JPS5860436A - Optical reproducing or recording and reproducing device - Google Patents

Optical reproducing or recording and reproducing device

Info

Publication number
JPS5860436A
JPS5860436A JP15894981A JP15894981A JPS5860436A JP S5860436 A JPS5860436 A JP S5860436A JP 15894981 A JP15894981 A JP 15894981A JP 15894981 A JP15894981 A JP 15894981A JP S5860436 A JPS5860436 A JP S5860436A
Authority
JP
Japan
Prior art keywords
light
photodetector
disk
reflected
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.)
Pending
Application number
JP15894981A
Other languages
Japanese (ja)
Inventor
Shunji Ohara
俊次 大原
Tomio Yoshida
吉田 富夫
Isao Sato
勲 佐藤
Kenji Koishi
健二 小石
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP15894981A priority Critical patent/JPS5860436A/en
Publication of JPS5860436A publication Critical patent/JPS5860436A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording 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
    • G11B7/08Disposition or mounting of heads or light sources relatively to record carriers
    • G11B7/09Disposition 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
    • G11B7/0908Disposition 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 for focusing only

Abstract

PURPOSE:To increase the focus sensitivity of an optical system without increasing its scale, by focusing reflected light from a disk through a convex lens and also split it into two beams through a total reflection mirror, and then obtaining a tracking error signal from one beam while obtaining a focus error signal from the other beam through a concabe lens. CONSTITUTION:Light emitted from a light source 1 is focused on a disk 6 through a convergent lens 2 and a diaphragm lens 7. Its reflected light travels backward, and is stopped down by a convex lens 7 and then split into two beams through a total reflection mirror 11; one beam is made incident to two- split photodetectors 12a and 12b, and a tracking error signal is obtained from the difference between their outputs. The other beam is spread slightly by a concave lens 13 and guided to two-split photodetectors 14a and 14b to obtain a focus error signal from their output difference. Use of the concave lens 13 increases focus sensitivity without increasing the scale of the obtical system.

Description

【発明の詳細な説明】 本発明は、ビデオディスク等のよう(こディスク上に記
録された情報を光学的憂こ読み取る光学的再生装置、あ
るいはディスクに情報を光学的に記録 “再生しようと
する光学的記録再生装置蚤こ係り、特にディスクよりの
反射光を利用し、各4m−IJ−ボをかけるためのサー
ボ信号および再生信号を得るための光学系に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical reproducing device that optically reads information recorded on a disc, such as a video disc, or a device that optically records information on a disc and The present invention relates to an optical recording/reproducing apparatus, and in particular to an optical system for obtaining a servo signal and a reproduction signal for applying each 4m-IJ-bore using reflected light from a disk.

一般にビデオディスクや光学的記録再生装首iこおいて
は、情報を高密度に記録、再生ずるために、ディスク上
のトラックは、例えばその幅が0.6μmそのピッチが
1.6μmと微細なスパイラルJ)るいは同心円の形状
となっている。前記ディスクには一1gm 以下1こ絞
り込まれた微小スポット光が照射され、その反射光から
ディスク上の情報が批み出されている。
In general, in video discs and optical recording/reproducing devices, in order to record and reproduce information at high density, the tracks on the disc have a width of, for example, 0.6 μm and a pitch of 1.6 μm. Spiral J) Or has the shape of concentric circles. The disc is irradiated with a very small spot light of less than 1 gm, and the information on the disc is extracted from the reflected light.

かかる装置においては、少なくとも2つのサーボ技術が
必要である。1つはディスクの旧転憂こ伴い回転方向と
垂直な方面にディスクが面ブレを起した時に前記面ブレ
に対しQtr記の−lμ口l 以下に絞られた微小スポ
ット光が常にディスク上に照射できるように光学系を追
従させるサーボであってこのサーボはフォーカスサーボ
と呼ばれている。
In such a device, at least two servo techniques are required. One is due to the deterioration of the disk, and when the disk causes surface wobbling in a direction perpendicular to the rotation direction, a minute spot light focused to less than -lμl in Qtr is always focused on the disk. This servo is called a focus servo, which causes the optical system to follow the light so that it can irradiate light.

