JP2744448B2 - Optical information recording / reproducing device - Google Patents

Optical information recording / reproducing device

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Publication number
JP2744448B2
JP2744448B2 JP63325295A JP32529588A JP2744448B2 JP 2744448 B2 JP2744448 B2 JP 2744448B2 JP 63325295 A JP63325295 A JP 63325295A JP 32529588 A JP32529588 A JP 32529588A JP 2744448 B2 JP2744448 B2 JP 2744448B2
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JP
Japan
Prior art keywords
light
optical information
optical
information recording
grating
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
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JP63325295A
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Japanese (ja)
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JPH02172030A (en
Inventor
茂 大内田
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Ricoh Co Ltd
Original Assignee
Ricoh Co Ltd
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Application filed by Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP63325295A priority Critical patent/JP2744448B2/en
Priority to US07/454,366 priority patent/US5015835A/en
Publication of JPH02172030A publication Critical patent/JPH02172030A/en
Application granted granted Critical
Publication of JP2744448B2 publication Critical patent/JP2744448B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Optical Head (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、光情報記録媒体を用いて情報の記録、再生
等を行う光情報記録再生装置に関する。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical information recording / reproducing apparatus for recording / reproducing information using an optical information recording medium.

従来の技術 従来、光情報記録再生装置に回折格子(グレーテイン
グ)を用いたものとしては、まず、第一の従来例として
特開昭61−230634号公報に開示されているものがある。
すなわち、第6図に示すように、半導体レーザ1から出
射されたレーザ光はコリメートレンズ2で平行化され、
偏光ビームスプリツタ3に入射する。この場合、その入
射光の偏光方向は偏光ビームスプリツタ3の溝と平行方
向の状態となるようにしてあるため回折して1/4波長板
4に入射し円偏光波となり、対物レンズ5により集光さ
れ光情報記録媒体としての光デイスク6に照射されこれ
により情報の記録が行われる。また、その光デイスク6
からの反射光は前記1/4波長板4で直線偏光波に変換さ
れこれにより偏光ビームスプリツタ3を透過し、光情報
検出光学系7に導かれ臨界角回折格子8に入射する。こ
こでは、その入射光は2回の臨界角回折と全反射を生じ
回折光となつて4分割された受光素子9に入射し、これ
によりそれら分割された受光素子9により差信号をとつ
てフオーカスエラー信号の検出や、トラツクエラー信号
の検出を行つている。
2. Description of the Related Art Conventionally, as an optical information recording / reproducing apparatus using a diffraction grating (grating), there is a first conventional example disclosed in JP-A-61-230634.
That is, as shown in FIG. 6, the laser light emitted from the semiconductor laser 1 is collimated by the collimator lens 2,
The light enters the polarization beam splitter 3. In this case, the polarization direction of the incident light is set to be in a state parallel to the groove of the polarization beam splitter 3, so that the light is diffracted and enters the quarter-wave plate 4 to become a circularly polarized wave. The light is condensed and applied to an optical disk 6 as an optical information recording medium, whereby information is recorded. In addition, the optical disk 6
The reflected light is converted into a linearly polarized wave by the 波長 wavelength plate 4, thereby transmitting through the polarization beam splitter 3, guided to the optical information detection optical system 7 and incident on the critical angle diffraction grating 8. Here, the incident light undergoes two critical angle diffractions and total reflection to form a diffracted light and is incident on the light receiving element 9 divided into four parts. The detection of a spill error signal and the detection of a track error signal are performed.

