JPS6256581B2 - - Google Patents

Info

Publication number
JPS6256581B2
JPS6256581B2 JP55125613A JP12561380A JPS6256581B2 JP S6256581 B2 JPS6256581 B2 JP S6256581B2 JP 55125613 A JP55125613 A JP 55125613A JP 12561380 A JP12561380 A JP 12561380A JP S6256581 B2 JPS6256581 B2 JP S6256581B2
Authority
JP
Japan
Prior art keywords
light beam
condenser lens
axis direction
light
recording medium
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
Application number
JP55125613A
Other languages
Japanese (ja)
Other versions
JPS5750335A (en
Inventor
Mitsushige Kondo
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP55125613A priority Critical patent/JPS5750335A/en
Publication of JPS5750335A publication Critical patent/JPS5750335A/en
Publication of JPS6256581B2 publication Critical patent/JPS6256581B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/135Means for guiding the beam from the source to the record carrier or from the record carrier to the detector
    • G11B7/1381Non-lens elements for altering the properties of the beam, e.g. knife edges, slits, filters or stops
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/135Means for guiding the beam from the source to the record carrier or from the record carrier to the detector
    • G11B7/1398Means for shaping the cross-section of the beam, e.g. into circular or elliptical cross-section

Description

【発明の詳細な説明】 この発明は、半導体レーザを光源として用いた
光学式情報再生装置に関し、特に出射光束が偏平
な半導体レーザを用い、光スポツトをミクロンオ
ーダに集光するようにしたものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical information reproducing device using a semiconductor laser as a light source, and in particular uses a semiconductor laser with a flat emitted light beam to condense a light spot on the micron order. be.

従来この種の装置として第1図に示すものがあ
つた。図において、1は半導体レーザ、2は断面
形状が偏平な半導体レーザの出射光束、3は拡散
する偏平な出射光束を図示のように断面形状が偏
平な平行光2aにするコリメートレンズ、4は偏
光ビームスプリツタ、5は4分の1波長位相板、
6はトラツキングアクチエータで、矢印A方向に
トラツキング信号により回動する回転軸7とこれ
に固着されたミラー8とで構成され、集光レンズ
9に入射する光束2bの入射角度を変え、光スポ
ツト10の位置を矢印B方向に変位させてトラツ
キングを補正する。11はビデオ信号、PCMオ
ーデイオ信号等の入つた情報記録媒体、12は情
報記録媒体の情報単位を構成するピツト、13は
ピツト列よりなる情報トラツクで、例えば1.7μ
mピツチで記録されている。14は情報記録媒体
11を回転させるモータ、15は集光レンズ9を
光軸方向Cに動かすオートフオーカシングアクチ
エータ、2cは情報記録媒体より読取られた情報
信号を含む反射光束、17は反射光束2cを電気
信号に変える光検知器である。また同図bは集光
レンズ9の有効径と、これに入射する光束2bの
大きさの関係を示す図で、光束2bの長径方向の
大きさが集光レンズ9有効径よりはみ出さないよ
うに構成されている。なお光束2bの大きさは中
心での最大強度の1/e2になる点の大きさで定義す
るものとする。
A conventional device of this type is shown in FIG. In the figure, 1 is a semiconductor laser, 2 is an emitted light beam from the semiconductor laser with a flat cross-sectional shape, 3 is a collimating lens that transforms the diffused flat emitted light beam into parallel light 2a with a flat cross-sectional shape as shown, and 4 is a polarized light beam. Beam splitter, 5 is a quarter wavelength phase plate,
Reference numeral 6 denotes a tracking actuator, which is composed of a rotating shaft 7 that rotates in the direction of arrow A in response to a tracking signal, and a mirror 8 fixed to this shaft, and changes the angle of incidence of the light beam 2b entering the condenser lens 9, thereby changing the angle of incidence of the light beam 2b. Tracking is corrected by displacing the position of the spot 10 in the direction of arrow B. 11 is an information recording medium containing a video signal, PCM audio signal, etc.; 12 is a pit constituting an information unit of the information recording medium; and 13 is an information track consisting of a row of pits, for example 1.7μ.
It is recorded in m pitches. 14 is a motor that rotates the information recording medium 11; 15 is an autofocusing actuator that moves the condensing lens 9 in the optical axis direction C; 2c is a reflected light beam containing the information signal read from the information recording medium; 17 is a reflected light beam; This is a photodetector that converts the luminous flux 2c into an electrical signal. Figure b is a diagram showing the relationship between the effective diameter of the condenser lens 9 and the size of the light beam 2b incident thereon. It is composed of Note that the size of the luminous flux 2b is defined as the size of the point where the maximum intensity at the center is 1/e 2 .

