JPH0636497Y2 - Optical system device - Google Patents
Optical system deviceInfo
- Publication number
- JPH0636497Y2 JPH0636497Y2 JP10560185U JP10560185U JPH0636497Y2 JP H0636497 Y2 JPH0636497 Y2 JP H0636497Y2 JP 10560185 U JP10560185 U JP 10560185U JP 10560185 U JP10560185 U JP 10560185U JP H0636497 Y2 JPH0636497 Y2 JP H0636497Y2
- Authority
- JP
- Japan
- Prior art keywords
- light
- optical system
- shielding
- system device
- objective lens
- 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
Links
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- Optical Recording Or Reproduction (AREA)
Description
【考案の詳細な説明】 (利用分野) 本考案はコンパクトディスク再生装置等、ディスクより
光学的に情報を読出す光学系装置に関する。DETAILED DESCRIPTION OF THE INVENTION (Field of Use) The present invention relates to an optical system device such as a compact disc reproducing device for optically reading information from a disc.
(従来の技術) 従来の光源からの1本の光束を回折格子によって回折光
を生じせしめ、その中の0次とその両側の±1次回折光
を取り出し、該3本の回折光束(ビーム)をディスク等
の記録媒体上にビームスポットの中心を結ぶ線がトラッ
ク方向に対して微小なオフセット角を持つように対物レ
ンズを介して収束せしめ、HF信号を読み出す0次の主光
束の前後に配される±1次光束の副光束の光量差によっ
て、主光束スポットのトラッキング状態を判別する3ビ
ーム法と呼ばれるトラッキング制御方式が周知である。(Prior Art) One light flux from a conventional light source is caused to generate diffracted light by a diffraction grating, and the 0th order and ± 1st order diffracted light on both sides thereof are extracted, and the three diffracted light fluxes (beams) are extracted. A line connecting the centers of beam spots on a recording medium such as a disk is converged through an objective lens so that it has a minute offset angle with respect to the track direction, and is arranged before and after the 0th-order main light flux for reading out an HF signal. A tracking control method called a three-beam method is known in which the tracking state of the main light beam spot is determined by the difference in the light amount of the sub-light beams of the ± first-order light beams.
上述の3ビーム法とは第3図の如く記録ピット(P)列
から成るトラックTnに対して収束される主光束のスポッ
トS1の前後に副光束のスポットS2,S3が位置した状態
で、且つ記録情報目的トラックTnの中心から副スポット
S2,S3が互いに反対方向に(隣接する記録トラックTn−
1、Tn+1に近づく方向)外れるように調整され、記録
ディスク上には光束のスポット列が上記目的トラックTn
に対して略1度、あるいはそれ以下の所定のオフセット
角を持つように一列に並んで焦点を結んでいる。The above-mentioned three-beam method is a state in which the sub-beam spots S2 and S3 are positioned before and after the main beam spot S1 converged on the track Tn composed of the recording pit (P) row as shown in FIG. Recorded information Target track Sub spot from center of track Tn
S2 and S3 are in opposite directions (adjacent recording tracks Tn-
1, the direction of approaching Tn + 1) is adjusted so that the spots of the light flux on the recording disk are the target track Tn.
The focal points are aligned in a line so as to have a predetermined offset angle of about 1 degree or less.
しかし光学系小型化を目的として有限収束系(光源から
の発散光路中にビームスプリッタやハーフミラー等の光
路分離手段を設けた光学系)を利用すると0次と±1次
を各々受光する検出器間でクロストークが発生しやすい
という欠点があった。However, if a finite converging system (an optical system in which an optical path separating means such as a beam splitter or a half mirror is provided in the divergent optical path from the light source) is used for the purpose of downsizing the optical system, a detector that receives 0th order and ± 1st order respectively There was a drawback that crosstalk was likely to occur between the two.
また焦点制御のため所謂非点収差法を使用する場合は、
本出願人による特願昭59-166415号で提案しているよう
に、光束列方向に周縁を遮光すれば、光束が非点収差に
よって90°捩れるのを利用してクロストークを防止する
ことができる。When using the so-called astigmatism method for focus control,
As proposed in Japanese Patent Application No. 59-166415 by the present applicant, if the peripheral edge is shielded in the direction of the light flux, the light flux is twisted by 90 ° due to astigmatism to prevent crosstalk. You can
しかしながらトラッキング制御が光学系一体駆動型でな
く、対物レンズ単体を駆動する場合にはトラッキングに
従って返光の光軸が移動し、(移動量は±0.3〜0.4mm)
遮光量の変動が大であること、また、有限収束系では従
来のファーフィールド中での遮光場所では平行光ではな
く収束光となるため、光束径が小さくなり、遮光量の調
整が容易でないという欠点がある。However, when the tracking control is not of the optical system integrated drive type and the objective lens alone is driven, the optical axis of the returned light moves according to the tracking (the amount of movement is ± 0.3 to 0.4 mm).
