JPH02294942A - Optical memory device - Google Patents

Optical memory device

Info

Publication number
JPH02294942A
JPH02294942A JP1114621A JP11462189A JPH02294942A JP H02294942 A JPH02294942 A JP H02294942A JP 1114621 A JP1114621 A JP 1114621A JP 11462189 A JP11462189 A JP 11462189A JP H02294942 A JPH02294942 A JP H02294942A
Authority
JP
Japan
Prior art keywords
optical system
optical
light
objective lens
mirror
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.)
Granted
Application number
JP1114621A
Other languages
Japanese (ja)
Other versions
JP2745673B2 (en
Inventor
Masatoshi Yonekubo
政敏 米窪
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 JP1114621A priority Critical patent/JP2745673B2/en
Publication of JPH02294942A publication Critical patent/JPH02294942A/en
Priority to US07/842,729 priority patent/US5151890A/en
Application granted granted Critical
Publication of JP2745673B2 publication Critical patent/JP2745673B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Optical Recording Or Reproduction (AREA)
  • Optical Head (AREA)

Abstract

PURPOSE:To reduce optical beam shifting quantity attended with the rotation of a galvanomirror and to stabilize the operation by providing an afocal optical system composed of the two groups of optical systems having the positive refracting power between an objective lens and the galvanomirror. CONSTITUTION:Light emitted from a semiconductor laser 201 is in parallel light by a collimator 202 and transmitted through a prism 204 for servo signal separation. Then, the optical path of the light is bent by a reflecting mirror 205 and bent almost in a seeking direction by a galvanomirror 206. The light passes through the afocal optical system where the light is condensed by a first group optical system 102 and goes to the parallel light again by a second group optical system 103, guided to an objective lens 105 by a reflecting mirror 207 and condensed on an optical storing medium 106. Since the rotational angle of the mirror 206 can be reduced by prolonging the focal distance of the optical system 102 rather than that of the optical system 103, a medium 106 can be rotated at high speed and a distributed optical memory device can be easily manufactured.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、光記憶の分野において分離型の光学系を用い
た光メモリー装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an optical memory device using a separate optical system in the field of optical storage.

〔従来の技術〕[Conventional technology]

従来の光メモリー装置は、ひとつのシャーシにすべての
光学系及びフォーカスアクチュエー夕、トラックアクチ
ュエータを搭載した一体型光ヘツドを用いて、そのすべ
てをシークさせる方法がとられていた。しかしそれては
ムービングマスが大きいために、シークタイムを短くて
きない。この課題を解決するために、対物レンズと反射
鏡フォーカスアクチュエー夕をシークさせ、他の光学系
及びトラッキングアクチュエー夕であるいわゆるガルバ
ノミラーはシークさせない方法の、分離型光学系を有す
る光メモリー装置が考案されている。
Conventional optical memory devices use an integrated optical head in which all optical systems, a focus actuator, and a track actuator are mounted on a single chassis, and seek is performed on all of them. However, since the moving mass is large, the seek time cannot be shortened. In order to solve this problem, an optical memory device has a separate optical system in which the objective lens and the reflector focus actuator are allowed to seek, but the other optical systems and the tracking actuator, so-called galvanometer mirrors, are not allowed to seek. has been devised.

第3図に従来の光メモリー装置光の側面図の例を示す。FIG. 3 shows an example of a side view of a conventional optical memory device.

半導体レーザ201より出射した光はコリメータレンズ
202により乎行光となり、プリズム203、204を
透過し、反射鏡205により光路を曲げられガルハノミ
ラ−206に入射する。光はほぼシー夕方向にそって進
み反射鏡207により光路を曲げられ対物レンズ105
にいたり、光記憶媒体106に集光する。
The light emitted from the semiconductor laser 201 becomes a traveling light by a collimator lens 202, passes through prisms 203 and 204, has its optical path bent by a reflecting mirror 205, and enters a galvano mirror 206. The light travels approximately in the sea and evening direction, and its optical path is bent by the reflecting mirror 207 and passes through the objective lens 105.
The light is focused on the optical storage medium 106.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかしながら、前述の従来技術では、第4図のごとく、
ガルバノミラ−206の回転に伴って、対物レンズ10
5に入射ずる光ビームがシフトするという問題を有して
いる。
However, in the above-mentioned conventional technology, as shown in FIG.
As the galvanometer mirror 206 rotates, the objective lens 10
5 has the problem that the light beam incident on it is shifted.

