JPH0271201A - Diffraction grating element for optical information reproducing device - Google Patents

Diffraction grating element for optical information reproducing device

Info

Publication number
JPH0271201A
JPH0271201A JP63224130A JP22413088A JPH0271201A JP H0271201 A JPH0271201 A JP H0271201A JP 63224130 A JP63224130 A JP 63224130A JP 22413088 A JP22413088 A JP 22413088A JP H0271201 A JPH0271201 A JP H0271201A
Authority
JP
Japan
Prior art keywords
diffraction grating
light source
light
optical information
optical axis
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.)
Granted
Application number
JP63224130A
Other languages
Japanese (ja)
Other versions
JP2794114B2 (en
Inventor
Michitaka Okuda
通孝 奥田
Kiyoshi Matsui
清 松井
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.)
Kyocera Corp
Original Assignee
Kyocera Corp
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 Kyocera Corp filed Critical Kyocera Corp
Priority to JP63224130A priority Critical patent/JP2794114B2/en
Publication of JPH0271201A publication Critical patent/JPH0271201A/en
Application granted granted Critical
Publication of JP2794114B2 publication Critical patent/JP2794114B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To facilitate control among respective members and to reduce the number of parts and the production cost by irradiating a diffraction grating with the reproducing light to record interference fringes on the diffraction grating so that a specific reproducing condition is satisfied and obtaining a least circle of confusion. CONSTITUTION:Two spot light sources which emit light whose wavelengths are different from the wavelength of the light emitted from a light source for reproducing are provided, and a first spot light source is arranged in a prescribed position on the optical axis, and a second spot light source is arranged in a prescribed position on an axis which forms a prescribed angle with the optical axis, and the diffraction grating is irradiated by both spot light sources to record interference fringes. In this case, the reproducing condition satisfies an inequality I. Consequently, a part of the light transmitted through the diffraction grating element is diffracted to become astigmatic light, and a satisfactory least circle of confusion is formed in a position distance from the origin. Thus, the control among respective members is easily performed.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、光デイスク装置、光測定器等の光学式情報再
生装置に関し、特に該光学式情報再生装置に用いる回折
格子素子を改良した光学式情報再生装置用回折格子素子
に関するものである。
Detailed Description of the Invention [Field of Industrial Application] The present invention relates to an optical information reproducing device such as an optical disk device or an optical measuring device, and particularly to an optical information reproducing device with an improved diffraction grating element used in the optical information reproducing device. The present invention relates to a diffraction grating element for a type information reproducing device.

〔従来の技術〕[Conventional technology]

第3図(a)、(b)は従来の光学式情報再生装置を示
す図である。
FIGS. 3(a) and 3(b) are diagrams showing a conventional optical information reproducing device.

ここで同図(a)に示す光学式情報再生装置にあっては
、半導体レーザ100から放射されたレーザ光は、回折
格子101とコリメータ103とPBS105と1/4
波長板107と複数の各種レンズからなる対物レンズ1
09を通過して光ディスク等の光学式情報記録媒体11
1上で集光され且つ反射きれる。該反射されたレーザ光
は再び対物レンズ109と1/4波長板107を通過し
てPBS105に入射し、そのレーザ光の一部は直角方
向に反射きれる。そして該反射光は円柱レンズ113と
凹レンズ115を通過して6分割光検出器117に至り
、該6分割光検出器117により記録情報信号、フォー
カス誤差信号、トランキング誤差信号を検出する。
Here, in the optical information reproducing device shown in FIG.
Objective lens 1 consisting of a wavelength plate 107 and a plurality of various lenses
09 and optical information recording medium 11 such as an optical disk.
The light is condensed and reflected on 1. The reflected laser light passes through the objective lens 109 and the quarter-wave plate 107 again and enters the PBS 105, and a portion of the laser light is reflected in the right angle direction. The reflected light passes through a cylindrical lens 113 and a concave lens 115 and reaches a six-divided photodetector 117, where the six-divided photodetector 117 detects a recording information signal, a focus error signal, and a trunking error signal.

