JPH02192040A - Optical pickup device - Google Patents

Optical pickup device

Info

Publication number
JPH02192040A
JPH02192040A JP1103689A JP1103689A JPH02192040A JP H02192040 A JPH02192040 A JP H02192040A JP 1103689 A JP1103689 A JP 1103689A JP 1103689 A JP1103689 A JP 1103689A JP H02192040 A JPH02192040 A JP H02192040A
Authority
JP
Japan
Prior art keywords
light
objective lens
recording medium
information recording
optical information
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
JP1103689A
Other languages
Japanese (ja)
Inventor
Masahiko Nakayama
昌彦 中山
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP1103689A priority Critical patent/JPH02192040A/en
Publication of JPH02192040A publication Critical patent/JPH02192040A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To accurately detect the tilt of an optical information recording medium by detecting the displacement of the condensing position of a 0-th order reflected light by means of an objective lens with a divided light receiving element. CONSTITUTION:When a parallel light flux from a light source side is made incident on an objective lens 50, a part of the light flux is made incident on an optical information recording medium 6 as 0-th order light (j), and when it is reflected as the parallel light flux, it is made incident on the objective lens 50 as the 0-th order reflected light. Further one part of it is diffracted to be a condensed light flux 1, and condensed to the light source side focal position of the objective lens 50. When the optical information recording medium 6 has the tilt, the condensing position of the condensed light flux 1 is shifted in the direction orthogonal to the optical axis of the objective lens 50 away from the focal position. That is, at a divided light receiving element 90, the position of a spot S shifts in the direction of either one light receiving part, a tilt detecting signal is obtained from the output of the light receiving part, and the corresponding relation between the tilt detecting signal and a tilt angle theta is obtained. Thus the tilt of the optical information recording medium 6 can be accurately detected.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、光ピックアップ装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to an optical pickup device.

[従来の技術] 光ピックアップ装置は、光情報記録媒体に情報の記録お
よび/または再生を行うための装置として知られている
[Prior Art] An optical pickup device is known as a device for recording and/or reproducing information on an optical information recording medium.

情報の記録および/または再生を適正に行うには、レー
ザー光源からの光束を対物レンズにより光情報記録媒体
の記録面上にスポット状に正しく集光させるためのフォ
ーカシング制御と、集光スポットに正しくトラック上を
辿らせるためのトラッキング制御とが必要である。
In order to record and/or reproduce information properly, it is necessary to control the focusing so that the beam from the laser light source is correctly focused into a spot on the recording surface of the optical information recording medium using the objective lens, and to properly focus the light beam on the focused spot. Tracking control is required to follow the track.

第5図は、従来から良く知られた光ピックアップ装置の
1例を要部のみ略示している。
FIG. 5 schematically shows only the essential parts of an example of a conventionally well-known optical pickup device.

第5図(I)に於いて、レーザー光源としての半導体レ
ーザー1からの光束は、カップリングレンズ2により平
行光束化されたのち、偏光ビームスプリッタ−3と17
4波長板4を透過して対物レンズ5に入射し、同レンズ
5の作用にて光情報記録媒体6の記録面上に略1μmの
径のスポット状に集光する。
In FIG. 5(I), a light beam from a semiconductor laser 1 as a laser light source is collimated by a coupling lens 2, and is then collimated by a polarizing beam splitter 3 and 17.
The light passes through the four-wavelength plate 4, enters the objective lens 5, and is focused by the action of the lens 5 into a spot having a diameter of approximately 1 μm on the recording surface of the optical information recording medium 6.

上記記録面による反射光は、対物レンズ5と1/4波長
板4を透過して再度偏光ビームスプリッタ−3に入射し
、同ビームスプリッタ−3により反射されて集光レンズ
7に入射し、同レンズを透過すると集束性の光束となる
The reflected light from the recording surface passes through the objective lens 5 and the quarter-wave plate 4, enters the polarizing beam splitter 3 again, is reflected by the beam splitter 3, enters the condensing lens 7, and enters the polarizing beam splitter 3 again. When the light passes through the lens, it becomes a convergent light beam.

この集束性の光束は、一部を2分割受光素子8で遮断さ
れて2分割受光素子9に入射する。
A portion of this convergent light beam is blocked by the two-split light receiving element 8 and enters the two-split light receiving element 9 .

