JPH04214242A - Optical head - Google Patents

Optical head

Info

Publication number
JPH04214242A
JPH04214242A JP2400976A JP40097690A JPH04214242A JP H04214242 A JPH04214242 A JP H04214242A JP 2400976 A JP2400976 A JP 2400976A JP 40097690 A JP40097690 A JP 40097690A JP H04214242 A JPH04214242 A JP H04214242A
Authority
JP
Japan
Prior art keywords
light
beam splitter
transmitted
semiconductor laser
polarized
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
JP2400976A
Other languages
Japanese (ja)
Inventor
Hideo Shimizu
秀雄 清水
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP2400976A priority Critical patent/JPH04214242A/en
Publication of JPH04214242A publication Critical patent/JPH04214242A/en
Pending legal-status Critical Current

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  • Optical Head (AREA)

Abstract

PURPOSE:To reduce the noise of emitted light and to prevent the deterioration of a reproducing signal by deviating the polarized direction of incident light at a prescribed angle from the polarized direction of a semiconductor laser by the rotational angle of a transmitted light quantity correcting means. CONSTITUTION:When the main axis direction of a 1/2 wavelength plate 21 is rotated in the polarized direction of the semiconductor laser 1 only at the angle of, the polarized direction of a laser beam Btheta which is transmitted through the 1/2 wavelength plate 21 is changed only by the amount of 2, and the beam is made incident on a polarized beam splitter 24 with keeping the light quantity I d. This beam can be resolved into a vertical axis component I b1 (transmitted and polarized beam) and a horizontal axis component I d2 (total reflection polarized beam) by light vector Btheta. That means, the transmitted light quantity in the polarized beam splitter can be corrected by the transmitted light quantity correcting means 20, the transmitted light quantity in the apparent polarized beam splitter can be corrected, and the bonding efficiency of the apparent polarized beam splitter can be matched with a prescribed design value, the noise of the emitted light of the semiconductor laser can be reduced and the deterioration of the reproducing signal can be prevented.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】この発明は、微小スポットに収束
したレーザービームを情報記憶媒体に照射することによ
り、情報を高密度で記録,再生する光記憶装置の光ヘッ
ド、ことにビームスプリッタの品質のばらつきによって
生ずる光ビームの強度の変動を抑制した光ヘッドに関す
る。
[Industrial Application Field] This invention aims to improve the quality of optical heads, especially beam splitters, of optical storage devices that record and reproduce information at high density by irradiating an information storage medium with a laser beam focused on a minute spot. The present invention relates to an optical head that suppresses variations in the intensity of a light beam caused by variations in the intensity of the light beam.

【0002】0002

【従来の技術】光記憶装置は、近年磁気光学効果を利用
した光磁気記憶装置が登場し、ハードディスクやフロッ
ピーディスクに代わる大容量の書換え可能な外部記憶装
置としてコンピュータ分野への活用が注目されている。 また、記憶媒体の温度変化により結晶質ー非晶質の可逆
性のある相変化を利用した相変化型光記憶装置等も開発
が進められている。
[Background Art] Magneto-optical storage devices that utilize magneto-optical effects have recently appeared, and their use in the computer field is attracting attention as large-capacity rewritable external storage devices that replace hard disks and floppy disks. There is. Additionally, phase change optical storage devices and the like are being developed that utilize reversible phase change from crystalline to amorphous due to changes in the temperature of the storage medium.

【0003】これらの記憶装置での情報の記録,再生,
書換え等の操作は、いずれも光ヘッドにより微小スポッ
トに収束したレーザービームを記憶媒体に照射すること
により行われるが、質の良い記録,再生を行うためには
レーザービームの強度が安定で、かつ発光ノイズを含ま
ないことが求められる。
[0003] Recording and reproduction of information in these storage devices,
Operations such as rewriting are performed by irradiating the storage medium with a laser beam focused on a minute spot using an optical head, but in order to perform high-quality recording and playback, the intensity of the laser beam must be stable and It is required that the light emission noise is not included.