また同図(b)の構造の光学式情報再生装置にあっては
、半導体レーザ119から放射されたレーザ光は、ハー
フミラ−121によってその一部の光が直角方向に反射
され、さらに該反射された光は対物レンズ123を通過
して光ディスク等の光学式情報記録媒体125上で集光
され且つ反射きれる。そして該反射されたレーザ光は再
び対物レンズ123を通過し、またハーフミラ−121
と凹レンズ127を通過した後に4分割光検出器129
に至り、該4分割光検出器129により記録情報信号、
フォーカス誤差信号、トラッキング誤差信号を検出する
In addition, in the optical information reproducing device having the structure shown in FIG. 2(b), part of the laser light emitted from the semiconductor laser 119 is reflected in the right angle direction by the half mirror 121, and the reflected light is further reflected. The light passes through an objective lens 123, is focused on an optical information recording medium 125 such as an optical disk, and is completely reflected. Then, the reflected laser beam passes through the objective lens 123 again, and also passes through the half mirror 121.
After passing through a concave lens 127, a four-split photodetector 129
Then, the four-division photodetector 129 detects a recording information signal,
Detects focus error signal and tracking error signal.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかしながら、上記第3図(a)に示す構造の光学式情
報再生装置にあっては、多数のレンズを組み合わせて構
成しているため、その構造が複雑で各部材間の調節が必
要となり部品点数も多くなりその製造コストが増大する
という問題点があった。
However, since the optical information reproducing device having the structure shown in FIG. 3(a) is constructed by combining a large number of lenses, the structure is complex and requires adjustment between each member, resulting in a large number of parts. There is a problem in that the number of parts increases and the manufacturing cost increases.

また上記第3図(b)に示す構造の光学式情報再生装置
にあっては、ハーフミラ−121を使用しているため、
4分割光検出器129上に集光した非点収差の光にはコ
マ収差が発生してしまうという問題点があった。
Furthermore, since the optical information reproducing device having the structure shown in FIG. 3(b) uses a half mirror 121,
There is a problem in that comatic aberration occurs in the astigmatic light focused on the four-split photodetector 129.

また上記第3図(a)、(b)のいずれの場合も非点収
差位置とサイズ調整の為に凹レンズ115.127を付
加しなければならないという問題点があった。
Furthermore, in both cases of FIGS. 3(a) and 3(b), there is a problem in that concave lenses 115 and 127 must be added to adjust the astigmatism position and size.

本発明は上述の点に鑑みてなされたものであり、部品点
数が少なく、その構造が簡単で、製造が容易なコマ収差
が生じない光学式情報再生装置用回折格子素子を提供す
ることにある。
The present invention has been made in view of the above-mentioned points, and an object of the present invention is to provide a diffraction grating element for an optical information reproducing device that has a small number of parts, has a simple structure, is easy to manufacture, and does not cause coma aberration. .

〔課題を解決するための手段〕[Means to solve the problem]

