JPS62283687A - Light emitting device - Google Patents

Light emitting device

Info

Publication number
JPS62283687A
JPS62283687A JP61126532A JP12653286A JPS62283687A JP S62283687 A JPS62283687 A JP S62283687A JP 61126532 A JP61126532 A JP 61126532A JP 12653286 A JP12653286 A JP 12653286A JP S62283687 A JPS62283687 A JP S62283687A
Authority
JP
Japan
Prior art keywords
light
emitting device
light source
parallel
light emitting
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
JP61126532A
Other languages
Japanese (ja)
Inventor
Yuichi Nakamura
裕一 中村
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.)
Toshiba Corp
Toshiba Intelligent Technology Co Ltd
Original Assignee
Toshiba Corp
Toshiba Intelligent Technology 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 Toshiba Corp, Toshiba Intelligent Technology Co Ltd filed Critical Toshiba Corp
Priority to JP61126532A priority Critical patent/JPS62283687A/en
Publication of JPS62283687A publication Critical patent/JPS62283687A/en
Pending legal-status Critical Current

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  • Optical Head (AREA)
  • Semiconductor Lasers (AREA)
  • Led Devices (AREA)

Abstract

PURPOSE:To reduce the size and weight of a light emitting device by using a light transmission member having a function for correcting a light from a light source to parallel beam and an ellipse correcting function. CONSTITUTION:The second surface (plane of emission) 3b of a light transmission member 3 is brought in coincidence with the end 5a of an opening side, and a first surface (plane of incidence) 3a is disposed in a housing 5. Electrodes 6 are energized to emit a light beam L1 from a light source 12 toward a light transmission member 3. The beam L1 is refracted at the first surface ea of the member 3, corrected to a parallel beam (light beam L2) to the second surface 3b. lt is elliptically corrected by the second surface 3b to an emitted light beam L3 in which its perpendicular section is circular and its optical axis coincides with the axial direction of the housing 5. The beam L3 is applied as a spot S on a recording film 33 opposed to a guide groove 34, and the reflected light is introduced through the film 33 and a disk substrate 32 to an objective lens 22 side.

Description

【発明の詳細な説明】 3、発明の詳細な説明 [発明の目的] (産業上の利用分野) 本発明は例えば光学ヘッド等に用いられる半導体レーザ
ダイオードのような光源から発せられる光ビームを補正
して出射する発光装置に関する。
Detailed Description of the Invention 3. Detailed Description of the Invention [Object of the Invention] (Industrial Application Field) The present invention corrects a light beam emitted from a light source such as a semiconductor laser diode used in an optical head, etc. The present invention relates to a light emitting device that emits light.

(従来の技術) 例えば、画像情報ファイル装置等における光ディスクに
対して情報の記録または再生を行う際には半導体レーザ
ダイオードを光源とする発光装置を有した光学ヘッドが
用いられる。
(Prior Art) For example, when recording or reproducing information on an optical disk in an image information file device or the like, an optical head having a light emitting device using a semiconductor laser diode as a light source is used.

しかしながら半導体レーザダイオードから放射される光
は、拡散光でありかつその直交断面形状が楕円であるた
め、拡散光を平行光に、かつ、その断面形状を円形に補
正することがこの光の収束性を向上し、強度分布を一様
にする上で不可欠となる。
However, the light emitted from a semiconductor laser diode is diffused light and its orthogonal cross-sectional shape is an ellipse, so correcting the diffused light to parallel light and its cross-sectional shape to a circular shape improves the convergence of this light. This is essential for improving the intensity and making the intensity distribution uniform.

このような発光装置の従来例を第7図を参照して説明す
る。
A conventional example of such a light emitting device will be explained with reference to FIG.

同図に示す発光装置50は、半導体レーザダイオードを
用いた光源12と、この光源12から発生される光ビー
ムを平行光に補正する複数のレンズ群からなるコリメー
トレンズ11と、このコリメートレンズ11により平行
光となった光を入射し、これに対して楕円補正を行って
光ビームの直交断面が円形の平行光を出射する補正プリ
ズム13とを有して構成される。
The light emitting device 50 shown in the figure includes a light source 12 using a semiconductor laser diode, a collimating lens 11 consisting of a plurality of lens groups that corrects the light beam generated from the light source 12 into parallel light, and this collimating lens 11. The correction prism 13 receives parallel light, performs ellipse correction on the light, and emits parallel light whose orthogonal cross section is circular.

