構成図。 1・・・・・・・・・半導体レーザ 2・・・・・・・・・偏波面 3・・・・・・・・・コリメートレンズ4・・・・・・
・・・ビームスプリッタ5・・・・・・・・・ミラー 6・・・・・・・・・対物レンズ 7・・・・・・・・・光磁気ディスク 8・・・・・・・・・検光子 9・・・・・・・・・4分割P工Nフォトダイオード1
0・・・・・・ナイフェツジ 11・・・・・・レンズ 12・・・・・・4分割P工N7オトダイオード13・
・・・・・バイアス磁場用電磁石14・・・・・・光磁
気ディスク 15・・・・・・光学系 16・・・・・・板バネ 17.18・・・・・・磁 石 19・・・・・・板バネ 100・・・半導体レーザ 101・・・コリメートレンズ 102・・・対物レンズ 103・・・光磁気ディスク 104・・・検光子 105・・・4分割フォトダイオード 106・・・バイアス磁場用電磁石 107・・・レンズ 108・・・偏光ビームスプリッタ 109・・・光検出器 110・・・光検出器 111・・・差動増幅器 112・・・偏光面 113・・・検光子 113′・・・検光子を上から見た図 114・・・・・・4分割光検出器 114′・・・4分割光検出器を上から見た図9 : 
今分官=JPIN7オトデイオード+2:4/7I言り
PIN7* トダイオードンλ 第1図 笛3図
FIG. 1 is a configuration diagram of an optical system according to an embodiment of the present invention. Figure 2 (α>, Cb> is a configuration diagram of an actuator according to an embodiment of the present invention. Figure 3 is a configuration diagram of a conventional transmissive optical head. Figure 4 is a configuration diagram of a differential detection system. Figure 5 is a simplified configuration diagram of the differential detection system. 1... Semiconductor laser 2... Polarization plane 3... Collimation Lens 4...
...Beam splitter 5...Mirror 6...Objective lens 7...Magneto-optical disk 8...・Analyzer 9・・・・・・4 division P N photodiode 1
0... Naifetsuji 11... Lens 12... 4-split P engineering N7 Otodiode 13.
...Bias magnetic field electromagnet 14...Magneto-optical disk 15...Optical system 16...Plate spring 17.18...Magnet 19. . . . Leaf spring 100 . . . Semiconductor laser 101 . Bias magnetic field electromagnet 107...Lens 108...Polarizing beam splitter 109...Photodetector 110...Photodetector 111...Differential amplifier 112...Polarization plane 113...Analyzer 113 '...Figure 114 when the analyzer is viewed from above...Four-split photodetector 114'...Figure 9 when the four-split photodetector is viewed from above:
Ima Branch = JPIN7 Otodayode+2:4/7I PIN7* Todaiodeonλ Figure 1 Flute Figure 3

Claims (2)

【特許請求の範囲】[Claims] (1)記録媒体を透過した光からRF信号を再生する透
過型光ヘッドにおいて、 a)フォーカシング、トラッキングのためのサーボ信号
を前記記録媒体により反射された光から得ることと、 b)入射側光学系と透過側光学系をトラッキング方向と
フォーカシング方向へ一体駆動させるアクチュエータを
備えていることを特徴とする光ヘッド。
(1) In a transmissive optical head that reproduces an RF signal from light transmitted through a recording medium, a) servo signals for focusing and tracking are obtained from light reflected by the recording medium, and b) incident side optics. An optical head comprising an actuator that integrally drives the system and the transmission side optical system in the tracking direction and the focusing direction.
(2)前記記録媒体が光磁気記録媒体であることを特徴
とする特許請求の範囲第1項記載の光ヘッド。
(2) The optical head according to claim 1, wherein the recording medium is a magneto-optical recording medium.
JP18557486A 1986-08-07 1986-08-07 Optical head Pending JPS6342040A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18557486A JPS6342040A (en) 1986-08-07 1986-08-07 Optical head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18557486A JPS6342040A (en) 1986-08-07 1986-08-07 Optical head

Publications (1)

Publication Number Publication Date
JPS6342040A true JPS6342040A (en) 1988-02-23

Family

ID=16173189

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18557486A Pending JPS6342040A (en) 1986-08-07 1986-08-07 Optical head

Country Status (1)

Country Link
JP (1) JPS6342040A (en)

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