JPH0210529A - Optical head - Google Patents

Optical head

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Publication number
JPH0210529A
JPH0210529A JP63160090A JP16009088A JPH0210529A JP H0210529 A JPH0210529 A JP H0210529A JP 63160090 A JP63160090 A JP 63160090A JP 16009088 A JP16009088 A JP 16009088A JP H0210529 A JPH0210529 A JP H0210529A
Authority
JP
Japan
Prior art keywords
light
optical element
optical
cross
optical head
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
JP63160090A
Other languages
Japanese (ja)
Other versions
JP2635372B2 (en
Inventor
Akihiro Sakaguchi
彰洋 坂口
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 JP63160090A priority Critical patent/JP2635372B2/en
Publication of JPH0210529A publication Critical patent/JPH0210529A/en
Application granted granted Critical
Publication of JP2635372B2 publication Critical patent/JP2635372B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Optical Head (AREA)

Abstract

PURPOSE:To make the optical head miniaturized, light and thin structive by using an optical element for converting a cross section shape of an optical beam. CONSTITUTION:An incident light beam is reflected by splitting into >= 2 in one direction on an reflecting surface of the optical element 10 formed in a sequential stepped shape as the reflecting surface set up at a prescribed inclination, thus changing the conversion ratio of the direction of a major axis to the direction of a minor axis of the cross section shape of the optical beam. By this method, a shaping prism for shaping the major axial direction and the minor axial direction of the optical beam of an ellipse, etc., in length and suppressing a loss quantity of light can be out of use, and the constitution of the optical head which should have been in complicated constitution can be simplified, while the miniaturization with light weight and thin formation can be attained.

Description

【発明の詳細な説明】 産業上の利用分野 本発明はビデオディスク等のようにディスク上に記録さ
れた情報を光学的に読み取る光学的再生装置、あるいは
ディスクに情報を光学的に記録。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to an optical reproducing device that optically reads information recorded on a disc such as a video disc, or to optically records information on a disc.

再生もしくは消去する装置に用いられる光ヘッドに関す
るものである。
The present invention relates to an optical head used in a reproducing or erasing device.

従来の技術 近年、光学的記録再生装置は音響、映像分野からコンピ
ュータ外部記憶媒体に利用されるようになってきた。ま
ず、従来の光学的記録再生装置の一例について説明する
2. Description of the Related Art In recent years, optical recording and reproducing devices have come to be used as external storage media for computers in the audio and video fields. First, an example of a conventional optical recording/reproducing device will be described.

第8図は従来の光学的記録再生装置の光学系を示すもの
であシ、1は半導体レーザ、2は半導体レーザから出射
された光を平行光にするコリメートレンズ、3はビーム
整形をして光量損を抑制する整形プリズム、4はディス
クから反射して戻ってきた光束をフォトダイオードへ導
くための偏光ビームスプリッタ、6は偏光ビームスプリ
ッタと組合せてディスク面で反射した光が半導体レーザ
に戻って生じるバックトークを防止する4分の1波長板
、6はディスク上で約1μmのビームスポットを形成す
る対物レンズである。
Figure 8 shows the optical system of a conventional optical recording/reproducing device. 1 is a semiconductor laser, 2 is a collimating lens that converts the light emitted from the semiconductor laser into parallel light, and 3 is a beam-shaping lens. A shaping prism suppresses light loss; 4 is a polarizing beam splitter for guiding the light beam reflected from the disk and returned to the photodiode; 6 is a polarizing beam splitter for guiding the light beam reflected from the disk surface back to the semiconductor laser; A quarter wavelength plate prevents backtalk from occurring, and 6 is an objective lens that forms a beam spot of about 1 μm on the disk.

以上のように構成された光学的記録再生装置において、
半導体レーザ1から出射された光ビームは、第9図に示
すように遠視野像は回折現象によって決まるビームの拡
がシをもち、接合面に垂直方向の拡がり角θ±の方が、
接合面に平行方向の拡がシ角θlに比べ約2倍ないし3
倍大きくなる。
In the optical recording/reproducing device configured as above,
As shown in FIG. 9, the light beam emitted from the semiconductor laser 1 has a far-field pattern with a beam spread determined by the diffraction phenomenon, and the spread angle θ± in the direction perpendicular to the cemented surface is
The expansion in the direction parallel to the joint surface is approximately 2 to 3 times larger than the angle θl.
Become twice as large.

