JPH01307726A - Beam splitter - Google Patents

Beam splitter

Info

Publication number
JPH01307726A
JPH01307726A JP63139119A JP13911988A JPH01307726A JP H01307726 A JPH01307726 A JP H01307726A JP 63139119 A JP63139119 A JP 63139119A JP 13911988 A JP13911988 A JP 13911988A JP H01307726 A JPH01307726 A JP H01307726A
Authority
JP
Japan
Prior art keywords
beam splitter
light
polarized light
optical
polarizing beam
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
JP63139119A
Other languages
Japanese (ja)
Inventor
Mitsuru Fujita
満 藤田
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.)
Toyo Communication Equipment Co Ltd
Original Assignee
Toyo Communication Equipment 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 Toyo Communication Equipment Co Ltd filed Critical Toyo Communication Equipment Co Ltd
Priority to JP63139119A priority Critical patent/JPH01307726A/en
Publication of JPH01307726A publication Critical patent/JPH01307726A/en
Pending legal-status Critical Current

Links

Landscapes

  • Optical Head (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は光学部品の構成、殊に光ディスクの情報の記録
、読堰シ装置に用いられる偏光素子の構成に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to the configuration of optical components, particularly to the configuration of polarizing elements used in information recording and reading devices on optical discs.

(従来技術) 近年、情報の高度化及び大量化に伴ない各種データの保
管は磁気媒体による70ッピーディスク、磁気テープ及
び光学系記録媒体である光ディスク等によシ行なわれ、
これらのうち光ディスクは記憶容量が他の記憶媒体の容
量に比べ極めて大きい為コンパクトディスクをはじめと
する各種記憶媒体として普及している。
(Prior Art) In recent years, with the increasing sophistication and mass increase in information, various types of data have been stored using magnetic media such as 70-pin discs, magnetic tapes, and optical recording media such as optical discs.
Among these, optical disks have a much larger storage capacity than other storage media, and are therefore popular as various storage media including compact disks.

第5図(atは従来用いられている光デイスク記録装置
の光学部品の構成を示すブロック図である。
FIG. 5 (at is a block diagram showing the configuration of optical components of a conventionally used optical disc recording device.

同図に於いて1はレーザー光源であって、該レーザー光
源よシ出射した断面が楕円形の光束はビーム整形プリズ
ム2を透過することKよ多断面が円形の光束となシ次段
の偏光ビームスプリッタ3に入射し、該入射光の一部は
前記偏光ビームスプリッタ3の接合面で反射することに
よシモニター用受光器4に入射する。
In the figure, reference numeral 1 denotes a laser light source, and a beam of light with an elliptical cross section emitted from the laser light source passes through a beam shaping prism 2. The light enters the beam splitter 3, and a portion of the incident light is reflected by the junction surface of the polarizing beam splitter 3 and enters the monitor light receiver 4.

−万、前記偏光ビームスプリッタ3を透過した大部分の
P偏光は次段の174波長板5を透過することによシ円
偏光となり光ディスク6に照射する。
Most of the P-polarized light that has passed through the polarizing beam splitter 3 becomes circularly polarized light when it passes through the 174-wave plate 5 in the next stage and is irradiated onto the optical disk 6.

更に前記元ディスクに記憶されている情報に基づき反射
し、該反射した円偏光は再び1/4波長板5を迅過しS
偏光となる。
Further, the reflected circularly polarized light is reflected based on the information stored in the original disk, and the reflected circularly polarized light passes through the quarter-wave plate 5 again and becomes S.
It becomes polarized light.

従って次段の偏光ビームスプリッタ3の接合面にて反射
し、読取り若しくはサーボ用受光器7に入射し、前記デ
ィスクの情報を読取るものである。
Therefore, it is reflected at the joint surface of the polarizing beam splitter 3 in the next stage, enters the reading or servo light receiver 7, and reads the information on the disk.

このように構成した光学系に於いて前述したモニター用
受光器は半導体レーザーの出力制御に用いるものであり
、該レーザーの出力轢装置とのできないものとなってい
る。
In the optical system constructed in this way, the above-mentioned monitoring light receiver is used to control the output of the semiconductor laser, and cannot be used with the output tracking device for the laser.