そしてフォーカスエラー信号は、2分割受光素子8の端
縁部をナイフェツジとして、公知のナイフェツジ法によ
り2分割受光素子9から得られ、このフォーカスエラー
信号に基づき対物レンズ5を光軸方向へ変位させるサー
ボ制御でフォーカシング制御が行おれる。
The focus error signal is obtained from the two-split light receiving element 9 by a known knife method using the edge of the two-split light receiving element 8 as a knife, and a servo that displaces the objective lens 5 in the optical axis direction based on this focus error signal. Focusing control can be performed using the control.

一方、トラックエラー信号は2分割受光素子8から得ら
れる。2分割受光素子8は第5図(II)に示すように
受光面が受光部A、Bに2分割されており、各受光部A
、Bから光電変換出力a、bが得られるようになってい
る。受光部A、Bを分ける分割線はトラック方向に対応
している。
On the other hand, the track error signal is obtained from the two-split light receiving element 8. As shown in FIG. 5 (II), the two-split light receiving element 8 has a light receiving surface divided into two light receiving parts A and B, and each light receiving part A
, B can obtain photoelectric conversion outputs a and b. The dividing line that separates the light receiving sections A and B corresponds to the track direction.

さて、第6図を参照すると、光情報記録媒体6の記録面
にはトラックTrが形成され、トラック間はトラック案
内部Gにより分離されている。
Now, referring to FIG. 6, tracks Tr are formed on the recording surface of the optical information recording medium 6, and the tracks are separated by track guides G.

第6図(a)に示す状態では、光束はトラックTr上に
正しく集光しており、2分割受光素子8上における光強
度分布、即ちファーフィールド像FFIは2分割受光素
子8の受光部A、Bを分ける分割線に対して対称となる
。しかるに光束の集光状態が第6図(b)に示すように
トラックTrからトラック案内部Gの側にずれると、ト
ラックTrからの反射光と、これに対してπ/2の位相
差をもつトラック案内部Gからの反射光との干渉効果が
上記分割線に関して非対称となりファーフィールド像F
FIは第6図(b)に示すように集光スポットのずれた
側の光強度が大きくなる。従って受光部A、Bからの出
力a、bを電圧信号に変換してえられる電圧信号Va、
Vbからトラックエラー信号として(Va−vb)を構
成し、このトランクエラー信号をOとするようにサーボ
制御を行うことによって1〜ラツキング制御を行うこと
ができる。
In the state shown in FIG. 6(a), the light beam is correctly focused on the track Tr, and the light intensity distribution on the two-split light receiving element 8, that is, the far field image FFI is the light receiving part A of the two-segment light receiving element 8. , B are symmetrical with respect to the dividing line that separates them. However, when the convergence state of the light beam shifts from the track Tr to the track guide section G as shown in FIG. The interference effect with the reflected light from the track guide section G is asymmetrical with respect to the above dividing line, and the far field image F
In FI, as shown in FIG. 6(b), the light intensity increases on the side where the focused spot is shifted. Therefore, the voltage signal Va obtained by converting the outputs a and b from the light receiving sections A and B into voltage signals,
By configuring (Va-vb) as a track error signal from Vb and performing servo control to set this trunk error signal to O, 1 to racking control can be performed.

トラッキング制御の精度を劣化させる原因として光情報
記録媒体6の傾きによるトラックエラー信号のオフセッ
トがある。
An offset of the tracking error signal due to the inclination of the optical information recording medium 6 is a cause of deterioration of the accuracy of tracking control.

即ち、第7図(a)に示すように対物レンズ5の光軸に
対して光情報記録媒体6が傾いていないときは問題がな
いが、第7図(b)に示すように対物レンズ5の光軸に
対して光情報記録媒体6の記録面の法線方向がθだけ傾
くと、記録面からの反射光の主光線の方向は2θだけず
れ、対物レンズ5を透過したのちは、照明光束の主光線
に対し2fθだけずれる。ここにfは対物レンズ5の焦
点距離である。反射光束は結局、2分割受光素子8に対
しても2fθだけずれる。するとこのずれに伴い、受光
部A、Bの受光する光束断面積が互いに異なるものとな
るので、トラックずれによるファーフィールド像の変化
による出力a、bの変化の他に上記断面積変化による出
力変化が生じ、これがトラックエラー信号にオフセット
成分として入り込み、トラッキング制御の精度を劣化さ
せる。
That is, as shown in FIG. 7(a), there is no problem when the optical information recording medium 6 is not tilted with respect to the optical axis of the objective lens 5, but as shown in FIG. 7(b), the objective lens 5 When the normal direction of the recording surface of the optical information recording medium 6 is tilted by θ with respect to the optical axis of It is shifted by 2fθ with respect to the chief ray of the luminous flux. Here, f is the focal length of the objective lens 5. In the end, the reflected light beam is also shifted by 2fθ with respect to the two-split light receiving element 8. Then, due to this deviation, the cross-sectional areas of the light beams received by the light receiving sections A and B become different from each other, so in addition to the change in outputs a and b due to the change in the far field image due to the track deviation, the output change due to the above-mentioned change in cross-sectional area. This occurs and enters the tracking error signal as an offset component, degrading the accuracy of tracking control.