【0004】図4は従来の光ヘッドを模式化して示す構
成図であり、半導体レーザ1から出射した光はコリメー
トレンズ2により平行レーザビームB1 とされ、ビー
ム整形プリズム3で円形ビームB2 に成形される。レ
ーザビームB2 はビームスプリッタ4を透過して立ち
上げミラー5で方向を変え、アクチュエータ6に保持さ
れた対物レンズ7で収束され、光磁気ディスク8の記録
媒体面上に1μm 程度の光スポット9として照射され
、例えば情報の記録が行われる。
FIG. 4 is a schematic configuration diagram showing a conventional optical head. Light emitted from a semiconductor laser 1 is converted into a parallel laser beam B1 by a collimating lens 2, and shaped into a circular beam B2 by a beam shaping prism 3. Ru. The laser beam B2 passes through the beam splitter 4, changes direction with the mirror 5, is focused by the objective lens 7 held by the actuator 6, and forms a light spot 9 of about 1 μm on the recording medium surface of the magneto-optical disk 8. It is irradiated and, for example, information is recorded.

【0005】記録媒体面上で変調され、反射した反射光
B2 は、再び対物レンズ7,立ち上げミラー5,を経
由してビームスプリッタ4で側方に反射され、1/2波
長板10,凸レンズ11,シリンドリカルレンズ12を
経て6分割フォトダイオード13に集光され、記録媒体
面上のデータ信号が検出される。
The reflected light B2 that has been modulated and reflected on the recording medium surface is reflected laterally by the beam splitter 4 via the objective lens 7 and the raising mirror 5 again, and is then reflected to the side by the beam splitter 4 and then passed through the 1/2 wavelength plate 10 and the convex lens. 11, the light is focused on a six-segment photodiode 13 through a cylindrical lens 12, and a data signal on the surface of the recording medium is detected.

【0006】6分割フォトダイオード13では、データ
信号の他に、対物レンズ7のフォーカスエラー信号と、
トラッキングエラー信号が検出され、これらエラー信号
に基づき、アクチュエータ駆動回路14によりアクチュ
エータ6が駆動され、光スポット9は光磁気ディスク8
の垂直方向および半径方向に移動して記憶媒体面上のデ
ータトラックを追尾する制御が行われる。
In addition to the data signal, the 6-divided photodiode 13 receives a focus error signal from the objective lens 7;
Tracking error signals are detected, and based on these error signals, the actuator 6 is driven by the actuator drive circuit 14, and the optical spot 9 is moved onto the magneto-optical disk 8.
Control is performed to move in the vertical direction and radial direction to track data tracks on the surface of the storage medium.

【0007】半導体レーザ1の出射光量は、ビームスプ
リッタ4で反射した光をモニタ用フォトダイオード15
が検出し、半導体レーザ駆動回路16により、半導体レ
ーザ1の駆動電流が制御され、レーザビームB1 の光
量が安定化され、これにより記録信号および再生信号を
安定化し、記録,再生を行うことができる。
The amount of light emitted from the semiconductor laser 1 is determined by monitoring the light reflected by the beam splitter 4 with a monitoring photodiode 15.
is detected, the semiconductor laser drive circuit 16 controls the drive current of the semiconductor laser 1, and the light intensity of the laser beam B1 is stabilized, thereby stabilizing the recording signal and the reproduction signal, so that recording and reproduction can be performed. .

【0008】[0008]

