JP2879601B2 - Optical information recording / reproducing device - Google Patents

Optical information recording / reproducing device

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Publication number
JP2879601B2
JP2879601B2 JP22559290A JP22559290A JP2879601B2 JP 2879601 B2 JP2879601 B2 JP 2879601B2 JP 22559290 A JP22559290 A JP 22559290A JP 22559290 A JP22559290 A JP 22559290A JP 2879601 B2 JP2879601 B2 JP 2879601B2
Authority
JP
Japan
Prior art keywords
light
signal
recording
receiving element
divided
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 - Fee Related
Application number
JP22559290A
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Japanese (ja)
Other versions
JPH04106734A (en
Inventor
雅章 祖父江
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
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Priority to JP22559290A priority Critical patent/JP2879601B2/en
Publication of JPH04106734A publication Critical patent/JPH04106734A/en
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Publication of JP2879601B2 publication Critical patent/JP2879601B2/en
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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、光磁気ディスクなどの光学的記録媒体を用
いて情報の記録,再生,消去を行う光学的情報記録再生
装置に関する。
Description: TECHNICAL FIELD The present invention relates to an optical information recording / reproducing apparatus for recording, reproducing, and erasing information using an optical recording medium such as a magneto-optical disk.

(従来の技術) 従来の光学的情報記録再生装置の光ピックアップで
は、記録媒体上に約1.6μmの間隔で形成される情報ト
ラックに、対物レンズによるレーザ光ビームを直径約1
μmの微小なビームスポットに絞って照射し、情報の記
録,再生,消去を行う。このため、記録媒体と対物レン
ズの間隔を1μm程度の精度で約4mmの間隔で保ちなが
ら、前記情報トラックの略中央に0.1μm程度の精度で
ビームスポットを照射させる必要がある。
(Prior Art) In a conventional optical pickup of an optical information recording / reproducing apparatus, an information track formed at an interval of about 1.6 μm on a recording medium is irradiated with a laser beam by an objective lens having a diameter of about 1 μm.
Irradiation is performed by focusing on a fine beam spot of μm to record, reproduce, and erase information. For this reason, it is necessary to irradiate a beam spot with a precision of about 0.1 μm to approximately the center of the information track while maintaining a gap between the recording medium and the objective lens at a precision of about 1 μm and a spacing of about 4 mm.

また記録媒体は情報処理速度を向上させるために毎分
数千回転の高速で回転しており、記録媒体の面振れ、芯
振れなどによって情報トラックの位置変化が高速で発生
している。このため、対物レンズを焦点方向に駆動させ
るフォーカス制御、およびビームスポット位置を情報ト
ラックの直交方向に制御するトラッキング制御を行って
いる。この制御のためのエラー信号検出には、公知のプ
ッシュプル法,臨界角法,非点収差法,ナイフエッジ法
などが使用され、記録媒体からの反射光を分割受光素子
で受光し、この分割受光素子の分割された各素子からの
出力の差をとった差出力に基づいて前記制御を行ってい
る。
Further, the recording medium rotates at a high speed of several thousand rotations per minute in order to improve the information processing speed, and the position change of the information track occurs at a high speed due to the surface deflection, the core deflection and the like of the recording medium. Therefore, focus control for driving the objective lens in the focal direction and tracking control for controlling the beam spot position in the direction perpendicular to the information track are performed. A known push-pull method, a critical angle method, an astigmatism method, a knife edge method, or the like is used for detecting an error signal for this control. Light reflected from a recording medium is received by a divided light receiving element, and the divided light is received. The control is performed based on a difference output obtained by calculating a difference between outputs from the respective divided light receiving elements.