次に動作について説明する。半導体レーザ1よ
り出射された断面が偏平な出射光束2は、コリメ
ートレンズ3により偏平な平行光2aにされ、偏
平ビームスプリツタ4、4分の1波長位相板5を
透過し、ミラー8により反射され、集光レンズ9
を透過し、偏平な光スポツト10となつて情報ト
ラツク13に照射され反射される。この反射光は
情報トラツク13上のピツト12に照射された場
合と、ピツト以外の所に照射された場合とで、再
び集光レンズ9を透過してくる光強度が異なる。
なお情報記録媒体の光スポツト10は、集光レン
ズ9に入射する偏行光束2bの長径方向に平行な
方向のスポツト径の方が、短径方向に平行なスポ
ツト径より小さくなる。例えば波長0.78μmで、
長径と短径の比が4である半導体レーザ、及び開
口数0.5の集光レンズを用いて、偏平光束の長径
方向の大きさを集光レンズの有効径と等しくした
場合、キルヒホツフの回折積分を用いてスポツト
径を計算すると、偏平光束の長径方向に平行な方
向のスポツト径1.29μm、偏平光束の短径方向に
平行な方向のスポツト径4.0μmを得る。
Next, the operation will be explained. An emitted light beam 2 with a flat cross section emitted from the semiconductor laser 1 is converted into flat parallel light 2a by a collimating lens 3, transmitted through a flat beam splitter 4 and a quarter wavelength phase plate 5, and reflected by a mirror 8. and condensing lens 9
The light passes through the light beam, becomes a flat light spot 10, is irradiated onto an information track 13, and is reflected. The intensity of this reflected light, which passes through the condenser lens 9 again, differs depending on whether it is irradiated onto the pit 12 on the information track 13 or when it is irradiated onto a location other than the pit.
In the light spot 10 of the information recording medium, the spot diameter in the direction parallel to the major axis direction of the polarized light beam 2b incident on the condenser lens 9 is smaller than the spot diameter parallel to the minor axis direction. For example, at a wavelength of 0.78 μm,
When using a semiconductor laser with a ratio of major axis to minor axis of 4 and a condensing lens with a numerical aperture of 0.5, and making the size of the flat beam in the major axis direction equal to the effective diameter of the condensing lens, the Kirchhoff diffraction integral is When the spot diameter is calculated using this method, the spot diameter in the direction parallel to the major axis direction of the flat light beam is 1.29 μm, and the spot diameter in the direction parallel to the short axis direction of the flat light beam is 4.0 μm.

情報記録媒体11で反射された光2cは集光レ
ンズ9で集光され、ミラー8、4分の1波長位相
板5をとおつて、偏光ビームスプリツタ4により
分離され、光検知器17に入射して電気信号に変
換され、この信号から読み出したビデオ信号、
PCMオーデイオ信号などがとり出される。なお
この装置には集光レンズの合焦点(最小スツト位
置)の情報記録媒体面よりの位置ずれを検出する
オートフオーカシングセンサ(図示、省略)を装
備しており、このオートフオーシングセンサーの
出力は、オートフオーカシングアクチエーター1
5に加えられ、絶えず集光レンズの合焦点が情報
記録媒体面上に位置するように集光レンズ9と情
報記録媒体11との距離を制御する。またこの装
置には情報トラツク13上よりの光スポツト10
のずれを検出するオートトラツキングセンサ(図
示省略)を備えており、そのオートトラツキング
センサの出力は、オートトラツキングアクチエー
タ6に加えられ、光スポツト10が絶えず情報ト
ラツク13上に位置するように制御される。
The light 2c reflected by the information recording medium 11 is focused by a condenser lens 9, passes through a mirror 8 and a quarter wavelength phase plate 5, is separated by a polarizing beam splitter 4, and enters a photodetector 17. The video signal is converted into an electrical signal and read out from this signal.
PCM audio signals etc. are extracted. This device is equipped with an auto-focusing sensor (not shown, omitted) that detects the positional deviation of the focal point (minimum focus position) of the condenser lens from the information recording medium surface. Output is auto focusing actuator 1
5, and controls the distance between the condenser lens 9 and the information recording medium 11 so that the focal point of the condenser lens is always located on the surface of the information recording medium. This device also has a light spot 10 from above the information track 13.
The output of the auto-tracking sensor is applied to the auto-tracking actuator 6 so that the light spot 10 is constantly positioned on the information track 13. controlled by.

