JPS63146238A - Optical head - Google Patents

Optical head

Info

Publication number
JPS63146238A
JPS63146238A JP61292939A JP29293986A JPS63146238A JP S63146238 A JPS63146238 A JP S63146238A JP 61292939 A JP61292939 A JP 61292939A JP 29293986 A JP29293986 A JP 29293986A JP S63146238 A JPS63146238 A JP S63146238A
Authority
JP
Japan
Prior art keywords
aperture
short axis
parallel
light
cross
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
JP61292939A
Other languages
Japanese (ja)
Other versions
JPH0727660B2 (en
Inventor
Toru Nakamura
徹 中村
Hideki Aiko
秀樹 愛甲
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP61292939A priority Critical patent/JPH0727660B2/en
Publication of JPS63146238A publication Critical patent/JPS63146238A/en
Publication of JPH0727660B2 publication Critical patent/JPH0727660B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To prevent an appearance of stray light without enlarging optical elements in shape by providing an aperture of a specific shape with an elliptical opening between a collimator lens and a beam shaping means. CONSTITUTION:The aperture 7 is provided having an approximately elliptical opening with its minor axis (p) and major axis (q) in the same direction with those minor and major axes of a parallel beam cross section under the condition of q/p b/a and p<c and is positioned between the collimator lens 2 from which a parallel beam having an approximately elliptical cross section with a minor axis (a) and major axis (b) is outgoing and the beam shaping means having an incident effective opening diameter on minor axis side (c) which magnifies the minor axis of said parallel beam by b/a approximately. Thus, even if a radiation angle on the side of parallel to the coupling direction of a semiconduc tor laser chip is larger than the standard, an incident beam into the optical elements is limited by the aperture so that genetic stray light can be prevented.

Description

【発明の詳細な説明】 産業上の利用分舒 本発明は、光デイスク装置等の光学へ、ンドに関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical disc device such as an optical disc device.

従来の技術 現代は情報化時代といわれており、その中核をなす高密
度大容量メモリーの技術開発が盛んに行なわれている。
Conventional Technology The modern era is called the information age, and the technology development of high-density, large-capacity memory, which forms the core of this age, is actively being carried out.

メモリーに要求される能力としては、前述の高密度、大
容量に加え、高信頼性、高速アクセス等が挙げられ、そ
れらすべてを漫足するものとして光デイスクメモリーが
最も注目されている。光デイスクメモリーは、光学的に
情報を記録媒体に記録するものであり、最近では記録し
た情報の消去も可能な光磁気ディスクに関する研究も数
多く行なわれている。
In addition to the above-mentioned high density and large capacity, the capabilities required of memory include high reliability and high speed access, and optical disk memory is attracting the most attention as a device that satisfies all of these requirements. An optical disk memory is a device that optically records information on a recording medium, and recently, a lot of research has been conducted on magneto-optical disks that can also erase recorded information.

本発明は上述したような光デイスクメモリーにおける光
学ヘッドに関するものである。
The present invention relates to an optical head in an optical disk memory as described above.

従来、光学ヘッドに関する技術としては、数多〈の研究
発表等が行なわれており、これは光デイスクメモリーに
関する文献等に詳しく述べられている。
In the past, numerous research publications have been made regarding technology related to optical heads, which are described in detail in literature related to optical disk memories.

以下、図面を参照しながら、上述したような従来の光学
ヘッドについて説明を行なう。
Hereinafter, the conventional optical head as described above will be explained with reference to the drawings.

第3図は従来の光学ヘッドの概略的な構成およびその動
作原理を説明するものである。第3図において、1は半
導体レーザ、2はコリメートレンズ、3は光学素子、4
は対物レンズ、6は情報記録媒体であるディスク、6は
検出手段であり、半導体レーザチップ接合方向平行側を
図示している。
FIG. 3 explains the schematic structure of a conventional optical head and its operating principle. In Fig. 3, 1 is a semiconductor laser, 2 is a collimating lens, 3 is an optical element, and 4 is a semiconductor laser.
6 is an objective lens, 6 is a disk that is an information recording medium, and 6 is a detection means, and the side parallel to the semiconductor laser chip bonding direction is illustrated.

以上のように構成された従来例について、以下その動作
について説明を行なう。
The operation of the conventional example configured as described above will be explained below.