また、第二の従来例として、第7図に示すように、デ
ユアルグレーテイング10を用いたものがある。すなわ
ち、半導体レーザ11からの出射光はコリメートレンズ12
により平行化された後、2枚の整形プリズム13を介して
ビームスプリツタ14により反射され対物レンズ15により
集光され光磁気デイスク16に照射され、これにより情報
の記録が行われる。また、この光磁気デイスク16からの
反射光は前記ビームスプリツタ14を透過して光情報検出
光学系17に導かれ、集光レンズ18により集光されデユア
ルグレーテイング10の表裏面にそれぞれ形成されたグレ
ーテイング19を透過又は回折する。このうち、透過して
そのまま直進した0次光Tは4分割受光素子20に導か
れ、回折された1次光Kは2分割受光素子21に導かれ
る。そして、光磁気信号は0次光Tと1次光Kとの光量
差により検出し、また、フオーカスエラー信号は0次光
Tを用い非点収差法により検出し、トラツクエラー信号
は1次光Kを用いプシユプル法等により検出する。
As a second conventional example, as shown in FIG. 7, there is one using a dual grating 10. That is, the light emitted from the semiconductor laser 11 is
After being collimated, the light is reflected by the beam splitter 14 via the two shaping prisms 13 and condensed by the objective lens 15 to irradiate the magneto-optical disk 16, whereby information is recorded. The reflected light from the magneto-optical disk 16 passes through the beam splitter 14 and is guided to the optical information detection optical system 17, where it is collected by the condenser lens 18 and formed on the front and back surfaces of the dual grating 10 respectively. Is transmitted or diffracted. Of these, the zero-order light T that has passed through and travels straight as it is is guided to the four-divided light receiving element 20, and the diffracted first-order light K is guided to the two-divided light receiving element 21. The magneto-optical signal is detected based on the difference in light amount between the 0th-order light T and the 1st-order light K, the focus error signal is detected by the astigmatism method using the 0th-order light T, and the track error signal is detected by the 1st-order light. It is detected by the push-pull method using light K.

発明が解決しようとする課題 まず、第一の従来例では、追記型の光デイスク及びCD
には適用できるが、光磁気デイスクの信号検出には適用
することができず、また、このような従来の構成ではグ
レーテイングに付随して生じる波長変動に応じて回折角
度が変動する問題を解決することができない。また、第
二の従来例では、デユアルグレーテイングを透過、回折
した0次光及び1次光のビーム間隔の精度が悪いためス
ポツト位置のズレが生じやすく、その結果、信号検出に
誤差が生じやすくなり、光情報信号検知器の配置も厳密
な寸法精度をもって行なわなければならないものであ
る。
Problems to be Solved by the Invention First, in the first conventional example, a write-once optical disc and a CD
However, it cannot be applied to signal detection of magneto-optical disks, and the conventional configuration solves the problem that the diffraction angle fluctuates according to the wavelength fluctuation accompanying the grating. Can not do it. Further, in the second conventional example, the accuracy of the beam interval between the 0th-order light and the 1st-order light transmitted and diffracted through the dual grating is poor, so that the spot position is likely to shift, and as a result, an error is likely to occur in signal detection. That is, the arrangement of the optical information signal detector must be performed with strict dimensional accuracy.

課題を解決するための手段 半導体レーザから出射されたレーザ光を光情報記録媒
体に照射して情報の記録を行うと共に、その光情報記録
媒体からの反射光を集光レンズにより集光して光情報検
出光学系に導き情報の再生や、トラツクエラー信号及び
フオーカスエラー信号を検出する光情報記録再生装置に
おいて、前記光情報記録媒体により反射され前記集光レ
ンズにより集光された光の光路上に、一面に等ピツチの
直線状をした第一回折格子が形成されこの面と相対する
側の面にピツチの異なる同心円状をなす第二回折格子が
形成されたデユアルグレーテイングを配設し、このデユ
アルグレーテイングにより、回折されて進む1次光の光
路上に配置された少なくとも3分割された第一受光素子
と回折されずに直進する0次光の光路上に配置された少
なくとも3分割された第二受光素子とを有する光情報信
号検知器を設けた。
Means for Solving the Problems A laser beam emitted from a semiconductor laser is irradiated on an optical information recording medium to record information, and reflected light from the optical information recording medium is condensed by a condensing lens to generate light. In an optical information recording / reproducing apparatus for guiding information to an information detection optical system and reproducing information, and detecting a track error signal and a focus error signal, an optical information recording / reproducing apparatus is provided on an optical path of light reflected by the optical information recording medium and condensed by the condenser lens. A dual grating in which a first diffraction grating having an equal pitch linear shape is formed on one surface, and a concentric second diffraction grating having a different pitch is formed on a surface opposite to this surface, Due to this dual grating, at least three divided first light receiving elements arranged on the optical path of the primary light diffracted and traveling are arranged on the optical path of the zero-order light traveling straight without being diffracted. And an optical information signal detector having at least three divided second light receiving elements.

作用 デユアルグレーテイングの両面に形成される回折格子
のうち一方の第二回折格子に同心円状をしたピツチの異
なる形状にして集光機能をもたせるようにしたことによ
り、0次光と1次光との結像点の光軸方向に対する距離
間隔を広くとることができ、光情報記録再生器の配置を
容易に行なうことができる。
The concentrating pitch of one of the diffraction gratings formed on both surfaces of the dual grating is made different from that of the concentric pitch so that the zeroth-order light and the first-order light can be obtained. Can be widened in the direction of the optical axis, and the optical information recording / reproducing device can be easily arranged.