従来の装置は以上のように構成されているの
で、出射光束2が等方光の円形出射光束光源から
の出射光を集光した場合と比較して、(例えば波
長0.78μmの円形光束を、開口数0.5の集光レン
ズで集光した場合、集光レンズ有効径と、円形光
束の径が等しいと仮定すると、キルヒホツフの回
折積分によるスポツト径の計算値は1.42μmとな
る。)集光レンズ入射光束の長径方向に平行な方
向のスポツト径は、上記に計算したようにほぼ等
しいが、短径方向に平行な方向のスポツト径はは
るかに大きくなる。そのため第1図cのように情
報トラツク13と交差する向きに光スポツト10
の長手方向がくるよう集光した場合、等方光集光
により再生した場合と比較して、隣接トラツクを
同時再生する割合が大きくなる。すなわちクロス
トーク特性の悪化となる。また情報トラツクと平
行に光スポツトの長手方向がくるよう集光した場
合、等方光により再生した場合と比較して、空間
周波数特性の悪化となる。等の欠点があつた。
Since the conventional device is configured as described above, compared to the case where the output light beam 2 is an isotropic circular output beam condensing the output light from a light source (for example, a circular beam with a wavelength of 0.78 μm, When condensing light with a condensing lens with a numerical aperture of 0.5, assuming that the effective diameter of the condensing lens is equal to the diameter of the circular beam, the calculated value of the spot diameter based on Kirchhoff's diffraction integral is 1.42 μm.) Condensing lens The spot diameters in the direction parallel to the major axis direction of the incident light beam are approximately equal as calculated above, but the spot diameters in the direction parallel to the minor axis direction are much larger. Therefore, as shown in FIG.
When the light is focused so that the longitudinal direction of the track is aligned, the ratio of simultaneous reproduction of adjacent tracks becomes higher than when reproduction is performed by isotropic light concentration. In other words, the crosstalk characteristics deteriorate. Furthermore, if the light is focused so that the longitudinal direction of the light spot is parallel to the information track, the spatial frequency characteristics will deteriorate compared to the case where reproduction is performed using isotropic light. There were other drawbacks.

この発明は上記のような従来のものの欠点を除
去するためになされたもので、集光レンズに入射
する偏平な光束2bの長径方向の大きさを、その
集光レンズの有効径より大きくし、光スポツトを
小さくし長径方向を情報トラツク13と平行な向
にすることにより、クロストーク特性および空間
周波数特性の改善を図つたものである。
This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and the size of the flat light beam 2b incident on the condenser lens in the long axis direction is made larger than the effective diameter of the condenser lens. By reducing the size of the light spot and oriented the long axis direction parallel to the information track 13, crosstalk characteristics and spatial frequency characteristics are improved.