半導体レーザ1からの発散光は、コリメートレンズ2に
より平行光に変換される。一般に半導体レーザの発する
光は発散光であり、放射角は、半導体レーザチップ接合
方向平行側では小さく、垂直側では大きい。したがって
コリメートレンズ2の出力である平行光束は、断面形状
が第3図の紙面に平行な面内に短軸を、紙面に垂直な面
内に長軸を有する略だ円状となる。光学素子3は、ビー
ム整形およびビームの分離の2つの機能を有しており、
コリメートレンズ2からの平行光を屈折させることによ
り短軸側の径を拡大し、断面形状が略円形状の平行光束
に変換する。光学素子3からの出力光は、対物レンズ4
によシ、ディスク6上に集光され、情報の記録、再生等
を行なう。ディスク6からの反射光は、逆の経路をたど
り、光学素子3により反射・分離され、検出手段6によ
り、ディスク6上の情報信号、フォーカス誤差信号およ
びトラッキング誤差信号等の検出を行なう。このように
第3図に示した従来例は比較的簡単な構成でビーム整形
を行なうことができるため、現在では、記録再生用の光
学ヘッドに多く用いられている。
Divergent light from the semiconductor laser 1 is converted into parallel light by the collimating lens 2. Generally, the light emitted by a semiconductor laser is diverging light, and the radiation angle is small on the side parallel to the semiconductor laser chip bonding direction and large on the side perpendicular to the semiconductor laser chip bonding direction. Therefore, the parallel light beam output from the collimating lens 2 has a substantially elliptical cross-sectional shape with its short axis in a plane parallel to the plane of the paper of FIG. 3 and its long axis in a plane perpendicular to the plane of the paper in FIG. The optical element 3 has two functions: beam shaping and beam separation.
By refracting the parallel light from the collimating lens 2, the diameter on the minor axis side is expanded and converted into a parallel light beam having a substantially circular cross-sectional shape. The output light from the optical element 3 is transmitted to the objective lens 4.
The light is then focused onto the disk 6, and information is recorded, reproduced, etc. The reflected light from the disk 6 follows the opposite path, is reflected and separated by the optical element 3, and the detection means 6 detects an information signal, a focus error signal, a tracking error signal, etc. on the disk 6. As described above, the conventional example shown in FIG. 3 can perform beam shaping with a relatively simple configuration, and is therefore currently widely used in optical heads for recording and reproduction.

発明が解決しようとする問題点 しかしながら上記のような構成では、光学素子3のエツ
ジ部分である点Aや点Bに光が当った場合、そこで光の
散乱が生じ、それが光学ヘッド筐体内壁面でさらに乱反
射するなどにょシ、迷光が発生してしまう。この迷光が
検出手段6に入射することにより、フォーカス、トラッ
キング誤差信号の検出を誤ったり、再生情報信号の品質
劣化を起こすという問題点を有していた。一般に光学素
子3の入射有効口径は、半導体レーザチップ接合方向平
行側の標準的な放射角等で決定され、その場合迷光は発
生しないようになっている。しかし、半導体レーザ1の
放射角は相当な個体差があるため、放射角が標準よりも
大きい場合は、前述のような迷光が発生し易くなる。こ
れを防ぐためには、光学素子3の形状を大きくし、入射
有効口径を大きくするという手段があるが、これは光学
ヘッドの大型化を招くという欠点を有していた。
Problems to be Solved by the Invention However, with the above configuration, when light hits points A and B, which are the edge portions of the optical element 3, scattering of light occurs there, and this scatters onto the inner wall surface of the optical head housing. This causes even more diffuse reflection and stray light. When this stray light enters the detection means 6, there is a problem in that the detection of focus and tracking error signals may be erroneous, and the quality of the reproduced information signal may deteriorate. Generally, the effective entrance aperture of the optical element 3 is determined by a standard radiation angle on the side parallel to the direction in which the semiconductor laser chips are bonded, and in this case, stray light is not generated. However, since there are considerable individual differences in the radiation angle of the semiconductor laser 1, if the radiation angle is larger than the standard, stray light as described above is likely to occur. In order to prevent this, there is a method of enlarging the shape of the optical element 3 and increasing the effective entrance aperture, but this has the drawback of increasing the size of the optical head.

