JPH0495243A - Producing device for master optical disk - Google Patents

Producing device for master optical disk

Info

Publication number
JPH0495243A
JPH0495243A JP21104290A JP21104290A JPH0495243A JP H0495243 A JPH0495243 A JP H0495243A JP 21104290 A JP21104290 A JP 21104290A JP 21104290 A JP21104290 A JP 21104290A JP H0495243 A JPH0495243 A JP H0495243A
Authority
JP
Japan
Prior art keywords
recording
laser beam
optical disc
recording laser
producing
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
JP21104290A
Other languages
Japanese (ja)
Inventor
Fumiaki Ueno
植野 文章
Michiyoshi Nagashima
道芳 永島
Toshinori Kishi
貴志 俊法
Hiroyuki Ogawa
裕之 小川
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP21104290A priority Critical patent/JPH0495243A/en
Publication of JPH0495243A publication Critical patent/JPH0495243A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To easily equalize the intensity of recording laser beams between two master optical disks by providing a means which changes polarizing state of the recording laser beams and a polarized beam splitter and dividing a recording laser beam into two parts by the beam splitter. CONSTITUTION:A polarized beam splitter 7 is provided together with a means 6 which changes the state of the recording laser beam. Then a recording laser beam is divided into two parts by the splitter 7. A wavelength plate 6, for example, is provided between a laser device 4 and the splitter 7 as a means which changes the polarizing state of the recording laser beam. Thus the intensity ratio between two laser beams can be optionally changed up to 100:0 from 0:100 with use of a 1/2 wavelength plate 6. In other words, the intensity ratio can be changed between two laser beams when the plate 6 is turned against the optical axis of the incident light. As a result, the intensity of the recording laser beams can be equalized on a substrate 1.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は光ディスク原盤の作成装置に関すも従来の技術 光ディスク原盤は 表面を研磨したガラス等の基板にフ
ォトレジストを塗布し これを記録すべき情報信号によ
り強度変調したレーザー光を用いて感光させ、その感光
度に対応した信号ピットを形成して作成すも 情報信号の転送レートを高めるた取 二つの信号を同時
に記録し 再生することが行われていも二つの信号を同
時に記録するために レーザー装置を二台用いる力\ 
若しくζよ −台のレーザー装置から出た光をハーフミ
ラ−で二つに分ける必要があム ニ台のレーザー装置を
用いると、二つのレーザー光の安定性に問題が生じたり
、維持管理に手間がかかるなどの問題があるの六 −台
のレーザー装置から出た光をハーフミラ−で二つに分け
る方法が用いられも 第3図はそのような従来の光ディ
スク原盤の作成装置の構成を、レーザー光の照射構成を
主にして示したものである。
[Detailed Description of the Invention] Industrial Field of Application The present invention relates to an apparatus for producing an optical disc master.The conventional technology for an optical disc master is to apply a photoresist to a substrate made of glass or the like with a polished surface, and record information signals on this. In order to increase the transfer rate of the information signal, two signals are recorded and played back at the same time. The power of using two laser devices to record two signals at the same time
It is necessary to divide the light emitted from two laser devices into two by a half mirror.If two laser devices are used, problems may arise with the stability of the two laser beams, and maintenance may become difficult. Although a method is used in which the light emitted from six laser devices is divided into two by a half mirror, there are problems such as time and effort. This mainly shows the laser beam irradiation configuration.