以下この発明の一実施例を第2図について説明
する。この例はコリメートレンズ3aを集光レン
ズ9の有効径に対して、入射光束2bの長径方向
の大きさが、第2図bに示すように集光レンズ9
の有効径より大きく、かつ、入射光束2bの長径
方向が情報トラツク13と平行になるように、結
果として第2図cに示すように光スポツト10の
長径方向が情報トラツク13と直交するように構
成する。例えば波長0.78μmで、長径と短径の比
が4である半導体レーザ及び開口数0.5の集光レ
ンズを用いて、入射光束2bの短径方向の大きさ
を集光レンズ有効径と等しくした場合、キルヒホ
ツフの回折積分を用いてスポツト径を計算する
と、入射光束2bの長径方向に平行な方向のスポ
ツト径は1.24μm、短径方向に平行な方向のスポ
ツト径1.48μmとなる。
An embodiment of the present invention will be described below with reference to FIG. In this example, the size of the collimating lens 3a in the major axis direction of the incident light beam 2b is such that the size of the collimating lens 3a in the long axis direction is set to the condensing lens 9 as shown in FIG.
is larger than the effective diameter of the optical spot 10, and the major axis direction of the incident light beam 2b is parallel to the information track 13, and as a result, the major axis direction of the optical spot 10 is perpendicular to the information track 13, as shown in FIG. 2c. Configure. For example, when using a semiconductor laser with a wavelength of 0.78 μm and a ratio of major axis to minor axis of 4 and a condenser lens with a numerical aperture of 0.5, the size of the incident light beam 2b in the minor axis direction is made equal to the effective diameter of the condenser lens. , Kirchhoff's diffraction integral is used to calculate the spot diameter, the spot diameter in the direction parallel to the major axis direction of the incident light beam 2b is 1.24 μm, and the spot diameter in the direction parallel to the minor axis direction is 1.48 μm.

なお、上記のように光学系を構成した場合集光
レンズ外に逃げる光が多くなる。例えば、長径と
短径の比が4である半導体レーザを、集光レンズ
の有効径と、短径とを等しくするよう配置した場
合、計算によれば集光レンズで集光される有効パ
ワーは33%で残り67%は無効パワーとなる。しか
しながら最近の半導体レーザは3mw以上のパワ
ーを出せるものが多く、結果としてこの例の場合
では1mw以上の有効パワーを取出せる。このよ
うな情報再生装置では1mwのパワーがあれば、
通常充分である。したがつて集光レンズ外に逃げ
るパワーが多少あつても通常必要なレーザパワー
を利用できる。なおレーザパワーが大きいもの
程、集光レンズ外に逃げる光を多くでき、それだ
け集光レンズ有効径より入射光束2bの大きさを
大きくすることができる。結果として小さなスポ
ツト径とすることができる。
Note that when the optical system is configured as described above, a large amount of light escapes to the outside of the condenser lens. For example, if a semiconductor laser with a ratio of major axis to minor axis of 4 is arranged so that the effective diameter of the condenser lens is equal to the minor axis, the effective power condensed by the condenser lens is calculated as follows: At 33%, the remaining 67% is invalid power. However, many recent semiconductor lasers can produce a power of 3 mw or more, and as a result, in this example, an effective power of 1 mw or more can be obtained. For such an information reproducing device, if the power is 1mW,
Usually sufficient. Therefore, even if some power escapes to the outside of the condenser lens, the normally required laser power can be used. Note that the larger the laser power is, the more light can escape to the outside of the condenser lens, and the size of the incident light beam 2b can be made larger than the effective diameter of the condenser lens. As a result, a small spot diameter can be achieved.

なおその他の構成については従来装置と同じで
ある。
Note that the other configurations are the same as the conventional device.

以上のように、この発明は、集光レンズに入射
する偏平な光束の長径方向、または長径方向およ
び短径方向の大きさを集光レンズの有効径より大
きくして入射させるように構成したので、同じ開
口数の集光レンズを用いて従来装置より小さな光
スポツトに集光でき、空間周波数特性およびクロ
ストーク特性を大幅に改善できる効果がある。
As described above, the present invention is configured so that the size of the flat light beam incident on the condenser lens in the major axis direction, or in the major axis direction and the minor axis direction, is made larger than the effective diameter of the condenser lens. Using a condensing lens with the same numerical aperture, the present invention can condense light into a smaller light spot than the conventional device, and has the effect of significantly improving spatial frequency characteristics and crosstalk characteristics.