また光磁気記録方法では、記録媒体の磁気膜に着磁さ
せて記録を行い、再生はその磁化により照射するレーザ
光の偏光面が回転する力−回転を検出することによる記
録信号(RF信号)を読み出している。一般的には、複屈
折材料で構成されるウォラストンプリズムでRF信号を有
する記録媒体からのレーザ反射光を互いに直交する偏光
性を有するP波,S波に分離し、それぞれを分割受光素子
で受光して、電気信号に変換することでRF信号を取り出
している。
In the magneto-optical recording method, recording is performed by magnetizing a magnetic film of a recording medium, and reproduction is performed by detecting a force-rotation of a rotation of a polarization plane of a laser beam irradiated by the magnetization, and a recording signal (RF signal). Is being read. In general, a Wollaston prism composed of a birefringent material separates laser reflected light from a recording medium having an RF signal into P-waves and S-waves having polarization properties orthogonal to each other, and each of them is divided by a light-receiving element. The RF signal is extracted by receiving the light and converting it to an electric signal.

上述した信号検出方法は、情報トラックの位置変化に
対して検出感度が非常に高く、ビームスポットを高速
で、かつ高精度に制御できるものである必要がある。
The above-described signal detection method needs to have a very high detection sensitivity to a change in the position of the information track, and can control the beam spot at high speed and with high accuracy.

(発明が解決しようとする課題) 上記の従来技術において、検出感度を高くとるために
は、できるだけ多い光量で信号を電気信号に変換し、C/
N比を向上させる必要がある。
(Problems to be Solved by the Invention) In the above-mentioned conventional technology, in order to increase the detection sensitivity, a signal is converted into an electric signal with as much light as possible, and C /
It is necessary to improve the N ratio.

しかし従来技術では、トラッキングエラー信号,フォ
ーカスエラー信号,RF信号を検出するための光路系は、
別々に構成されており、記録媒体からの反射光をビーム
スプリッタ,ナイフエッジプリズム,ハーフミラーなど
の光学手段により分岐している。このため光学手段を経
るごとに光量減少を生じていた。
However, in the conventional technology, an optical path system for detecting a tracking error signal, a focus error signal, and an RF signal is:
The light reflected from the recording medium is split by optical means such as a beam splitter, a knife edge prism, and a half mirror. For this reason, the amount of light decreases every time the light passes through the optical means.

例えば、特開昭61−280034号公報に示された装置で
は、記録媒体からの限られた反射光を有効に活用するた
めに、反射光を各種の信号に共用して用いているが、光
磁気用ピックアップのかなりの光量が振り分けられるRF
信号において、光量の約50%しか共用されておらず、光
量を有効に利用していない。
For example, in the apparatus disclosed in Japanese Patent Application Laid-Open No. 61-280034, the reflected light is used commonly for various signals in order to effectively utilize the limited reflected light from the recording medium. RF that can distribute a considerable amount of light from a magnetic pickup
Only about 50% of the light amount is shared in the signal, and the light amount is not used effectively.

本発明の目的は、大きな光量によって、RF信号とトラ
ッキングエラー信号とを取り出すことができ、検出信号
の信頼性を高められる光学的情報記録再生装置を提供す
ることにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide an optical information recording / reproducing apparatus capable of extracting an RF signal and a tracking error signal with a large amount of light and improving the reliability of a detection signal.

(課題を解決するための手段) 上記の目的を達成するため、本発明は、光ビームを対
物レンズを介して記録媒体にビームスポットとして照射
し、記録媒体からの反射光を複屈折結晶を介して分割受
光素子に入射させ、前期反射光の記録情報による偏光面
の変角を前記複屈折結晶により偏光方向によって選択分
離して、前記分割受光素子によって得られる差出力によ
り記録信号を取り出す光学的情報記録再生装置におい
て、前記記録信号を取り出す反射光の光路中に設けられ
る非点収差発生手段を、前記分割受光素子の受光面で前
記反射光がその偏光成分の分割方向では集光され、かつ
前記分割方向に対して略直交するトラッキングエラー検
出方向には非集光となるように前記複屈折結晶近傍に設
置し、前記分割受光素子によって記録信号を取り出すと
ともにトラッキングエラー信号を取り出すことを可能に
したことを特徴とする。
(Means for Solving the Problems) In order to achieve the above object, the present invention irradiates a light beam as a beam spot on a recording medium via an objective lens, and reflects reflected light from the recording medium via a birefringent crystal. Optical splitting of the polarization plane by the recorded information of the reflected light is selectively separated by the birefringent crystal according to the polarization direction, and a recording signal is extracted by a difference output obtained by the split light receiving element. In the information recording / reproducing apparatus, astigmatism generating means provided in an optical path of reflected light for extracting the recording signal, the reflected light is condensed on a light receiving surface of the divided light receiving element in a direction in which the polarization component is divided, and It is installed near the birefringent crystal so as not to converge light in the tracking error detection direction that is substantially orthogonal to the division direction, and a recording signal is collected by the division light receiving element. And a tracking error signal can be extracted.