第3図において、フォトレジストを塗布した基板1 t
−1スピンドル2によって回転駆動されるとともへ −
軸移動台3によって基板1の半径方向に移送されも 記
録用レーザー装置4の発する記録用レーザー光は ミラ
ー5を経てハーフミラ−21で二つに分けられた徴 そ
れぞれ電気光学効果等を利用した強度変調器8、8aに
よって記録すべき信号に応じて強度変調を受ζす、互い
に焦点距離の異なる二枚のレンズを焦点を共有するよう
に配置したビームエキスパンダー9、9aによってビー
ム径を拡大された抵 一方はミラーlOを経て偏光ビー
ムスプリッタ−12で反射され もう一方はミラー11
を経て1/2波長板20で偏波面を90度回転し 偏光
ビームスプリッタ−12を透過すも 偏光ビームスプリ
ッタ−12で両方の光を合成した抵 ダイクロイックミ
ラー13、ミラー14を経て、 レンズアクチュエータ
ー15によって基板1に絞り込まれて照射されも制御用
レーザー装置16による制御用レーザー光は焦点制御用
であり、偏光ビームスプリッタ−17、1/4波長板1
8、ダイクロイックミラー13、 ミラー14を経て、
 レンズアクチュエーター15によって絞り込まれて基
板lに照射されもこの制御用レーザー光の基板lからの
反射光(戴ミラー14、ダイクロイックミラー13、1
/4波長板18を経て偏光ビームスプリッタ−17によ
って入射光と分けられて、焦点位置検出用受光素子19
に導かれも 受光素子19によって得られた信号を基に
してレンズアクチュエーター11の駆動がなされ 記録
用レーザー光が基板1に常に焦点が合っているよう焦点
制御が行われも発明が解決しようとする課題 基盤に照射されるレーザー光の強度は レーザー光が二
つに分けられて以降透過若しくは反射するミラー等の光
学部品の特性に影響されもこのた八 基盤に照射される
レーザー強度をそれぞれのレーザー光で等しくするため
にζよ 光学部品の特性に応じてレーザー光を二つに分
ける際の強度比を調整する必要があa しかし 従来例の光ディスク原盤の作成装置で(よ レ
ーザー光をハーフミラ−で二つの光に分けているたべ 
それぞれのレーザー光の強度比はハーフミラ−を交換し
なければ変えることができなかっtら また ハーフミラ−を交換すると、ハーフミラ−からレ
ンズアクチュエーターまでの光学部品を再び調整する必
要が生じも また ハーフミラ−の反射と透過の割合を
微妙に変化させることは困難であも 本発明ζ友 上記の欠点を排除した光ディスク原盤の作
成装置の供給を目的としたものであも課題を解決するた
めの手段 本発明は上記の目的を、記録用レーザー光の偏光状態を
変化させる手段と偏光ビームスプリッタ−を有し 前記
偏光ビームスプリッタ−で記録用レーザー光を二つに分
けることにより達成すも作用 本発明の装置で&友 記録用レーザー光の偏光状態を変
化させて偏光ビームスプリッタ−の透過光量と反射光量
の割合を変化させることができもまた 記録用レーザー
光の偏光状態を変化させてL 偏光ビームスプリッタ−
からレンズアクチュエーターまでの光学部品を再び調整
する必要は生じなしも このた八 二つの記録レーザー光の光ディスク原盤での
強度を容易に調整することができ、また等しくすること
もできも 実施例 以下本発明を実施例によって詳細に説明する。
In FIG. 3, a substrate 1t coated with photoresist
−1 Rotationally driven by spindle 2 and to −
The recording laser beam emitted by the recording laser device 4 is transferred in the radial direction of the substrate 1 by the axis moving table 3, and is divided into two by the half mirror 21 after passing through the mirror 5. The beam diameter is expanded by beam expanders 9, 9a which receive intensity modulation according to the signal to be recorded by modulators 8, 8a, and are composed of two lenses having different focal lengths arranged so as to share a focal point. One side is reflected by the polarizing beam splitter 12 through the mirror 10, and the other side is reflected by the mirror 11.
After that, the plane of polarization is rotated by 90 degrees with a 1/2 wavelength plate 20 and transmitted through a polarizing beam splitter 12. Both lights are combined by a polarizing beam splitter 12, pass through a dichroic mirror 13 and a mirror 14, and then a lens actuator 15. The control laser beam focused and irradiated onto the substrate 1 by the control laser device 16 is for focus control, and is directed to the polarization beam splitter 17 and the quarter-wave plate 1.