It is said that the fluctuation of the light shielding amount is large, and that in the finite focusing system, since the light is convergent light instead of parallel light at the light shielding place in the conventional far field, the light beam diameter is small and it is not easy to adjust the light shielding amount. There are drawbacks.
即ち光束周縁を平行に遮光する場合、平行光の反射光束
径(直径)6mmに対しては光束端からの距離が0.6〜0.8m
m程度であるのに比較して収束光の場合は、光束径2mm程
度になり、光束端距離は0.2〜0.3mm程度となる。That is, when the peripheral edge of the light flux is shielded in parallel, the distance from the light flux end is 0.6 to 0.8 m for a reflected light flux diameter (diameter) of parallel light of 6 mm.
In the case of convergent light as compared with about m, the beam diameter is about 2 mm, and the beam end distance is about 0.2 to 0.3 mm.
(考案の目的) 信号検出特性に優れ、クロストークを防止して小型化に
適する光学系装置を提供するものである。(Purpose of the Invention) To provide an optical system device which has excellent signal detection characteristics, prevents crosstalk, and is suitable for downsizing.
(考案の概要) コリメータレンズと対物レンズ間の光路を遮光の対象と
するものである。(Outline of the Invention) The optical path between the collimator lens and the objective lens is to be shielded.
(実施例) 以下図面に従って実施例を説明する。(Examples) Examples will be described below with reference to the drawings.
第1図において光源(1)からの発散光は回折格子
(2)を介し、0次回折光束と±1次回折光束が取り出
され、ハーフミラー(3)を介し、平行光にするための
コリメータレンズ(4)、ミラー(5)、対物レンズ
(6)を経てディスク(7)に照射される。In FIG. 1, the divergent light from the light source (1) is extracted through a diffraction grating (2) into a 0th-order diffracted light beam and a ± 1st-order diffracted light beam, and a collimator for converting the light into parallel light through a half mirror (3). The disk (7) is irradiated through the lens (4), the mirror (5) and the objective lens (6).
ディスク(7)からの反射光は対物レンズ(6)、ミラ
ー(5)、コリメータレンズ(4)、ハーフミラー
(3)を介し、発散光と分離され、凹レンズ(9)、シ
リンダレンズ(10)を経て検出器(11)に導かれる。The reflected light from the disk (7) is separated from the divergent light through the objective lens (6), the mirror (5), the collimator lens (4) and the half mirror (3), and the concave lens (9) and the cylinder lens (10). It is led to the detector (11) via.
フォーカス、トラッキング検出法については非点収差
法、3ビーム法等周知の方法を用いれば良い。再生信号
は0次光から得る。A well-known method such as an astigmatism method or a three-beam method may be used for the focus and tracking detection methods. The reproduction signal is obtained from the 0th order light.
ディスク(7)上の収束状態は前述第3図の如くとな
る。The converged state on the disk (7) is as shown in FIG.
遮蔽については光束の両周縁を0次、±1次光束の回折
方向に沿って、換言すればディスク上のスポット列の方
向に沿って行われる。The shielding is performed along both edges of the light beam along the diffraction directions of the 0th and ± 1st order light beams, in other words, along the direction of the spot array on the disc.
第2図に遮蔽板(8)の配置を示す。可動部(20)に対
物レンズ(6)と共にマウントされ、磁気回路(21)、
駆動コイル(22)をして図示方向に一体的に駆動され
る。ピット進行方向は紙面垂直方向となる。FIG. 2 shows the arrangement of the shielding plate (8). Mounted together with the objective lens (6) on the movable part (20), the magnetic circuit (21),
A driving coil (22) is used to drive the coil in the illustrated direction. The pit traveling direction is perpendicular to the paper surface.
非点収差用のシリンダレンズ(10)通過後の光束は第4
図の如く状態で受光される。The light flux after passing through the cylinder lens (10) for astigmatism is the fourth
Light is received in the state as shown in the figure.