(作 用) 上記の手段を採用したため、RF信号とトラッキングエ
ラー信号とを、複屈折結晶と非点収差発生手段と分割受
光素子からなる一つの光学系(光路)によって検出で
き、従来に比べて、光量ロスが減少し、RF信号とトラッ
キングエラー信号を検出するための記録媒体からの反射
光光量を有効利用することが可能になる。
(Operation) By adopting the above means, the RF signal and the tracking error signal can be detected by one optical system (optical path) including the birefringent crystal, the astigmatism generating means, and the divided light receiving element. As a result, the light amount loss is reduced, and the amount of reflected light from the recording medium for detecting the RF signal and the tracking error signal can be effectively used.

(実施例) 以下、本発明の実施例を図面に基づいて説明する。(Example) Hereinafter, an example of the present invention will be described with reference to the drawings.

第1図は本発明の一実施例の構成図、第2図は第1図
の実施例の要部を示す斜視図であり、1はレーザダイオ
ード、2はカップリングレンズ、3はビームスプリッ
タ、4は対物レンズ、5は光磁気ディスクなどの記録媒
体、6は前記ビームスプリッタ3の光分岐路に設けられ
た集光レンズ、7はナイフエッジプリズム、8は2分割
されたフォーカス信号用分割受光素子、9は4分割(a
〜d)されたRF/トラッキング信号用分割受光素子、10
はナイフエッジプリズム7で反射された反射光を受ける
複屈折結晶であるウォラストンプリズム、11はウォラス
トンプリズム10の光が透過する対向面に設けられた非点
収差発生手段である一対のシリンドリカルレンズであ
る。
FIG. 1 is a structural view of one embodiment of the present invention, and FIG. 2 is a perspective view showing a main part of the embodiment of FIG. 1, wherein 1 is a laser diode, 2 is a coupling lens, 3 is a beam splitter, Reference numeral 4 denotes an objective lens, 5 denotes a recording medium such as a magneto-optical disk, 6 denotes a condenser lens provided in an optical branch of the beam splitter 3, 7 denotes a knife edge prism, and 8 denotes a divided light receiving device for a focus signal. The element 9 is divided into four parts (a
-D) divided photodetectors for RF / tracking signals, 10
Is a Wollaston prism that is a birefringent crystal that receives the light reflected by the knife edge prism 7; It is.