この発光装置50によれば、光源12からの光ビームを
平行光で、かつ、断面円形の光ビームに補正して出射す
ることができるので、画像情報記録装置における光ディ
スクに対して情報の記録又は再生を行う際に必要な光ビ
ームの光量を得ることができる。
According to this light emitting device 50, the light beam from the light source 12 can be corrected and emitted as a parallel light beam and a light beam with a circular cross section, so that information can be recorded or The amount of light beam necessary for reproduction can be obtained.

しかしながら、光源12からの光ビームを平行光にする
ためのコリメートレンズ11及び楕円補正するための補
正プリズム13を有するため、この発光装置50の全体
形状が大型化し、かつ、補正プリズム13に対する光v
、12の角度配置もこの補正プリズム13の傾斜角度に
応じて厳密な精度が要求されるという問題がある。
However, since it includes a collimating lens 11 for collimating the light beam from the light source 12 and a correction prism 13 for correcting the ellipse, the overall shape of this light emitting device 50 becomes large, and the light beam directed to the correction prism 13 is
, 12 also have a problem in that strict precision is required depending on the inclination angle of the correction prism 13.

(発明が解決しようとする問題点) 上述したように従来の発光装置ではその形状が大型化し
重量も重くなると共に、光源と補正プリズムとの配置上
の制約を伴うという問題がある。
(Problems to be Solved by the Invention) As described above, conventional light emitting devices have problems in that they are large in size and heavy in weight, and are accompanied by restrictions on the arrangement of the light source and the correction prism.

そこで本発明は、光源からの光ビームに対して平行光に
補正する機能及び楕円補正機能を有し、かつ、小型軽母
な発光装置を提供することを目的(問題点を解決するた
めの手段) 本発明の発光装置は、光源と、この光源から発生された
光をビームを平行光にする非球面形状を有した入射面及
び前記平行光の断面形状を略円形に補正する平面形状を
有した出射面を有する光透過性部材とを有する。
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a light emitting device that has a function of correcting a light beam from a light source to parallel light and an ellipse correction function, and is small and lightweight (means for solving the problem). ) The light emitting device of the present invention has a light source, an entrance surface having an aspherical shape to convert the light generated from the light source into a parallel beam, and a planar shape that corrects the cross-sectional shape of the parallel light to a substantially circular shape. and a light-transmitting member having a light exit surface.

(作 用) 上記構成の装置の作用を以下に説明する。(for production) The operation of the apparatus having the above configuration will be explained below.

光源からの光ビームは、光透過性部材の非球面形状を有
した入射面に入射し、この入射面の作用により平行光と
なって光透過性部材の内部を進行する。そして、この平
行光は平面形状を有した出射面に至り、その断面形状が
略円形に補正された侵この出射面から外部に出射される
The light beam from the light source enters the aspherical incident surface of the light-transmitting member, and becomes parallel light due to the action of the incident surface, and travels inside the light-transmitting member. Then, this parallel light reaches an exit surface having a planar shape, and is emitted to the outside from the exit surface whose cross-sectional shape has been corrected to be approximately circular.

(実施例) 以下に本発明の実施例を詳細に説明する。(Example) Examples of the present invention will be described in detail below.

まず、第41図乃至第6図を参照して本発明の詳細な説
明する。
First, the present invention will be explained in detail with reference to FIGS. 41 to 6.

同図において、Gは非球面でおる屈折面りを有し、かつ
、屈折率nの光透過性部材(例えばガラス)であるもの
とする。そして、この屈折面りのIn点を直交するX軸
、y軸の原点Aにとるものとする。また、同図において
光透過性部材Gの屈折面りの右側は屈折率1の空気であ
るものとする。
In the figure, G is a light-transmitting member (for example, glass) having an aspherical refractive surface and having a refractive index n. It is assumed that the In point of this refraction surface is taken as the origin A of the orthogonal X and Y axes. Further, in the figure, it is assumed that the right side of the refractive surface of the light-transmitting member G is air having a refractive index of 1.