8. After dichroic mirror 13 and mirror 14,
The control laser light that is narrowed down by the lens actuator 15 and irradiated onto the substrate 1 is reflected from the substrate 1 (daily mirror 14, dichroic mirror 13, 1
The incident light is separated from the incident light by a polarizing beam splitter 17 through a /4 wavelength plate 18 and sent to a light receiving element 19 for focal position detection.
Even if the lens actuator 11 is driven based on the signal obtained by the light receiving element 19 and the focus control is performed so that the recording laser beam is always focused on the substrate 1, the invention attempts to solve the problem. The intensity of the laser beam irradiated to the target substrate is influenced by the characteristics of optical parts such as mirrors that transmit or reflect after the laser beam is divided into two. In order to make the light equal, it is necessary to adjust the intensity ratio when dividing the laser beam into two parts according to the characteristics of the optical components. The plate is divided into two lights.
The intensity ratio of each laser beam cannot be changed without replacing the half mirror, and if the half mirror is replaced, it becomes necessary to readjust the optical components from the half mirror to the lens actuator. Although it is difficult to subtly change the ratio of reflection and transmission, the present invention is aimed at providing an optical disk master production device that eliminates the above-mentioned drawbacks. The apparatus of the present invention achieves the above object by having a means for changing the polarization state of a recording laser beam and a polarizing beam splitter, and dividing the recording laser beam into two by the polarizing beam splitter. By changing the polarization state of the recording laser beam, the ratio between the amount of transmitted light and the amount of reflected light from the polarizing beam splitter can be changed.
There is no need to readjust the optical components from the lens actuator to the lens actuator.In addition, the intensities of the two recording laser beams at the optical disc master can be easily adjusted and made equal. The invention will be explained in detail by way of examples.

第1図は本発明の第1の実施例の光ディスク原盤作成装
置の構成図であム 記録用レーザー光の偏光状態を変化
させる手段として、記録用レーザー装置と偏光ビームス
プリッタ−との間に波長板を設けていも 同図(b)C
L  基板1、 ミラー14の近傍の正面図であム フォトレジストを塗布した基板1ζ友 スピンドル2に
よって回転駆動されるととも&へ 一軸移動台3によっ
て基板lの半径方向に移送される。
FIG. 1 is a block diagram of an optical disc master production apparatus according to a first embodiment of the present invention. As a means for changing the polarization state of a recording laser beam, a wavelength Even if a board is installed, Figure (b)C
L is a front view of the substrate 1 and the vicinity of the mirror 14. The substrate 1 coated with photoresist is rotated by the spindle 2 and transferred in the radial direction of the substrate 1 by the uniaxial moving stage 3.