他方はディスクの回転に伴い前記トランクが偏心等によ
りディスクの半径方向に移動した時にこれ]こ対し常齋
こ前記微小スポット光が前記トラック上を照射するよう
に光学系を追従させるサーボであって、このサーボはト
ラッキングサーボと呼ばれている。
The other is a servo that causes an optical system to follow this when the trunk moves in the radial direction of the disk due to eccentricity or the like as the disk rotates, so that the minute spot light illuminates the track. , this servo is called a tracking servo.

前記フォーカスおよびトラッキングサーボを行うための
サーボ信号はディスクの反射光より得ており、具体的な
光学系としては例えば第1因に示すような光学系が提案
されている。
The servo signal for performing the focus and tracking servo is obtained from the reflected light of the disk, and as a specific optical system, for example, the optical system shown in the first factor has been proposed.

第1図の光学系において、(1)は例えば半導体レーザ
からなる光源、(2)は半導体レーザから出た光ヲ集め
る集光レンズ、(3)は偏光ビームスプリッタで、半導
体レーザ(1)から出た光を第1図に示す様に折り曲げ
ディスクiこ導く。(4)はA/4板、(5)は微小ス
ポット光に絞り込むための絞りレンズ、(6)はディス
クで、ディスク(6)上に前記微小スポット光が照射さ
れ、信号の記録再生あるいは再生のみが(4ン 行なわれる。ディスク(6)よりの反射光はv4板を八 再び通り、その偏光方向が変えられ偏光ビームスプリッ
タ(3)を通過する。(7)は凸レンズ、(8月まウェ
ッジと呼ばれる三角スプリズムで、ffdLウェッジ(
8)で光は2分割されかつ方向を変えられて光検出器(
9) (10にそれぞれ導かれる。、前記ウェッジ(8
)の形状は第2図に示されている。光検出器(9〕はそ
の光入射方向からみると(9a)(9b)に示すように
2分割されており、この2分割された各光検出器(9a
)(9b)の出力の差より前記フォーカスサーボのため
のフォーカス誤差信号を得ている。また光検出器01は
その光入射面からみると(10aXxob)に示すよう
に2分割されており、この2分書すされた各光検出器(
loa)(10b)の出力の差より前記トラッキング−
サーボのためのトラッキング誤差信号を得、前記4ケの
各光検出器(9aX9b)(10a)(10b)の出力
の総和よりディスク上に記録された情報を読み出す再生
信号を得ている。
In the optical system shown in Fig. 1, (1) is a light source made of, for example, a semiconductor laser, (2) is a condensing lens that collects the light emitted from the semiconductor laser, and (3) is a polarizing beam splitter that separates the light from the semiconductor laser (1). The emitted light is guided through a bent disk i as shown in FIG. (4) is an A/4 board, (5) is an aperture lens for narrowing down the light to a minute spot, and (6) is a disk.The minute spot light is irradiated onto the disk (6), and the signal is recorded or reproduced. The reflected light from the disk (6) passes through the V4 plate eight times, its polarization direction is changed, and it passes through the polarizing beam splitter (3). (7) is a convex lens, (Aug. A triangular prism called a wedge, ffdL wedge (
At step 8), the light is split into two and redirected to the photodetector (
9) (each guided by 10), said wedge (8
) is shown in FIG. The photodetector (9) is divided into two parts as shown in (9a) and (9b) when viewed from the direction of light incidence.
) (9b) A focus error signal for the focus servo is obtained from the difference in the outputs of (9b). In addition, the photodetector 01 is divided into two parts as shown in (10aXxob) when viewed from its light incident surface, and each photodetector (
The tracking -
A tracking error signal for servo is obtained, and a reproduction signal for reading information recorded on the disk is obtained from the sum of the outputs of the four photodetectors (9aX9b) (10a) (10b).