【発明が解決しようとする課題】上述の光ヘッドにおい
て、ビームスプリッタ4の結合効率α,すなわち入射光
量に対する透過光量の割合は、設計上は所定値に決めら
れるが、実際には個々の製品毎にかなりのばらつきがあ
り、ビームスプリッタ4の透過光量が光ヘッドごとに変
化する。そこで通常、半導体レーザ1の出射光量を製品
毎に調整して透過光量を所定値に保持する対策が採られ
る。ところが、ビームスプリッタ4の結合効率が所定値
より大きく、半導体レーザ1の出射光量を絞った場合、
半導体レーザの駆動電流が小さくなり、逆に半導体レー
ザの発光ノイズが大きくなるため、情報の再生に際して
フォトダイオード13が検出した再生信号中のノイズが
増大し、再生信号の信号対ノイズ比(S/N)が悪化す
る,いわゆる再生信号の劣化が起こり、これが原因で質
の高い記録情報の再生が困難になるという問題が発生す
る。
[Problems to be Solved by the Invention] In the above-mentioned optical head, the coupling efficiency α of the beam splitter 4, that is, the ratio of the amount of transmitted light to the amount of incident light, is determined to a predetermined value in design, but in reality it varies for each individual product. There is considerable variation in the amount of light transmitted through the beam splitter 4, and the amount of light transmitted through the beam splitter 4 varies from optical head to optical head. Therefore, a measure is usually taken to adjust the amount of light emitted from the semiconductor laser 1 for each product to maintain the amount of transmitted light at a predetermined value. However, when the coupling efficiency of the beam splitter 4 is greater than a predetermined value and the amount of light emitted from the semiconductor laser 1 is reduced,
The driving current of the semiconductor laser becomes smaller, and conversely the emission noise of the semiconductor laser becomes larger. Therefore, the noise in the reproduced signal detected by the photodiode 13 when reproducing information increases, and the signal-to-noise ratio (S/ N) deteriorates, so-called deterioration of the reproduced signal occurs, and this causes a problem in that it becomes difficult to reproduce high-quality recorded information.

【0009】この発明の目的は、ビームスプリッタの結
合効率のばらつきの影響を排除し、結合効率が所定値よ
り高い場合にも、再生信号の劣化を生じない光ヘッドを
得ることにある。
An object of the present invention is to eliminate the influence of variations in the coupling efficiency of beam splitters and to obtain an optical head that does not cause deterioration of reproduced signals even when the coupling efficiency is higher than a predetermined value.

【課題を解決するための手段】上記課題を解決するため
に、この発明によれば、半導体レーザから出射した光を
コリメートレンズで平行光とし、ビームスプリッタを透
過して収束レンズに入射させ、磁気光学的または光学的
に情報が記録される記録媒体に収束光として照射して情
報の記録を行うとともに、情報記録部からの反射光を前
記収束レンズを介して前記ビームスプリッタで反射させ
、この反射光を受光素子に導いて光強度,偏光状態の変
化を検出し、記録情報の再生および制御を行うものにお
いて、前記ビームスプリッタが前記半導体レーザの出射
光の偏光方向と直交する方向の偏光光を全反射する偏光
ビームスプリッタからなり、この偏光ビームスプリッタ
の前記平行光の入射側光路上に回転可能に配され,その
回転角により前記偏光ビームスプリッタに入射する平行
光の偏光方向を制御する前記偏光ビームスプリッタの透
過光量補正手段を備えてなるものとする。
[Means for Solving the Problems] In order to solve the above problems, according to the present invention, light emitted from a semiconductor laser is made into parallel light by a collimating lens, transmitted through a beam splitter, and made incident on a converging lens. Information is recorded by optically or optically irradiating a recording medium on which information is recorded as convergent light, and the reflected light from the information recording section is reflected by the beam splitter via the converging lens, and the reflected light is In a device that guides light to a light receiving element and detects changes in light intensity and polarization state to reproduce and control recorded information, the beam splitter transmits polarized light in a direction perpendicular to the polarization direction of the light emitted from the semiconductor laser. The polarized beam is composed of a polarized beam splitter that performs total reflection, and is rotatably arranged on the incident side optical path of the parallel light of this polarized beam splitter, and controls the polarization direction of the parallel light incident on the polarized beam splitter by its rotation angle. It is assumed that a beam splitter transmitting light amount correcting means is provided.

【0010】また、透過光量補正手段が、1/2波長板
と、この1/2波長板を所定の角度領域内で回転可能に
支持する回転機構部とからなるものとする。
It is also assumed that the transmitted light amount correcting means includes a 1/2 wavelength plate and a rotation mechanism that supports the 1/2 wavelength plate so as to be rotatable within a predetermined angular range.

