JP3077426B2 - Optical information recording / reproducing device - Google Patents

Optical information recording / reproducing device

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Publication number
JP3077426B2
JP3077426B2 JP04332603A JP33260392A JP3077426B2 JP 3077426 B2 JP3077426 B2 JP 3077426B2 JP 04332603 A JP04332603 A JP 04332603A JP 33260392 A JP33260392 A JP 33260392A JP 3077426 B2 JP3077426 B2 JP 3077426B2
Authority
JP
Japan
Prior art keywords
light
polarized
information recording
wave
plate
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 - Fee Related
Application number
JP04332603A
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Japanese (ja)
Other versions
JPH06180853A (en
Inventor
秀一 小名山
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.)
NEC Corp
Original Assignee
NEC Corp
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Filing date
Publication date
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Priority to JP04332603A priority Critical patent/JP3077426B2/en
Publication of JPH06180853A publication Critical patent/JPH06180853A/en
Application granted granted Critical
Publication of JP3077426B2 publication Critical patent/JP3077426B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Optical Recording Or Reproduction (AREA)
  • Optical Head (AREA)
  • Lens Barrels (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、光を利用して情報の記
録再生を行なう情報入出力装置に好適な光情報記録再生
装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical information recording / reproducing apparatus suitable for an information input / output device for recording / reproducing information using light.
Related to the device .

【0002】[0002]

【従来の技術】図3に従来の超解像度光情報記録再生装
置の一例を示す。
2. Description of the Related Art FIG. 3 shows an example of a conventional super-resolution optical information recording / reproducing apparatus.

【0003】基本構成は、レーザー源であるレーザー光
を発するレーザーダイオード1、光軸近傍の光を遮断す
る遮光板9、レーザー光を分岐するビームスプリッタ
2、レーザー光を集光する対物レンズ4、対物レンズを
駆動するアクチェエータ5、戻り光を電気信号に変換す
る受光素子であるフォトダイオード7から成る。
The basic configuration is as follows: a laser diode 1, which emits laser light as a laser source; a light-shielding plate 9, which blocks light near the optical axis; a beam splitter 2, which branches laser light; an objective lens 4, which focuses laser light; Akucheeta 5 for driving the objective lens, a photodiode 7 as a light receiving element for converting the return light into an electric signal.

【0004】レーザーダイオード1から発したレーザー
光は、光軸近傍に遮光領域を持つ遮光板9を透過するこ
とにより光軸近傍が抜けたレーザー光となりビームスプ
リッタ2へと向う。ビームスプリッタ2を透過したレー
ザー光は対物レンズ4により情報記録媒体6上に焦点を
結ぶ。この時、ビームスポット11は近軸付近の遮光に
よる超解像効果により、遮光板の無い場合の通常スポ
ット10に比べ小さいビーム径とすることが出来る(φ
b<φc)。情報記録媒体6で反射したレーザー光は、
再び対物レンズ4を通りビームスプリッタ2で反射さ
れ、フォトダイオード7へ向う。フォトダイオード7で
電気信号に変換され、信号再生回路で再生信号や誤差信
号を得る。
The laser light emitted from the laser diode 1 passes through a light-shielding plate 9 having a light-shielding area near the optical axis, and becomes laser light passing near the optical axis to the beam splitter 2. The laser beam transmitted through the beam splitter 2 is focused on the information recording medium 6 by the objective lens 4. At this time, the beam diameter of the beam spot 11 can be made smaller than that of the normal spot 10 without the light shielding plate 9 due to the super-resolution effect of light shielding near the paraxial axis (φ
b <φc). The laser beam reflected by the information recording medium 6 is
It is reflected by the street beam splitter 2 through the objective lens 4 again, toward the photodiode 7. The signal is converted into an electric signal by the photodiode 7, and a reproduced signal and an error signal are obtained by a signal reproducing circuit.

【0005】以上の構成により、超解像の光ビームを使
った高密度な情報の記録再生を行うことが出来る。
With the above configuration, high-density information can be recorded and reproduced using a super-resolution light beam.

【0006】[0006]

【発明が解決しようとする課題】以上述べた様な構成で
は、情報記録媒体からの戻り光を効率良くフォトダイ
オードヘ導くため、遮光板を光路系の往路、つまり
レーザーダイオードとビームスプリッタの間に配置
しなければならない。そのため、対物レンズがトラッ
ク方向に移動した場合遮光板の中心とレーザー光の光
軸にずれが生じ良好な超解像ビームが得られないという
問題があった。
In the configuration described above, in order to efficiently guide the return light from the information recording medium 6 to the photodiode 7 , the light-shielding plate 9 is connected to the outward path of the optical path system, that is, It must be located between the laser diode 1 and the beam splitter 2 . Therefore, when the objective lens 4 is moved in the track direction, there is a problem that the center of the light shielding plate 9 and the optical axis of the laser light are displaced, and a good super-resolution beam cannot be obtained.