前記第1図の光学系には以下の欠点を有している。すな
わち (1)  ディスク(6)よりの反射光がウェッジ(8
)を通過する時、その光束幅が広いためウェッジ(8)
により収差を受け、各光検出器、特に反射光の集光位置
よりズレ1こファーフィールド像よりトラッキング誤差
信号を得ている光検出器01上での反射光の波面が乱れ
、トラッキング誤差信号に悪影棲を与えてしまう。
The optical system shown in FIG. 1 has the following drawbacks. That is, (1) the reflected light from the disk (6) is reflected from the wedge (8
), the beam width is wide when passing through the wedge (8)
Due to the aberration caused by this, the wavefront of the reflected light on each photodetector, especially the photodetector 01 which obtains the tracking error signal from the far-field image, is disturbed by one deviation from the focused position of the reflected light, resulting in a tracking error signal. It gives a bad impression.

(2)  フォーカス誤差信号検出用の光検出器(9)
がそのフォーカス位置調整方向(2分割の方向と垂直な
方向)にΔ!移動した時、ディスク(6)上に集光され
た集光位置が光軸方向にΔX移動したとすると、フォー
カス感度mは m=Δt/ΔX ・−・・−・・・(1)となる。前記
フォーカス感度mは、絞りレンズ(5)の焦点距離k 
fs 、凸レンズ(7)の焦点距離をf7    ・と
すると m手」−・・・−・・・・・(2) fs で与えられる。 (2)式にてフォーカス感度mを大キ
くシようとすれば凸レンズ(7)の焦点側′M1fy 
ヲ大きくしなければならない、しかし前記f1を大きく
すれば、凸レンズ(7)と光検出器(9)との間のFf
H離A カJ’z <なってしまい、光学系内Uドが大
キくなり、かつ温度変化等により光検出器(9)σ)位
置が動きやすくなり、ディスク上に安定して入射光をフ
ォーカスすることが困難となる。
(2) Photodetector for focus error signal detection (9)
is Δ! in the focus position adjustment direction (direction perpendicular to the direction of 2 divisions)! Assuming that the light condensing position on the disk (6) moves by ΔX in the optical axis direction when moving, the focus sensitivity m becomes m=Δt/ΔX (1) . The focus sensitivity m is determined by the focal length k of the aperture lens (5).
fs, and the focal length of the convex lens (7) is f7.m, then it is given by fs. If we try to increase the focus sensitivity m using equation (2), then the focal side of the convex lens (7) ′M1fy
However, if f1 is increased, Ff between the convex lens (7) and the photodetector (9) can be increased.
H R A F J'z <, the U-D in the optical system becomes large, and the position of the photodetector (9) σ) tends to move due to temperature changes, etc., and the incident light stably falls on the disk. It becomes difficult to focus.

本発明は主に以−りの点に鑑みてなされゴこものであり
、第1図の光学系において、凸レンズにより絞られるデ
ィスクよりの反射光を全反射ミラー昏こより2分割し、
2分割されtこ一方の光より1−ラッキング誤差信号を
得、また他方の光を四L・ンズにより若干拡大して絞り
込むようにし、前記凹レンズを透過した光よりフォーカ
ス誤差信号を得るような構成にすることにより、各制御
値)Jを得るためのディスクよりの前記反射光が収差を
受けることなく、従って波面の乱れもなく、かつ前記凹
レンズを入れることにより光学系を大きくしないで。
The present invention was made mainly in view of the following points, and in the optical system shown in FIG.
The structure is such that a 1-racking error signal is obtained from one light that is divided into two, and the other light is slightly expanded and narrowed down by a four-lens lens, and a focus error signal is obtained from the light that has passed through the concave lens. By doing so, the reflected light from the disk for obtaining each control value J is not subjected to aberrations, therefore, there is no disturbance of the wavefront, and by inserting the concave lens, the optical system is not enlarged.