このビームの光量損失を少なくして平行光にするように
、コリメートレンズ2を用いる。また、記録再生装置な
どの記録も行なう光デイスク光学系では、光源から記録
面までの光量損が重要な問題となる。また対物レンズ6
に入射する光の強度分布が等方向でないと、ディスク上
でビームスポットが円形に絞れない。したがってビーム
を整形する整形プリズム3と組合せて光量損を抑制する
A collimating lens 2 is used to reduce the loss in the amount of light of this beam and make it a parallel beam. Furthermore, in an optical disk optical system that also performs recording, such as a recording/reproducing device, the loss of light amount from the light source to the recording surface becomes an important problem. Also, objective lens 6
If the intensity distribution of the light incident on the disk is not uniform, the beam spot cannot be narrowed down to a circular shape on the disk. Therefore, in combination with the shaping prism 3 that shapes the beam, loss of light amount can be suppressed.

この整形されたビームを対物レンズに入射させる。この
とき式(1)で表現されるガウシアンの強度分布を持つ
入射ビームは、第8図のごとく対物レンズで集光されて
、スポット像を形成する。
This shaped beam is made incident on an objective lens. At this time, the incident beam having a Gaussian intensity distribution expressed by equation (1) is condensed by an objective lens to form a spot image as shown in FIG.

!(p) = exp (−2127w2)    −
−−−−・(1)対物レンズが無収差の回折限界レンズ
とすれば、像面でのスポット半径W0は次式で表わされ
る。
! (p) = exp (-2127w2) −
(1) If the objective lens is an aberration-free diffraction-limited lens, the spot radius W0 on the image plane is expressed by the following equation.

w0= K *λ/NA        ・・・・・・
(2)K :レンズの開口形状や入射ビーム の断面の強度分布などで決まる 定数 NA:対物レンズの開口数 発明が解決しようとする課題 しかしながら上記のような構成では、次のような問題点
を有している。
w0= K *λ/NA ・・・・・・
(2) K: Constant determined by the shape of the lens aperture and the intensity distribution of the cross section of the incident beam NA: Numerical aperture of the objective lens Problems to be solved by the invention However, the above configuration has the following problems. have.

光源たとえば半導体レーザから出射されたビームを平行
光に変換した後、楕円ビームの断面形状を円形に整形す
るためのプリズムとビームをディスク側に進む方向を変
える全反射ミラーを有し、光ヘッドの小型化・薄型化に
対して大きな整置となっていた。
After converting the beam emitted from a light source, such as a semiconductor laser, into parallel light, the optical head has a prism for shaping the cross-sectional shape of the elliptical beam into a circular shape and a total reflection mirror that changes the direction of the beam toward the disk. This was a big change in layout in response to miniaturization and thinning.

本発明は上記問題点に鑑み、小型・軽量・薄型にできる
光学的記録再生装置用の光ヘッドを提供することを目的
とするものである。
SUMMARY OF THE INVENTION In view of the above problems, it is an object of the present invention to provide an optical head for an optical recording/reproducing device that can be made small, lightweight, and thin.

課題を解決するための手段 上記課題を解決するために、本発明の光ヘッドは、入射
した光ビームを所定の傾斜角に設定した反射面を順次階
段状に形成した光学素子の反射面上で一方向で2以上に
分割して反射させるようにしたことによシ、光ビームの
断面形状の長軸方向と短軸方向の変換比を変えるように
したものである。
Means for Solving the Problems In order to solve the above problems, the optical head of the present invention reflects an incident light beam on the reflection surface of an optical element in which the reflection surface is set at a predetermined angle of inclination and is sequentially formed in a step-like manner. By dividing the light beam into two or more parts in one direction for reflection, the conversion ratio between the long axis direction and the short axis direction of the cross-sectional shape of the light beam is changed.

作  用 本発明は、上記した構成によって、楕円等の光ビームの
長軸方向と短軸方向の長さを整形して光量損を抑制する
整形プリズムを廃止でき、従来複雑な構成を持たざるを
得なかった光ヘツド構成を簡単にすることができ、小型
・軽量・薄型化できる。
Effect of the Invention With the above-described configuration, the present invention can eliminate the need for a shaping prism that suppresses light loss by shaping the lengths of a light beam such as an ellipse in the major axis direction and minor axis direction, and eliminates the need for a conventionally complicated configuration. The optical head configuration, which was previously difficult to achieve, can be simplified, and it can be made smaller, lighter, and thinner.