このとき光透過性部材Gex軸と平行に進行する光が屈
折面りの一点Pで屈折し、空気中に想定した前記屈折面
りと対称な面(同図で点線で示す)の焦点Fに集束する
場合を考える。
At this time, the light traveling parallel to the Gex axis of the light-transmitting member is refracted at a point P on the refraction surface, and reaches a focal point F on a surface (indicated by a dotted line in the figure) that is symmetrical to the refraction surface, which is assumed to be in the air. Consider the case of focusing.

いま、AF=f、P点の座標を(x、y)(但しx<Q
)とすれば下記(1)式が得られる。
Now, AF=f, the coordinates of point P are (x, y) (however, x<Q
), the following equation (1) can be obtained.

−nx+ (y2 + (f−x)2ビ= f ・(1
](1)式を整理すると下記(2)式となる。
-nx+ (y2 + (f-x)2bi= f ・(1
] When formula (1) is rearranged, the following formula (2) is obtained.

y2− (n2−1 > x2 +2f (n−1) 
x=0・・・(2) この(2)式は双曲線の左側の枝の頂点を原点にとった
一般式 と同一形式となる。
y2- (n2-1 > x2 +2f (n-1)
x=0...(2) This equation (2) has the same form as the general equation whose origin is the vertex of the left branch of the hyperbola.

したがって、前記屈折面りは双曲面となり、光透過性部
材G中をxlFI!Iと平行に進行する光は全て焦点F
に収束することになる。
Therefore, the refractive surface becomes a hyperboloid, and xlFI! All light traveling parallel to I is at the focal point F
It will converge to .

そして、第5図に示すように上述したような双曲面を第
2面2bとし、入射光に対して垂直な第1面2aを付加
した光透過性部材2を用いることにより、X軸に平行な
光に対しては球面収差の除去された光透過性部材2を構
成することができる。
As shown in FIG. 5, by using a light-transmitting member 2 having a second surface 2b which is a hyperboloid as described above and a first surface 2a perpendicular to the incident light, parallel to the X-axis For such light, it is possible to construct a light-transmitting member 2 in which spherical aberration is removed.

上述した光透過性部材2において、光の進行方向が逆の
場合を考えると、焦点Fからこの光透過性部材2の第2
面2bに向って拡散する光は、この双曲面で屈折し、X
軸に平行な光となって第1面2aから出射されることに
なる。この場合、拡散光は平行光に補正されるが、その
直交断面形状は何等補正されない。
In the above-mentioned light-transmitting member 2, if we consider the case where the traveling direction of light is reversed, from the focal point F to the second
The light diffusing toward surface 2b is refracted by this hyperboloid, and
The light becomes parallel to the axis and is emitted from the first surface 2a. In this case, the diffused light is corrected to parallel light, but its orthogonal cross-sectional shape is not corrected in any way.

したがって、焦点Fからの光が半導体レーザダイオード
等による放射光のように直交断面形状が楕円でおれば、
前記平行光の直交断面形状も楕円のままとなる。
Therefore, if the light from the focal point F has an elliptical orthogonal cross section like the light emitted by a semiconductor laser diode, then
The orthogonal cross-sectional shape of the parallel light also remains elliptical.

そこで、第6図に示すように、光透過性部材3第1面(
入射面>3aが双曲面で、第2面(出射面>3bが第1
面3aで平行光となった光の光軸に対し所定の傾斜角φ
を有する傾斜平面を有するものを用いる。
Therefore, as shown in FIG. 6, the first surface of the light-transmitting member 3 (
The entrance surface > 3a is a hyperboloid, the second surface (the exit surface > 3b is the first
A predetermined inclination angle φ with respect to the optical axis of the light that has become parallel light at the surface 3a
A device with an inclined plane having .

この光透過性部材3によれば、拡散光で、かつ、直交断
面形状が楕円となる光を、球面収差がなく直交断面が円
形の平行光に補正することが可能となる。
According to the light transmitting member 3, it is possible to correct diffused light having an elliptical orthogonal cross section to parallel light having no spherical aberration and having a circular orthogonal cross section.

次に上記原理に基づく発光装置の実施例を第1図を参照
して説明する。
Next, an embodiment of a light emitting device based on the above principle will be described with reference to FIG.