【0007】図4に以上の説明図を示す。図の様にfだ
け対物レンズ4が移動すると超解像ビームスポット12
は良好なビームが得られなくなる。
FIG. 4 shows the above explanation. When the objective lens 4 moves by f as shown in FIG.
Cannot obtain a good beam.

【0008】本発明の目的は、光利用効率を低下させる
ことなく、対物レンズが移動した際も常に良好な超解像
度のビームスポットを形成する超解像度光情報記録再生
装置を提供することにある。。
An object of the present invention is to provide a super-resolution optical information recording / reproducing apparatus which always forms a good super-resolution beam spot even when the objective lens moves without reducing the light use efficiency. .

【0009】[0009]

【課題を解決するための手段】本発明は、上述の目的を
達成するために、レーザー光を出射するレーザー源と、
前記レーザー源から発したレーザー光を直線偏光P波と
S波に分離してP波のみを透過せしめるとともに、情報
記録媒体から戻るS波を反射して前記レーザー光源の出
射光路から分離する偏光ビームスプリッタと、光軸近傍
直線偏光P波のみ遮断する偏光波透過選別領域を持つ
偏光分離板及び該偏光分離板の偏光波透過選別領域以外
の領域を透過した直線偏光P波を円偏光に変える1/4
波長板から成る偏光波透過選別手段と、前記偏光波透過
選別手段を透過したレーザー光を情報記録媒体上に超解
像で集光する対物レンズと、前記対物レンズをフォーカ
ス、トラックの少なくとも2軸方向に駆動するアクチュ
エータと、前記情報記録媒体で反射されて入射時と逆向
きの円偏光として前記1/4波長板に入射し、該1/4
波長板により直線偏光S波とされて前記偏光分離板の全
領域を透過し、前記偏光ビームスプリッタにて反射され
て前記レーザー光源の出射光路から分離された戻り光
電気信号に変換する受光素子とを具備することを特徴と
するものである。 また、本発明は、前記アクチュエータ
が、前記偏光波透過選別手段と前記対物レンズを一体化
してフォーカス、トラックの少なくとも2軸方向に駆動
すること、或いは前記偏光波透過選別手段が、偏光分離
板と1/4波長板が一体であること等を、他の特徴とす
るものである。
According to the present invention, there is provided a laser source for emitting a laser beam.
The laser light emitted from the laser source is converted into a linearly polarized P-wave.
Separates into S wave and transmits only P wave,
The S-wave returning from the recording medium is reflected to emit the laser light source.
It has a polarization beam splitter that separates from the emission path, and a polarization wave transmission selection area that blocks only linearly polarized P waves near the optical axis.
Other than the polarized light separating plate and the polarized wave transmission selection area of the polarized light separating plate
1/4 that converts the linearly polarized P wave transmitted through the region
A polarized wave transmitting / selecting means comprising a wavelength plate, an objective lens for condensing the laser beam transmitted through the polarized wave transmitting / selecting means on an information recording medium at a super resolution, and focusing the objective lens on at least two axes of a track. Actuator that drives in the direction, and is reflected by the information recording medium,
Incident on the 波長 wavelength plate as circularly polarized light,
The plate is converted into linearly polarized S waves by the wavelength plate,
Area, and is reflected by the polarizing beam splitter.
; And a light receiving element for converting into an electric signal the separated return light from the emission optical path of the laser light source Te and
Is what you do. Further, the present invention provides the actuator
Integrates the polarized wave transmission selection means and the objective lens
Focus and drive in at least two axes of track
Or the polarization wave transmission and sorting means comprises polarization separation.
Another feature is that the plate and the quarter-wave plate are integrated.
Things.