即ち、主光束L1、副光束L2,L3は検出器(11)の各検出
器(52),(51),(53)に結像される。That is, the main light flux L1 and the sub-light fluxes L2, L3 are imaged on the detectors (52), (51), (53) of the detector (11).
この際、仮想線Cは丁度遮蔽板(8)の遮蔽方向と位置
を示し、略円形のスポットに於て、仮想線Cよりも外側
の部分は受光されない。At this time, the imaginary line C just indicates the shielding direction and position of the shielding plate (8), and in the substantially circular spot, the portion outside the imaginary line C is not received.
即ち遮蔽方向は隣接する検出器側に近い受光部分を遮光
することに一致し、相互光束漏れによるクロストークは
激減する。That is, the shielding direction corresponds to shielding the light receiving portion close to the adjacent detector side, and the crosstalk due to the mutual light flux leakage is drastically reduced.
なお遮蔽板(8)については、金属板等により完全に遮
光する構成でも良く、ハーフミラー等により実質的に周
縁光を検出器外に落とす構成でも良い。The shielding plate (8) may be configured to completely shield the light with a metal plate or the like, or may be configured to substantially drop the peripheral light to the outside of the detector with a half mirror or the like.
(考案の効果) 以上述べたように本考案によれば有限収束系の収束光路
内に遮光板を置かなくても良いので、遮光量調整が容易
であり、小型化に適する。(Effect of the Invention) As described above, according to the present invention, since it is not necessary to place the light shielding plate in the convergent optical path of the finite converging system, it is easy to adjust the light shielding amount and suitable for downsizing.
また、有限収束系で3ビーム法を採用する場合の検出器
上でのクロストークが防止できる。Moreover, crosstalk on the detector can be prevented when the three-beam method is adopted in the finite focusing system.
以上の効果を有する。It has the above effects.
第1図は実施例光学系の配置図、第2図は実施例要部構
成図、第3図は3ビーム法を説明するための図、第4図
は遮蔽方向の説明図である。 符号の説明 1……光源、2……回折格子 3……ハーフミラー、4……コリメータレンズ 5……ミラー、6……対物レンズ 7……ディスク、8……遮蔽板 11……検出器FIG. 1 is a layout diagram of an optical system of an embodiment, FIG. 2 is a configuration diagram of essential parts of the embodiment, FIG. 3 is a diagram for explaining a three-beam method, and FIG. 4 is an explanatory diagram of a shielding direction. Explanation of reference numerals 1 ... Light source, 2 ... Diffraction grating 3 ... Half mirror, 4 ... Collimator lens 5 ... Mirror, 6 ... Objective lens 7 ... Disk, 8 ... Shielding plate 11 ... Detector
Claims (1)
射させて複数のビームを発生させた後、ハーフミラーお
よびコリメータレンズを介して対物レンズによりディス
クの情報トラック上にほぼ直線的に並んだ3つのビーム
スポットとして照射し、その反射光を前記ハーフミラー
により取り出して光検出器に導き再生信号等を検出する
ようにした光学系装置において、 前記コリメータレンズと前記対物レンズの間の光路中に
光束周縁部を遮蔽する遮蔽板を設けたことを特徴とする
光学系装置。1. A divergent light beam emitted from a light source is made incident on a diffraction grating to generate a plurality of beams, and then an objective lens is arranged through a half mirror and a collimator lens to arrange the information tracks on a disk substantially linearly. In the optical system device, which irradiates three beam spots, reflects the reflected light through the half mirror and guides it to a photodetector to detect a reproduction signal or the like, in an optical path between the collimator lens and the objective lens. An optical system device characterized in that a shielding plate for shielding the peripheral portion of the light flux is provided in the optical system.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10560185U JPH0636497Y2 (en) | 1985-07-12 | 1985-07-12 | Optical system device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10560185U JPH0636497Y2 (en) | 1985-07-12 | 1985-07-12 | Optical system device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6215120U JPS6215120U (en) | 1987-01-29 |
JPH0636497Y2 true JPH0636497Y2 (en) | 1994-09-21 |
Family
ID=30980185
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP10560185U Expired - Lifetime JPH0636497Y2 (en) | 1985-07-12 | 1985-07-12 | Optical system device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0636497Y2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2535013Y2 (en) * | 1992-03-18 | 1997-05-07 | 川崎重工業株式会社 | Variable pitch propeller changing device and shaft connection structure |
-
1985
- 1985-07-12 JP JP10560185U patent/JPH0636497Y2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPS6215120U (en) | 1987-01-29 |
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