しかしながら、偏光ビームスプリッタの分光特性は第5
図(blに示す如きものが一般的であシ。
However, the spectral characteristics of a polarizing beam splitter are
The one shown in figure (bl) is common.

上述したモニター出力を得る為にはP偏光の透過率が1
00%となる波長な用いることができず。
In order to obtain the monitor output mentioned above, the transmittance of P-polarized light must be 1.
00% cannot be used.

例えば前記透過率が95%程度となる波長λ、を用い、
偏光ビームスプリッタに於ける反射光を得るものである
For example, using a wavelength λ at which the transmittance is about 95%,
This is to obtain the reflected light at the polarizing beam splitter.

従って1分光特性上波長に対する透過率の変動が極めて
太きいところを使用するため、温度変化及び製造のバラ
ツキ等により光源の波長が必ずしも一定とならない場合
にVi%ニター出カに変動を生じ、適宜モニター出力制
御回路を調整する必要があった。
Therefore, since the wavelength of the light source is not necessarily constant due to temperature changes, manufacturing variations, etc., the Vi%niter output will fluctuate due to the 1-spectral characteristics where the transmittance varies extremely widely with respect to the wavelength. It was necessary to adjust the monitor output control circuit.

更に、前記偏光ビームスプリッタの分光特性は製造工程
2例えは接@i力の蒸着状態等により変動する為、波長
が一定の場合に於いてもモニター出力に変動を生じてし
まう間か点があった。
Furthermore, since the spectral characteristics of the polarizing beam splitter vary depending on the manufacturing process, for example, the deposition state of the contact force, there may be a point where the monitor output fluctuates even when the wavelength is constant. Ta.

また上記問題点を回避するために半導体レーザーの光出
射側端面と相対する非出射側端面から僅かに出力されろ
光を測定し、出力制御等のモニタ信号として用いろ方法
もあるが、該方法に於いても九ディスク等からの反射光
が前記半導体レーザーの非出射側端面からの光を測定す
るセンサに入射し、正しい測定ができない欠点がおった
In order to avoid the above problem, there is also a method of measuring a small amount of light output from the non-emitting side end face opposite to the light emitting end face of the semiconductor laser and using it as a monitor signal for output control, etc. However, there was a drawback in that the reflected light from the nine disks etc. entered the sensor that measured the light from the non-emission side end face of the semiconductor laser, making it impossible to make accurate measurements.

(発明の目的) 本発明は上述した問題点に鑑みなされたものでおって、
安価な光学部品を加えることのみKより偏光ビームスプ
リッタの分光特性上安定した部分を用いてモニタ出力等
に用いる反射な得ることかできる偏光ビームスプリッタ
を提供することを目的とする。
(Object of the invention) The present invention has been made in view of the above-mentioned problems, and includes:
It is an object of the present invention to provide a polarizing beam splitter that can obtain reflections for use in monitor output, etc. by simply adding inexpensive optical components and using a portion of the polarizing beam splitter that is more stable in terms of spectral characteristics.

(発明の概gり 本発明は上述した目的を達成する為に、光ディスク読み
取υ等に用いられるビームスプリッタであって、P偏光
を透過し、S偏光を反射する偏光素子を有し、該偏光素
子に於ける反射によりP偏光の分岐出力を得るタイプの
偏光装置に於いて、前記偏光素子の入射光軸上且つ入射
側に偏光面を回転させる為の旋光子若しくは波長板を具
えるよう構成する。
(Summary of the Invention) In order to achieve the above-mentioned object, the present invention is a beam splitter used for reading optical discs, etc., which has a polarizing element that transmits P-polarized light and reflects S-polarized light. In a polarizing device of the type that obtains a branched output of P-polarized light by reflection at the element, it is configured to include an optical rotator or a wavelength plate for rotating the plane of polarization on the incident optical axis and on the incident side of the polarizing element. do.

(実施例) 以下9本発明を図面に示した実施例に基づいて詳細に説
明する。
(Examples) The present invention will be described in detail below based on the embodiments shown in the drawings.

第1図(a)は本発明の構成を示す図である。。FIG. 1(a) is a diagram showing the configuration of the present invention. .