【0011】さらに、回転機構部が、1/2波長板をそ
の外周側で支持する鏡筒と、この鏡筒を回転可能に包囲
し,所定の角度領域に切り欠き部を有する軸受け部と、
前記鏡筒から前記切り欠き部内に突設されて回転方向の
一方側にばね付勢されたアームと、前記切り欠き部内で
前記アームに係合して回転角を調整する調整ネジ部とか
らなるものとする。
[0011] Furthermore, the rotation mechanism section includes a lens barrel that supports the 1/2 wavelength plate on its outer circumferential side, and a bearing portion that rotatably surrounds the lens barrel and has a notch in a predetermined angular region.
It consists of an arm that protrudes from the lens barrel into the notch and is biased by a spring to one side in the rotational direction, and an adjustment screw that engages with the arm within the notch to adjust the rotation angle. shall be taken as a thing.

【0012】0012

【作用】この発明の構成において、従来のビームスプリ
ッタを、半導体レーザの偏光方向に直交する方向の偏光
光を全反射する偏光ビームスプリッタに置き換え、透過
光量補正手段の回転角により入射光の偏光方向を前記半
導体レーザの偏光方向から所定角度だけずらすよう構成
したことにより、角度の増加とともに偏光ビームスプリ
ッタの反射光量が増し、逆に透過光量が減るので、偏光
ビームスプリッタの結合効率が所定値より大きい場合、
半導体レーザの出射光量を減らすことなく偏光ビームス
プリッタの透過光量を減らして所定の光量に補正する機
能が得られる。従って、半導体レーザを十分大きな駆動
電流で駆動して発光ノイズを低減することが可能になり
、再生信号の劣化を阻止することができる。
[Operation] In the configuration of the present invention, the conventional beam splitter is replaced with a polarizing beam splitter that totally reflects polarized light in a direction perpendicular to the polarization direction of the semiconductor laser, and the polarization direction of the incident light is adjusted by the rotation angle of the transmitted light amount correction means. is configured to be shifted by a predetermined angle from the polarization direction of the semiconductor laser, and as the angle increases, the amount of reflected light from the polarizing beam splitter increases and, conversely, the amount of transmitted light decreases, so that the coupling efficiency of the polarizing beam splitter is greater than a predetermined value. case,
It is possible to obtain a function of reducing the amount of light transmitted through the polarizing beam splitter and correcting it to a predetermined light amount without reducing the amount of light emitted from the semiconductor laser. Therefore, it is possible to drive the semiconductor laser with a sufficiently large drive current to reduce emission noise, and it is possible to prevent deterioration of the reproduced signal.

【0013】また、透過光量補正手段を回転機構部に支
持された1/2波長板とすれば、回転角の調整により偏
光ビームスプリッタに入射するレーザービームの偏光方
向を所定量容易に変化させ、透過光量を所定値に補正す
ることができる。
Further, if the transmitted light amount correcting means is a 1/2 wavelength plate supported by the rotation mechanism, the polarization direction of the laser beam incident on the polarization beam splitter can be easily changed by a predetermined amount by adjusting the rotation angle. The amount of transmitted light can be corrected to a predetermined value.

【0014】さらに、回転機構部を、鏡筒に支持された
1/2波長板を、切り欠きを有する軸受け部で支承し、
調整ねじで位置決めするよう構成すれば、1/2波長板
の主軸の回転角を精度よく,かつ簡単に調整し,位置決
めする機能が得られる。
[0014] Furthermore, in the rotation mechanism part, a half-wave plate supported by the lens barrel is supported by a bearing part having a notch,
If the positioning is performed using an adjustment screw, the rotation angle of the main axis of the half-wave plate can be easily and precisely adjusted, and the function of positioning can be obtained.