同図に示す発光装置10は、一方の端部が基板4で閉塞
され、他方の端部が傾斜を有しつつ開口された筒状のハ
ウジング5と、このハウジング5の内部で前記基板4と
一体的に形成された光源載置部4a上に載置された半導
体レーザダイオードを用いた光源12と、前記ハウジン
グ5の開口部に装着された光透過性部材3と、前記基板
4から第1図において下方に向けて突出配置され、がっ
、前記光源12に電気的に接続された電極6とを有して
構成されている。
The light emitting device 10 shown in the figure includes a cylindrical housing 5 in which one end is closed with a substrate 4 and the other end is opened with a slope, and the substrate 4 is connected inside the housing 5. A light source 12 using a semiconductor laser diode placed on an integrally formed light source placement part 4a, a light transmitting member 3 attached to an opening of the housing 5, and a first In the figure, the electrode 6 is arranged to protrude downward and is electrically connected to the light source 12.

前記ハウジング5の開口部側の端面5aはハウジング5
の軸線方向に対し一定の角度だけ傾斜した傾斜面に形成
されている。そして、前記光透過性部材3の第2面(出
射面)3bを前記開口部側の端部5aに一致ざぜると共
に、その第1面(入射面)3aをハウジング5の内部に
臨ませている。
The end face 5a of the housing 5 on the opening side is the housing 5
It is formed into an inclined surface that is inclined at a certain angle with respect to the axial direction. Then, the second surface (output surface) 3b of the light transmitting member 3 is aligned with the end 5a on the opening side, and the first surface (incidence surface) 3a is made to face the inside of the housing 5. There is.

前記光源12は、この光源12から発せられる光ビーム
の光軸がハウジング5の軸線方向に対し所定の角度0と
なるように光源載置部4a上に載置され、これにより光
透過性部材3の第2面3bから出射する光の光軸がハウ
ジング5の軸線と一致するようになっている。
The light source 12 is placed on the light source placement part 4a so that the optical axis of the light beam emitted from the light source 12 forms a predetermined angle of 0 with respect to the axial direction of the housing 5, so that the light transmitting member 3 The optical axis of the light emitted from the second surface 3b of the housing 5 coincides with the axis of the housing 5.

次に上記構成の実施例装置の作用を説明する。Next, the operation of the embodiment apparatus having the above configuration will be explained.

電極6に通電することにより光源12から光透過性部材
3に向けて光ビームL1が発せられる。
By energizing the electrode 6, a light beam L1 is emitted from the light source 12 toward the light-transmitting member 3.

この光ビームL1は光透過部材3の第1而3aで屈折し
平行光(光ビームL2 )に補正されて第2百3bに至
る。そして、この第2面3bにより楕円補正が行われて
、直交断面が円形でその光軸がハウジング5の軸線方向
と一致した出射光ビームL3となって出射される。
This light beam L1 is refracted by the first beam 3a of the light transmitting member 3, corrected into parallel light (light beam L2), and reaches the second beam 3b. Then, ellipse correction is performed by the second surface 3b, and an output light beam L3 whose orthogonal cross section is circular and whose optical axis coincides with the axial direction of the housing 5 is emitted.

次に上記発光装置10を用いた光学ヘッド20の概略構
成及びこの光学ヘッド20を用いて例えば光ディスク3
1に対して情報の記録又は再生を行う方法について説明
する。
Next, a schematic configuration of an optical head 20 using the above-mentioned light emitting device 10 and an optical disc 3 using this optical head 20 will be described.
A method of recording or reproducing information to or from 1 will be explained.

この光ディスク31の一例を第3図を参照して説明する
。同図に示す光ディスク31は、円弧状のプリグループ
が設けられた円板状のディスク基板32上に記録膜33
を蒸着等により形成してプリグループに対応する案内溝
34を設けると共に、この案内溝34に而する前記記録
膜33に対し所定の間隔で記録情報としてのピット35
を設けることにより構成された再生専用タイプのもので
ある。そして、前記対物レンズ22により前記案内溝3
4に面する記録膜33に対して光ビームL3をスポット
Sとして照射し、その反射光を記録膜33及びディスク
基板32を介して対物レンズ22側に導くようになって
いる。
An example of this optical disc 31 will be explained with reference to FIG. 3. The optical disc 31 shown in the figure has a recording film 33 on a disc-shaped disc substrate 32 on which arc-shaped pre-groups are provided.
A guide groove 34 corresponding to the pre-group is formed by vapor deposition or the like, and pits 35 as recording information are formed at predetermined intervals on the recording film 33 in this guide groove 34.
This is a reproduction-only type that is configured by providing a. Then, the guide groove 3 is
A light beam L3 is irradiated as a spot S onto the recording film 33 facing 4, and the reflected light is guided to the objective lens 22 side via the recording film 33 and the disk substrate 32.