前記フォーカス(し度mを高めれるよう番こしたことを
特徴とする新規な光学系を提供することを目的とする、 以下図面に従い本発明の詳細な説明する。第8図は本発
明の一実施例を示した図で、第1図と向−の構成要素に
ついては同じ番号を付した。第8図(こおいて例えば半
導体レーザからなる先触(1)から出た光がディスク(
6)lこ照射されるまでの入射光路は第1図と同様であ
る。ディスク(6)からの反射光は凸レンズ(7)によ
り絞られ、全反射ミラー住めにより2分割さii、、一
方の光は図の様に光検出器(ロ)に導かれる。光検出器
0才はその光入射方向からみると、 (12a)(12
b)に示すように2分剤されている。
The present invention will be described in detail below with reference to the drawings, which aims to provide a novel optical system characterized by increasing the focus (m). This is a diagram showing an embodiment, and the same numbers are given to the components opposite to those in FIG. 1. In FIG.
6) The incident optical path until the light is irradiated is the same as that shown in FIG. The reflected light from the disk (6) is condensed by a convex lens (7), divided into two parts by a total reflection mirror (ii), and one of the lights is guided to a photodetector (b) as shown in the figure. When looking at the photodetector 0 years old from its light incident direction, (12a) (12
It is divided into two parts as shown in b).

前記2分割された他方の光は凹レンズに)により若干拡
げて絞られ、前記凹レンズを透過した光のほぼ集光位置
に置かれた光検出器04に導かれる。
The other of the two divided beams is slightly expanded and condensed by a concave lens, and guided to a photodetector 04 placed approximately at the convergence position of the light that has passed through the concave lens.

この光学系において曲記両ザーボは以下のように実現さ
れている。ディスク(6)はモータ(ト)により回転し
、その回転により矢印X方向にディスク面は面ブレし、
矢印Yh向にディスク上のトラックは偏心により移動す
る。そこで前記面ブレにかかわらず、ディスク面上に入
射光がフォーカスされるよう1こ、フォーカシング駆動
装置Oゆをこより絞りレンズ(5)を矢印Xの方向lと
動かすフォーカスサーボがかけられ、また前記トラック
の移動に対して前記ディスク面上にフォーカスされた入
射光が追従するように、トラッキング駆1lX11装置
0ηにより絞りレンズ(5)を矢印Y方向に動かすトラ
ッキングサーボがかけられている。前記トラッキングタ
ーボのためのトラッキング誤差信号は前記光検出器Q′
4上のファーフィールド像から得られ、削り己フォーカ
シングサーボのためのフォーカシング誤差信号は前記光
検出器α→上のニヤフィールド像から得ている。
In this optical system, both curved servos are realized as follows. The disk (6) is rotated by a motor (g), and due to the rotation, the disk surface wobbles in the direction of arrow X.
The track on the disk moves in the direction of arrow Yh due to eccentricity. Therefore, a focus servo is applied to move the aperture lens (5) in the direction of the arrow A tracking servo is applied to move the aperture lens (5) in the direction of arrow Y by a tracking driver 11X11 device 0η so that the incident light focused on the disk surface follows the movement of the track. The tracking error signal for the tracking turbo is transmitted to the photodetector Q'
The focusing error signal for the focusing servo is obtained from the near field image on the photodetector α→.

@8図の構成でフォーカシング誤差信号が得られる原理
について詳しく説明する。第4図はフォーカシング誤差
信号を得る方法についてのみ説明するために第8図を簡
略化した図であり、第8因と同様の構成要素については
同一の符号を付した。
@8 The principle of obtaining a focusing error signal with the configuration shown in FIG. 8 will be explained in detail. FIG. 4 is a simplified diagram of FIG. 8 in order to explain only the method of obtaining the focusing error signal, and the same reference numerals are given to the same components as the eighth factor.