本発明は上記従来問題点に鑑みてなされたもので、半導
体レーザチップ接合方向平行側の放射角が標準よりも大
きい場合でも、光学素子の形状を大型化することなしに
迷光の発生を防ぐことのできる光学ヘッドを提供するこ
とを目的とするものである。
The present invention has been made in view of the above-mentioned conventional problems, and it is an object of the present invention to prevent the generation of stray light without increasing the size of the optical element even when the radiation angle on the side parallel to the joining direction of semiconductor laser chips is larger than the standard. The purpose of this invention is to provide an optical head that can perform the following functions.

問題点を解決するための手段 上記目的を達成するために本発明の光学ヘッドは、コリ
メートレンズと、コリメートレンズからの断面形状が短
軸a、長軸すの略だ円状平行光束の短軸側を約b/a 
、倍に拡大する前記短軸側入射有効口径がCのビーム整
形手段の間に位置し、前記平行光束断面形状の短軸、長
軸と向きを同じくするよう配置された短軸p、長軸qの
略だ円状開口を有し、 q/p舛b / a p<c であるアパーチャを有する構成となっている。
Means for Solving the Problems In order to achieve the above object, the optical head of the present invention includes a collimating lens, and a cross-sectional shape from the collimating lens in which the short axis is a short axis and the long axis is an approximately elliptical short axis of a parallel light beam. Approximately b/a side
, the short axis side effective entrance aperture which is expanded twice is located between the beam shaping means C, and the short axis p and the long axis are arranged so as to have the same direction as the short axis and long axis of the cross-sectional shape of the parallel beam. It has a substantially elliptical opening of q, and has an aperture of q/p/a p<c.

作  用 本発明は上記した構成により、半導体レーザ    一
チップ接合方向平行側の放射角が標準よりも太きい場合
でも、光学素子に入射する光束はアパーチャにより制限
されるため、迷光の発生を防ぐことが可能となる。
Effect of the Invention With the above-described configuration, the present invention prevents the generation of stray light because the light flux incident on the optical element is limited by the aperture even when the radiation angle on the side parallel to the semiconductor laser chip bonding direction is wider than standard. becomes possible.

実施例 以下、本発明の一実施例を図面にもとづいて説明する。Example Hereinafter, one embodiment of the present invention will be described based on the drawings.

第1図は本発明の一実施例における光学ヘッドの概略図
を示すものである。第1図において、1は半導体レーザ
、2はコリメートレンズ、3は光学素子、4は対物レン
ズ、5はディスク、6は検出手段、7はアパーチャであ
る。
FIG. 1 shows a schematic diagram of an optical head in an embodiment of the present invention. In FIG. 1, 1 is a semiconductor laser, 2 is a collimating lens, 3 is an optical element, 4 is an objective lens, 5 is a disk, 6 is a detection means, and 7 is an aperture.

以上のように構成された光学ヘッドの一実施例について
、以下その動作について説明を行なう。
The operation of an embodiment of the optical head configured as described above will be explained below.

基本的な動作は、第3図を用いて説明した従来例の場合
と同様である。標準的な放射角を半導体レーザ1が有し
ていた場合、コリメートレンズ2により、断面形状が短
軸a、長軸すの略だ円状平行光束が得られる。
The basic operation is the same as that of the conventional example explained using FIG. When the semiconductor laser 1 has a standard radiation angle, the collimating lens 2 provides a parallel light beam having a substantially elliptical cross-sectional shape with the short axis a and the long axis s.

光学素子3は、前述の短軸側光束径を屈折させることに
より、約b/a 倍に拡大し、断面形状が略円形状の平
行光束へと変換する。
The optical element 3 refracts the diameter of the light beam on the short axis side, thereby enlarging it approximately b/a times and converting it into a parallel light beam having a substantially circular cross-sectional shape.