次に上記構成の光学ヘッド20の作用を第3図(a>、
(b)に示す光ディスク21における記録情報の再生を
行う場合を例にとって説明する。
Next, FIG. 3 (a>,
An example of reproducing recorded information on the optical disc 21 shown in FIG. 12(b) will be explained.

発光装置10の光源12で発生した光ビームL1は光透
過性部材3の第1面3aに至り前記原理に基づいて平行
光である光ビームL2となる。この光ビームL2は光透
過性部材3内を進行し第2面3bに至ってここで前記原
理に基づいて楕円補正され直交断四の形状が略円形の光
ビームL3となる。この光ビームL3はビームスプリッ
タ21を透過し対物レンズ22で集光されて光ディスク
31の案内溝34にスポットSとして照射される。
The light beam L1 generated by the light source 12 of the light emitting device 10 reaches the first surface 3a of the light-transmitting member 3 and becomes a parallel light beam L2 based on the above-mentioned principle. This light beam L2 travels through the light-transmitting member 3, reaches the second surface 3b, and is subjected to ellipse correction based on the above-mentioned principle to become a light beam L3 whose orthogonal section has a substantially circular shape. This light beam L3 passes through the beam splitter 21, is focused by the objective lens 22, and is irradiated as a spot S onto the guide groove 34 of the optical disc 31.

そして、その反射光は記録1151j33及びディスク
基板32を透過して対物レンズ22に至り平行光となっ
てビームスプリッタ21に入射する。ざらにこの光ビー
ムL3はビームスプリッタ21で反射されて集光レンズ
23に至り、この集光レンズ23の作用で集光され光検
出器24に入射する。
Then, the reflected light passes through the recording 1151j33 and the disk substrate 32, reaches the objective lens 22, becomes parallel light, and enters the beam splitter 21. Roughly, this light beam L3 is reflected by the beam splitter 21 and reaches the condensing lens 23, where it is condensed by the action of the condensing lens 23 and enters the photodetector 24.

このような光学ヘッド20の一連の作用により、光検出
器24の出力信号として前記ピット35の有無に基づく
反射率の相違に基因した記録情報信号、即ら、再生信号
を得ることができると共に、光ディスク31に対するフ
ォーカス信号及びトラッキング信号を得ることができ、
例えば図示しない対物レンズ22用の駆動手段により対
物レンズ22を第2図において上下おるいは左右に移動
してフォーカス補正あるいはトラッキング補正を行うこ
とが可能となる。
Through this series of actions of the optical head 20, it is possible to obtain, as an output signal of the photodetector 24, a recorded information signal, that is, a reproduced signal, which is based on the difference in reflectance based on the presence or absence of the pits 35, and A focus signal and a tracking signal for the optical disc 31 can be obtained,
For example, by driving means for the objective lens 22 (not shown), the objective lens 22 can be moved up and down or left and right in FIG. 2 to perform focus correction or tracking correction.

この光学ヘッド20によれば、発光装置10を小型、軽
量に構成できるため、この光学ヘッド20自体の小型、
軽量化が可能となる。これにより、この光学ヘッド20
の光ディスク31に対するアクセス時間の短縮化が図れ
る等の効果を有するものである。
According to this optical head 20, since the light emitting device 10 can be configured to be small and lightweight, the optical head 20 itself can be made small and lightweight.
It becomes possible to reduce the weight. As a result, this optical head 20
This has the effect of shortening the access time to the optical disc 31.

本発明は上記実施例に限定されるものではなく、その要
旨の範囲内で種々の変形が可能でおる。
The present invention is not limited to the above embodiments, and various modifications can be made within the scope of the invention.

例えば、上記実施例では光透過性部材の非球面として双
曲面を用いた場合について説明したが、この他桁円面や
放物線面を用いても同様な瀘能を発揮させることができ
る。
For example, in the above embodiments, a hyperbolic surface is used as the aspheric surface of the light-transmitting member, but the same filtering performance can be achieved by using a circular surface or a parabolic surface.