【0015】[0015]

【実施例】以下、この発明を実施例に基づいて説明する
。  図1はこの発明の実施例になる光ヘッドを模式化
して示す構成図であり、従来の装置と同じ部分には同一
参照符号を付すことにより、詳細な説明を省略する。図
において、24は半導体レーザ1の偏光方向に直交する
方向の偏光光を全反射する偏光ビームスプリッタであり
、その入射光路上に配されたビーム整形プリズム3とコ
リメートレンズ2との間には、たとえば回転機構部31
と、これに回転可能に支持された1/2波長板21とで
構成される透過光量補正手段20が設けられ、偏光ビー
ムスプリッタ24の透過光量の補正が、偏光ビームスプ
リッタ24の結合効率の所定値からのずれに対応して行
われる。
EXAMPLES The present invention will be explained below based on examples. FIG. 1 is a block diagram schematically showing an optical head according to an embodiment of the present invention, and the same parts as in the conventional device are designated by the same reference numerals, and detailed explanation thereof will be omitted. In the figure, 24 is a polarizing beam splitter that totally reflects polarized light in a direction perpendicular to the polarization direction of the semiconductor laser 1, and between the beam shaping prism 3 and the collimating lens 2 arranged on the incident optical path, For example, the rotation mechanism section 31
and a 1/2 wavelength plate 21 rotatably supported thereon, a transmitted light amount correcting means 20 is provided, and correction means 20 for correcting the amount of transmitted light of the polarizing beam splitter 24 achieves a predetermined coupling efficiency of the polarizing beam splitter 24. This is done in response to deviations from the value.

【0016】図2は透過光量補正手段による透過光量の
補正作用を示すベクトル図である。図において、垂直軸
を半導体レーザ1が出射するレーザビームの偏光方向、
水平軸を偏光ビームスプリッタ24が全反射する偏光光
の偏光方向とし、半導体レーザ1の出射光量をId,偏
光ビームスプリッタの結合効率をα, その透過光量を
Io ,とする。ここで、1/2波長板21の主軸方向
を半導体レーザの偏光方向に対して角度Θだけ回転する
と、1/2波長板21を透過したレーザビームBθの偏
光方向は、2Θだけ変化し、光量Id を保持して偏光
ビームスプリッタ24に入射する。光ベクトルBθは、
これを垂直軸成分Id1(透過偏光光)と、水平軸成分
Id2(全反射偏光光)とに分解することができ、例え
ば透過偏光光の光量Id1は、Id1=Id ・Cos
2Θで表される。また、偏光ビームスプリッタ24の透
過光量Io は、Io =Id ・α・Cos2Θとな
り、結合効率α分だけId1より小さくなり、逆に全反
射光量はα分だけ増加してId2/αとなる。
FIG. 2 is a vector diagram showing the effect of correcting the amount of transmitted light by the amount of transmitted light correcting means. In the figure, the vertical axis is the polarization direction of the laser beam emitted by the semiconductor laser 1,
The horizontal axis is the polarization direction of the polarized light totally reflected by the polarizing beam splitter 24, the amount of light emitted from the semiconductor laser 1 is Id, the coupling efficiency of the polarizing beam splitter is α, and the amount of transmitted light is Io. Here, when the main axis direction of the 1/2 wavelength plate 21 is rotated by an angle Θ with respect to the polarization direction of the semiconductor laser, the polarization direction of the laser beam Bθ transmitted through the 1/2 wavelength plate 21 changes by 2Θ, and the light amount Id and enters the polarizing beam splitter 24. The light vector Bθ is
This can be decomposed into a vertical axis component Id1 (transmitted polarized light) and a horizontal axis component Id2 (totally reflected polarized light). For example, the light amount Id1 of the transmitted polarized light is Id1=Id ・Cos
It is expressed as 2Θ. Further, the amount of transmitted light Io of the polarizing beam splitter 24 becomes Io =Id.α.Cos2Θ, which is smaller than Id1 by the coupling efficiency α, and conversely, the amount of total reflected light increases by α and becomes Id2/α.