第4図において、(イ)は絞りレンズ(5)とディスク
(6)間が所望の距離より近づきすぎた場合、(2)は
丁度所望の距離、すなわちディスク面上に入射光がフォ
ーカスされた場合、(ハ)は前記所望の距離より長くな
った場合をそれぞれ示している。まず第4因(イ)に示
したように絞りレンズ(5)とディスク(6)とか前記
所望の距離より近づきすぎると、凹レンズQ3により絞
られる反射光の集光位置Piは、光検出器α◆より遠く
なる。従ってこの場合光検出器(14a)玉受光される
光量より光検出器(1ab) tこ受光される光量の方
が多くなる。逆に第4因(ハ)に示すように絞りレンズ
(5)とディスク(6)とが前記所望の距離よりも遠ざ
かると、光検出器(x4b)に受光される光量より光検
出器(14a)に受光される光量の方が多くなる。また
第4図(ロ)に示すようにディスク(6)上に入射光が
フォーカスされた場合は、光検出器α◆上に凹レンズに
よりフォーカスされた光が照射されるため、光検出器(
14a)(14b)の受光量は等しくなる。従って前記
両光検出器(14a)と(14b)の出力の差動をとれ
ば第6図に示すような8字のフォーカス誤差信号が得ら
れ、前記フォーカス誤差信号を用い、前記光検出器(1
4a)(14b)の受光量が等しくなるようにサーボを
かければ、フォーカスサーボが実現できる。第5図は第
8図の光学系fこおけるフォーカス誤差信号の様子を示
し、縦1i1flVeはフォーカス誤差信号、横軸ΔX
はジャストフォ−カス位置(第4図(ロ))からの焦点
のズレ量(以下ディフォーカス量と呼ぶ)を示している
In Figure 4, (a) indicates that the aperture lens (5) and the disk (6) are too close together than the desired distance, and (2) indicates that the incident light is focused at exactly the desired distance, that is, on the disk surface. In this case, (c) indicates a case where the distance is longer than the desired distance. First, as shown in the fourth factor (A), if the diaphragm lens (5) and the disk (6) are too close to each other than the desired distance, the condensing position Pi of the reflected light focused by the concave lens Q3 will be shifted to the photodetector α. ◆It becomes further away. Therefore, in this case, the amount of light received by the photodetector (1ab) is greater than the amount of light received by the photodetector (14a). Conversely, as shown in the fourth factor (c), when the aperture lens (5) and the disk (6) are separated from each other by more than the desired distance, the amount of light received by the photodetector (x4b) is lower than the amount of light received by the photodetector (x4b). ) will receive more light. In addition, when the incident light is focused on the disk (6) as shown in FIG. 4 (b), the focused light is irradiated onto the photodetector α
The amounts of light received by 14a and 14b are equal. Therefore, by taking the difference between the outputs of the two photodetectors (14a) and (14b), a focus error signal of 8 characters as shown in FIG. 6 is obtained, and using the focus error signal, the photodetector (14b) 1
Focus servo can be achieved by applying servo so that the amounts of light received in 4a and 14b are equal. Figure 5 shows the state of the focus error signal in the optical system f in Figure 8, where the vertical axis 1i1flVe is the focus error signal, and the horizontal axis ΔX
indicates the amount of focus deviation (hereinafter referred to as defocus amount) from the just focus position (FIG. 4(b)).

ト 一方ラッキング誤差信号は、第8図にお+する光Δ 検出器(x2a)(t2b)の差より得ている。to On the other hand, the racking error signal is expressed by the light Δ It is obtained from the difference between the detectors (x2a) and (t2b).

第8図に示した本発明の光学系の特徴を以下に述べる。The features of the optical system of the present invention shown in FIG. 8 will be described below.

(1)反射光の波面に乱れが無い。こオ目、t13a図
(こ示した光学系の構成において、反射光路中に前述の
ウェッジ等の収差を生じさせる光学部品が無いため、反
射光の波mlが乱されない。そのため特に反射光のファ
ーフィールド1象の動きからトラッキング誤差信号を得
ている本方式では、トラッキング誤差信号の品質は第1
図の従来の構成に比べかなり良くなる。
(1) There is no disturbance in the wavefront of reflected light. Figure t13a (In the configuration of the optical system shown here, there is no optical component that causes aberrations such as the aforementioned wedge in the reflected optical path, so the reflected light wave ml is not disturbed. Therefore, the reflected light wave ml is not disturbed. In this method, which obtains the tracking error signal from the movement of one field elephant, the quality of the tracking error signal is
This is considerably better than the conventional configuration shown in the figure.