具体的な弊害としては、下記の項目がある。Specific adverse effects include the following items.

・対物レンズ入射光量が変化し、光記憶媒体上のエネル
ギー密度の精度がわるく、書き込み不良が発生する。
- The amount of light incident on the objective lens changes, the accuracy of the energy density on the optical storage medium deteriorates, and writing errors occur.

・対物レンズ入射光量分布が変化し、 集光スポット形
状が不安定で、読ミ取り不良が発生する。
- The distribution of light incident on the objective lens changes, the shape of the focused spot becomes unstable, and reading errors occur.

・対物レンズによるケラレを生じさせないために、コリ
メート ビーム径を太きくしなければならず、光利用効
率が低下し、高価な高出力半導体レーザを使用しなけれ
ばならない。
- In order to avoid vignetting caused by the objective lens, the diameter of the collimated beam must be increased, which reduces the light utilization efficiency and requires the use of expensive high-power semiconductor lasers.

・第5図の光ビームの断面図ごとく出射光ビーム501
に対する戻り光ビームの位置が、ガルバノミラー初期位
置の場合の502から503のごとく移動し、サーボ信
号検出用センサー上で光ビームが移動し正確なサーボ信
号が得られない。これは特にプッシュプル法によるトラ
ックエラー検出法の場合甚だしい。
- Output light beam 501 as shown in the cross-sectional view of the light beam in Figure 5
The position of the returned light beam moves from 502 in the case of the initial position of the galvano mirror to 503, and the light beam moves on the servo signal detection sensor, making it impossible to obtain an accurate servo signal. This is especially serious in the case of the track error detection method using the push-pull method.

なぜならば光ビームの移動方向504とプッシュプル法
に用いる二分割センサーの分割線505の方向が直交ず
るからてある。
This is because the moving direction 504 of the light beam and the direction of the dividing line 505 of the two-part sensor used in the push-pull method are perpendicular to each other.

そこて本発明は上記のような課題を解決するものて゛あ
り、その目的とするところは、ガルハノミラーの回転に
伴う光ビームシフ1・の量を低減し安定な動作が可能な
光メモリー装置を提供することである。
The present invention is intended to solve the above-mentioned problems, and its purpose is to provide an optical memory device capable of stable operation by reducing the amount of optical beam shift 1 caused by the rotation of the Galhano mirror. That's true.

〔課題を解決するための手段〕[Means to solve the problem]

本発明の光メモリー装置は、対物レンズと、トラッキン
グのために反射鏡を駆動するガルハノミラーを用いた分
離型光学系を有する光メモリー装置において、該対物レ
ンズと該カルハノミラーの間の光路に、正の屈折力を有
しガルバノミラー側に設置した第一群光学系と、正の屈
折力を有し対物レンズ側に設置した第二群光学系とより
なるアフォーカル光学系を設置した事を特徴とする。
The optical memory device of the present invention includes an objective lens and a separate optical system using a Galhano mirror that drives a reflecting mirror for tracking, in which a positive It is characterized by the installation of an afocal optical system consisting of a first group optical system that has refractive power and is installed on the galvano mirror side, and a second group optical system that has positive refractive power and is installed on the objective lens side. do.

〔作用〕[Effect]

本発明におけるアフオーカル光学系の作用は下記のこと
くである。
The effects of the afocal optical system in the present invention are as follows.

第1図に示すごとく、ガルハノミラーにより光軸101
に対してθ1の角度で第一群光学系1o2に入射した光
ビームは、第一群光学系102の焦点距tllflの位
置に一度集光し、そこから第二群光学系103の焦点距
離f2の位置に設置した第二群光学系103にいたる。
As shown in Fig. 1, the optical axis 101 is
The light beam incident on the first group optical system 1o2 at an angle of θ1 with respect to This leads to the second group optical system 103 installed at the position.