実施例 本発明の一実施例の基礎となる構成を第1図ないし第
4図(a)(b)(c)に基づいて説明する。なお、こ
こでは、本発明に係る光情報検出光学系についてのみ述
べる。
Embodiment A basic structure of an embodiment of the present invention will be described with reference to FIGS. 1 to 4 (a), (b) and (c). Here, only the optical information detection optical system according to the present invention will be described.

デユアルグレーテイング22は、平行平板型をしてお
り、集光レンズ23に位置する側の面に等ピツチの直線状
をした第一回折格子24が形成され、これと相対する側の
面に同様な等ピツチの直線状をした第二回折格子25が形
成されている。このデユアルグレーテイング22は、光情
報記録媒体としての図示しない光磁気デイスクから反射
された光が光情報検出光学系26の集光レンズ23により集
光された光路上に位置して設けられている。また、これ
ら第一回折格子24及び第二回折格子25を有するデユアル
グレーテイング22を通過して2分割された0次光T及び
1次光Kのうち、1次光Kの光路上に位置して受光面a,
b,cをもつ第一受光素子27が配置され、0次光Tの光路
上に位置して受光面d,e,fをもつ第二受光素子28が配置
された光情報信号検知器29が設けられている。この場
合、光情報信号検知器29は、1次光Kの集光点Pの後方
に位置し、しかも、0次光Tの集光点Qの前方に位置す
る、PQ間に挟まれた状態になつている。
The dual grating 22 has a parallel plate shape, and a first diffraction grating 24 having a straight line of equal pitch is formed on a surface on the side located on the condenser lens 23, and a similar surface is formed on a surface on the side opposite to this. A second diffraction grating 25 having a substantially equal pitch linear shape is formed. The dual grating 22 is provided on an optical path where light reflected from a not-shown magneto-optical disc as an optical information recording medium is condensed by the condenser lens 23 of the optical information detection optical system 26. . Further, of the 0th-order light T and the 1st-order light K that have passed through the dual grating 22 having the first diffraction grating 24 and the second diffraction grating 25, they are located on the optical path of the 1st-order light K. Light receiving surface a,
An optical information signal detector 29 in which a first light receiving element 27 having b, c is disposed, and a second light receiving element 28 having light receiving surfaces d, e, f positioned on the optical path of the zero-order light T is disposed. Is provided. In this case, the optical information signal detector 29 is located behind the converging point P of the primary light K and is located in front of the converging point Q of the 0th-order light T and is sandwiched between PQs. It has become.

このような構成において、光磁気デイスクからの反射
光は光情報検出光学系26内の集光レンズ23により集光さ
れ収束光となり、この状態でデユアルグレーテイング22
の第一回折格子24に入射しその偏光方向成分毎に分離さ
れ、回折しないで直進する0次光Tと回折されて進む1
次光Kとの2つの光に分離される。さらに、0次光Tは
第二回折格子25により回折されずそのまま直進してい
き、1次光Kはその第二回折格子25によりさらに回折さ
れて進んでいく。そして、第一,第二回折格子24,25は
共に収束機能をもたないため、それら0次光T及び1次
光Kの集光位置は集光レンズ23により決定され、集光点
P,Qの位置にそれぞれ結像する。この場合、1次光Kは
回折されるため光路長が0次光Tに比べ多少長くなり、
その分、集光点Pの位置は前方となる。そして、これら
2つの集光点P,Qの間に位置して配置された光情報信号
検知器29の第一受光素子27及び第二受光素子28に、0次
光T及び1次光Kを第3図に示すようにそれぞれ入射さ
せることにより、第一受光素子27には1次光Kの収束後
の状態のビームが照射され、また、第二受光素子28には
0次光Tの収束前の状態のビームが照射されることにな
る。
In such a configuration, the reflected light from the magneto-optical disk is converged by the converging lens 23 in the optical information detection optical system 26 to become convergent light. In this state, the dual grating 22
Incident on the first diffraction grating 24, and is separated for each polarization direction component thereof.
It is split into two lights, the next light K. Further, the zero-order light T travels straight without being diffracted by the second diffraction grating 25, and the first-order light K is further diffracted by the second diffraction grating 25 and proceeds. Since the first and second diffraction gratings 24 and 25 do not have a convergence function, the condensing positions of the zero-order light T and the first-order light K are determined by the converging lens 23,
An image is formed at each of the positions P and Q. In this case, since the primary light K is diffracted, the optical path length is slightly longer than that of the zero-order light T,
As a result, the position of the converging point P is forward. Then, the 0th-order light T and the 1st-order light K are applied to the first light receiving element 27 and the second light receiving element 28 of the optical information signal detector 29 located between these two converging points P and Q. 3, the first light receiving element 27 is irradiated with a beam in a state after the primary light K is converged, and the second light receiving element 28 is converged with the zero order light T. The beam in the previous state will be irradiated.