実施例 以下、本発明の一実施例の光学的記録再生装置用の光ヘ
ッドについて、図面を参照しながら説明する。
EXAMPLE Hereinafter, an optical head for an optical recording/reproducing apparatus according to an example of the present invention will be described with reference to the drawings.

第1図は本発明の第1の実施例における光学的記録再生
装置の光ヘッドを示すものである。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、8は光ビームの
断面形状変換用の光学素子、6は4分の1波長板、6は
対物レンズである。
FIG. 1 shows an optical head of an optical recording/reproducing apparatus according to a first embodiment of the present invention. In FIG. 1, 1 is a semiconductor laser, 2 is a collimating lens, 8 is an optical element for converting the cross-sectional shape of a light beam, 6 is a quarter wavelength plate, and 6 is an objective lens.

この光学素子10は、端面に、反射面として、入射ビー
ムをY方向で2以上に分割して反射する階段状の反射面
を形成して、半導体レーザ1からの光ビームをY方向の
断面の長さを長くするようにして反射させるようにして
いる。
This optical element 10 has a step-like reflective surface formed on the end face as a reflective surface that divides an incident beam into two or more parts in the Y direction and reflects the light beam from the semiconductor laser 1 in a cross section in the Y direction. The length is made longer to reflect the light.

第2図は光ビームの断面形状変換用の光学素子1oのビ
ーム断面形状を変える動作を示す。
FIG. 2 shows the operation of changing the beam cross-sectional shape of the optical element 1o for changing the cross-sectional shape of the light beam.

第2図に示すように入射した光ビームの断面形状の長軸
方向(X方向)あるいは短軸方向(Y方向)の長さを 変換比>7 =(a cosθ十b )/bで拡大する
ことができる。
As shown in Figure 2, the length of the cross-sectional shape of the incident light beam in the major axis direction (X direction) or minor axis direction (Y direction) is expanded by a conversion ratio of >7 = (a cos θ + b )/b. be able to.

以上のように本実施例によれば、光源から発光された光
ビームを所定の角度に設定した反射面を順次階段状に形
成した光学素子10に、一定方向から入射させ、その素
子面上で反射させることによシ、光ビーム断面形状の長
軸方向と短軸方向の変換比を変えることができる。
As described above, according to this embodiment, a light beam emitted from a light source is incident from a fixed direction onto the optical element 10 in which reflective surfaces set at a predetermined angle are sequentially formed in a step-like manner. By reflecting the light beam, the conversion ratio between the long axis direction and the short axis direction of the cross-sectional shape of the light beam can be changed.

第3図に本発明の第2の実施例の光ビームの断面形状を
変換する光学素子1oを示す。この光学素子10は、端
面を所定角度にした薄いプレート11を多数積み重ねて
、端面を階段状にし、その端面に対する入射ビームを分
割して反射することにより反射された光ビームの断面形
状の長袖方向と短軸方向の変換比率を自由に設定できる
FIG. 3 shows an optical element 1o for converting the cross-sectional shape of a light beam according to a second embodiment of the present invention. This optical element 10 is constructed by stacking a large number of thin plates 11 whose end faces are at a predetermined angle, making the end faces step-like, and dividing and reflecting a beam incident on the end faces in the long direction of the cross-sectional shape of the reflected light beam. and the conversion ratio in the short axis direction can be freely set.

第4図に本発明の第3の実施例の光ビームの断面形状を
変換する光学素子10を示す。
FIG. 4 shows an optical element 10 for converting the cross-sectional shape of a light beam according to a third embodiment of the present invention.

この実施例では、端面に所定の角度で反射面を設けた薄
いプレート11を各々蝶番12で結合して積重ね、相互
に摺動可能に構成して自由にプレート間の重ね合せ位置
を変える機構13を設けることによシ、自由に光ビーム
形状の変換率を設定できる。
In this embodiment, thin plates 11 each having a reflective surface at a predetermined angle on the end face are connected by hinges 12 and stacked, and a mechanism 13 is configured to be able to slide on each other and freely change the overlapping position between the plates. By providing this, it is possible to freely set the conversion rate of the light beam shape.