上記問題点を解決するため本発明は光学式情報再生装置
用回折格子素子を、光源と、該光源から発射された射出
光を光学式情報記録媒体上に集束する対物レンズと、前
記光源と対物レンズの間であって前記光源から対物レン
ズに向かう光軸に垂直な位置に配置され前記光源から射
出された射出光を透過するとともに前記光学式情報記録
媒体からの反射光の一部を前記光軸から+1次方向に回
折する回折格子と、該+1次回折光をその最小錯乱円で
検出する検出器とを具備し、前記光学式情報記録媒体上
の情報を再生する光学式情報再生装置であって、 前記回折格子への干渉縞の記録は、前記再生時の光源か
ら発する光の波長とは異なる波長の光を発する2つの点
光源を具備し、その第1の点光源を前記光軸上の所定位
置に配置し、またその第2の点光源を前記光軸と所定角
度をなす軸上の所定位置に配置し、該両点光源から回折
格子に光を照射することによって行なわれ、その再生条
件が、μ=入C/λ。
In order to solve the above-mentioned problems, the present invention provides a diffraction grating element for an optical information reproducing device, which includes a light source, an objective lens that focuses emitted light emitted from the light source onto an optical information recording medium, and a lens that combines the light source and the objective lens. It is arranged between the lenses at a position perpendicular to the optical axis from the light source to the objective lens, and transmits the emitted light emitted from the light source, and also transmits a part of the reflected light from the optical information recording medium. An optical information reproducing device that reproduces information on the optical information recording medium, comprising a diffraction grating that diffracts from the axis in the +1st order direction and a detector that detects the +1st order diffracted light with its circle of least confusion. In order to record interference fringes on the diffraction grating, two point light sources are provided that emit light of a wavelength different from the wavelength of light emitted from the light source during reproduction, and the first point light source is positioned on the optical axis. and the second point light source is placed at a predetermined position on an axis that makes a predetermined angle with the optical axis, and the diffraction grating is irradiated with light from both point light sources. The reproduction conditions are μ=input C/λ.

mは任意定数 但し、RII:記録時の第1の点光源から回折格子まで
の距離 Ro:記録時の第2の点光源から回折格子までの距離 θ。:記録時の第2の点光源から回折格子上の光軸に至
る軸と光軸がなす 角度 Ro=再生時の光源から回折格子までの距離 として構成した。
m is an arbitrary constant. RII: Distance from the first point light source to the diffraction grating during recording Ro: Distance θ from the second point light source to the diffraction grating during recording. : Angle Ro between the axis from the second point light source to the optical axis on the diffraction grating during recording and the optical axis = distance from the light source to the diffraction grating during reproduction.

〔作用〕[Effect]

上記の如く光学式情報再生装置用回折格子素子を構成す
ることにより、光源と光学式情報記録媒体の間に対物レ
ンズと回折格子素子を配置するだけで、良好な非点収差
の最小錯乱円か得られ、従ってその構造が簡単で各部材
間の調節も容易で部品点数も少なく、その製造コストも
安くできる。また回折格子素子は2つの点光源から放射
する光を用いるだけで作成できるので、複雑な構造の干
渉縞を作る必要はなく、その製造は非常に容易となる。
By configuring the diffraction grating element for an optical information reproducing device as described above, it is possible to obtain a circle of minimum confusion with good astigmatism by simply arranging the objective lens and the diffraction grating element between the light source and the optical information recording medium. Therefore, the structure is simple, the adjustment between each member is easy, the number of parts is small, and the manufacturing cost can be reduced. Furthermore, since the diffraction grating element can be created by simply using light emitted from two point light sources, there is no need to create interference fringes with a complicated structure, and its manufacture is extremely easy.

〔実施例〕〔Example〕

以下、本発明の一実施例を図面に基づいて詳細に説明す
る。
Hereinafter, one embodiment of the present invention will be described in detail based on the drawings.

第1図は本発明にかかる回折格子素子を用いた光学式情
報再生装置を示す図である。
FIG. 1 is a diagram showing an optical information reproducing device using a diffraction grating element according to the present invention.

同図に示すように、この光学式情報再生装置は、回折格
子素子1と半導体レーザ3と凸レンズからなる対物レン
ズ5と4分割光検出器または6分割光検出器からなる検
出器9を具備している。
As shown in the figure, this optical information reproducing device includes a diffraction grating element 1, a semiconductor laser 3, an objective lens 5 consisting of a convex lens, and a detector 9 consisting of a 4-split photodetector or a 6-split photodetector. ing.

またここで7は光ディスク等の光学式情報記録媒体であ
る。
Further, 7 is an optical information recording medium such as an optical disk.

ここで、対物レンズ5は光学式情報記録媒体7に対向す
る位置に配置される。
Here, the objective lens 5 is placed at a position facing the optical information recording medium 7.