第1図において、レーザダイオード1からでたレーザ
光はカップリングレンズ2,ビームスプリッタ3,対物レン
ズ4を通り記録媒体5に集光し、記録媒体5にて反射さ
れた反射光は、再び対物レンズ4,ビームスプリッタ3へ
と進み、ビームスプリッタ3にて全光量または一部の光
量が検出系に向かい、検出系では集光レンズ6にて集光
させられ、ナイフエッジプリズム7によって、さらにフ
ォーカス信号用分割受光素子8とRF/トラッキング信号
用分割受光素子9へと分割される。また。RF/トラッキ
ング信号検出系ではウォラストンプリズム10にてP波成
分とS波成分に分離されRF/トラッキング信号用分割受
光素子9に集光されるが、第2図に示すように、ウォラ
ストンプリズム10を通過してRF/トラッキング信号用分
割受光素子9に入射する光は、シリンドリカルレンズ11
で受光素子面において光のP波成分,S波成分の分割方向
(矢印A方向)では集光点となり、トラッキングエラー
信号方向(矢印B方向)には集光点とならないような非
点収差を呈するようになる。これにより、下記の
(1),(2)式から、これまでRF信号にしか用いられ
ていなかった反射光からRF信号の特性を劣化させること
なくトラッキングエラー信号を取り出すことが可能とな
る。
In FIG. 1, a laser beam emitted from a laser diode 1 passes through a coupling lens 2, a beam splitter 3, and an objective lens 4 and is condensed on a recording medium 5, and the reflected light from the recording medium 5 is again reflected by the objective lens. The beam proceeds to the lens 4 and the beam splitter 3, and the entire or a part of the light amount is directed to the detection system by the beam splitter 3, is collected by the condenser lens 6 in the detection system, and is further focused by the knife edge prism 7. The signal is divided into a divided light receiving element for signal 8 and a divided light receiving element 9 for RF / tracking signal. Also. In the RF / tracking signal detection system, a P-wave component and an S-wave component are separated by a Wollaston prism 10 and condensed on an RF / tracking signal split light receiving element 9, as shown in FIG. The light passing through 10 and entering the split light receiving element 9 for RF / tracking signal is transmitted through a cylindrical lens 11.
In the surface of the light-receiving element, astigmatism such that it becomes a converging point in the direction of division of the P-wave component and S-wave component of light (direction of arrow A) and does not become a converging point in the tracking error signal direction (direction of arrow B) Will be presented. As a result, from the following equations (1) and (2), it is possible to extract the tracking error signal from the reflected light, which has been used only for the RF signal, without deteriorating the characteristics of the RF signal.

RF信号=(a+c)−(b+d) ……(1) トラッキングエラー信号=(a+b)−(c+d)…
…(2) 上記のトラッキングエラー信号の検出についてより具
体的に説明する。第3図(a),(b)に示す説明図の
ように、記録媒体5には多数のトラック溝5aが形成され
ていて、レーザ光の微小スポットSが溝5aの中心に位置
する必要がある。第3図(a)はスポットSが溝5aの中
心にある場合の反射光の強度分布を示し、第3図(b)
はスポットSが溝5aの中心から外れた場合の反射光の強
度分布を示しており、第3図(b)の状態ではスポット
Sが中心から外れ、溝5aの壁の部分で回折をおこし、ト
ラッキング方向に強度分布が非対称に変化して強度分布
差を発生する。この非対称性をRF/トラッキング信号用
分割受光素子9によって検出して、その非対称性を補正
する方向にスポットSの位置を変化させることによって
トラッキング制御が行われる。
RF signal = (a + c)-(b + d) (1) Tracking error signal = (a + b)-(c + d)
(2) The detection of the tracking error signal will be described more specifically. As shown in FIGS. 3A and 3B, a large number of track grooves 5a are formed in the recording medium 5, and the minute spot S of the laser beam needs to be located at the center of the groove 5a. is there. FIG. 3A shows the intensity distribution of the reflected light when the spot S is located at the center of the groove 5a, and FIG.
Shows the intensity distribution of the reflected light when the spot S deviates from the center of the groove 5a. In the state of FIG. 3 (b), the spot S deviates from the center and diffracts at the wall of the groove 5a. The intensity distribution changes asymmetrically in the tracking direction to generate an intensity distribution difference. This asymmetry is detected by the divided light receiving element 9 for RF / tracking signals, and tracking control is performed by changing the position of the spot S in a direction in which the asymmetry is corrected.

この場合、検出を行なうRF/トラッキング信号用分割
受光素子9を小さくした方が光ピックアップの小型化,
低価格化が行えることから、反射光をある程度集光して
RF/トラッキング用信号分割受光素子9の受光面のスポ
ットSの径を小さくする必要がある。しかし、前記受光
面で集光点にしてスポットSの径を最小となるようにし
た場合、反射光の強度分布が変化してトラッキングエラ
ー信号が乱れることになるので、前記受光面の位置は集
光点から十分離れた位置にするのが一般的である。
In this case, the size of the optical pickup is reduced by making the divided light receiving element 9 for RF / tracking signal for detection smaller.
Since the price can be reduced, the reflected light can be collected to some extent
It is necessary to reduce the diameter of the spot S on the light receiving surface of the signal splitting light receiving element 9 for RF / tracking. However, if the diameter of the spot S is minimized by setting the focal point on the light receiving surface, the intensity distribution of the reflected light changes and the tracking error signal is disturbed. Generally, the position is sufficiently far from the light spot.