同図に於いて10Fiレーザー光源、11はビーム整形
プリズムであって、該ビーム整形プリズム11の出射の
光軸上に旋光子に、偏光ビームスプリッタ13及び1/
4波長板14vk:具え。
In the figure, a 10Fi laser light source, 11 is a beam shaping prism, and a polarizing beam splitter 13 and a polarizing beam splitter 13 and 1/2
4 wavelength plate 14vk: equipped.

前記偏光ビームスプリッタ13の凡そ垂直方向にはモニ
タ用受光器15及び情報読取り用受光器16を設ける。
A monitor light receiver 15 and an information reading light receiver 16 are provided approximately perpendicularly to the polarizing beam splitter 13.

このように構成した光学系に於いて光源1よ多断面が楕
円形なるP偏光が出射すると該P偏光はビーム整形プリ
ズム11を透過することによ多断面が円形となシ次段の
旋光子12に入射し該旋光子12出力は第1図(b) 
K示す如くσだけ回転した直線偏光となる。(ここでσ
は旋光子の旋光能ρ及び旋光子の光軸方向の厚みtとす
るとθ=ρ・tで表される。) 従って1次段の偏光ビームスプリッタに前記0だけ回転
した10なろ光量を有する直線偏光が入射するとIo3
i6”tの光量が反射し受光器15に入射する。
In the optical system configured in this manner, when P-polarized light having an elliptical cross-section is emitted from the light source 1, the P-polarized light passes through the beam shaping prism 11, where the cross-section becomes circular, and then the optical rotator in the next stage 12 and the output of the optical rotator 12 is shown in Fig. 1(b).
As shown by K, it becomes linearly polarized light rotated by σ. (Here σ
is expressed as θ=ρ·t, where ρ is the optical rotation power of the optical rotator and t is the thickness of the optical rotator in the optical axis direction. ) Therefore, when linearly polarized light having a light intensity of 10 rotated by 0 is incident on the primary stage polarizing beam splitter, Io3
The amount of light i6''t is reflected and enters the light receiver 15.

一方、前記偏光ビームスプリッタ13を透過し次Io−
Iosin”θなる光量を有すP(ifは次段の1/4
波長板14Y透過し円偏光となシ党ディスク17に照射
され、該光ディスク17に記録された情報に基づき反射
し、再び174波長板14を透過することによシS偏光
となシ偏光ビームスプリッタ13の接合面で反射し受光
器16に入射する。
On the other hand, the next Io-
P with a light amount of Iosin"θ (if is 1/4 of the next stage
A polarizing beam splitter that transmits the 174 wavelength plate 14 and becomes circularly polarized light, which is irradiated onto the optical disc 17, reflected based on the information recorded on the optical disc 17, and then transmitted through the 174 wavelength plate 14 again, which becomes S polarized light. It is reflected by the junction surface of 13 and enters the light receiver 16.

前述した如く偏光ビームスプリッタ13に入射するP偏
光なθだけ回転させることによシモ二タ出力としての反
射を得るので、従来用いられていた如く偏光ビームスプ
リッタの分光特性の不安定な所を用いる必要がなく第2
図にて実線で示したような安定した波長−透過率の特性
上で使用することができろ。
As mentioned above, by rotating the P-polarized light incident on the polarizing beam splitter 13 by θ, reflection as a simulator output is obtained, so a part of the polarizing beam splitter with unstable spectral characteristics is used as conventionally used. No need for second
It can be used with stable wavelength-transmittance characteristics as shown by the solid line in the figure.

従って、光源の波長が温度変化等により数nm程度変動
してもモニタ出力となる反射光量及び偏光ビームスプリ
ッタを透過する光量は安定し、更に前記偏光ビームスプ
リッタの製造工程。
Therefore, even if the wavelength of the light source fluctuates by several nanometers due to temperature changes, the amount of reflected light that becomes the monitor output and the amount of light that passes through the polarizing beam splitter are stable, and the manufacturing process of the polarizing beam splitter is also stable.

例えば接合面の蒸着状態若しくは接着状態等によシその
分光特性が第3図破線で示す如く波長に対し相対的に変
動しても使用波長を設定時に於いて波長に対する透過率
が安定した領域であるλ。に設定しておけば前述した偏
光ビームスプリッタの製造工程による分光特性のバラツ
キにも影響を受けることがない。
For example, even if the spectral characteristics vary relative to the wavelength, as shown by the broken line in Figure 3, due to the vapor deposition state or adhesion state of the bonding surface, the transmittance is stable in the range when the wavelength to be used is set. Some λ. If it is set to , it will not be affected by the above-mentioned variations in spectral characteristics due to the manufacturing process of the polarizing beam splitter.