(2)  フォーカス感度が高くなる。従来の構成では
フォーカス感度n】は前述のように ・」二 m″″2f5 で与えられる。従ってフォーカス感度mを上げるために
は凸レンズ(7)の焦点距1mfyを大きくしなければ
ならず、そのため光学系か大きくなってしまう欠点があ
った。しかしロ68図の凹レンズ(ハ)を入れた本発明
の構成では光学系を大きくせずに等価的昏こ焦点距離f
7を太きくシtこと同じ効果を有し、フォーカス感度を
上げることかできる。第6図に凹レンズが無い場合(イ
)と、有る場合(0)の反射光路の比較を示した。従来
の(イ)の構成の場合フォーカス感度11】aは ma:i fs で与えられる。−力木発明の凹レンズを用いた(口)の
場合のフォーカス感度inbはmb−1□ f5 で与えられ、従って本発明の構成によれば、光学系の大
きさは全く変えずフォーカス感度をf;/f7倍上げる
ことができる。具体的Eこf、 ””80゜(fls−
7)とするとfヂ/ f、キ8倍程度フォーカス感度を
上げることができる。
(2) Focus sensitivity increases. In the conventional configuration, the focus sensitivity n] is given by 2m''2f5 as described above. Therefore, in order to increase the focus sensitivity m, it is necessary to increase the focal length 1 mfy of the convex lens (7), which has the disadvantage that the optical system becomes large. However, with the configuration of the present invention including the concave lens (c) in Figure 68, the equivalent focal length f can be obtained without enlarging the optical system.
Making 7 thicker has the same effect and can increase focus sensitivity. FIG. 6 shows a comparison of the reflected optical paths when there is no concave lens (A) and when there is a concave lens (0). In the case of the conventional configuration (a), the focus sensitivity 11]a is given by ma:ifs. - The focus sensitivity inb in the case (mouth) using the concave lens invented by Rikiki is given by mb-1□ f5. Therefore, according to the configuration of the present invention, the focus sensitivity can be adjusted to f without changing the size of the optical system at all. ;/f can be raised by 7 times. Concrete Ekof, ””80゜(fls-
7), the focus sensitivity can be increased by about 8 times f/f.

(3)  また反射光の結像位置P2にてフォーカス誤
差信号を得るよう番こしているため、ディスク上に記録
されている情報(ビット)から受ける反射光の回折の影
響も軽減することができ、高品質なフォーカス誤差信号
を得ることかできるよう(こなる。
(3) Furthermore, since the focus error signal is obtained at the imaging position P2 of the reflected light, the influence of diffraction of the reflected light from the information (bits) recorded on the disk can be reduced. , so that a high-quality focus error signal can be obtained.

なお、第3図の構成において、ミラー01)よりの反射
光からトラッキング誤差信号を、ミラー01こより反射
されない他方の光からフォーカス課差信号ヲ得るような
構成にしているか、全く逆0)構成でも上記同様な効果
が得られる。しかし第8図の様な組み合イ〕せの方がよ
り安定である。何故なら温度変化等による光軸変動(光
学部品の動き)の影響はトラッキング誤差信号よりフォ
ーカス誤差信号に与える影響の方がかなり厳しい。従っ
て温度変化によって全反射ミラーαηが動いてもフォー
カス誤差信号に影響が出ないように、第8因に示すよう
な構成にしているわけである。
In addition, in the configuration shown in FIG. 3, the tracking error signal is obtained from the light reflected from the mirror 01), and the focus difference signal is obtained from the other light that is not reflected from the mirror 01, or the configuration is completely reversed. Effects similar to those described above can be obtained. However, the combination shown in Figure 8 is more stable. This is because the influence of optical axis fluctuations (movement of optical components) due to temperature changes and the like has a much more severe influence on the focus error signal than on the tracking error signal. Therefore, the structure shown in the eighth factor is used so that the focus error signal is not affected even if the total reflection mirror αη moves due to temperature changes.