ここで、半導体レーザ1のチップ接合方向の放射角が標
準より大きい場合、コリメートレンズ2により得られる
平行光束断面形状は、短軸側が増大し、光学素子3の入
射有効口径Cよりも大きくなってしまい、光学素子3の
エツジ部で迷光が発生することは従来例で述べた。アノ
く−チャ7は、これを防止するだめのものであり、その
形状は第2図に示すような、短軸p、長軸qの略だ円状
開口を有している。ここで軸Aを第1図の紙面に平行に
なるように配置し、a、b、cおよびp、qの関係を q / p岬b / a p<c とすれば、前述のように半導体レーザ1のチップ接合方
向の放射角が標準より大きい場合でも、アパーチャアに
より、コリメートレンズ2の出力光束は規制されるため
、光学素子3にはCよりも小さな光束が入射するため迷
光は発生しない。又、q / p”F b / aとす
ることにより、略円形の平行光束を、光学素子3により
得ることが可能である。
Here, when the radiation angle of the semiconductor laser 1 in the chip joining direction is larger than the standard, the cross-sectional shape of the parallel beam obtained by the collimating lens 2 increases on the short axis side and becomes larger than the effective entrance aperture C of the optical element 3. As described in the conventional example, stray light is generated at the edge portion of the optical element 3. The annotation 7 is intended to prevent this, and has a substantially elliptical opening with a short axis p and a long axis q, as shown in FIG. If axis A is arranged parallel to the plane of the paper in Figure 1, and the relationship between a, b, c and p, q is q/pb/a p<c, then the semiconductor Even if the radiation angle of the laser 1 in the chip bonding direction is larger than the standard, the output light flux of the collimating lens 2 is regulated by the aperture, so a light flux smaller than C enters the optical element 3, so no stray light occurs. . Further, by setting q/p''F b /a, it is possible to obtain a substantially circular parallel light beam with the optical element 3.

なお、本実施例においては、アパーチャアの形状を第2
図に示すように穴開き型としたが、これは不要な光束を
制限するものであれば、どのような形式でも良い。
Note that in this example, the shape of the aperture is
Although the hole type is used as shown in the figure, any type may be used as long as it limits unnecessary light flux.

以上のように本実施例によれば、コリメートレンズと、
コリメートレンズからの、断面形状が短軸a、長軸すの
略だ円状平行光束の短軸側を約b/a 倍に拡大する、
短軸側入射有効口径がCの光学素子の間に、向きを同じ
くするよう配置された短軸p、長軸qの略だ円状開口を
有するアノ<−チャを設け、 q / p絢b / a ea とすることにより、半導体レーザのチップ接合方向平行
側の放射角が標準よりも大きい場合でも、大口径の光学
素子を用いることなしに迷光の発生を防ぐことが可能で
ある。
As described above, according to this embodiment, the collimating lens,
The short axis side of the parallel light beam from the collimating lens, which has a cross-sectional shape of approximately ellipse with a short axis a and a long axis D, is magnified by approximately b/a times.
An annular aperture having a substantially elliptical aperture with a short axis p and a long axis q arranged in the same direction is provided between optical elements having an effective incident aperture on the short axis side C, and q / p aperture b. / a ea , even if the radiation angle of the semiconductor laser on the side parallel to the chip bonding direction is larger than standard, it is possible to prevent the generation of stray light without using a large diameter optical element.

発明の効果 本発明は光学ヘッドとして、コリメートレンズと、コリ
メートレンズからの、断面形状が短軸d。
Effects of the Invention The present invention provides an optical head including a collimating lens and a cross-sectional shape from the collimating lens having a short axis d.

長軸すの略だ円状平行光束の短軸側を約り/a倍に拡大
する、短軸側入射有効口径がCのビーム整形手段との間
に、短軸p、長軸qの略だ円状開口を有するアパーチャ
を設け、 q/p舛b / a p<c とすることにより、半導体レーザのチップ接合方向平行
側の放射角が標準よりも大きい場合でも、大口径のビー
ム整形手段を用いることなしに、迷光の発生を防ぎ、高
精度のフォーカス、トラッキング誤差信号の検出と、S
N比の良い情報信号の検出が可能であるという効果を得
ることができるすぐれた光学ヘッドを実現できるもので
ある。
A beam shaping means having an effective entrance aperture on the short axis side that magnifies the short axis side of the approximately ellipsoidal parallel light beam by a factor of about /a is connected between the long axis p and the long axis q. By providing an aperture with an elliptical opening and making q/p/a p<c, even if the radiation angle on the side parallel to the chip bonding direction of the semiconductor laser is larger than the standard, a large diameter beam shaping means can be used. It is possible to prevent the occurrence of stray light, detect high-precision focusing and tracking error signals, and
This makes it possible to realize an excellent optical head that can detect information signals with a good N ratio.