記録用レーザー装置4の発する直線偏光した記録用レー
ザー光4L  ミラー5を経て波長板6によって偏光状
態が変換され 偏光ビームスプリッタ−(以下PBSと
略記する)7によってS偏光成分は反射されP偏光成分
は透過されることにより二つの記録用レーザー光に分け
られも PBS 7によって反射されたレーザービームは強度変
調器8によって記録すべき信号に応じて強度変調を受1
す、ビームエクスパンダ−9によってビーム径を拡大さ
れた&  PBS12により反射され4  PBS7を
透過したレーザービームはミラー11を経て強度変調器
8aによって記録すべき信号に応じて強度変調を受1す
、ビームエクスパンダー9aによってビーム径を拡大さ
れた徽PBS12を透過すム 偏波面の90度異なる二つのレーザービーム(よPBS
12によって反射もしくは透過されることによって合成
されも 合成された記録用レーザー光(よ ダイクロイ
ックミラー13、 ミラー14を経て、 レンズアクチ
ュエーター15によって基板1に絞り込まれも 一般番ζ ある面(ここではPBSの反射面)の法線と
入射光の光軸とのなす面(入射面)に対して偏光方向が
平行な光をP偏光 入射面に対して偏光方向が垂直な光
をS偏光と称している。偏光状態として沫 直線偏光・
円偏光・楕円偏光があり、直線偏光の場合の偏波面の向
きゃ、楕円偏光の場合の楕円率を含んでいも 制御用レーザー装置を用いた焦点制御系は 第3図と同
じであん 焦点位置検出用受光素子198よ 例えばナ
イフェツジ法ではレンズと、 レンズの焦点面との間の
ナイフェツジと二分割した光検出器を念仏 非点収差法
では円筒レンズと四分割した光検出器を含a 本発明の
説明では このような焦点制御が可能な光検出器を一括
して焦点位置検出用受光素子として称していも 記録用レーザー装置としては 例えばアルゴンレーザー
が用いられる力交 クリプトンレーザー・エキシマレー
ザ−等フォトレジストが感度を有する波長を発生させる
レーザー装置であれば良1.%制御用レーザー装置とし
てζよ 例えばヘリウムネオンレーザ−が用いられる戟
 半導体レーザー等フォトレジストが感度を有さない波
長を発生させるレーザー装置であれば良(〜 波長板としては 例えば用いる波長に応じて厚みを決め
た水晶の板が用いられも 水晶の結晶軸(2軸)と入射光の偏波面との角度や水晶
板の厚さや入射光の波長によって、直線偏光がそのまま
透過されたり、円偏光に変換されたり、楕円偏光に変換
されたり、また 偏波面が90度回転した直線偏光に変
換されたりすもP偏光またはS偏光の場合にζ友 PB
Sによって100%透過したり、 100%反射したり
す4円偏光に変換された場合41  P偏光成分とS偏
光成分の強さが等しいのn  PBS7によって同じ強
さの二つの光に分けられも 楕円偏光に変換された場合41  P偏光成分とS偏光
成分の強さが異なるのn  PBS7によって強さの異
なった二つの光に分けられも つまり、水晶の結晶軸(2軸)と入射光の偏波面との角
度を変えることによって、分けられた二つのビームの強
度比を変化させることができム波長板として172波長
板を用いると、二つのレーザービームの強度比を0:1
00から100:0まで任意の割合に変化させることが
できa本実施例で(友 波長板6を入射光の光軸に対し
て回転させることにより二つのレーザービームの強度比
を変化させも このた敷 二つのレーザービームの強度比を容易に変化
させることができも また 二つのレーザービームの強
度比を変化させてもレーザー光の光軸を変えないので、
PBS7からレンズアクチュエーター15までの光学部
品を調整しなおす必要も生じな(一 基板に二つの情報信号を記録する場合、二つの情報信号
の信号品質を等しくする必要があム このた数 記録用
レーザー光の強度を基板上で等しくする必要があも しかL  PBS7からPBS12までの光学部品の特
性のばらつき!、PBS12からレンズアクチュエータ
ー15までの光学部品の入射光の偏波面による特性の違
いなどによって、同じ強さの二つのビームに分けても基
板上に照射されるときの強度は異なってしまうことが多
(を 本実施例で(よ 波長板を調整するだけで二つのビーム
の強度比を変えられるので、基板上の記録用レーザー光
の強度を精確に等しくすることができも また 必要に
応じて任意の強度比にすることもできも 次に 本発明の第2の実施例について第2図を用いて説
明すも 本実施例においては 記録用レーザー光の偏光
状態を変化させる手段として、記録用レーザー装置をレ
ーザー光の光軸を中心として回転可能にして設けられて
いも 第2図に於ては 直線偏光したレーザー光を発する記録
用レーザー装置がレーザー光の光軸を中心として回転可
能となした戊 並びに波長板が設けられていない点以外
は 第1図と同じであるので、図の詳細な説明は省略す
も 記録用レーザー装置から発せられた記録用レーザー光の
偏波面は 記録用レーザー装置を回転させることによっ
て回転L  PBSに対してP偏光からS偏光まで変化
させることができも記録用レーザー光の偏波面が紙面に
平行つまりP偏光の場合i、t、PBS7で100%透
過する。
A linearly polarized recording laser beam 4L emitted by a recording laser device 4 passes through a mirror 5, the polarization state is converted by a wavelength plate 6, the S-polarized component is reflected by a polarizing beam splitter (hereinafter abbreviated as PBS) 7, and the P-polarized component is converted into a P-polarized component. The laser beam is transmitted and divided into two recording laser beams, and the laser beam reflected by the PBS 7 is intensity modulated by an intensity modulator 8 according to the signal to be recorded.