また回折格子素子1は半導体レーザ3と対物レンズ5の
間に配置され、かつ前記半導体レーザ3から対物レンズ
5を通って光学式情報記録媒体7に向かう光軸11に対
して回折格子素子1の面が垂直になるように配置されて
いる。
Further, the diffraction grating element 1 is disposed between the semiconductor laser 3 and the objective lens 5, and the diffraction grating element 1 is disposed between the semiconductor laser 3 and the objective lens 5. The surfaces are arranged vertically.

また検出器9は前記光軸11が回折格子素子1と交わる
点から前記光軸11に対してθ、たけ傾いた軸(+1次
回折光軸)方向であって、該+1次回折光が最小錯乱円
となる位置であり、且つ該軸に対してその面が垂直にな
るように配置されている。
Further, the detector 9 is arranged in the direction of an axis (+1st-order diffraction optical axis) that is inclined by θ with respect to the optical axis 11 from the point where the optical axis 11 intersects with the diffraction grating element 1, and the +1st-order diffraction light is and is arranged so that its surface is perpendicular to the axis.

そして半導体レーザ3から発射された射出光は、回折格
子素子1を透過し、対物レンズ5によって光学式情報記
録媒体7上で集束する。そして該集束した光は該光学式
情報記録媒体7で反射され、再び対物レンズ5を通過し
て回折格子素子1に至る。そしてこの回折格子素子1に
よって前記反射された光の内の一部は+1次方向に回折
する。そしてこの+1次方向に回折された光は検出器9
上に到達し、該検出器9によって前記光学式情報記録媒
体7上の情報を電気信号に再生するとともに、フォーカ
ス誤差信号とトラッキング誤差信号を検出するのである
Then, the emitted light emitted from the semiconductor laser 3 passes through the diffraction grating element 1 and is focused on the optical information recording medium 7 by the objective lens 5. The focused light is then reflected by the optical information recording medium 7, passes through the objective lens 5 again, and reaches the diffraction grating element 1. A part of the light reflected by this diffraction grating element 1 is diffracted in the +1st order direction. The light diffracted in the +1st order direction is sent to the detector 9.
The detector 9 reproduces the information on the optical information recording medium 7 into an electrical signal and detects a focus error signal and a tracking error signal.

次に上記回折格子素子1上に干渉縞を作成する方法を説
明する。
Next, a method for creating interference fringes on the diffraction grating element 1 will be explained.

第2図(a)は上記回折格子素子1上に干渉縞を記録す
る方法を示す図であ両。
FIG. 2(a) is a diagram showing a method of recording interference fringes on the diffraction grating element 1.

同図に示すように、回折格子素子1はその面がX−Y平
面上に位置するとともにその原点(0゜0.0)が回折
格子素子1の中央部にくるように配置する。そして2軸
(光軸)上であって回折格子素子1から+RR離れた位
置L2に参照光としてのレーザー光源(第1の点光源)
を配置する。
As shown in the figure, the diffraction grating element 1 is arranged so that its surface is located on the X-Y plane and its origin (0° 0.0) is located at the center of the diffraction grating element 1. Then, a laser light source (first point light source) as a reference light is located at a position L2 on the second axis (optical axis) and +RR away from the diffraction grating element 1.
Place.

またY−Z平面内であってZ軸から原点を中心に00だ
け傾いた軸上であって該原点から+Ro離れた位置し1
に物体光としてのレーザー光源(第2の点光源)を配置
する。そしてこれらLl、L2に配置したレーザー光源
からレーザー光を発射することにより、回折格子素子1
上に干渉縞を記録する。
Also, it is located within the Y-Z plane, on an axis tilted by 00 from the Z axis with the origin as the center, and located +Ro away from the origin.
A laser light source (second point light source) as an object light is placed at . By emitting laser light from the laser light sources arranged at these Ll and L2, the diffraction grating element 1
Record the interference fringes on top.