【0017】このように実施例によれば、透過光量補正
手段20により、偏光ビームスプリッタ24の結合効率
αの所定値に対する偏差に対応して偏光ビームスプリッ
タの透過光量を補正することができ、見掛け上偏光ビー
ムスプリッタの結合効率を所定の設計値に一致させるこ
とができる。このとき、半導体レーザ1の出射レーザビ
ームの光量Id を変える必要がなく、したがって半導
体レーザを十分大きな駆動電流で駆動できるので、半導
体レーザの発光ノイズを低減し、再生信号の劣化を防止
することができる。
As described above, according to the embodiment, the transmitted light amount correcting means 20 can correct the amount of transmitted light of the polarizing beam splitter in accordance with the deviation of the coupling efficiency α of the polarizing beam splitter 24 from a predetermined value, and the apparent amount of transmitted light can be corrected. The coupling efficiency of the upper polarizing beam splitter can be made to match a predetermined design value. At this time, there is no need to change the light intensity Id of the laser beam emitted from the semiconductor laser 1, and therefore the semiconductor laser can be driven with a sufficiently large drive current, reducing the emission noise of the semiconductor laser and preventing deterioration of the reproduced signal. can.

【0018】図3はこの発明の実施例になる回転機構部
の構成を示す平面図であり、回転機構部31は、1/2
波長板21を支持する鏡筒33と、鏡筒33を回転可能
に支持する軸受け部34,およびその所定の角度領域に
形成された切り欠き部35と、鏡筒33から切り欠き部
35内に突設されたアーム32,およびアーム32を回
転方向の一方に付勢するばね37と、アーム32の反ば
ね側に切り欠き部内で係合するよう軸受け部34に結合
した調整ねじ36とで構成され、切り欠き部35の開口
角は偏光ビームスプリッタの結合効率のばらつきによる
透過光量の変動を補正できる範囲に決められる。
FIG. 3 is a plan view showing the configuration of a rotating mechanism section according to an embodiment of the present invention, and the rotating mechanism section 31 has a 1/2
A lens barrel 33 that supports the wavelength plate 21 , a bearing portion 34 that rotatably supports the lens barrel 33 , a notch portion 35 formed in a predetermined angular region thereof, and a portion from the lens barrel 33 into the notch portion 35 . Consisting of a protruding arm 32, a spring 37 that biases the arm 32 in one direction of rotation, and an adjustment screw 36 coupled to a bearing portion 34 so as to engage within a notch on the side opposite to the spring of the arm 32. The aperture angle of the notch 35 is determined within a range that can correct variations in the amount of transmitted light due to variations in the coupling efficiency of the polarizing beam splitter.

【0019】上述の回転機構部31に1/2波長板21
を支持した透過光量補正手段20は、1/2波長板を所
望の角度Θ回転し、位置決めする操作を調整ねじ36に
よって容易に行うことができる。
[0019] A 1/2 wavelength plate 21 is attached to the rotation mechanism section 31 described above.
The transmitted light amount correcting means 20 supporting the 1/2 wavelength plate can be easily rotated by a desired angle Θ and positioned using the adjustment screw 36.

【0020】[0020]

