JPS5817550A - Adjusting mechanism for optical head - Google Patents
Adjusting mechanism for optical headInfo
- Publication number
- JPS5817550A JPS5817550A JP11528781A JP11528781A JPS5817550A JP S5817550 A JPS5817550 A JP S5817550A JP 11528781 A JP11528781 A JP 11528781A JP 11528781 A JP11528781 A JP 11528781A JP S5817550 A JPS5817550 A JP S5817550A
- Authority
- JP
- Japan
- Prior art keywords
- light
- prisms
- optical head
- photodetector
- optical system
- 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
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/12—Heads, e.g. forming of the optical beam spot or modulation of the optical beam
- G11B7/135—Means for guiding the beam from the source to the record carrier or from the record carrier to the detector
- G11B7/1359—Single prisms
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/08—Disposition or mounting of heads or light sources relatively to record carriers
- G11B7/09—Disposition or mounting of heads or light sources relatively to record carriers with provision for moving the light beam or focus plane for the purpose of maintaining alignment of the light beam relative to the record carrier during transducing operation, e.g. to compensate for surface irregularities of the latter or for track following
Abstract
Description
【発明の詳細な説明】
本発明は、光ディスクよシ情報を読みとる光学ヘッドの
受光部調整機構に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a light receiving section adjustment mechanism of an optical head that reads information from an optical disc.
従来、誤差信号の零点調整は、光学系の光軸に対し二分
@また線四分割ホトディテクターの中心を微妙に移動さ
せる事のみによ!DIIIEしていた。Conventionally, the zero point adjustment of the error signal was done only by subtly moving the center of the bisecting/quadrant photodetector with respect to the optical axis of the optical system! I was doing DIIIE.
まず、頂角αが小さい2枚の薄いプリズムからなる偏角
プリズムについてその働きを説明する。プリズムの属折
率をnとすれば、1枚のプリズムにほぼ−直に入射する
光のふれの角は(n−1)(!であり、第1図(イ)の
様に平行して置かれた場合、ふれの角は2倍になC2(
n−1)aである。この状態よシ、各々のプリズムを互
に逆方向に角度0だけ回転すると、最初の状態における
プリズムの稜に自直な面内でふれの角aは次式に従い変
化するJ =x 2(n −1)d −as#上記の状
態が第1図(ロ)であシーを00からiso’まで変え
る事により入射光のふれの角を士g(n−1)gの範囲
内で任意に変える事が可能である。First, the function of the deflection prism, which is made up of two thin prisms with a small apex angle α, will be explained. If the genus refractive index of a prism is n, then the angle of deflection of light that almost directly enters one prism is (n-1) (!), and the angle of deflection of light that is almost directly incident on one prism is (n-1) (!). When placed, the corner of the deflection is doubled to C2 (
n-1) a. In this state, when each prism is rotated by an angle of 0 in opposite directions, the deflection angle a changes in the plane perpendicular to the prism ridge in the initial state according to the following formula: J = x 2 (n -1) d -as# The above state is shown in Figure 1 (b).By changing the sea from 00 to iso', the angle of deflection of the incident light can be arbitrarily set within the range of g(n-1)g. It is possible to change.
この発明を光学ヘッドのトラッキング誤差信号検出部に
応用した実施例に従って詳細に説明する。The present invention will be explained in detail according to an embodiment in which the invention is applied to a tracking error signal detection section of an optical head.
光学ヘッドの一例は第2図の如く、半導体レーザーの光
を光源として光デイスク直上に黴少な光スポットを結儂
させ、光デイスク上の記録ドツトの有無を情報としてデ
ィスク面からの反射光の強度変化から読み取る。光ヘッ
ドが記鎌ドツトの点列、即ちトラックを追随させる九め
には、受光部第3図(謬)に入射する光強度分布の対称
軸3−1を受光部光学系の光軸3−3と一致させ光軸上
に置いた二分割ホトディテクターの出力の差が零となる
様に111mする必要がある。特に入射光強度分布の対
称軸3−1集光レンズの光軸3−3二分割ホトディテク
ターの中心を一直線上に列べる事はトラックキング誤差
信号検出にとって重要な事である。An example of an optical head, as shown in Figure 2, uses semiconductor laser light as a light source to create a small light spot directly above an optical disk, and uses the presence or absence of recording dots on the optical disk as information to measure the intensity of the reflected light from the disk surface. Read from changes. In the ninth step when the optical head follows the dot sequence of the recorded sickle dots, that is, the track, the symmetry axis 3-1 of the light intensity distribution incident on the light receiving section (Fig. 3) is aligned with the optical axis 3-1 of the light receiving section optical system. 3 and placed on the optical axis so that the difference in the output of the two-split photodetector placed on the optical axis becomes zero. In particular, it is important for the tracking error signal detection to align the centers of the two-split photodetector with the axis of symmetry 3-1 of the incident light intensity distribution, the optical axis 3-3 of the condensing lens, on a straight line.