【0010】[0010]

【実施例】次に本発明の一実施例について、図1及び図
2を参照して説明する。図1は本発明における光学系を
示した図である。レーザーダイオード1を出たレーザー
光は偏光ビームスプリッタ2により直線偏光P波とS波
に分離され、P波のみが対物レンズ4へと向う。該レー
ザー光は、対物レンズ4とともにアクチュエータのレン
ズホルダ5に同時に保持された偏光波透過選別手段3へ
入射する。ここでこの偏光波透過選別手段3は、たとえ
ば偏光フィルム等から成る偏光波透過選別領域3cをそ
のほぼ中心付近に持つ偏光分離板3aと直線偏光を円偏
光に変換するλ/4板(1/4波長板)3bから成る。
Next, an embodiment of the present invention will be described with reference to FIGS. FIG. 1 is a diagram showing an optical system according to the present invention. The laser light that has exited the laser diode 1 is split into linearly polarized P-waves and S-waves by a polarization beam splitter 2, and only the P-wave is directed to the objective lens 4. The laser light is incident on the polarized wave transmission / selection means 3 simultaneously held by the objective lens 4 and the lens holder 5 of the actuator. Here, the polarized wave transmission selection means 3 is composed of, for example, a polarized light separating plate 3a having a polarized wave transmission selection region 3c made of, for example, a polarizing film near its center, and a λ / 4 plate ( 1/1) for converting linearly polarized light into circularly polarized light. 4 wavelength plate) 3b.

【0011】この際、前記偏光波透過適別領域へ入射す
る光軸近傍の直線偏光P波が完全に遮断される様に光軸
O−O’に対して偏光波透過選別手段3の回軸方向取付
け角を設定する。これにより、前記直線偏光P波は偏光
波透過選別領域3c以外の光のみがそのままλ/4板3
bへと入射する。
At this time, the rotation axis of the polarization wave transmission and sorting means 3 is shifted with respect to the optical axis OO 'so that the linearly polarized P wave near the optical axis which enters the polarization wave transmission suitable area is completely cut off. Set the direction mounting angle. As a result, only the light other than the polarized wave transmission selection area 3c of the linearly polarized P wave is directly
b.

【0012】光軸近傍の光が除却された直線偏光P波は
λ/4板3bを透過することにより、円偏光に変換され
対物レンズ4で集光され、情報記録媒体6上に超解像の
ビームスポットを形成する。情報記録媒体6からの反射
光は、反射により入射時とは逆向きの円偏光となり対物
レンズ4を透過し、偏光波透過選別手段3へ再度入射す
る。入射時と逆向きの円偏光でλ/4板3bに入射する
ため偏光分離板3aには入射時とは90°回転した直線
偏光、つまりこの場合S波となって入射する。
The linearly polarized P wave from which light near the optical axis is eliminated is transmitted to the λ / 4 plate 3b, converted into circularly polarized light, condensed by the objective lens 4, and super-resolution on the information recording medium 6. Is formed. The reflected light from the information recording medium 6 becomes circularly polarized light in the opposite direction to that at the time of incidence due to reflection, passes through the objective lens 4, and enters the polarized wave transmission selection means 3 again. Since the light enters the λ / 4 plate 3b as circularly polarized light having a direction opposite to that at the time of incidence, the light enters the polarization separation plate 3a as linearly polarized light rotated by 90 ° from that at the time of incidence, that is, in this case, an S wave.

【0013】したがって該レーザー光は偏光波透過選別
領域3cをも含めた全ての光が偏光分離板3aを透過
し、次の偏光ビームスプリッタでは逆にほとんどの光
フォトダイオード7側へと反射することになる。以上
の構成により、光利用効率を低下させることなく、対物
レンズ移動時も常に良好な超解像ビームスポットを生成
し、高密度な情報の記録再生を実現することが出来る。
[0013] Thus the laser beam is all light including a polarized light transmission selection area 3c is transmitted through the polarization separating plate 3a, reflections most of the light in the opposite the next polarizing beam splitter 2 to the photodiode 7 side Will do. With the above configuration, a good super-resolution beam spot is always generated even when the objective lens is moved without lowering the light use efficiency, and high-density information recording and reproduction can be realized.

【0014】図2は、一体型偏光波透過選別手段の実施
例であり、この図では、λ/4板のほぼ中心付近にたと
えば偏光フィルム等で偏光波透過選別領域を形成するこ
とで一体型の偏光波透過選別手段を実現している。
FIG. 2 shows an embodiment of the integrated polarized wave transmission / selection means. In this figure, a polarized wave transmission / selection region is formed near the center of the λ / 4 plate by, for example, a polarizing film or the like. The polarization wave transmission selection means of (1) is realized.