また全反射ミラー(II)の位置であるが、第6図(ロ
)をみてもわかるよう(こ光軸中心x −x’輔より少
しずれた位置におき、フォーカス誤差信号検出用の光検
出器(14a)(14b)の方に半分以上の光が入るよ
うにしている。これはフォーカスサーボ引き込み時に絞
りレンズ(5)とディスク(6)間の距離がn「望の距
離より長くなった場合(第4図e))、反射光の集光位
置P3(第4図)が全反射ミラー(ロ)よりディスク側
に来て、反射光が全て全廃9>i ミラーより反射され
て(14a) (14b)のフォーカス誤差信号検出用
の光検出器に光が入射しなくなるということを防ぐtこ
めである。
Also, regarding the position of the total reflection mirror (II), as can be seen from Fig. 6 (b), it is placed at a position slightly shifted from the optical axis center More than half of the light enters the lenses (14a) and (14b).This is because the distance between the aperture lens (5) and the disc (6) is longer than the desired distance when the focus servo is pulled in. In the case (Fig. 4e)), the condensing position P3 (Fig. 4) of the reflected light is closer to the disk than the total reflection mirror (b), and all the reflected light is reflected from the total reflection mirror (14a). ) This is to prevent light from not entering the photodetector for detecting the focus error signal in (14b).

以上説明してきたようfこ、本発明の構成によれば、ウ
ェッジ等の高価で、かつ反射光の波面を乱す特殊な光学
部品を使わないO)で、特にトラッキング誤差信号の品
質が良くなり、また凹レンズを新しく入れることにより
光学系を大きくすることなしにフォーカス感度を誦める
ことができる等の大きな効果を有している。
As explained above, according to the configuration of the present invention, the quality of the tracking error signal is particularly improved without using special optical components such as wedges that are expensive and disturb the wavefront of reflected light. Also, by inserting a new concave lens, it has great effects such as being able to adjust the focus sensitivity without increasing the size of the optical system.

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

第1図は従来の光学的記録再生装置の光学系を示す構成
図、第2図は第1図のウェッジを示す斜視図、第8図は
本発明の光学的記録再生装置の光学系を示す構成図、第
4図は焦点ズレが生じた場合の反射光の5様子を示す説
明図、第6因は本発明の構成から得られるフォーカス誤
差信号を示す特性図、第6図は凹レンズを用いない場合
と用いた場合の反射光の比較からフォーカス輝度の違い
を説明するための図である。 (1)・・・光源(半尋体レーザ) 、 (+i)・・
・絞りレンズ、(6)・・・ディスク、(7)・・・凸
レンズ、OJ)・・・全反射ミラー、(12aX12b
)・・・2分;q1]された第1の光検出器、(ト)・
・・凹レンズ、(14a)(14b)・・・2分割され
た第2の光検出器 代理人 珠本−1)弘 第4図 (112 〜1 h
FIG. 1 is a configuration diagram showing an optical system of a conventional optical recording/reproducing device, FIG. 2 is a perspective view showing the wedge of FIG. 1, and FIG. 8 is a diagram showing an optical system of an optical recording/reproducing device of the present invention. The configuration diagram, Fig. 4 is an explanatory diagram showing the five states of reflected light when a focus shift occurs, and the sixth factor is a characteristic diagram showing the focus error signal obtained from the configuration of the present invention. FIG. 6 is a diagram for explaining the difference in focus brightness from a comparison of reflected light when the lens is not used and when it is used. (1)...Light source (half-body laser), (+i)...
・Aperture lens, (6)...disk, (7)...convex lens, OJ)...total reflection mirror, (12aX12b
)...2 minutes; q1] first photodetector, (g).
... Concave lens, (14a) (14b) ... Second photodetector agent divided into two Tamamoto-1) Hiro Figure 4 (112 ~ 1 h