【発明の効果】この発明は前述のように、従来のビーム
スプリッタを、半導体レーザの偏光方向に直交する方向
の偏光光を全反射する偏光ビームスプリッタに置き換え
、透過光量補正手段の回転角により入射光の偏光方向を
前記半導体レーザの偏光方向から所定角度だけずらすよ
う構成した。その結果、角度の増加とともに偏光ビーム
スプリッタの反射光量が増し、逆に透過光量が減るので
、偏光ビームスプリッタの結合効率が所定値より大きい
場合、半導体レーザの出射光量を減らすことなく偏光ビ
ームスプリッタの透過光量を減らして所定の光量に補正
する機能が得られるので、半導体レーザの出射光量を減
らすことにより発光ノイズが増加するという従来の問題
点が排除され、半導体レーザを十分大きな駆動電流で駆
動して発光ノイズを低減し、再生信号の劣化を阻止でき
る光ヘッドを提供できる。
Effects of the Invention As described above, the present invention replaces the conventional beam splitter with a polarizing beam splitter that totally reflects polarized light in a direction perpendicular to the polarization direction of a semiconductor laser, and adjusts the angle of rotation of the transmitted light amount correction means to The polarization direction of the light is shifted by a predetermined angle from the polarization direction of the semiconductor laser. As a result, as the angle increases, the amount of reflected light from the polarizing beam splitter increases and the amount of transmitted light decreases, so if the coupling efficiency of the polarizing beam splitter is greater than a predetermined value, the polarizing beam splitter can be The ability to reduce the amount of transmitted light and correct it to a predetermined light amount eliminates the conventional problem of increased light emission noise due to reducing the amount of light emitted from the semiconductor laser, and allows the semiconductor laser to be driven with a sufficiently large drive current. Therefore, it is possible to provide an optical head that can reduce light emission noise and prevent deterioration of reproduced signals.

【0021】また、透過光量補正手段を回転機構部に支
持された1/2波長板とすれば、回転角の調整により偏
光ビームスプリッタに入射するレーザービームの偏光方
向を所定量容易に変化させ、透過光量を所定値に補正で
きるので、個々にばらつきのある偏光ビームスプリッタ
の結合効率を見掛け上設計値に一致させることができる
Furthermore, if the transmitted light amount correcting means is a 1/2 wavelength plate supported by the rotation mechanism, the polarization direction of the laser beam incident on the polarization beam splitter can be easily changed by a predetermined amount by adjusting the rotation angle. Since the amount of transmitted light can be corrected to a predetermined value, the coupling efficiency of the polarizing beam splitter, which varies individually, can be made to match the design value in appearance.

【0022】さらに回転機構部を、鏡筒に支持された1
/2波長板を切り欠きを有する軸受け部で支承し、調整
ねじで位置決めするよう構成すれば、1/2波長板の主
軸の回転角を精度よく,かつ簡単に調整し,位置決めす
る機能が得られる。
[0022] Furthermore, the rotation mechanism section is supported by the lens barrel.
If the 1/2 wavelength plate is supported by a bearing with a notch and positioned using an adjustment screw, the rotation angle of the main axis of the 1/2 wavelength plate can be precisely and easily adjusted and positioned. It will be done.

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

【図1】この発明の実施例になる光ヘッドを模式化して
示す構成図
FIG. 1 is a schematic configuration diagram of an optical head according to an embodiment of the present invention.

【図2】実施例における透過光量補正手段の透過光量の
補正作用を示すベクトル図
[Fig. 2] A vector diagram showing the correcting action of the transmitted light amount by the transmitted light amount correction means in the embodiment.

【図3】この発明の実施例になる回転機構部を示す平面
FIG. 3 is a plan view showing a rotation mechanism according to an embodiment of the present invention.

【図4】従来の光ヘッドを模式化して示す構成図[Figure 4] A schematic configuration diagram of a conventional optical head.

【符号の説明】[Explanation of symbols]

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    ビームスプリッタ 5    立ち上げミラー 6    アクチュエータ 7    対物レンズ 8    光磁気ディスク 9    光スポット 10    1/2波長板 13    6分割フォトダイオード 20    透過光量補正手段 21    1/2波長板 24    偏光ビームスプリッタ 31    回転機構部 32    アーム 33    鏡筒 34    軸受け部 35    切り欠き部 36    調整ねじ Id   半導体レーザの出射光量 Io   透過光量 Θ    回転角 α    結合効率 1 Semiconductor laser 2 Collimating lens 3 Beam shaping prism 4 Beam splitter 5 Stand-up mirror 6 Actuator 7 Objective lens 8 Magneto-optical disk 9. Light spot 10 1/2 wavelength plate 13 6-segment photodiode 20 Transmitted light amount correction means 21 1/2 wavelength plate 24 Polarizing beam splitter 31 Rotating mechanism section 32 Arm 33 Lens barrel 34 Bearing part 35 Notch part 36 Adjustment screw Id Emitted light amount of semiconductor laser Io Transmitted light amount Θ Rotation angle α Coupling efficiency