そこで、今、フオーカスエラー信号、トラツクエラー
信号、光磁気信号を検出する方法について説明する。ま
ず、フオーカスエラー信号を検出する場合、初期の合焦
点の位置にある時には第一受光素子27及び第二受光素子
28にそれぞれ照射される0次光T及び1次光Kのスポツ
ト径は第4図(b)に示すように共に等しい大きさであ
るが、光磁気デイスクの焦点位置がズレると第4図
(a)に示すように前方にピントがズレている時には0
次光Tのスポツト径は小さくなり1次光Kのスポツト径
は大きくなり、これとは逆に、第4図(c)に示すよう
に後方にピントがズレている時には0次光Tのスポツト
径は大きくなり1次光Kのスポツト径は小さくなる。こ
のように光磁気デイスクの焦点位置がズレると2つのス
ポツト径は相反するように変化する関係を利用して、
(a+c−b)−(d+f−e)を求めることによつて
フオーカスエラー信号を検出することができる。また、
3分割された受光素子27,28のうち両側の光量差を利用
して、(a+d)−(c+f)を求めることによりトラ
ツクエラー信号を検出することができる。さらに、受光
素子27,28の光量差、すなわち、0次光と1次光との光
量差(a+b+c)−(d+e+f)を求めることによ
り光磁気信号を検出することができる。
Therefore, a method for detecting a focus error signal, a track error signal, and a magneto-optical signal will now be described. First, when a focus error signal is detected, the first light receiving element 27 and the second light receiving element
The spot diameters of the 0th-order light T and the 1st-order light K applied to each of the light-emitting elements 28 are equal to each other as shown in FIG. 4 (b). When the camera is out of focus as shown in FIG.
The spot diameter of the next-order light T becomes smaller and the spot diameter of the first-order light K becomes larger. On the contrary, as shown in FIG. The diameter increases and the spot diameter of the primary light K decreases. By utilizing the relationship that the two spot diameters change so as to be contradictory when the focal position of the magneto-optical disc shifts,
By calculating (a + c−b) − (d + fe), a focus error signal can be detected. Also,
The track error signal can be detected by obtaining (a + d)-(c + f) using the light quantity difference between both sides of the light receiving elements 27 and 28 divided into three. Further, a magneto-optical signal can be detected by obtaining a light amount difference between the light receiving elements 27 and 28, that is, a light amount difference (a + b + c)-(d + e + f) between the zero-order light and the primary light.

次に、前述の構造に基づいて形成された本発明の一実
施例を第5図(a)(b)(c)に基づいて説明する。
これは、デユアルグレーテイング22に形成される片方の
回折格子の表面形状を変えた場合の例である。すなわ
ち、デユアルグレーテイング22は、集光レンズ23に位置
する側の第一回折格子24は前述の場合と変わらず等ピツ
チの直線形状となつているが、これと反対側に位置する
第二回折格子30はピツチの異なる同心円状の一部をなす
ように形成されている。従つて、集光レンズ23以外にこ
のようなピツチの異なる同心円状をなす第二回折格子30
を設け集光機能をもたせたことによつて回折される1次
光Kはより一層手前の位置に集光点Pをもつようになる
ため、その分、3分割された受光素子27,28をもつ光情
報信号検知器29の配置に裕度をもたせることができる。
Next, an embodiment of the present invention formed based on the above-described structure will be described with reference to FIGS. 5 (a), (b) and (c).
This is an example in which the surface shape of one diffraction grating formed on the dual grating 22 is changed. That is, in the dual grating 22, the first diffraction grating 24 on the side located on the condenser lens 23 has the same pitch linear shape as in the above case, but the second diffraction grating located on the opposite side is The grating 30 is formed so as to form a part of a concentric circle having different pitches. Therefore, in addition to the condenser lens 23, such a concentric second diffraction grating 30 having a different pitch is used.
The primary light K diffracted by providing the light condensing function has the light converging point P at a position further in front, and accordingly, the light receiving elements 27 and 28 divided into three parts are provided. The optical information signal detector 29 can be provided with a margin.