また第6図に示すように、端面に所定の角度を設けた薄
いグレート11を積み重ね、棒状のレバー14 、15
で、積み重ねたプレート110両端面を傾けることによ
って、光ビームの長軸と短軸の長さを所望の比に変換す
ることができる。
Further, as shown in FIG. 6, thin grates 11 with end faces set at a predetermined angle are stacked, and rod-shaped levers 14, 15
By tilting both end faces of the stacked plates 110, the lengths of the major and minor axes of the light beam can be converted to a desired ratio.

第6図は本発明の第4の実施例の光ビームの断面形状を
変換する光学素子10を示す。この光学素子10は、−
枚のプレートにV型の溝16を平行に形成し、このプレ
ートを任意の角度に設定して光ビームを入射させること
によシ、光ビーム断面形状を変換できる。
FIG. 6 shows an optical element 10 for converting the cross-sectional shape of a light beam according to a fourth embodiment of the present invention. This optical element 10 is -
The cross-sectional shape of the light beam can be changed by forming V-shaped grooves 16 in parallel on one plate and setting the plate at an arbitrary angle to allow the light beam to enter the plate.

第7図に本発明の第6の実施例を示す。これは、所定の
角度に設定した反射面の高さ、角度あるいは反射面と反
射面の距離をそれぞれ変えることにより、入射ビームの
断面における光強度分布を一方向のみ自由に変えること
ができる。たとえば第7図に示すようにガウシアン分布
で入射した光ビームを方形波に変えて反射させることが
できる。
FIG. 7 shows a sixth embodiment of the present invention. This is because the light intensity distribution in the cross section of the incident beam can be freely changed in only one direction by changing the height and angle of the reflecting surfaces set at a predetermined angle or the distance between the reflecting surfaces. For example, as shown in FIG. 7, a light beam incident with a Gaussian distribution can be converted into a square wave and reflected.

これによシビームを一方向ではあるが、見かけ上でNA
を大きくすることができ、第1図に示す対物レンズ6を
通過後、ビームスポットを小さく絞ることができる。
This allows the beam to be moved in one direction, but with an apparent NA
After passing through the objective lens 6 shown in FIG. 1, the beam spot can be narrowed to a small size.

発明の効果 以上のように本発明は、光ビーム断面形状を変換する光
学素子を光学的記録再生装置の光ヘッドに用いることに
よシ、小型・軽量・薄型で波長変動による光軸ずれのな
い光ヘッドにすることができる。
Effects of the Invention As described above, the present invention uses an optical element that converts the cross-sectional shape of a light beam in an optical head of an optical recording/reproducing device, thereby achieving a compact, lightweight, and thin device that is free from optical axis deviation due to wavelength fluctuations. It can be made into an optical head.

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

第1図は本発明の第1の実施例における光ヘッドの側面
図、第2図はその拡大側面図、第3図〜第7図は本発明
の第2〜第6の実施例の光ヘッドの側面図、第8図は従
来例の光ヘッドの斜視図、第9図はその対物レンズ前後
のビームを示す模式1・・・・・・半導体レーザ、2・
・・・・・コリメートレンズ、3・・・・・・ビーム整
形プリズム、4・・山・偏光ビームスプリッタ、5・・
・・・・4分の1波長板、6・・・・・・対物レンズ、
8・・・・・・光学素子。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名/−
一一手導俸レーザ 第 図 第 図 2−−−コリ〆一トレンに 6−−一対物レンス・・ 10−−“光学素子 第 図 纂 図 第 図 第 図 第 図
FIG. 1 is a side view of an optical head according to a first embodiment of the present invention, FIG. 2 is an enlarged side view thereof, and FIGS. 3 to 7 are optical heads according to second to sixth embodiments of the present invention. 8 is a perspective view of a conventional optical head, and FIG. 9 is a schematic diagram showing the beams before and after the objective lens.
...Collimating lens, 3...Beam shaping prism, 4...Mountain/polarizing beam splitter, 5...
... Quarter wavelength plate, 6 ... Objective lens,
8...Optical element. Name of agent: Patent attorney Toshio Nakao and 1 other person/-
11-hand laser beam diagram Figure 2 --- Collision, one train, 6 -- one objective lens... 10 -- "Optical element diagram, diagram, diagram, diagram, diagram, diagram.