次にRF信号の検出についてより具体的に説明する。RF
信号は記録媒体5に記録された磁化の方向を検知するこ
とで取り出される。記録媒体5の反射面は記録された磁
化の方向により照射されたレーザ光の偏光面を微小に回
転させる。この偏光面の回転が発生すると、ウォラスト
ンプリズム10に入射する光のP波成分とS波成分との光
量比が変化し、ウォラストンプリズム10によって、第4
図の説明図のように、P波成分とS波成分を分離し、そ
れぞれを検出することによって回転方向を測定して磁化
方向を検知できる。ウォラストンプリズム10は、偏光面
の方向により屈折率が違う特性を有する水晶などの複屈
折材料を組合せ、偏光面の違いによって光の進行方向を
変化させP波成分とS波成分とを分離させるものであ
り、ウォラストンプリズム10の分離角は任意に変えられ
るが、大きさの制限から分離角は0.5゜から2゜とする
のがよく、第2図のように分離角が小さくても分離が完
全に行わるように反射光を集光させてRF/トラッキング
信号用分割受光素子9に入射させるのがよい。
Next, detection of an RF signal will be described more specifically. RF
The signal is extracted by detecting the direction of the magnetization recorded on the recording medium 5. The reflection surface of the recording medium 5 slightly rotates the polarization plane of the irradiated laser beam according to the direction of the recorded magnetization. When this rotation of the polarization plane occurs, the light amount ratio between the P-wave component and the S-wave component of the light incident on the Wollaston prism 10 changes.
As shown in the diagram, the P-wave component and the S-wave component are separated from each other, and by detecting each component, the direction of rotation can be measured to detect the magnetization direction. The Wollaston prism 10 combines a birefringent material such as quartz having a characteristic in which the refractive index varies depending on the direction of the polarization plane, and changes the traveling direction of light by the difference in the polarization plane to separate the P wave component and the S wave component. Although the separation angle of the Wollaston prism 10 can be changed arbitrarily, the separation angle is preferably 0.5 ° to 2 ° due to size restrictions. Even if the separation angle is small as shown in FIG. It is preferable that the reflected light is condensed and made incident on the divided light receiving element 9 for RF / tracking signal so that the light is completely reflected.

上記の実施例において、従来ではRF信号,トラッキン
グ制御信号を別々の光学系で検出していたが、これを一
つの光学系(光路)で検出できるのでRF信号とトラッキ
ング制御信号の光量を増加させることが可能となる。本
件発明者のこれまでの経験によれば、光学的情報記録再
生装置の記録再生速度,記録密度の性能向上にはトラッ
キング信号とRF信号の信号量の増加が特に有効であるた
め、本実施例により光学的記録再生装置の性能向上を図
ることができる。また、一つの光学系にすることにより
光ピックアップを小型化でき、かつ構成部品の点数を減
少させる効果もある。
In the above embodiment, the RF signal and the tracking control signal are conventionally detected by separate optical systems. However, since these signals can be detected by one optical system (optical path), the amounts of the RF signal and the tracking control signal are increased. It becomes possible. According to the inventor's experience so far, it is particularly effective to improve the recording / reproducing speed and the recording density of the optical information recording / reproducing apparatus by increasing the signal amount of the tracking signal and the RF signal. Thus, the performance of the optical recording / reproducing apparatus can be improved. Further, by using one optical system, the size of the optical pickup can be reduced, and the number of components can be reduced.

(発明の効果) 以上説明したように、本発明によれば、一つの光学系
(光路)を用いてRF信号とトラッキングエラー信号を検
出できるため、情報媒体からの限られた反射光から光量
を減少させることなく信号検出ができ、信頼性の高い光
学的情報記録再生装置を提供できる。
(Effects of the Invention) As described above, according to the present invention, since the RF signal and the tracking error signal can be detected using one optical system (optical path), the light amount can be obtained from the limited reflected light from the information medium. A signal can be detected without reduction, and a highly reliable optical information recording / reproducing apparatus can be provided.