【0015】[0015]

【発明の効果】以上説明した様に本発明は、レーザー源
から発したレーザー光を、まず偏光ビ ームスプリッタに
おいて、直線偏光P波とS波に分離してP波のみを透過
せしめ、さらに光軸近傍に直線偏光P波のみ遮断する偏
光波透過選別領域を持つ偏光分離板及び該偏光分離板の
偏光波透過選別領域以外の領域を透過した直線偏光P波
を円偏光に変える1/4波長板から成る偏光波透過選別
手段を透過させた後、対物レンズを介して情報記録媒体
上に超解像で集光し、さらに情報記録媒体で反射された
レーザー光を入射時と逆向きの円偏光として前記1/4
波長板に入射させ、この1/4波長板により直線偏光S
波とされた戻り光を偏光分離板の全領域を透過させ、最
後に偏光ビームスプリッタにおいて前記レーザー光源の
出射光路から分離して受光素子に導く構成としたから、
レーザー光の偏光を利用して対物レンズの直前において
近軸付近の遮光による超解像効果を発揮させることがで
き、しかも偏光波透過選別手段に近接配置された対物レ
ンズをトラック方向に駆動したときの情報記録媒体上に
形成されるビーム径の絞り効果に対する影響は、偏光波
透過選別手段が対物レンズから遠く離れた位置に配置さ
れていた従来装置に比べ非常に軽微であり、したがって
常に良好な超解像度のビームスポットを形成することに
より高精度の記録再生が可能であり、また偏光波透過選
別手段に含まれる偏光分離板は、光軸近傍に直線偏光P
波のみ遮断する偏光波透過選別領域を持つため、光軸近
傍を透過領域とし光軸周辺を半透過領域とする透過選別
領域を持ったフィルタ等と比較したときに、光透過面積
が光軸からの半径の二乗に比例することを考慮するまで
もなく、光透過率の損失が必要最小限に抑えることがで
き、したがって光利用効率の低下懸念はほとんどなく、
また情報記録媒体に向かうレーザー光に関しては偏光波
透過選別領域を通過しようとする直線偏光P波だけが遮
断されるのに対し、情報記録媒体にて反射される戻るレ
ーザー光が1/4波長板においてすべて直線偏光S波に
変えられているため、偏光波透過選別領域に関係なく偏
光分離板の全領域を通過させることができ、これにより
戻り光を非常に高い効率でもって受光素子へと導くこと
が可能であり、この点においても光利用効率の確保を果
たすことができ、高密度信号の記録再生精度を大幅に向
上することができる等の優れた効果を奏する。 また、本
発明は、アクチュエータが、前記偏光波透過選別手段と
前記対物レンズを一体化してフォーカス、トラックの少
なくとも2軸方向に駆動する構成とし たから、偏光波透
過選別手段を対物レンズに近接配置した物理的な理由か
ら、対物レンズと偏光波透過選別手段とがトラック方向
に相対的な位置ずれを生じたとしても情報記録媒体上に
形成されるビーム径の絞り効果に対する影響は軽微であ
るのは当然であるが、偏光波透過選別手段と対物レンズ
を一体化してアクチュエータが駆動することで、こうし
た軽微な影響すら排除することができ、偏光波透過選別
手段における近軸付近の遮光による超解像効果をさらに
徹底強化することで、高密度信号の記録再生精度の大幅
な向上に寄与することができる等の効果を奏する。
た、本発明は、偏光波透過選別手段が、偏光分離板と1
/4波長板が一体であるため、偏光波透過選別手段の光
軸方向の厚みを減らし、光情報記録再生装置の薄型化設
計に寄与することができる等の効果を奏する。
As described above, the present invention provides a laser source
The laser beam emitted from, first, a polarizing over beam splitter
Separates into linearly polarized P-waves and S-waves and transmits only P-waves
In addition, polarization that blocks only linearly polarized P-waves near the optical axis
Polarization separation plate having light-wave transmission selection region and polarization separation plate
Linearly polarized P wave transmitted through a region other than the polarized wave transmission selection region
Polarized wave transmission screening consisting of a quarter-wave plate that converts light into circularly polarized light
After passing through the means, the information recording medium through the objective lens
Focused at super resolution on top, and reflected by the information recording medium
The laser light is converted into circularly polarized light having a direction opposite to that of the incident light,
And a linearly polarized light S
The wave-formed return light is transmitted through the entire area of the polarization separation plate,
Later, in the polarizing beam splitter, the laser light source
Because it is configured to be separated from the output light path and guided to the light receiving element,
Just before the objective lens using the polarization of the laser light
The super-resolution effect by shading near the paraxial can be exhibited.
And an objective lens placed close to the polarized wave transmission selection means
On the information recording medium when the lens is driven in the track direction.
The effect of the formed beam diameter on the aperture effect depends on the polarization wave.
The transmission selection means is located far away from the objective lens.
Is very small compared to conventional
To always form a good super-resolution beam spot
Higher precision recording / reproduction is possible, and polarized wave transmission selection
The polarization separation plate included in another means has a linear polarization P near the optical axis.
Because it has a polarized wave transmission selection area that blocks only waves, it is close to the optical axis.
Transmission sorting where the side is a transmissive area and the periphery of the optical axis is a semi-transmissive area
Light transmission area when compared to filters etc.
Until it is proportional to the square of the radius from the optical axis
No loss of light transmittance can be minimized
Therefore, there is almost no concern about a decrease in light use efficiency,
In addition, the polarized light is
Only linearly polarized P-waves trying to pass through the transmission sorting area are blocked.
While the return is reflected by the information recording medium.
Laser light is converted to linearly polarized S waves in a quarter-wave plate
Has been changed, so that the polarization
It can pass through the whole area of the light separating plate,
Guide the return light to the light receiving element with very high efficiency
It is possible to secure light use efficiency in this regard as well.
And greatly improve the recording and reproduction accuracy of high-density signals.
It has excellent effects, such as being able to increase. Also book
The invention is characterized in that the actuator comprises the polarized wave transmission selection means.
The objective lens is integrated to reduce focus and track
Without even a structure for driving the two-axis direction treasure polarized wave Toru
Is it a physical reason to place the over-selection means close to the objective lens?
The objective lens and the polarized wave transmission selection means
Even if there is a relative misalignment on the information recording medium,
The effect of the formed beam diameter on the aperture effect is minimal.
Naturally, polarized wave transmission selection means and objective lens
This is done by integrating the
Even small effects can be eliminated, and polarized wave transmission sorting
Super-resolution effect due to light shielding near paraxial in means
Thoroughly strengthened recording / playback accuracy of high-density signals
This has the effect of being able to contribute to a significant improvement. Ma
Further, in the present invention, the polarized wave transmission / selection means comprises a polarized light separating plate and
Since the 波長 wavelength plate is integrated, the light of the polarized wave transmission
Reduce the thickness in the axial direction and make the optical information recording / reproducing device thinner.
It has effects such as being able to contribute to the total.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明の一実施例の光路図である。FIG. 1 is an optical path diagram of an embodiment of the present invention.