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】半導体レーザから出射した光をコリメート
レンズで平行光とし、ビームスプリッタを透過して収束
レンズに入射させ、磁気光学的または光学的に情報が記
録される記録媒体に収束光として照射して情報の記録を
行うとともに、情報記録部からの反射光を前記収束レン
ズを介して前記ビームスプリッタで反射させ、この反射
光を受光素子に導いて光強度,偏光状態の変化を検出し
、記録情報の再生および制御を行うものにおいて、前記
ビームスプリッタが前記半導体レーザの出射光の偏光方
向と直交する方向の偏光光を全反射する偏光ビームスプ
リッタからなり、この偏光ビームスプリッタの前記平行
光の入射側光路上に回転可能に配され,その回転角によ
り前記偏光ビームスプリッタに入射する平行光の偏光方
向を制御する前記偏光ビームスプリッタの透過光量補正
手段を備えてなることを特徴とする光ヘッド。
Claim 1: Light emitted from a semiconductor laser is made into parallel light by a collimating lens, transmitted through a beam splitter, and incident on a convergent lens, and irradiated as convergent light onto a recording medium on which information is recorded magneto-optically or optically. to record information, and to reflect the reflected light from the information recording section by the beam splitter via the converging lens, and to guide the reflected light to a light receiving element to detect changes in light intensity and polarization state; In the apparatus for reproducing and controlling recorded information, the beam splitter is a polarizing beam splitter that totally reflects polarized light in a direction perpendicular to the polarization direction of the emitted light from the semiconductor laser, and An optical head comprising: a means for correcting the amount of transmitted light of the polarizing beam splitter, which is rotatably disposed on the incident side optical path and controls the polarization direction of parallel light incident on the polarizing beam splitter according to the rotation angle thereof. .
【請求項2】透過光量補正手段が、1/2波長板と、こ
の1/2波長板を所定の角度領域内で回転可能に支持す
る回転機構部とからなることを特徴とする請求項1記載
の光ヘッド。
2. The transmitted light amount correcting means comprises a 1/2 wavelength plate and a rotation mechanism that rotatably supports the 1/2 wavelength plate within a predetermined angular range. Light head as described.
【請求項3】回転機構部が、1/2波長板をその外周側
で支持する鏡筒と、この鏡筒を回転可能に包囲し,所定
の角度領域に切り欠き部を有する軸受け部と、前記鏡筒
から前記切り欠き部内に突設されて回転方向の一方側に
ばね付勢されたアームと、前記切り欠き部内で前記アー
ムに係合して回転角を調整する調整ネジ部とからなるこ
とを特徴とする請求項2記載の光ヘッド。
3. The rotation mechanism includes a lens barrel that supports the 1/2 wavelength plate on its outer circumferential side, and a bearing portion that rotatably surrounds the lens barrel and has a notch in a predetermined angular region. It consists of an arm that protrudes from the lens barrel into the notch and is biased by a spring to one side in the rotational direction, and an adjustment screw that engages with the arm within the notch to adjust the rotation angle. The optical head according to claim 2, characterized in that:
JP2400976A 1990-12-10 1990-12-10 Optical head Pending JPH04214242A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2400976A JPH04214242A (en) 1990-12-10 1990-12-10 Optical head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2400976A JPH04214242A (en) 1990-12-10 1990-12-10 Optical head

Publications (1)

Publication Number Publication Date
JPH04214242A true JPH04214242A (en) 1992-08-05

Family

ID=18510836

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2400976A Pending JPH04214242A (en) 1990-12-10 1990-12-10 Optical head

Country Status (1)

Country Link
JP (1) JPH04214242A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002185073A (en) * 2000-10-04 2002-06-28 Pioneer Electronic Corp Laser light intensity controller

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002185073A (en) * 2000-10-04 2002-06-28 Pioneer Electronic Corp Laser light intensity controller

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