光情報記録媒体の傾きを考慮してトラッキング制御を補
正するには、光情報記録媒体の傾きが検出されねばなら
ない。
In order to correct the tracking control in consideration of the tilt of the optical information recording medium, the tilt of the optical information recording medium must be detected.

光情報記録媒体の傾きを検出する方法としては、従来特
開昭60−9018号公報に開示された方法や特公昭6
3−22369号公報に開示された方法が知られている
Conventional methods for detecting the tilt of an optical information recording medium include the method disclosed in Japanese Patent Application Laid-open No. 60-9018 and the method disclosed in Japanese Patent Publication No. 60-9018.
A method disclosed in Japanese Patent No. 3-22369 is known.

[発明が解決しようとする課題] 上記方法の内、前者の方法は、光ピックアップ装置に上
記傾きを検出するための専用の光源を必要とするため光
ピックアップ装置のコストが高く付くという問題がある
[Problem to be Solved by the Invention] Among the above methods, the former method requires a dedicated light source for detecting the above-mentioned tilt in the optical pickup device, which causes a problem that the cost of the optical pickup device is high. .

また、後者の方法はトラックエラー信号を発生させるた
めの受光素子の出力の直流成分を利用して傾きの検出を
行うが、上記直流成分には光情報記録媒体の傾きの情報
の他に、トラックの偏心成分の情報も含まれるので、正
確な傾きを検出するのは難しい。
In addition, the latter method detects the inclination by using the DC component of the output of the light receiving element to generate a track error signal, but in addition to the information on the inclination of the optical information recording medium, the DC component also includes information about the inclination of the optical information recording medium. It is difficult to accurately detect the inclination because it also includes information on eccentric components.

本発明は上述した事情に鑑みてなされたものであって、
その目的とする所はトラッキング制御の精度劣化の原因
となる光情報記録媒体の傾きを容易、且つ確実に検出し
うる機能を備えた新規な光ピックアップ装置の提供にあ
る。
The present invention was made in view of the above-mentioned circumstances, and
The objective is to provide a novel optical pickup device that has a function of easily and reliably detecting the tilt of an optical information recording medium, which causes deterioration in accuracy of tracking control.

[課題を解決するための手段] 以下、本発明を説明する。[Means to solve the problem] The present invention will be explained below.

本発明の光ピックアップ装置は、「レーザー光源からの
光束を光情報記録媒体上にスポット状に集光させるのに
、回折現象を利用する対物レンズを用いる」こと、「対
物レンズの光源側の焦点位置の近傍に、複数の受光部を
持つ分割受光素子を配備する」こと、「この分割受光素
子の各受光部からの出力を用いて上記光情報記録媒体の
傾き検出信号を構成するようにした」ことを特徴として
いる。
The optical pickup device of the present invention uses an objective lens that utilizes a diffraction phenomenon to condense a light beam from a laser light source into a spot on an optical information recording medium, and a focal point on the light source side of the objective lens. A divided light-receiving element having a plurality of light-receiving parts is arranged near the position of the divided light-receiving element, and the output from each light-receiving part of the divided light-receiving element is used to configure the tilt detection signal of the optical information recording medium. ”.