第4図(a)は本発明の他の実施例の構成を示す図であ
って、前述した実施例と異なる点は旋光子の替わりに1
72波長板18を設けた点である。該1/2波長板18
は第4図(blに示す如く。
FIG. 4(a) is a diagram showing the configuration of another embodiment of the present invention, and the difference from the embodiment described above is that an optical rotator is replaced with a
This is because a 72 wavelength plate 18 is provided. The 1/2 wavelength plate 18
As shown in Figure 4 (bl).

入射するP偏光の偏光軸に対し光学軸をαだけ回転させ
、該172波長板を出射する光の偏波面なa(ここでθ
=α)回転させるものでおる。
The optical axis is rotated by α with respect to the polarization axis of the incident P-polarized light, and the polarization plane of the light emitted from the 172-wave plate is a (here θ
= α) Something that rotates it.

従りて1次段の偏光ビームスプリッタ13に前記偏波面
がσ回転した光量I<1なる光が入射するとl0su”
σに相当する光量は接合面にて反射し、 Io−I@s
in”θに相当する光量は透過し。
Therefore, when light whose polarization plane is σ-rotated and the amount of light I<1 is incident on the first stage polarizing beam splitter 13, l0su''
The amount of light corresponding to σ is reflected at the joint surface, and Io-I@s
The amount of light corresponding to in"θ is transmitted.

以後前述した実施例と同様の動作を行なうので偏光ビー
ムスプリッタに於ける同射l該スプリッタの分光特性上
不安定な領域を用いろことなく得ることができろ。
Thereafter, since the same operation as in the above-mentioned embodiment is performed, it is possible to obtain the same radiation in the polarizing beam splitter without using a region where the spectral characteristics of the splitter are unstable.

伺9本発明の詳細な説明には分光手段として偏光ビーム
スプリッタを用いて説明したがこれに限るものでなくプ
リズム等の分光手段を用いてもよく、ヌ2分光手段を用
いる個所は光ディスク等の読み取り部のみに限るもので
なくP偏光を透過し、S偏光を反射する特性を有する分
光手段1cP偏光を照射した際、モニタ出力等に用いる
P偏光反射出力を得る場合であればよいこと紘自明であ
る。
9 In the detailed explanation of the present invention, a polarizing beam splitter was used as a spectroscopic means, but the invention is not limited to this, and a prism or other spectroscopic means may also be used. It is self-evident that the spectrometer is not limited to only the reading unit, but may be used as long as it is used to obtain a P-polarized reflected output used for monitor output, etc. when irradiating 1cP-polarized light with a spectroscopic means having the characteristic of transmitting P-polarized light and reflecting S-polarized light. It is.

(発明の効果) 本発明は上述した如く構成し且つ機能するものであるか
ら安価は光学部品を加えろことKよりビームスプリッタ
等の分光手段にP偏光を照射しても安定した反射出力を
得ることができ。
(Effects of the Invention) Since the present invention is configured and functions as described above, stable reflected output can be obtained by adding optical components at low cost even if P-polarized light is irradiated onto a spectroscopic means such as a beam splitter. It is possible.

光学部品の点数が増加することを補って余シあろもので
ある。
This is more than enough to compensate for the increase in the number of optical parts.