Claims (5)

【特許請求の範囲】[Claims] (1)光ビームを出射する光源と、所定の傾斜角を有し
、入射ビームをその断面の一方向で2つ以上に分割して
反射する階段状の反射面を有する光学素子とを備え、前
記光学素子に前記光源からの前記光ビームを所定の入射
角で入射させてその入射ビームと出射ビームの断面形状
の長軸の長さと短軸の長さの比を変換するようにしたこ
とを特徴とする光ヘッド。
(1) Comprising a light source that emits a light beam, and an optical element having a step-like reflective surface that has a predetermined inclination angle and that divides the incident beam into two or more parts in one direction of its cross section for reflection, The light beam from the light source is made incident on the optical element at a predetermined angle of incidence, and the ratio of the length of the major axis to the length of the minor axis of the cross-sectional shape of the incident beam and the output beam is converted. Features a light head.
(2)光学素子は、薄いプレートを多数積み重ねた積層
構造とし、各々のプレートの端面を一定の傾斜角をもっ
た端面として階段状の反射面を形成したものであること
を特徴とする請求項1記載の光ヘッド。
(2) A claim characterized in that the optical element has a laminated structure in which a large number of thin plates are stacked, and the end face of each plate is an end face with a constant inclination angle to form a step-like reflective surface. 1. The optical head described in 1.
(3)光学素子は、薄いプレートを多数積み重ねた積層
構造とし、各々のプレート端面を所定の傾斜角をもった
端面として階段状の反射面を形成し、前記プレートを相
互に摺動可能に重ね合せるリンク構造を備えたものであ
ることを特徴とする請求項1記載の光ヘッド。
(3) The optical element has a laminated structure in which a large number of thin plates are stacked, each plate end face is an end face with a predetermined inclination angle to form a step-like reflective surface, and the plates are stacked so as to be able to slide on each other. 2. The optical head according to claim 1, further comprising a matching link structure.
(4)光学素子は、V型の溝を表面に複数形成して反射
面としたものであることを特徴とする請求項1記載の光
ヘッド。
(4) The optical head according to claim 1, wherein the optical element has a plurality of V-shaped grooves formed on its surface to serve as a reflective surface.
(5)光学素子は、各々の反射面の傾斜角、高さあるい
は隣接する反射面間の距離を異ならせて反射光ビームの
断面での光強度分布を所望の光分布に変換するものとし
たことを特徴とする請求項1記載の光ヘッド。
(5) The optical element is designed to convert the light intensity distribution in the cross section of the reflected light beam into a desired light distribution by varying the inclination angle and height of each reflecting surface or the distance between adjacent reflecting surfaces. The optical head according to claim 1, characterized in that:
JP63160090A 1988-06-28 1988-06-28 Light head Expired - Fee Related JP2635372B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63160090A JP2635372B2 (en) 1988-06-28 1988-06-28 Light head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63160090A JP2635372B2 (en) 1988-06-28 1988-06-28 Light head

Publications (2)

Publication Number Publication Date
JPH0210529A true JPH0210529A (en) 1990-01-16
JP2635372B2 JP2635372B2 (en) 1997-07-30

Family

ID=15707643

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63160090A Expired - Fee Related JP2635372B2 (en) 1988-06-28 1988-06-28 Light head

Country Status (1)

Country Link
JP (1) JP2635372B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006006296A1 (en) * 2004-07-12 2006-01-19 Teac Corporation Optical pickup device and optical disk device
JP2015083980A (en) * 2009-10-01 2015-04-30 トルネード スペクトラル システムズ,インコーポレイテッド Optical slicer for improving spectral resolution of dispersive spectrograph

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6313142A (en) * 1986-07-03 1988-01-20 Matsushita Electric Ind Co Ltd Optical recording and reproducing device
JPH01251440A (en) * 1988-03-31 1989-10-06 Toshiba Corp Laser beam shaping device

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6313142A (en) * 1986-07-03 1988-01-20 Matsushita Electric Ind Co Ltd Optical recording and reproducing device
JPH01251440A (en) * 1988-03-31 1989-10-06 Toshiba Corp Laser beam shaping device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006006296A1 (en) * 2004-07-12 2006-01-19 Teac Corporation Optical pickup device and optical disk device
US7701814B2 (en) 2004-07-12 2010-04-20 Teac Corporation Optical pickup device and optical disk device
JP2015083980A (en) * 2009-10-01 2015-04-30 トルネード スペクトラル システムズ,インコーポレイテッド Optical slicer for improving spectral resolution of dispersive spectrograph

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