この第一群光学系102と第二群光学系103を距離f
l+f2たけ隔てて設置した系が、本発明のアフォーカ
ル光学系である。
This first group optical system 102 and second group optical system 103 are connected at a distance f
The system installed at a distance of l+f2 is the afocal optical system of the present invention.

第二群光学系103からの出射ビームの角度θ2は、 
  θ2−θ1*(fl/f2)て与えられる。この時
主光線104が光軸101と交わる位置に対物レンズ1
05を置けば光ビームシフトは起こらない。実際には、
対物レンズ105はシークに伴い移動するからシークエ
リアの中央が第1図の位置dとなるu 6計すれば、 
光ビームシフトを最も少なくてきる。106は光記憶媒
体である。
The angle θ2 of the output beam from the second group optical system 103 is
It is given by θ2−θ1*(fl/f2). At this time, the objective lens 1 is placed at the position where the principal ray 104 intersects with the optical axis 101.
If 05 is placed, no light beam shift will occur. in fact,
Since the objective lens 105 moves with seeking, the center of the seek area is at position d in Figure 1.
Minimizes optical beam shift. 106 is an optical storage medium.

〔実施例〕〔Example〕

第2図は本発明の実施例の側面図であり、5.25イン
チの光磁気ディスクドライフに応用した例である。
FIG. 2 is a side view of an embodiment of the present invention, which is an example applied to a 5.25-inch magneto-optical disk drive.

半導体レーザ201から出射した光はコリメータ202
により平行光にされ、サーボ信号分離用プリズム203
、光磁気信号分離用プリズム204を透過し反射鏡20
5により光路を曲げられ、ガルハノミラー206によ冫
クほぼシー夕方向にまげられる。光ビームは第一群光学
系102により一度集光され、第二群光学系103によ
り再び平行光となる。その後光ビームは反射鏡207に
より対物レンズ105に導かれ、光記憶媒体106上に
集光される。
The light emitted from the semiconductor laser 201 passes through the collimator 202
The servo signal separation prism 203
, passes through the magneto-optical signal separation prism 204 and passes through the reflecting mirror 20
5, the optical path is bent by the galvano mirror 206, and the light is bent almost in the direction of the sky. The light beam is once condensed by the first group optical system 102, and then becomes parallel light again by the second group optical system 103. The light beam is then guided by a reflecting mirror 207 to the objective lens 105 and focused onto the optical storage medium 106.

ガルハノミラーの回転方向は従来と逆とする。The direction of rotation of the Galhano mirror is opposite to the conventional one.

本実施例における各パラメータは下記のごとくてある。Each parameter in this example is as follows.

第一群光学系焦点距離 17.3mm 第二群光学系焦点距g′li 15.4mm対物レンズ
焦点距離   3mm 対物レンズ開口数    0.55 ガルハノミラーから第一群光学系までの距離4mm 第一群光学系から第二群光学系までの距離32.7mm 第二群光学系からシークエリア中央におれる対物レンズ
までの距離   33mm シークエリア      32mm アフオーカル光学系への大射光ビーム径5mm アフォーカル光学系からの出射光ビーム径4.  45
mm 光スポットを光記憶媒体上で50μm移動させる場合の
各パラメータは下記のごとくである。
First group optical system focal length 17.3mm Second group optical system focal length g'li 15.4mm Objective lens focal length 3mm Objective lens numerical aperture 0.55 Distance from Garhano mirror to first group optical system 4mm First group optical Distance from the system to the second group optical system: 32.7 mm Distance from the second group optical system to the objective lens placed in the center of the seek area: 33 mm Seek area: 32 mm Large light beam diameter to the afocal optical system: 5 mm From the afocal optical system Output light beam diameter 4. 45
mm The parameters for moving the optical spot by 50 μm on the optical storage medium are as follows.

ガルハノミラーの回転角 0.42度 アフォーカル光学系への入射角 0,85度 アフオーカル光学系からの出射角 0.95度 本発明は新たな反射面を用いていないため、偏光特性も
問題なく光磁気記録が行なえた。
Rotation angle of the Galhano mirror: 0.42 degrees Incident angle to the afocal optical system: 0.85 degrees Output angle from the afocal optical system: 0.95 degrees Since the present invention does not use a new reflective surface, the polarization characteristics of the light can be adjusted without any problem. Magnetic recording was possible.