【図2】本発明における一体型偏光波透過選別手段の一
実施例を示す図である。
FIG. 2 is a view showing one embodiment of an integrated polarized wave transmission / selection means in the present invention.

【図3】従来の超解像度光情報記録再生装置の光路図で
ある。
FIG. 3 is an optical path diagram of a conventional super-resolution optical information recording / reproducing apparatus.

【図4】従来技術における問題点を図示した光路図であ
る。
FIG. 4 is an optical path diagram illustrating a problem in the related art.

【符号の説明】[Explanation of symbols]

1 レーザーダイオード 2 偏光ビームスプリッタ 3 偏光波透過選別手段 3a 偏光分離板 3b λ/4板 3c 偏光波透過選別領域 4 対物レンズ 5 二軸アクチュエータ 6 情報記録媒体 7 フォトダイオード 8 1体型偏光波透過選別手段 9 遮光板 9a 遮光領域 10 通常ビームスポット 11 超解像ビームスポット 11a メインビーム 11b サイドローブ 12 光軸移動時の超解像ビームスポット1 laser diode 2 polarization beam splitter 3 polarized wave transmission selection means 3a polarized separated plate 3b lambda / 4 plate 3c polarized wave transmissive selection area 4 the objective lens 5 biaxial actuator 6 information recording medium 7 photodiode 8 1 integrated polarized wave transmission selection means Reference Signs List 9 light shielding plate 9a light shielding area 10 normal beam spot 11 super-resolution beam spot 11a main beam 11b side lobe 12 super-resolution beam spot when moving optical axis

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平2−161628(JP,A) 特開 平4−125826(JP,A) 特開 昭63−259840(JP,A) 特開 平1−94544(JP,A) 特開 平6−52573(JP,A) 実開 昭63−113220(JP,U) (58)調査した分野(Int.Cl.7,DB名) G11B 7/135 G11B 7/00 ──────────────────────────────────────────────────続 き Continuation of front page (56) References JP-A-2-161628 (JP, A) JP-A-4-125826 (JP, A) JP-A-63-259840 (JP, A) JP-A-1- 94544 (JP, A) JP-A-6-52573 (JP, A) JP-A-63-113220 (JP, U) (58) Fields investigated (Int. Cl. 7 , DB name) G11B 7/135 G11B 7 / 00