また、本実施例の応用として、集光レンズ23の焦点距
離を短くして光情報検出光学系26全体の構成の小型化を
図ろうとする場合、第1図のような構成で0次光Tに非
点収差が発生し、信号検出の際に無視できないほどの悪
影響を及ぼすことも考えられるため、このような時には
片面の第二回折格子30をピツチの異なる曲線形状にする
ことによつて1次光Kにも非点収差を発生させ相殺して
検出される信号への悪影響を除去し、これにより小型化
を図ることも可能となる。ただし、この場合、1次光K
だけに集光機能を持たせるとその収束の状態が0次光T
と異なりスポツト径の変化の仕方が同じでなくなるた
め、信号検出後の電気的な補正も考慮しなければならな
い。
As an application of this embodiment, when the focal length of the condenser lens 23 is to be shortened to reduce the overall configuration of the optical information detection optical system 26, the zero-order light T In this case, astigmatism may occur, which may have a considerable effect on signal detection. In such a case, the second diffraction grating 30 on one side may be formed into a curved shape having a different pitch. Astigmatism is also generated in the next light K, and an adverse effect on a signal detected by canceling out the astigmatism is removed, thereby making it possible to reduce the size. However, in this case, the primary light K
If only the light condensing function is provided, the convergence state will be zero-order light T
Unlike this, the way of changing the spot diameter is not the same, so that electrical correction after signal detection must be considered.

発明の効果 本発明は上述のように、半導体レーザから出射された
レーザ光を光情報記録媒体に照射して情報の記録を行う
と共に、その光情報記録媒体からの反射光を集光レンズ
により集光して光情報検出光学系に導き情報の再生や、
トラツクエラー信号及びフオーカスエラー信号を検出す
る光情報記録再生装置において、前記光情報記録媒体に
より反射され前記集光レンズにより集光された光の光路
上に、一面に等ピツチの直線状をした第一回折格子が形
成されこの面と相対する側の面にピツチの異なる同心円
状をなす第二回折格子が形成されたデユアルグレーテイ
ングを配設し、このデユアルグレーテイングにより、回
折されて進む1次光の光路上に配置された少なくとも3
分割された第一受光素子と回折されずに直進する0次光
の光路上に配置された少なくとも3分割された第二受光
素子とを有する光情報信号検知器を設けたので、デユア
ルグレーテイングの片面をピツチの異なる曲線形状にし
て1状光に集光させる機能をもたることで0次光及び1
次光の集光点の光軸方向に対する距離間隔を広くとるこ
とができ、これにより3分割された受光素子をもつ光情
報信号検知器の配置を容易に行うことができると云う効
果を有するものである。
As described above, the present invention irradiates laser light emitted from a semiconductor laser onto an optical information recording medium to record information, and collects reflected light from the optical information recording medium by a condenser lens. It shines to the optical information detection optical system and reproduces information,
In an optical information recording / reproducing apparatus for detecting a track error signal and a focus error signal, an equal pitch linear shape is formed on an optical path of light reflected by the optical information recording medium and condensed by the condenser lens. A dual grating in which a first diffraction grating is formed and a concentric second diffraction grating having a different pitch is formed on a surface opposite to this surface is arranged, and the dual grating is diffracted by the dual grating. At least 3 arranged on the optical path of the next light
Since the optical information signal detector having the divided first light receiving element and at least three divided second light receiving elements disposed on the optical path of the zero-order light that travels straight without being diffracted is provided, The function of condensing one-sided light with curved surfaces having different pitches on one side enables the zero-order light and the
The distance between the condensing points of the next light in the optical axis direction can be widened, so that an optical information signal detector having a light receiving element divided into three can be easily arranged. It is.