また第一群光学系と第二群光学系をそれぞれ色消しレン
ズにする事により、半導体レーザの波長変化に対応させ
る事ができた。
Furthermore, by using achromatic lenses in each of the first group optical system and the second group optical system, it was possible to adapt to changes in the wavelength of the semiconductor laser.

さらに第一群光学系と第二群光学系の焦点距離の差を積
極的に大きくしてやる事により、ガルノAノミラーの必
要回転量をさらに減らすことも可能である。
Furthermore, by proactively increasing the difference in focal length between the first group optical system and the second group optical system, it is possible to further reduce the required rotation amount of the Garno A mirror.

もちろん本発明は3.5インチ等の光ディスクドライブ
にも応用可能である。
Of course, the present invention can also be applied to 3.5-inch optical disk drives.

〔発明の効果〕〔Effect of the invention〕

従来技術により上記実施例と同等の光メモリー装置を構
成し、光スポットを50μm移動させようとすると、光
ビームは最大1.43mm対物レンズ位置でシフトする
。これは対物レンズの瞳径の43.3%であり、とても
許容できない。
If an optical memory device equivalent to the above embodiment is configured using the conventional technology and an attempt is made to move the optical spot by 50 μm, the optical beam will shift by a maximum of 1.43 mm at the objective lens position. This is 43.3% of the pupil diameter of the objective lens, which is very unacceptable.

これに対して本発明によれば光ビームシフト量は、最大
0 . 2 7 mm、対物レンズ瞳径の8%であって
実に175.3に減少できた。
On the other hand, according to the present invention, the light beam shift amount is at most 0. 27 mm, which is 8% of the objective lens pupil diameter, was actually reduced to 175.3 mm.

さらに本実施例では第一群光学系の焦点距離を第二群光
学系の焦点距離よりも長くして、角倍率を1.12とし
、ガルハノミラーの回転角を11%少なくする事ができ
た。この効果は1寺に光記憶奴体を高速回転させる場合
、ガルハノミラーの設計上有効てある。
Furthermore, in this example, the focal length of the first group optical system was made longer than the focal length of the second group optical system, and the angular magnification was set to 1.12, making it possible to reduce the rotation angle of the Galhano mirror by 11%. This effect is effective in the design of Garhano Mirror when the optical memory body is rotated at high speed in one temple.

また、従来問題であった光記憶媒体上のエネルギー密度
の変動、集光スポット形状の変動、光利用効率の低下、
フォーカスサーボ信号の劣化は実用上問題がなくなった
In addition, conventional problems such as fluctuations in energy density on optical storage media, fluctuations in the shape of the focused spot, and reductions in light utilization efficiency,
Deterioration of the focus servo signal is no longer a practical problem.

従来最も問題であったプッシュプル法によるトラックエ
ラー信号の劣化も、従来から行なわれているミラーホー
ルド法による補正、あるいはメガネ型センサーと組み合
わせることにより十分に良質の信号かえられた。
The deterioration of the track error signal caused by the push-pull method, which has been the most problematic conventional method, has been corrected by the conventional mirror hold method, or by combining it with a glasses-type sensor, the signal can be returned to a sufficiently high quality.

このように本発明は、従来製造困難であった分離型光メ
モリー装置を製造可能とする大変重要な発明であって、
コンピュターの外部記憶装置の発展、特に高速化におお
いに貢献するものである。
As described above, the present invention is a very important invention that makes it possible to manufacture a separate optical memory device, which has been difficult to manufacture in the past.
It greatly contributed to the development of external storage devices for computers, especially to speeding them up.