The beam diameter is expanded by the beam expander 9, reflected by the PBS 12, and transmitted through the PBS 7. The laser beam passes through the mirror 11 and undergoes intensity modulation by the intensity modulator 8a according to the signal to be recorded. Two laser beams with polarization planes different by 90 degrees pass through the PBS 12 whose beam diameter has been expanded by the beam expander 9a.
The synthesized recording laser beam is reflected or transmitted by the dichroic mirror 13 and the mirror 14, and is narrowed down to the substrate 1 by the lens actuator 15. Light whose polarization direction is parallel to the plane (incident plane) formed by the normal line of the reflecting surface (reflecting surface) and the optical axis of the incident light is called P-polarized light, and light whose polarization direction is perpendicular to the incident plane is called S-polarized light. .Linearly polarized light
There is circularly polarized light and elliptically polarized light, and the direction of the plane of polarization in the case of linearly polarized light includes the ellipticity in the case of elliptically polarized light.The focus control system using a laser device for control is the same as shown in Figure 3.Focus position Detection light receiving element 198 For example, in the Naifetsu method, the lens and the knife between the focal plane of the lens and the photodetector divided into two parts are used.In the astigmatism method, the cylindrical lens and the photodetector divided into four parts are included.A This invention In the explanation, such photodetectors capable of focus control are collectively referred to as light receiving elements for detecting focus positions, but as recording laser devices, for example, argon lasers, krypton lasers, excimer lasers, etc. are used as photodetectors. 1. Any laser device that generates a wavelength to which the resist is sensitive is acceptable. For example, a helium-neon laser can be used as a laser device for controlling the %.Any laser device, such as a semiconductor laser, that generates a wavelength to which the photoresist is not sensitive may be used. Even if a crystal plate with a certain thickness is used, depending on the angle between the crystal axis (two axes) of the crystal and the polarization plane of the incident light, the thickness of the crystal plate, and the wavelength of the incident light, linearly polarized light may be transmitted as is, or circularly polarized light may be transmitted as is. In the case of P-polarized light or S-polarized light, PB
100% transmission or 100% reflection due to S 4 When converted to circularly polarized light 41 Is the intensity of the P polarized light component and the S polarized light component equal?n When the light is divided into two lights of the same intensity by PBS7 is an ellipse When converted to polarized light, the intensities of the P-polarized light component and the S-polarized light component are different. By changing the angle with the wavefront, the intensity ratio of the two separated beams can be changed.If a 172 wavelength plate is used as a wavelength plate, the intensity ratio of the two laser beams can be changed to 0:1.
In this embodiment, the intensity ratio of the two laser beams can be changed by rotating the wavelength plate 6 with respect to the optical axis of the incident light. Although the intensity ratio of the two laser beams can be easily changed, the optical axis of the laser beam does not change even if the intensity ratio of the two laser beams is changed.