[作  用] レーザー光源からの光束を平行光束として、「回折現象
を利用する対物レンズ」即ち、マイクロフレネルレンズ
やフレネル輪帯レンズに入射させて光情報記録媒体の記
録面上に集光させると、対物レンスの透過光束には所謂
0次光として、回折の影響を受けない成分があり、この
0次光は平行光束として記録面に入射し、反射されて対
物レンズに入射する。この光束を0次反射光束とよぶ、
この0次反射光束が対物レンズに再入射すると、その一
部は、対物レンズの回折現象によるレンズ作用で対物レ
ンズの、光源側の焦点に集光する。
[Operation] When the light flux from a laser light source is made into a parallel light flux and is incident on an "objective lens that utilizes the diffraction phenomenon", that is, a micro Fresnel lens or a Fresnel zone lens, and is focused on the recording surface of an optical information recording medium. The light beam transmitted through the objective lens includes a so-called zero-order light component that is not affected by diffraction, and this zero-order light enters the recording surface as a parallel light beam, is reflected, and enters the objective lens. This luminous flux is called the zero-order reflected luminous flux.
When this zero-order reflected light flux re-enters the objective lens, a part of it is focused at the focal point of the objective lens on the light source side by the lens action due to the diffraction phenomenon of the objective lens.

光情報記録媒体が傾くと0次反射光の方向が対物レンズ
の光軸に対して傾くため、対物レンズによる0次反射光
の集光位置が変位する。この変位を分割受光素子により
検出することにより光情報記録媒体の傾きを精度良く検
出できる。
When the optical information recording medium is tilted, the direction of the zero-order reflected light is tilted with respect to the optical axis of the objective lens, so that the focusing position of the zero-order reflected light by the objective lens is displaced. By detecting this displacement using the divided light receiving elements, the tilt of the optical information recording medium can be detected with high accuracy.

[実施例コ 以下、具体的な実施例に即して説明する。[Example code] Hereinafter, description will be given based on specific examples.

第1図は、本発明の1実施例を要部のみ略示している。FIG. 1 schematically shows only the essential parts of one embodiment of the present invention.

繁雑をさけるため、混同の恐れかないと思われるものに
付いては第5図に於けると同一の符号を用いた。また、
本発明に直接関係しないフォーカシング制御に拘る部分
は図示を省略した。
To avoid complication, the same reference numerals as in Figure 5 have been used for items that are unlikely to cause confusion. Also,
Portions related to focusing control that are not directly related to the present invention are omitted from illustration.

実施例に於いて、本発明の特徴とするところは、対物レ
ンス50として、回折を利用したマイクロフレネルレン
ズが用いられ、この対物レンズ50の光源側の焦点位置
近傍に分割受光素子90が配備されている点にある。
In the embodiment, the feature of the present invention is that a micro Fresnel lens using diffraction is used as the objective lens 50, and a divided light receiving element 90 is arranged near the focal position of the objective lens 50 on the light source side. The point is that

分割受光素子90は光束を大きく遮光しない様に可及的
に小さいものを用いる。また、その支持手段(図示され
ず)も光束を成るべく遮光しない様なものを用いる。
The divided light-receiving element 90 is made as small as possible so as not to block the luminous flux to a large extent. Further, the supporting means (not shown) is also of a type that does not block the light beam as much as possible.

さて、第1図(a)に於いて光源側からの平行光束が対
物レンズ50に入射すると、光束の一部は0次光jとし
て、平行光束のまま光情報記録媒体6に入射し、平行光
束として反射されると0次反射光となって対物レンズ5
0に入射する。
Now, in FIG. 1(a), when a parallel light flux from the light source side enters the objective lens 50, a part of the light flux enters the optical information recording medium 6 as a parallel light flux as zero-order light j, and the parallel light flux enters the optical information recording medium 6 as a parallel light flux. When reflected as a light beam, it becomes a 0th-order reflected light and passes through the objective lens 5.
0.

また、入射光束の一部は対物レンズ50の回折作用によ
り、集束光束iとなって光情報記録媒体6に向かって集
光し、記録面で反射されると発散性の光束として再度対
物レンズ50に入射する。
Further, due to the diffraction effect of the objective lens 50, a part of the incident light flux becomes a convergent light flux i and condenses toward the optical information recording medium 6, and when reflected on the recording surface, it returns to the objective lens 50 as a divergent light flux. incident on .

この発散性の反射光束は対物レンズ50を透過すると一
部は0次光mとして発散を続けるが、残りは回折されて
戻り光にとなる。フォーカシング制御、トラッキング制
御、情報再生にはこの戻り光kを用いる。
When this diverging reflected light flux passes through the objective lens 50, a part continues to diverge as zero-order light m, but the rest is diffracted and becomes return light. This returned light k is used for focusing control, tracking control, and information reproduction.