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

第1図は本発明の光学的情報記録再生装置の一実施例の
構成図、第2図は第1図の実施例の要部を示す斜視図、
第3図(a),(b)はトラッキングエラー信号検出の
説明図、第4図はウォラストンプリズムの説明図であ
る。 1……レーザダイオード、3……ビームスプリッタ、4
……対物レンズ、5……記録媒体、7……ナイフエッジ
プリズム、8……フォーカス信号用分割受光素子、9…
…RF/トラッキング信号用分割受光素子、10……複屈折
結晶、11……非点収差発生手段。
FIG. 1 is a configuration diagram of an embodiment of the optical information recording / reproducing apparatus of the present invention, FIG. 2 is a perspective view showing a main part of the embodiment of FIG.
3 (a) and 3 (b) are explanatory diagrams of tracking error signal detection, and FIG. 4 is an explanatory diagram of a Wollaston prism. 1 ... laser diode, 3 ... beam splitter, 4
... Objective lens, 5... Recording medium, 7... Knife edge prism, 8...
... Divided light receiving element for RF / tracking signal, 10 ... Birefringent crystal, 11 ... Astigmatism generation means.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】光ビームを対物レンズを介して記録媒体に
ビームスポットとして照射し、記録媒体からの反射光を
複屈折結晶を介して分割受光素子に入射させ、前記反射
光の記録情報による偏光面の変角を前記複屈折結晶によ
り偏光方向によって選択分離して、前記分割受光素子に
よって得られる差出力により記録信号を取り出す光学的
情報記録再生装置において、前記記録信号を取り出す反
射光の光路中に設けられる非点収差発生手段を、前記分
割受光素子の受光面で前記反射光がその偏光成分の分割
方向では集光され、かつ前記分割方向に対して略直交す
るトラッキングエラー検出方向には非集光となるように
前記複屈折結晶近傍に設置し、前記分割受光素子によっ
て記録信号を取り出すとともにトラッキングエラー信号
を取り出すことを可能にしたことを特徴とする光学的情
報記録再生装置。
A recording medium is irradiated with a light beam through an objective lens as a beam spot, and reflected light from the recording medium is made incident on a divided light receiving element via a birefringent crystal, and polarization of the reflected light according to recorded information is obtained. In an optical information recording / reproducing apparatus which selectively separates a deflection angle of a surface by a polarization direction by the birefringent crystal and extracts a recording signal by a difference output obtained by the divided light receiving element, the optical path of reflected light from which the recording signal is extracted The reflected light is condensed on the light-receiving surface of the divided light-receiving element in a direction in which the polarization component is divided, and is not reflected in a tracking error detection direction substantially orthogonal to the division direction. It is installed in the vicinity of the birefringent crystal so as to collect light, and the recording light signal is extracted by the divided light receiving element and the tracking error signal is extracted. The optical information recording and reproducing apparatus being characterized in that the capacity.
JP22559290A 1990-08-28 1990-08-28 Optical information recording / reproducing device Expired - Fee Related JP2879601B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22559290A JP2879601B2 (en) 1990-08-28 1990-08-28 Optical information recording / reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22559290A JP2879601B2 (en) 1990-08-28 1990-08-28 Optical information recording / reproducing device

Publications (2)

Publication Number Publication Date
JPH04106734A JPH04106734A (en) 1992-04-08
JP2879601B2 true JP2879601B2 (en) 1999-04-05

Family

ID=16831738

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22559290A Expired - Fee Related JP2879601B2 (en) 1990-08-28 1990-08-28 Optical information recording / reproducing device

Country Status (1)

Country Link
JP (1) JP2879601B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102411160A (en) * 2011-12-06 2012-04-11 福建福晶科技股份有限公司 Cylindrical polarization beam-splitting prism

Also Published As

Publication number Publication date
JPH04106734A (en) 1992-04-08

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