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

第1図は本発明の一実施例の基礎となる構成を示す光情
報検出光学系の平面図、第2図(a)は第一回折格子の
正面図、第2図(b)はデユアルグレーテイングの側面
図、第2図(c)は第二回折格子の正面図、第3図は光
情報信号検知器の正面図、第4図(a)(b)(c)は
フオーカスエラー信号の検出原理を示す説明図、第5図
(a)は本発明の一実施例を示す第一回折格子の正面
図、第5図(b)はそのデユアルグレーテイングの側面
図、第5図(c)はその第二回折格子の正面図、第6図
は第一の従来例を示す平面図、第7図(a)は第二の従
来例を示す平面図、第7図(b)はその各種信号の検出
回路を示す回路図である。 22……デユアルグレーテイング、23……集光レンズ、24
……第一回折格子、27……第一受光素子、28……第二受
光素子、29……光情報信号検知器、30……第二回折格
子、K……1次光、T……0次光
FIG. 1 is a plan view of an optical information detecting optical system showing a basic structure of one embodiment of the present invention, FIG. 2 (a) is a front view of a first diffraction grating, and FIG. 2 (b) is a dual gray. FIG. 2 (c) is a front view of the second diffraction grating, FIG. 3 is a front view of the optical information signal detector, and FIGS. 4 (a), (b) and (c) are focus error signals. FIG. 5 (a) is a front view of a first diffraction grating showing an embodiment of the present invention, FIG. 5 (b) is a side view of the dual grating, and FIG. c) is a front view of the second diffraction grating, FIG. 6 is a plan view showing a first conventional example, FIG. 7 (a) is a plan view showing a second conventional example, and FIG. FIG. 3 is a circuit diagram showing a detection circuit for various signals. 22 ... Dual grating, 23 ... Condenser lens, 24
... first diffraction grating, 27 ... first light receiving element, 28 ... second light receiving element, 29 ... optical information signal detector, 30 ... second diffraction grating, K ... primary light, T ... 0th order light

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】半導体レーザから出射されたレーザ光を光
情報記録媒体に照射して情報の記録を行うと共に、その
光情報記録媒体からの反射光を集光レンズにより集光し
て光情報検出光学系に導き情報の再生や、トラツクエラ
ー信号及びフオーカスエラー信号を検出する光情報記録
再生装置において、前記光情報記録媒体により反射され
前記集光レンズにより集光された光の光路上に、一面に
等ピツチの直線状をした第一回折格子が形成されこの面
と相対する側の面にピツチの異なる同心円状をなす第二
回折格子が形成されたデユアルグレーテイングを配設
し、このデユアルグレーテイングにより、回折されて進
む1次光の光路上に配置された少なくとも3分割された
第一受光素子と回折されずに直進する0次光の光路上に
配置された少なくとも3分割された第二受光素子とを有
する光情報信号検知器を設けたことを特徴とする光情報
記録再生装置。
An optical information recording medium is recorded by irradiating a laser beam emitted from a semiconductor laser onto an optical information recording medium, and light reflected from the optical information recording medium is collected by a condenser lens to detect optical information. In an optical information recording / reproducing apparatus for guiding information to an optical system and reproducing information, and detecting a track error signal and a focus error signal, an optical path of light reflected by the optical information recording medium and condensed by the condenser lens is provided on the optical path. A dual grating in which a first diffraction grating having an equal pitch linear shape is formed on one surface, and a concentric second diffraction grating having a different pitch is formed on a surface opposite to this surface is provided. Due to the grating, at least three divided first light receiving elements disposed on the optical path of the primary light diffracted and traveling at least are disposed on the optical path of the zero-order light traveling straight without being diffracted. 3 divided optical information recording and reproducing apparatus characterized by comprising an optical information signal detector and a second light receiving element.
JP63325295A 1988-12-23 1988-12-23 Optical information recording / reproducing device Expired - Fee Related JP2744448B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP63325295A JP2744448B2 (en) 1988-12-23 1988-12-23 Optical information recording / reproducing device
US07/454,366 US5015835A (en) 1988-12-23 1989-12-21 Optical information reading and writing device with diffraction means

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63325295A JP2744448B2 (en) 1988-12-23 1988-12-23 Optical information recording / reproducing device

Publications (2)

Publication Number Publication Date
JPH02172030A JPH02172030A (en) 1990-07-03
JP2744448B2 true JP2744448B2 (en) 1998-04-28

Family

ID=18175220

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63325295A Expired - Fee Related JP2744448B2 (en) 1988-12-23 1988-12-23 Optical information recording / reproducing device

Country Status (1)

Country Link
JP (1) JP2744448B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2761180B2 (en) * 1993-06-30 1998-06-04 株式会社リコー Micro displacement measuring device and optical pickup device

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63209029A (en) * 1987-02-25 1988-08-30 Fujitsu Ltd Optical pick-up device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63209029A (en) * 1987-02-25 1988-08-30 Fujitsu Ltd Optical pick-up device

Also Published As

Publication number Publication date
JPH02172030A (en) 1990-07-03

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