さて0次反射光が対物レンズ50に入射すると、その一
部が回折されて集光光束1となって対物レンズ50の光
源側焦点位置に集光する。
Now, when the zero-order reflected light enters the objective lens 50, a part of it is diffracted and becomes a condensed light beam 1, which is condensed at the focal position of the objective lens 50 on the light source side.

この集光光束1を利用して光情報記録媒体6の傾きを検
出する。第1図(a)では、光情報記録媒体6に傾きが
なく、集束光束1は対物レンズ5oの光源側焦点の位置
に集光する。
The inclination of the optical information recording medium 6 is detected using this condensed light beam 1. In FIG. 1(a), the optical information recording medium 6 is not tilted, and the focused light beam 1 is focused at the focal point of the objective lens 5o on the light source side.

しかるに第1図(b)に示すように光情報記録媒体6に
傾きがあると、集束光束lの集光位置は上記焦点位置か
ら、対物レンズ50の光軸に直交する方向へずれる。そ
のずれ量は、第2図に示すように対物レンズ50の焦点
距離をf、光情報記録媒体6の傾き角をθとして2fO
である。
However, if the optical information recording medium 6 is tilted as shown in FIG. 1(b), the convergence position of the convergent light beam l shifts from the focal position in a direction perpendicular to the optical axis of the objective lens 50. As shown in FIG. 2, the amount of deviation is 2fO, where f is the focal length of the objective lens 50 and θ is the tilt angle of the optical information recording medium 6.
It is.

分割受光素子90は、第3図に示すように受光面が受光
部C,Dに分割された2分割受光素子であり、集束光束
1は、光情報記録媒体6に傾きがないとき、そのスポッ
トSが第3図(a)に示すように受光部C,Dに均等に
入射するが、光情報記録媒体6に傾きがあると、第3図
(b)に示すようにスポットSの位置が受光部C,Dの
何れか一方へずれる。そこで受光部C,Dからの出力c
、dを電圧信号として得られる電圧信号Vc、Vdから
傾き検出信号として(Vc−Vd)を構成し、この傾き
検出信号と傾き角θとの対応関係を実測により定めれば
傾き検出信号により、光情報記録媒体6の傾きを精度良
く検出できるので、この検出結果に応じてトラックエラ
ー信号のオフセット成分を補正すれば良好なトラッキン
グ制御を実現できる。
The divided light-receiving element 90 is a two-part light-receiving element whose light-receiving surface is divided into light-receiving parts C and D as shown in FIG. As shown in FIG. 3(a), spot S is equally incident on the light receiving sections C and D, but if the optical information recording medium 6 is tilted, the position of the spot S will be changed as shown in FIG. 3(b). It shifts to either the light receiving part C or D. Therefore, the output c from the light receiving parts C and D
, d are obtained as voltage signals Vc and Vd as a tilt detection signal (Vc-Vd), and if the correspondence relationship between this tilt detection signal and the tilt angle θ is determined by actual measurement, the tilt detection signal yields: Since the inclination of the optical information recording medium 6 can be detected with high precision, good tracking control can be achieved by correcting the offset component of the tracking error signal according to the detection result.

上に説明した実施例では、分割受光素子として2分割受
光素子を用いたが、これに限らず、例えば第4図に示す
ような4分割受光素子91を用いても良い。この4分割
受光素子91は受光部E、F。
In the embodiment described above, a two-divided light-receiving element is used as the divided light-receiving element, but the present invention is not limited to this, and for example, a four-divided light-receiving element 91 as shown in FIG. 4 may be used. This four-divided light receiving element 91 includes light receiving portions E and F.

G、Hから光電変換出力ey f+ gy )1を得る
ことができる。この出力を変換して得られる電圧信号を
Ve、Vf、Vg、Vhとする。これら電圧信号を用い
ると光情報記録媒体6の、互いに直交する2方向の傾き
を検出できる。
A photoelectric conversion output ey f+ gy )1 can be obtained from G and H. Let the voltage signals obtained by converting this output be Ve, Vf, Vg, and Vh. By using these voltage signals, the inclination of the optical information recording medium 6 in two mutually orthogonal directions can be detected.