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

第1図は本発明の一実施例における光学ヘッドの概略図
、第2図はその要部の概略図、第3図は従来の光学ヘッ
ドの概略図である0 1・・・・・・半導体レーザ、2・・・・・・コリメー
トレンズ、3・・・・・・光学素子、4・・・・・・対
物レンズ、6・・・・・・ディスク、6・・・・・・検
出手段、7・・・・・・アパーチャ。
Fig. 1 is a schematic diagram of an optical head according to an embodiment of the present invention, Fig. 2 is a schematic diagram of its main parts, and Fig. 3 is a schematic diagram of a conventional optical head. Laser, 2...Collimating lens, 3...Optical element, 4...Objective lens, 6...Disk, 6...Detection means , 7...Aperture.

Claims (1)

【特許請求の範囲】  半導体レーザと、前記半導体レーザの発散光を平行光
束に変換するコリメートレンズと、前記コリメートレン
ズにより形成された、断面形状が短軸a、長軸bの略だ
円状である平行光束の前記短軸側を約b/a倍拡大し断
面形状を略円形状に変換する前記短軸側入射有効口径が
cのビーム整形手段と、前記ビーム整形手段の出力光を
情報記録媒体上に集光させる対物レンズと、前記情報記
録媒体からの反射光により、フォーカス誤差信号、トラ
ッキング誤差信号、情報信号等を検出する検出手段と、
前記コリメートレンズと前記ビーム整形手段との間に位
置し、前記平行光束断面形状の短軸、長軸と向きを同じ
くするよう配置された、短軸p、長軸qの略だ円状開口
を有するアパーチャにより構成され、 q/p≒b/a p<c であることを特徴とする光学ヘッド。
[Scope of Claims] A semiconductor laser, a collimating lens that converts the diverging light of the semiconductor laser into a parallel beam, and a cross-sectional shape formed by the collimating lens having a substantially elliptical shape with a short axis a and a long axis b. a beam shaping means having an effective entrance aperture on the short axis side of c for enlarging the short axis side of a certain parallel light beam by about b/a times and converting the cross-sectional shape into a substantially circular shape; and information recording of the output light of the beam shaping means. an objective lens for condensing light onto a medium, and a detection means for detecting a focus error signal, a tracking error signal, an information signal, etc. using reflected light from the information recording medium;
a substantially elliptical aperture with a short axis p and a long axis q, located between the collimating lens and the beam shaping means, and arranged so as to have the same direction as the short axis and long axis of the cross-sectional shape of the parallel beam. An optical head comprising an aperture having the following relationship: q/p≒b/a p<c.
JP61292939A 1986-12-09 1986-12-09 Optical head Expired - Lifetime JPH0727660B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61292939A JPH0727660B2 (en) 1986-12-09 1986-12-09 Optical head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61292939A JPH0727660B2 (en) 1986-12-09 1986-12-09 Optical head

Publications (2)

Publication Number Publication Date
JPS63146238A true JPS63146238A (en) 1988-06-18
JPH0727660B2 JPH0727660B2 (en) 1995-03-29

Family

ID=17788369

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61292939A Expired - Lifetime JPH0727660B2 (en) 1986-12-09 1986-12-09 Optical head

Country Status (1)

Country Link
JP (1) JPH0727660B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0558249A2 (en) * 1992-02-28 1993-09-01 Canon Kabushiki Kaisha Optical information recording/reproducing apparatus
JPH0628703A (en) * 1992-03-31 1994-02-04 Canon Inc Optical information recording and reproducing device

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61134942A (en) * 1984-12-05 1986-06-23 Nec Corp Optical head

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61134942A (en) * 1984-12-05 1986-06-23 Nec Corp Optical head

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0558249A2 (en) * 1992-02-28 1993-09-01 Canon Kabushiki Kaisha Optical information recording/reproducing apparatus
JPH0628703A (en) * 1992-03-31 1994-02-04 Canon Inc Optical information recording and reproducing device

Also Published As

Publication number Publication date
JPH0727660B2 (en) 1995-03-29

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