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

第1図は従来の光学式情報再生装置を示す図で
あり、第2図は、この発明の一実施例を示す図で
ある。 図において、1は半導体レーザ、2は出射光
束、2bは入射光束、2cは反射光束、3はコリ
メートレンズ、4は偏光ビームスプリツタ、5は
1/4波長板、8はトラツキングアクチエータ、9
は集光レンズ、10は光スポツト、11は情報記
録担体、13は記録トラツク、17は光検知器で
ある。なお、図中同一符号は同一、又は相当部分
を示す。
FIG. 1 is a diagram showing a conventional optical information reproducing device, and FIG. 2 is a diagram showing an embodiment of the present invention. In the figure, 1 is a semiconductor laser, 2 is an emitted light beam, 2b is an incident light beam, 2c is a reflected light beam, 3 is a collimating lens, 4 is a polarizing beam splitter, and 5 is a polarizing beam splitter.
1/4 wavelength plate, 8 is tracking actuator, 9
10 is a condensing lens, 10 is a light spot, 11 is an information recording carrier, 13 is a recording track, and 17 is a photodetector. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] 1 出射光束が偏平な半導体レーザと、情報記録
媒体と、この情報記録媒体上の情報トラツクへ上
記半導体レーザからの出射光束を集光する集光レ
ンズと、上記半導体レーザからの出射光束を上記
集光レンズへ導びく光学系とを備えたものにおい
て、当該集光レンズに入射する偏平光束の長径方
向が、上記情報記録媒体の情報トラツクと平行と
なるように、上記集光レンズに入射する偏平な光
束の短径方向の大きさが当該集光レンズの有効径
より大きくなるように、当該光学系を構成した光
学式情報再生装置。
1. A semiconductor laser with a flat emitted light beam, an information recording medium, a condensing lens for condensing the emitted light beam from the semiconductor laser onto an information track on the information recording medium, and a condensing lens for condensing the emitted light beam from the semiconductor laser onto an information track on the information recording medium. and an optical system that guides the light to the condenser lens, the flat light beam incident on the condenser lens is arranged so that the major axis direction of the flat light beam incident on the condenser lens is parallel to the information track of the information recording medium. An optical information reproducing device in which the optical system is configured such that the size of the light beam in the short axis direction is larger than the effective diameter of the condensing lens.
JP55125613A 1980-09-09 1980-09-09 Optical information reproducer Granted JPS5750335A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP55125613A JPS5750335A (en) 1980-09-09 1980-09-09 Optical information reproducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP55125613A JPS5750335A (en) 1980-09-09 1980-09-09 Optical information reproducer

Publications (2)

Publication Number Publication Date
JPS5750335A JPS5750335A (en) 1982-03-24
JPS6256581B2 true JPS6256581B2 (en) 1987-11-26

Family

ID=14914417

Family Applications (1)

Application Number Title Priority Date Filing Date
JP55125613A Granted JPS5750335A (en) 1980-09-09 1980-09-09 Optical information reproducer

Country Status (1)

Country Link
JP (1) JPS5750335A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04365781A (en) * 1991-06-14 1992-12-17 Toshiba Corp Cage room for elevator

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6157320U (en) * 1984-09-20 1986-04-17
JPH07105060B2 (en) * 1987-09-18 1995-11-13 三洋電機株式会社 Optical pickup device

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JPS5111021A (en) * 1974-07-17 1976-01-28 Daido Steel Co Ltd MODOSHUHOHO
JPS5265406A (en) * 1975-11-27 1977-05-30 Hitachi Ltd Inforamtion reproduction device
JPS5318A (en) * 1976-06-24 1978-01-05 Mitsubishi Electric Corp Optical video disc reproduction unit
JPS5391759A (en) * 1976-12-27 1978-08-11 Mansei Kogyo Kk Optics to obtain equal direction spot from various direction light beam
JPS5445156A (en) * 1977-09-16 1979-04-10 Hitachi Ltd Optical system
JPS5589924A (en) * 1978-12-27 1980-07-08 Toshiba Corp Optical information reproduction unit

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5111021A (en) * 1974-07-17 1976-01-28 Daido Steel Co Ltd MODOSHUHOHO
JPS5265406A (en) * 1975-11-27 1977-05-30 Hitachi Ltd Inforamtion reproduction device
JPS5318A (en) * 1976-06-24 1978-01-05 Mitsubishi Electric Corp Optical video disc reproduction unit
JPS5391759A (en) * 1976-12-27 1978-08-11 Mansei Kogyo Kk Optics to obtain equal direction spot from various direction light beam
JPS5445156A (en) * 1977-09-16 1979-04-10 Hitachi Ltd Optical system
JPS5589924A (en) * 1978-12-27 1980-07-08 Toshiba Corp Optical information reproduction unit

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04365781A (en) * 1991-06-14 1992-12-17 Toshiba Corp Cage room for elevator

Also Published As

Publication number Publication date
JPS5750335A (en) 1982-03-24

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