ここでこのLl、L2に配置したレーサー光源は点光源
であり、該光源から発射される光は球面波となり、従っ
て回折格子素子1上に形成される干渉縞は2光束球面波
の干渉によって作成されることとなる。
Here, the laser light sources placed at Ll and L2 are point light sources, and the light emitted from the light sources becomes a spherical wave. Therefore, the interference fringes formed on the diffraction grating element 1 are created by the interference of two beam spherical waves. It will be done.

また以上のことよりこの回折格子素子1の干渉縞の位相
伝達関数は、 φ(x、y)= ”  ”V”zt”)(=2nπ) 但し、λ0:記録時の光の波長 n=1.2,3.・・・ という簡単なものとなる。
Also, from the above, the phase transfer function of the interference fringes of this diffraction grating element 1 is as follows: φ(x, y) = ``V''zt'') (=2nπ) However, λ0: Wavelength of light during recording n = 1 .2,3. It's as simple as...

第2図(b)は、上記のように作成した回折格子素子1
を第1図の光学式情報再生装置の中に配置した場合に、
光学式情報記録媒体7から反射きれてきた光が該回折格
子素子1によって回折する状態を示す図である。即ち回
折格子素子1を再生用に用いた場合を示す。
FIG. 2(b) shows the diffraction grating element 1 prepared as described above.
When placed in the optical information reproducing device shown in Fig. 1,
3 is a diagram showing a state in which light that has been completely reflected from an optical information recording medium 7 is diffracted by the diffraction grating element 1. FIG. That is, the case where the diffraction grating element 1 is used for reproduction is shown.

同図に示すように、記録時とは異なる波長からなる反射
レーザー光が−Z軸方向から回折格子素子1に当たると
、O次回新党が2軸(光軸)上の原点からR6離れた位
置L3 (第1図に示す光源3のある位置)にその焦点
を結ぶとともに、回折格子素子1を通過する光の一部は
回折して非点収差の光となり、その+1次回折光はY−
Z平面内であってZ軸から傾きθRの軸上であって原点
からR1離れた位置し4に最少錯乱円を作る。そしてこ
の位置L4に検出器9が置かれており、各種信号が検出
される。
As shown in the figure, when a reflected laser beam having a wavelength different from that during recording hits the diffraction grating element 1 from the -Z axis direction, the O-th new beam is located at a position L3 that is R6 away from the origin on the second axis (optical axis). The light is focused at the position of the light source 3 shown in Figure 1, and a part of the light passing through the diffraction grating element 1 is diffracted and becomes astigmatic light, and the +1st order diffracted light is Y-
A circle of least confusion is created at 4, which is located within the Z plane, on an axis with an inclination θR from the Z axis, and is located R1 away from the origin. A detector 9 is placed at this position L4, and various signals are detected.

なお、ここでθ。とθ、の関係は、 θア=sin伺(μsinθ。) μ=(λC/λ0) ただし、λC;再生時の光の波長 λO;記録時の光の波長 である。Note that here θ. The relationship between and θ is θa=sin θ (μsinθ.) μ=(λC/λ0) However, λC: wavelength of light during reproduction λO: Wavelength of light during recording It is.

ところでとのL4の位置にできる最小錯乱円には、その
円内の光の状態が該円内金体に均等になっていて良好な
ものと、該円内金体で不均一になっていたりコマ収差等
の縞模様を生じていたり等して不良なものとがある。
By the way, in the circle of least confusion formed at the L4 position, there are two types: one in which the light condition within the circle is uniform across the metal bodies within the circle and is good, and the other in which the light condition is uneven among the metal bodies within the circle. Some are defective due to striped patterns due to coma aberration, etc.