Claims (1)

【特許請求の範囲】 1、 レーザから出た光を絞りレンズにより微小スポッ
ト光に絞り、ディスクに照射し、情報を読み出したりあ
るいは書き込んだりする光学的記録再生装置において、
前記ディスクからの反射光を収束する少なくとも1ヶ以
上の凸レンズと、並記収束しようとする反射光の光路中
に前記反射光を2分割し、2方向に分ける全反射ミラー
を設け、前記2分割された反射光の一方の光を受光し、
各出力の差からトラッキングサーボ信号を検出する第1
の2分割されtコ光検出器と、前記2分あされた他方の
光を再び絞る少なくとも1ヶ以上の凹レンズと、この凹
レンズを通した光を受光し、各出力の差からフォーカス
サーボ信号を検出する第2の分割された光検出器とを設
け、前記第1と第2の光検出器の各出力の総和から情報
を読みとる再生信号を検出するようにした光学的再生ま
たは記録再生装置。 2、 第1の光検出器をディスクよりの反射光の集光位
置よりずらして置き、第2の光検出器をディスクよりの
反射光の集光位置に置いたことを特徴とする特許請求の
範囲第1項記載の光学的再生または記録再生装置。 8、 全反射ミラーにより反射された光を第1 (7)
光検出器蚤こ導き、全反射ミラーにより反射されない他
方の反射光を第2の光検出器に導くよう蔽こしたことを
特徴とする特許請求の範囲第1項または第2項記載の光
学的再生または記録再生装置。 4、 ディスクよりの反射光の少なくとも半分以上の光
を第2の光検出器に導くように全反射ミラーを設置した
ことを特徴とする特許請求の範囲第1項または第2項ま
たは第8項記載の光学的再生または記録再生装置。
[Claims] 1. In an optical recording and reproducing device that focuses light emitted from a laser into a minute spot light using an aperture lens and irradiates it onto a disk to read or write information,
At least one or more convex lenses that converge the reflected light from the disk, and a total reflection mirror that divides the reflected light into two directions in the optical path of the reflected light to be converged, and a total reflection mirror that divides the reflected light into two directions. receive one of the reflected lights,
The first one detects the tracking servo signal from the difference between each output.
A photodetector that is divided into two parts, at least one concave lens that refocuses the other light that has been separated by two minutes, and a focus servo signal that receives the light that has passed through this concave lens and generates a focus servo signal from the difference in each output. 1. An optical reproducing or recording/reproducing apparatus, comprising a second divided photodetector for detection, and detecting a reproduction signal for reading information from the sum of respective outputs of the first and second photodetectors. 2. A patent claim characterized in that the first photodetector is placed at a position shifted from the position where the light reflected from the disk is focused, and the second photodetector is placed at the position where the light reflected from the disk is focused. The optical reproducing or recording/reproducing device according to scope 1. 8. The light reflected by the total reflection mirror is the first (7)
The optical detector according to claim 1 or 2, characterized in that the photodetector is guided so that the other reflected light that is not reflected by the total reflection mirror is guided to the second photodetector. Playback or recording/playback equipment. 4. Claim 1, 2, or 8, characterized in that a total reflection mirror is installed so as to guide at least half or more of the light reflected from the disk to the second photodetector. Optical playback or recording/playback device as described.
JP15894981A 1981-10-05 1981-10-05 Optical reproducing or recording and reproducing device Pending JPS5860436A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15894981A JPS5860436A (en) 1981-10-05 1981-10-05 Optical reproducing or recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15894981A JPS5860436A (en) 1981-10-05 1981-10-05 Optical reproducing or recording and reproducing device

Publications (1)

Publication Number Publication Date
JPS5860436A true JPS5860436A (en) 1983-04-09

Family

ID=15682848

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15894981A Pending JPS5860436A (en) 1981-10-05 1981-10-05 Optical reproducing or recording and reproducing device

Country Status (1)

Country Link
JP (1) JPS5860436A (en)

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