入射光強直分布の対称軸のずれはドツト形状の非対称性
、ディスク面のたわみ、光学ヘッドの組立精度また社取
付精度等から僅かながら発生するので偏光プリズムで入
射光をふシながら最終的に調整を取る。A slight deviation in the axis of symmetry of the incident light teorotic distribution occurs due to the asymmetry of the dot shape, the deflection of the disk surface, the assembly accuracy of the optical head, and the installation accuracy of the optical head, so the final adjustment is made while blocking the incident light with a polarizing prism. I take the.
硼確p’ptyガ’) スBK? (n =x 1.5
1 ; 830nm)で頂角gs112°の薄いプリズ
ム2枚を作シ上記偏角プリズムとして焦点距離18II
sの集光レンズ2−7の直紡に設叶、集光レンズの後方
151111の軸上に2■φの二分割ホトディテクター
を置くと偏角プリズムの最大ふれの角は約*2°、入射
光の対称軸のづれは*へ2・■まで許される。Definitely p'ptyga') BK? (n = x 1.5
1 ; 830 nm), and the apex angle gs is 112°, and the focal length is 18II as the deflection prism.
If a two-part photodetector of 2■φ is placed on the axis of 151111 behind the condenser lens, the maximum deflection angle of the deflection prism will be approximately *2°, The axis of symmetry of the incident light is allowed to shift by up to 2·■.
この発明に係る偏角プリズムは二分割ホトディテタター
の平衝を取る丸めのみならず四分割ホトディテクターの
平衝を取るためにも利用できて四分割ホトディテクター
から得られるトラッキング及びフォーカシング誤差信号
の零点調整に優れている。The deflection prism according to the present invention can be used not only for rounding to balance a two-segment photodetector, but also for balancing a four-segment photodetector, thereby adjusting the zero point of the tracking and focusing error signal obtained from the four-segment photodetector. Excellent.
第1図(イ) (0) 拡この発明を特徴づける偏角プ
リ学ヘッド受光部光学系の入射光強度分布及び主な光線
図である。
1−1.2・・・偏角プリズム
2−1・・・半導体レーザー 2−2・・・集光し/
ズ2−3・・・ビームスプリッタ−2−4・・・1/4
波畏板2−5・・・対物レンズ 2−6・・・光
ディスク2−7・・・集光レンズ
2−8・・・二分割ホトディテクター素子2−9・・・
差信号検出回路
3−1・・・入射光強度分布の対称軸FIG. 1(a) (0) is an incident light intensity distribution and main ray diagram of the polarization prism head light receiving part optical system that characterizes the present invention. 1-1.2... Deflection prism 2-1... Semiconductor laser 2-2... Focusing/
2-3...Beam splitter-2-4...1/4
Wave plate 2-5...Objective lens 2-6...Optical disk 2-7...Condensing lens 2-8...Two-split photodetector element 2-9...
Difference signal detection circuit 3-1... Symmetry axis of incident light intensity distribution
Claims (1)
トラッキング誤差信号検出のための光学系内に一対の薄
いプリズムを設けて二つのプリズムの回転によ〉光の進
行方向を黴少にふシ、誤差信号検出素子上、の光の位置
を変位させて誤差信号の零点を調整する事を特徴とする
光学ヘッドの調整機構。's? on the light receiving part of the optical head? A pair of thin prisms is provided in the optical system for focus odor sink and tracking error signal detection, and by rotating the two prisms, the direction of travel of the light is kept small, and the light is placed on the error signal detection element. An optical head adjustment mechanism that adjusts the zero point of an error signal by displacing the position of light.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11528781A JPS5817550A (en) | 1981-07-24 | 1981-07-24 | Adjusting mechanism for optical head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11528781A JPS5817550A (en) | 1981-07-24 | 1981-07-24 | Adjusting mechanism for optical head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5817550A true JPS5817550A (en) | 1983-02-01 |
Family
ID=14658921
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11528781A Pending JPS5817550A (en) | 1981-07-24 | 1981-07-24 | Adjusting mechanism for optical head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5817550A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4658389A (en) * | 1983-11-03 | 1987-04-14 | Deutsche Thomson Brandt Gmbh | Track follower system for correcting tangent errors in an optical record scanning system |
JPH025113U (en) * | 1988-06-20 | 1990-01-12 | ||
EP0558249A2 (en) * | 1992-02-28 | 1993-09-01 | Canon Kabushiki Kaisha | Optical information recording/reproducing apparatus |
-
1981
- 1981-07-24 JP JP11528781A patent/JPS5817550A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4658389A (en) * | 1983-11-03 | 1987-04-14 | Deutsche Thomson Brandt Gmbh | Track follower system for correcting tangent errors in an optical record scanning system |
JPH025113U (en) * | 1988-06-20 | 1990-01-12 | ||
JPH0739051Y2 (en) * | 1988-06-20 | 1995-09-06 | 京セラ株式会社 | Optical head adjustment mechanism |
EP0558249A2 (en) * | 1992-02-28 | 1993-09-01 | Canon Kabushiki Kaisha | Optical information recording/reproducing apparatus |
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