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

第1図(a)は本発明の一実施例を示す図、第1@(b
)は旋光子に於ける光軸を表す図、第2図及び第3図は
偏光ビームスプリッタに於ける透過率−波長の関係を示
す図、第4図(a)は本発明の変形実施例を示す図、第
4図(b)は172波長板に於ける人出射光軸及び光学
軸な示す図、第5図(a)は従来用いられていた装置の
構成を示す図。 第5図(bl H従来用いられていた偏光ビームスプリ
ッタに於ける透過率−波長の関係を示す図である。 1.10・・・・・・・・・光源、2.11・・・・・
・・・・ビーム整形プリズム、    3.13・・・
・・・・・・偏光ビームスプリッタ、    4,7,
15.16・・・・・・・・・受光器、    5.1
4・・・・・−・・・1/4波長板。 6.17・・・・・・・・・光ディスク、   12・
・・・・・・・・旋光子、   18・・・・・・・・
・1/2波長板。 特許出願人  東洋通信機株式会社 第2図 第3vR 結) 第り図
FIG. 1(a) is a diagram showing one embodiment of the present invention, and FIG.
) is a diagram showing the optical axis in the optical rotator, Figures 2 and 3 are diagrams showing the relationship between transmittance and wavelength in a polarizing beam splitter, and Figure 4 (a) is a modified embodiment of the present invention. FIG. 4(b) is a diagram showing the human output optical axis and optical axis in a 172-wavelength plate, and FIG. 5(a) is a diagram showing the configuration of a conventionally used device. Figure 5 (bl H is a diagram showing the relationship between transmittance and wavelength in a conventionally used polarizing beam splitter. 1.10......Light source, 2.11...・
...Beam shaping prism, 3.13...
...Polarizing beam splitter, 4,7,
15.16......Receiver, 5.1
4・・・・・・・・・1/4 wavelength plate. 6.17...Optical disc, 12.
・・・・・・・・・Polarization, 18・・・・・・・・・
・1/2 wavelength plate. Patent applicant: Toyo Tsushinki Co., Ltd. Figure 2 Figure 3 vR Conclusion) Figure 3

Claims (1)

【特許請求の範囲】[Claims] P偏光を透過し、S偏光を反射する偏光素子を有し、該
偏光素子に於ける反射によりP偏光分岐出力を得るタイ
プの偏光装置に於いて、前記偏光素子の入射光軸上且つ
入射側に偏光面を回転させる為の旋光子若しくは波長板
を具えたことを特徴とするビームスプリッタ。
In a polarizing device of a type that has a polarizing element that transmits P-polarized light and reflects S-polarized light, and obtains a P-polarized light branched output by reflection in the polarizing element, on the incident optical axis and on the incident side of the polarizing element. A beam splitter characterized in that it is equipped with an optical rotator or a wavelength plate for rotating the plane of polarization.
JP63139119A 1988-06-06 1988-06-06 Beam splitter Pending JPH01307726A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63139119A JPH01307726A (en) 1988-06-06 1988-06-06 Beam splitter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63139119A JPH01307726A (en) 1988-06-06 1988-06-06 Beam splitter

Publications (1)

Publication Number Publication Date
JPH01307726A true JPH01307726A (en) 1989-12-12

Family

ID=15237942

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63139119A Pending JPH01307726A (en) 1988-06-06 1988-06-06 Beam splitter

Country Status (1)

Country Link
JP (1) JPH01307726A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20030076894A (en) * 2002-03-23 2003-09-29 삼성전자주식회사 Optical pick-up apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20030076894A (en) * 2002-03-23 2003-09-29 삼성전자주식회사 Optical pick-up apparatus

Similar Documents

Publication Publication Date Title
US6266313B1 (en) Optical pickup for recording or reproducing system
KR100299201B1 (en) Optical pickup
WO1997042491A1 (en) Device and method for measuring birefringence in an optical data carrier
US6317400B1 (en) Optical pickup apparatus
US5563870A (en) Optical write/read head with laser power control
JPS61162838A (en) Light source drive device for optical disk recording and playback equipment
JP4330882B2 (en) Optical scanning device
JPS58175149A (en) Optical pickup device
JP2002157769A (en) Information recording and reproducing device
JP3545015B2 (en) Optical pickup
JPS58188342A (en) Semiconductor laser light noise reduction method
JPH0585970B2 (en)
KR100223815B1 (en) Numerical aperture control system of optical pickup system
JP2000021008A (en) Optical pickup device
KR100486291B1 (en) Compatible optical pickup apparatus
JPH05325245A (en) Information recording/reproducing device for optical recording medium
JP3526309B2 (en) Optical information recording / reproducing device
JP2865822B2 (en) Light head
KR100421458B1 (en) Optical pick-up
JPH06251414A (en) Optical pickup device
JPS6314330A (en) Optical head for optical disk
JPH03228232A (en) Optical pickup device
JPH0696459A (en) Light pickup
JP2004062934A (en) Optical head
JPH07182712A (en) Optical pickup device