また、上記実施例の発光装置はピットを設けた光ディス
クの光源部として用いる場合の他にも、イレーザブル光
ディスクとしての例えば光磁気ディスクヤ相変化型光デ
ィスク等の光学ヘッドに適用されることは言うまでもな
いことでおる。
It goes without saying that the light emitting device of the above embodiment is not only used as a light source for an optical disk provided with pits, but also applied to an optical head of an erasable optical disk, such as a magneto-optical disk or a phase-change optical disk. That's it.

[発明の効果コ 以上詳述した本発明によれば、光源からの光を平行光に
補正する機能及び楕円補正機能を兼備した光透過性部材
を用いたことによって、小型化。
[Effects of the Invention] According to the present invention described in detail above, the size can be reduced by using a light-transmitting member that has both the function of correcting the light from the light source into parallel light and the function of correcting ellipse.

軽量化が可能な発光装置を提供することができる。A light-emitting device that can be lightweight can be provided.

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

第1図は本発明の実施例装置を示す断面図、第2図は同
装置を用いた光学ヘッドの構成を示す概略説明図、第3
図は光ディスクの一部拡大説明図、第4図乃至第6図は
それぞれ本発明の原理説明図、第7図は従来の発光装置
を示す説明図である。 3・・・光ヤ過性部材、 3a・・・第1面、3b・・・第2面、10・・・発光
装置、 12・・・光源。 ゛°−1 第3図
FIG. 1 is a sectional view showing an embodiment of the present invention, FIG. 2 is a schematic explanatory view showing the configuration of an optical head using the same device, and FIG.
The figure is a partially enlarged explanatory diagram of an optical disc, FIGS. 4 to 6 are diagrams each illustrating the principle of the present invention, and FIG. 7 is an explanatory diagram showing a conventional light emitting device. 3... Photo-transmissive member, 3a... First surface, 3b... Second surface, 10... Light emitting device, 12... Light source.゛°−1 Figure 3

Claims (3)

【特許請求の範囲】[Claims] (1)光源と、この光源から発生された光ビームを平行
光にし、かつ、その断面形状を略円形に補正する非球面
形状を有した入射面及び平面形状を有した出射面を有す
る光透過性部材とを有することを特徴とする発光装置。
(1) Light transmission having a light source, an entrance surface with an aspherical shape that corrects the cross-sectional shape of the light beam to parallel light, and an exit surface with a planar shape that corrects the cross-sectional shape to a substantially circular shape. A light-emitting device characterized by having a sexual member.
(2)光源と光透過性部材とは所定の角度をもつて配置
されていることを特徴とする特許請求の範囲第1項記載
の発光装置。
(2) The light emitting device according to claim 1, wherein the light source and the light transmitting member are arranged at a predetermined angle.
(3)光透過性部材は、光源から発生される光ビームを
平行光に補正する非球面形状の入射面と、この平行光の
光軸に対し傾斜して形成されこの平行光の断面形状を略
円形に補正して出射する出射面とを有するものである特
許請求の範囲第1項記載の発光装置。
(3) The light-transmissive member has an aspherical entrance surface that corrects the light beam generated from the light source into parallel light, and an aspherical entrance surface that is inclined with respect to the optical axis of the parallel light to change the cross-sectional shape of the parallel light. 2. The light emitting device according to claim 1, wherein the light emitting device has a light emitting surface that emits light after being corrected to have a substantially circular shape.
JP61126532A 1986-05-31 1986-05-31 Light emitting device Pending JPS62283687A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61126532A JPS62283687A (en) 1986-05-31 1986-05-31 Light emitting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61126532A JPS62283687A (en) 1986-05-31 1986-05-31 Light emitting device

Publications (1)

Publication Number Publication Date
JPS62283687A true JPS62283687A (en) 1987-12-09

Family

ID=14937533

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61126532A Pending JPS62283687A (en) 1986-05-31 1986-05-31 Light emitting device

Country Status (1)

Country Link
JP (1) JPS62283687A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01305587A (en) * 1988-06-03 1989-12-08 Ricoh Co Ltd Semiconductor laser beam source
JP2017054883A (en) * 2015-09-08 2017-03-16 シャープ株式会社 Optical element, optical apparatus, and projection apparatus

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01305587A (en) * 1988-06-03 1989-12-08 Ricoh Co Ltd Semiconductor laser beam source
JP2017054883A (en) * 2015-09-08 2017-03-16 シャープ株式会社 Optical element, optical apparatus, and projection apparatus

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