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 レーザー光を出射するレーザー源と、前
記レーザー源から発したレーザー光を直線偏光P波とS
波に分離してP波のみを透過せしめるとともに、情報記
録媒体から戻るS波を反射して前記レーザー光源の出射
光路から分離する偏光ビームスプリッタと、光軸近傍に
直線偏光P波のみ遮断する偏光波透過選別領域を持つ偏
光分離板及び該偏光分離板の偏光波透過選別領域以外の
領域を透過した直線偏光P波を円偏光に変える1/4波
長板から成る偏光波透過選別手段と、前記偏光波透過選
別手段を透過したレーザー光を情報記録媒体上に超解像
で集光する対物レンズと、前記対物レンズをフォーカ
ス、トラックの少なくとも2軸方向に駆動するアクチュ
エータと、前記情報記録媒体で反射されて入射時と逆向
きの円偏光として前記1/4波長板に入射し、該1/4
波長板により直線偏光S波とされて前記偏光分離板の全
領域を透過し、前記偏光ビームスプリッタにて反射され
て前記レーザー光源の出射光路から分離された戻り光
電気信号に変換する受光素子とを具備することを特徴と
する光情報記録再生装置。
1. A laser source for emitting laser light, and a laser beam emitted from the laser source is linearly polarized P-wave and S-polarized.
Separate into waves and allow only P-waves to pass
Emitting the laser light source by reflecting the S wave returning from the recording medium
Polarizing beam splitter that separates from the optical path and near the optical axis
Polarized light having a polarized light transmission selection region that blocks only linearly polarized P waves
Other than the light separating plate and the polarized wave transmission selection region of the polarized light separating plate
Quarter wave that converts linearly polarized P wave transmitted through a region to circularly polarized light
A polarized wave transmitting / selecting means comprising a long plate, an objective lens for condensing the laser beam transmitted through the polarized wave transmitting / selecting means on an information recording medium at a super resolution, and at least two axes of focusing and tracking the objective lens Actuator that drives in the direction, and is reflected by the information recording medium,
Incident on the 波長 wavelength plate as circularly polarized light,
The plate is converted into linearly polarized S waves by the wavelength plate,
Area, and is reflected by the polarizing beam splitter.
An optical information recording / reproducing apparatus, comprising: a light receiving element for converting return light separated from an emission optical path of the laser light source into an electric signal.
【請求項2】 前記アクチュエータは、前記偏光波透過
選別手段と前記対物レンズを一体化してフォーカス、ト
ラックの少なくとも2軸方向に駆動することを特徴とす
る請求項1記載の光情報記録再生装置。
2. The apparatus according to claim 1, wherein the actuator integrates the polarized wave transmission / selection unit and the objective lens into a focus and a focus.
2. The optical information recording / reproducing apparatus according to claim 1, wherein the optical information recording / reproducing apparatus is driven in at least two axial directions of the rack .
【請求項3】 前記偏光波透過選別手段は、偏光分離板
1/4波長板が一体であることを特徴とする請求項1
記載の光情報記録再生装置。
3. The polarization wave transmission and sorting means, wherein a polarization separation plate and a 波長 wavelength plate are integrated.
The optical information recording / reproducing apparatus according to the above.
JP04332603A 1992-12-14 1992-12-14 Optical information recording / reproducing device Expired - Fee Related JP3077426B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP04332603A JP3077426B2 (en) 1992-12-14 1992-12-14 Optical information recording / reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP04332603A JP3077426B2 (en) 1992-12-14 1992-12-14 Optical information recording / reproducing device

Publications (2)

Publication Number Publication Date
JPH06180853A JPH06180853A (en) 1994-06-28
JP3077426B2 true JP3077426B2 (en) 2000-08-14

Family

ID=18256800

Family Applications (1)

Application Number Title Priority Date Filing Date
JP04332603A Expired - Fee Related JP3077426B2 (en) 1992-12-14 1992-12-14 Optical information recording / reproducing device

Country Status (1)

Country Link
JP (1) JP3077426B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2655077B2 (en) * 1994-05-17 1997-09-17 日本電気株式会社 Optical head device

Also Published As

Publication number Publication date
JPH06180853A (en) 1994-06-28

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