そこで本願発明者は、この最J\錯乱円内の光の各種の
状態が、再生時のRcの値によって変化することに着目
し、この値をそれぞれ変化することによって、その最ノ
」1錯乱円内の光の状態が良好になる状態のとき、即ち
第1図に示す検出器9によって正確に記録情報信号、フ
ォーカス誤差信号、トラッキング誤差信号を検出できる
ことを見出した。
Therefore, the inventor of the present application focused on the fact that the various states of light within this circle of maximum confusion change depending on the value of Rc at the time of reproduction, and by changing these values, the maximum confusion It has been found that when the light condition within the circle is good, that is, the recording information signal, focus error signal, and tracking error signal can be accurately detected by the detector 9 shown in FIG.

つまり、再生時の回折格子から+1次回折光の結像点ま
での距離をR1とすると、結像の公式より、 Cア = より、 となり、結像方向は、 θ、−5in−’(μsinθ0) また結像距離R1は が求められる。
In other words, if the distance from the diffraction grating during reproduction to the imaging point of the +1st-order diffracted light is R1, then from the imaging formula, C a =, and the imaging direction is θ, -5in-' (μsinθ0) Further, the imaging distance R1 is determined.

そして良好な最小錯乱円を得るためには少なくとも、 m’ RcK*−μRc(−R*   Ro)Y軸方向
のコマ収差係数Cyは、 であればよいことがわかった。
It was also found that in order to obtain a good circle of least confusion, the comatic aberration coefficient Cy in the Y-axis direction should at least be m'RcK*-μRc(-R*Ro).

つまりこの再生条件を満たせば、良好な最小錯乱円が得
られる。
In other words, if this reproduction condition is satisfied, a good circle of least confusion can be obtained.

従って以上の条件を満たすように、回折格子素子1上に
再生光を照射すれば、容易に良好な最小錯乱円を得るこ
とができる。
Therefore, if the reproduction light is irradiated onto the diffraction grating element 1 so as to satisfy the above conditions, a good circle of least confusion can be easily obtained.

〔発明の効果〕〔Effect of the invention〕

以上詳細に説明したように、本発明に係る光学式情報再
生装置用回折格子素子によれば、光源と光学式情報記録
媒体の間に対物レンズと回折格子素子を配置するだけで
、良好な非点収差の最少錯乱円が得られる。従ってその
構造が簡単で各部材間の調節も容易で部品点数も少なく
、その製造コストも安くできるという優れた効果を有す
る。
As explained in detail above, according to the diffraction grating element for an optical information reproducing device according to the present invention, good optical performance can be achieved by simply arranging the objective lens and the diffraction grating element between the light source and the optical information recording medium. A circle of least confusion of point aberration is obtained. Therefore, the structure is simple, the adjustment between each member is easy, the number of parts is small, and the manufacturing cost is low.

また回折格子素子は2つの点光源から放射する光を用い
るだけで作成できるので、複雑な構造の干渉縞を作る必
要はなく、その製造は非常に容易となる。
Furthermore, since the diffraction grating element can be created by simply using light emitted from two point light sources, there is no need to create interference fringes with a complicated structure, and its manufacture is extremely easy.

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

第1図は本発明にかかる回折格子素子を用いた光学式情
報再生装置を示す図、第2図(a)は回折格子素子1上
に干渉縞を記録する方法を示す図、第2図(b)は再生
時に光学式情報記録媒体7から反射されてきた光が回折
格子素子1によって回折する状態を示す図、第3図(a
)、(b)は従来の光学式情報再生装置を示す図である
。 図中、1・・・回折格子素子、3・・・半導体レーザ、
5・・・対物レンズ、7・・・光学式情報記録媒体、9
・・・検出器、11・・・光軸、である。
FIG. 1 shows an optical information reproducing device using a diffraction grating element according to the present invention, FIG. 2(a) shows a method of recording interference fringes on the diffraction grating element 1, and FIG. b) is a diagram showing a state in which the light reflected from the optical information recording medium 7 is diffracted by the diffraction grating element 1 during reproduction, and FIG.
) and (b) are diagrams showing a conventional optical information reproducing device. In the figure, 1...diffraction grating element, 3... semiconductor laser,
5... Objective lens, 7... Optical information recording medium, 9
. . . detector, 11 . . . optical axis.