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

第1図は本発明の原理説明図 第2図は本発明の実施例の側面図 第3図は従来の光メモリー装置の側面図第4図は従来の
光メモリー装置の説明図第5図は従来の光メモリー装置
の光ビーム断面図 1 0 1 ・ 102  ・ 103  ・ 1 0 4 ・ 105  ・ 106  ・ 201  ・ 20 2 ・ 203  ・ 2 0 4 ・ 2 0 5、 2 0 6 ・ 光軸 第一群光学系 第二群光学系 主光線 対物レンズ 光記億媒体 半導体レーザ コリメータレンズ サーボ信号分離用プリズム 光磁気信号分離用プリズム 7・・・反射鏡 ガルバノミラー 以上 出願人 セイコーエプソン林式会社 代理人 弁理士 鈴木喜三郎 他1名 菫 十 図
FIG. 1 is an explanatory diagram of the principle of the present invention. FIG. 2 is a side view of an embodiment of the present invention. FIG. 3 is a side view of a conventional optical memory device. FIG. 4 is an explanatory diagram of a conventional optical memory device. Cross-sectional view of light beams of conventional optical memory device Optical system Second group Optical system Principal ray Objective lens Optical storage medium Semiconductor laser Collimator Lens Servo signal separation prism Optical magnetic signal separation prism 7...Reflector Galvano mirror Above Applicant Seiko Epson Hayashi Shiki Company agent Patent attorney Kisaburo Suzuki and 1 other person

Claims (1)

【特許請求の範囲】[Claims] 対物レンズと、トラッキングのために反射鏡を駆動する
ガルバノミラーを用いた分離型光学系を有する光メモリ
ー装置において、該対物レンズと該ガルバノミラーの間
の光路に、正の屈折力を有しガルバノミラー側に設置し
た第一群光学系と、正の屈折力を有し対物レンズ側に設
置した第二群光学系とよりなるアフォーカル光学系を設
置した事を特徴とする光メモリー装置。
In an optical memory device having a separate optical system using an objective lens and a galvano mirror that drives a reflecting mirror for tracking, a galvano mirror with positive refractive power is provided in the optical path between the objective lens and the galvano mirror. An optical memory device comprising an afocal optical system consisting of a first group optical system installed on the mirror side and a second group optical system having positive refractive power and installed on the objective lens side.
JP1114621A 1989-05-08 1989-05-08 Optical memory device Expired - Lifetime JP2745673B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP1114621A JP2745673B2 (en) 1989-05-08 1989-05-08 Optical memory device
US07/842,729 US5151890A (en) 1989-05-08 1992-02-26 Optical system for optical memory device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1114621A JP2745673B2 (en) 1989-05-08 1989-05-08 Optical memory device

Publications (2)

Publication Number Publication Date
JPH02294942A true JPH02294942A (en) 1990-12-05
JP2745673B2 JP2745673B2 (en) 1998-04-28

Family

ID=14642441

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1114621A Expired - Lifetime JP2745673B2 (en) 1989-05-08 1989-05-08 Optical memory device

Country Status (1)

Country Link
JP (1) JP2745673B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2683932A1 (en) * 1991-11-19 1993-05-21 Atg Sa DEVICE FOR ACCESSING AND TRACKING TRACKS FOR OPTICAL DISC.
JPH05258329A (en) * 1992-01-21 1993-10-08 Internatl Business Mach Corp <Ibm> Optical data storage device
US7295722B2 (en) 2003-06-02 2007-11-13 Seiko Epson Corporation Scanning device, laser projector, and optical device

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50120358A (en) * 1974-03-04 1975-09-20
JPS57189145U (en) * 1981-05-27 1982-12-01

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50120358A (en) * 1974-03-04 1975-09-20
JPS57189145U (en) * 1981-05-27 1982-12-01

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2683932A1 (en) * 1991-11-19 1993-05-21 Atg Sa DEVICE FOR ACCESSING AND TRACKING TRACKS FOR OPTICAL DISC.
US5420840A (en) * 1991-11-19 1995-05-30 Art Tech Gigadisc "Atg" Separation type mono block optical head with tracking control achieved by a moveable mirror
JPH05258329A (en) * 1992-01-21 1993-10-08 Internatl Business Mach Corp <Ibm> Optical data storage device
US7295722B2 (en) 2003-06-02 2007-11-13 Seiko Epson Corporation Scanning device, laser projector, and optical device

Also Published As

Publication number Publication date
JP2745673B2 (en) 1998-04-28

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