即ち、第4図(a)の状態を、傾きのない状態(スポッ
トSが受光部E、F、G、Hに均等に入射しティる)と
すれば、(Ve+Vf)−(Vg+Vh)なる信号で一
方の方向の傾きを検出し、(Ve+Vg)−(Vf+V
h)なる信号で他方の方向の傾きを検出できるのである
That is, if the state shown in FIG. 4(a) is assumed to be a state with no inclination (the spot S is equally incident on the light receiving sections E, F, G, and H), a signal of (Ve + Vf) - (Vg + Vh) will be obtained. to detect the inclination in one direction, (Ve+Vg)-(Vf+V
The inclination in the other direction can be detected using the signal h).

[発明の効果] 以上、本発明によれば新規な光ピックアップ装置を提供
できる。この装置は、上記の如き構成となっているから
情報の記録や再生、フォーカシング制御やトラッキング
制御を行うのと同じ光源の光を利用して、容易且つ確実
に光情報記録媒体の傾きを検出できるので、上記傾きに
起因するトラックエラー信号のオフセット成分を有効に
補正して、良好なトラッキング制御を行うことが可能で
ある。
[Effects of the Invention] As described above, according to the present invention, a novel optical pickup device can be provided. Since this device has the above-mentioned configuration, it can easily and reliably detect the tilt of an optical information recording medium by using the light from the same light source used for information recording, reproduction, focusing control, and tracking control. Therefore, it is possible to effectively correct the offset component of the tracking error signal caused by the above-mentioned inclination and perform good tracking control.

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

第1図は、本発明の1実施例を説明するための図、第2
図および第3図は、光情報記録媒体の傾き検出を上記実
施例に即して説明するための図、第4図は、別実施例の
特徴部分を説明するための図、第5図乃至第7図は、従
来技術とその問題点を説明するための図である。 100.半導体レーザー、200.カップリンクレンズ
。 306.偏光ビムスプリッター、4.、.1/4波長板
、50゜0.マイクロフレネルレンズ、600.光情報
記録媒体、(S \ω を已 υ 咄 寸 (べ)
FIG. 1 is a diagram for explaining one embodiment of the present invention, and FIG.
3 and 3 are diagrams for explaining inclination detection of an optical information recording medium according to the above embodiment, FIG. 4 is a diagram for explaining characteristic parts of another embodiment, and FIGS. FIG. 7 is a diagram for explaining the prior art and its problems. 100. Semiconductor laser, 200. cup link lens. 306. Polarizing beam splitter, 4. ,. 1/4 wavelength plate, 50°0. Micro Fresnel lens, 600. Optical information recording medium, (S \ω 已υ

Claims (1)

【特許請求の範囲】 レーザー光源からの光束を光情報記録媒体上にスポット
状に集光させるのに、回折現象を利用する対物レンズを
用い、 上記対物レンズの光源側の焦点位置の近傍に、複数の受
光部を持つ分割受光素子を配備し、この分割受光素子の
各受光部からの出力を用いて上記光情報記録媒体の傾き
検出信号を構成するようにしたことを特徴とする、光ピ
ックアップ装置。
[Claims] An objective lens that utilizes a diffraction phenomenon is used to focus the light beam from a laser light source into a spot on an optical information recording medium, and near the focal position of the objective lens on the light source side, An optical pickup characterized in that a split light receiving element having a plurality of light receiving parts is provided, and the output from each light receiving part of the split light receiving element is used to configure the tilt detection signal of the optical information recording medium. Device.
JP1103689A 1989-01-20 1989-01-20 Optical pickup device Pending JPH02192040A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1103689A JPH02192040A (en) 1989-01-20 1989-01-20 Optical pickup device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1103689A JPH02192040A (en) 1989-01-20 1989-01-20 Optical pickup device

Publications (1)

Publication Number Publication Date
JPH02192040A true JPH02192040A (en) 1990-07-27

Family

ID=11766836

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1103689A Pending JPH02192040A (en) 1989-01-20 1989-01-20 Optical pickup device

Country Status (1)

Country Link
JP (1) JPH02192040A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH042322U (en) * 1990-04-17 1992-01-09
CN100405478C (en) * 2005-09-16 2008-07-23 上海乐金广电电子有限公司 Gradiometer in optical writing and playing apparatus and method thereof

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH042322U (en) * 1990-04-17 1992-01-09
CN100405478C (en) * 2005-09-16 2008-07-23 上海乐金广电电子有限公司 Gradiometer in optical writing and playing apparatus and method thereof

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