Claims (1)

【特許請求の範囲】 光源と、該光源から発射された射出光を光学式情報記録
媒体上に集束する対物レンズと、前記光源と対物レンズ
の間であって前記光源から対物レンズに向かう光軸に垂
直な位置に配置され前記光源から射出された射出光を透
過するとともに前記光学式情報記録媒体からの反射光の
一部を前記光軸から+1次方向に回折する回折格子と、
該+1次回折光をその最小錯乱円で検出する検出器とを
具備し、前記光学式情報記録媒体上の情報を再生する光
学式情報再生装置であって、 前記回折格子への干渉縞の記録は、前記再生時の光源か
ら発する光の波長とは異なる波長の光を発する2つの点
光源を具備し、その第1の点光源を前記光軸上の所定位
置に配置し、またその第2の点光源を前記光軸と所定角
度をなす軸上の所定位置に配置し、該両点光源から回折
格子に光を照射することによって行なわれ、その再生条
件が、1.1>m^2R_OR_R/m^2R_CR_
R−μR_C(R_R−R_O)>0.9μ=λ_C/
λ_O mは任意定数 但し、R_R:記録時の第1の点光源から回折格子まで
の距離 R_O:記録時の第2の点光源から回折格 子までの距離 θ_O:記録時の第2の点光源から回折格 子上の光軸に至る軸と光軸がなす 角度 R_C:再生時の光源から回折格子までの 距離 を満足することを特徴とする光学式情報再生装置用回折
格子素子。
[Scope of Claims] A light source, an objective lens that focuses emitted light emitted from the light source onto an optical information recording medium, and an optical axis that is between the light source and the objective lens and extends from the light source toward the objective lens. a diffraction grating arranged at a position perpendicular to the light source and transmitting the emitted light emitted from the light source and diffracting a part of the reflected light from the optical information recording medium in the +1st order direction from the optical axis;
an optical information reproducing apparatus for reproducing information on the optical information recording medium, comprising a detector for detecting the +1st-order diffracted light using its circle of least confusion, and recording interference fringes on the diffraction grating. , comprising two point light sources that emit light of a wavelength different from the wavelength of light emitted from the light source during reproduction, the first point light source being disposed at a predetermined position on the optical axis, and the second point light source being disposed at a predetermined position on the optical axis. This is performed by placing a point light source at a predetermined position on an axis that makes a predetermined angle with the optical axis, and irradiating light from both point light sources to the diffraction grating, and the reproduction condition is 1.1>m^2R_OR_R/ m^2R_CR_
R-μR_C(R_R-R_O)>0.9μ=λ_C/
λ_O m is an arbitrary constant. However, R_R: Distance from the first point light source to the diffraction grating during recording R_O: Distance from the second point light source to the diffraction grating during recording θ_O: Distance from the second point light source during recording A diffraction grating element for an optical information reproducing device, characterized in that the angle R_C between the axis leading to the optical axis on the diffraction grating and the optical axis satisfies the distance from the light source to the diffraction grating during reproduction.
JP63224130A 1988-09-06 1988-09-06 Optical information reproducing device Expired - Lifetime JP2794114B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63224130A JP2794114B2 (en) 1988-09-06 1988-09-06 Optical information reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63224130A JP2794114B2 (en) 1988-09-06 1988-09-06 Optical information reproducing device

Publications (2)

Publication Number Publication Date
JPH0271201A true JPH0271201A (en) 1990-03-09
JP2794114B2 JP2794114B2 (en) 1998-09-03

Family

ID=16809013

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63224130A Expired - Lifetime JP2794114B2 (en) 1988-09-06 1988-09-06 Optical information reproducing device

Country Status (1)

Country Link
JP (1) JP2794114B2 (en)

Also Published As

Publication number Publication date
JP2794114B2 (en) 1998-09-03

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