There is no need to readjust the optical components from the PBS 7 to the lens actuator 15. (When recording two information signals on one board, it is necessary to equalize the signal quality of the two information signals.) It is necessary to equalize the light intensity on the board.Due to variations in the characteristics of optical components from PBS7 to PBS12!, differences in characteristics due to the polarization plane of the incident light of optical components from PBS12 to lens actuator 15, etc. Even if the beams are divided into two beams with different strengths, the intensities irradiated onto the substrate often differ (as shown in this example). Therefore, the intensities of the recording laser beams on the substrate can be made exactly equal, or can be set to any intensity ratio as required. Next, FIG. 2 shows a second embodiment of the present invention. In this embodiment, as a means for changing the polarization state of the recording laser beam, the recording laser device is provided so as to be rotatable around the optical axis of the laser beam. is the same as Figure 1, except that the recording laser device that emits linearly polarized laser light is rotatable around the optical axis of the laser beam, and there is no wavelength plate, so the details of the figure are Although I will omit the detailed explanation, the plane of polarization of the recording laser beam emitted from the recording laser device can be changed from P polarization to S polarization with respect to the rotating L PBS by rotating the recording laser device. When the plane of polarization of the laser beam is parallel to the plane of the paper, that is, it is P-polarized light, it transmits 100% at i, t, and PBS7.

記録用レーザー光の偏波面が紙面に垂直つまりS偏光の
場合1;1.、PBS7で100%反射すも記録用レー
ザー光の偏波面が紙面に対して傾いている場合&上 偏
波面の傾きの度合に応じてPBS7の透過と反射の割合
が変化すも このように 記録用レーザー装置をレーザー光の光軸を
中心として回転させることによって、PBS7で分けら
れる二つのレーザービームの強度比を容易に変化させる
ことができも また 二つのレーザービームの強度比を変化させてもレ
ーザー光の光軸を変えないの玄 PBS7からレンズア
クチュエーター15までの光学部品を調整しなおす必要
も生じな(〜 本実施例において杖 記録用レーザー装置をレーザー光
の光軸を中心として回転させるだけで二つのビームの強
度比を変えられるの六 基板上の記録用レーザー光の強
度を精確に等しくすることができも また 必要に応じ
て任意の強度比にすることもできも 予め基板上に溝が形成された基板に情報信号を記録する
場合は 溝に沿って信号を記録する必要がある力(ミラ
ー14をトラッキングミラーに変え 焦点制御系にトラ
ッキング制御系を付加すれば記録できも トラッキング制御系ζよ 例えばプッシュプル法ではレ
ンズと二分割した光検出器を含へ 光検出器によって得
られた信号を基にしてトラッキングミラーの角度を変え
溝に常にトラッキングがかかつているようにトラッキン
グ制御が行われもトラッキング制御系を有する場合でk
 本発明の光ディスク原盤の作成装置は基板上の記録用
レーザー光の強度を精確に等しくすることL 必要に応
じて任意の強度比にすることもできも発明の効果 本発明の装置Cヨ  記録用レーザー光の偏光状態を変
化させる手段と偏光ビームスプリッタ−を有し 前記偏
光ビームスプリッタ−で記録用レーザ−光を二つに分け
ることにより、記録用レーザー光の偏光状態を変化させ
て偏光ビームスプリ・ツタ−の透過光量と反射光量の割
合を変化させることができも また 記録用レーザー光の偏光状態を変化させて舷 偏
光ビームスプリッタ−からレンズアクチュエーターまで
の光学部品を再び調整する必要は生じなt〜 このた数
 二つの記録レーザー光の光ディスク原盤での強度を容
易に等しくすることができ、保守が容易で信頼性の高い
光ディスク原盤の作成装置が得られも
When the polarization plane of the recording laser beam is perpendicular to the plane of the paper, that is, S-polarized light 1;1. , 100% reflection on PBS7 When the plane of polarization of the recording laser beam is tilted with respect to the paper surface & above The ratio of transmission and reflection of PBS7 changes depending on the degree of tilt of the plane of polarization. By rotating the laser device around the optical axis of the laser beam, the intensity ratio of the two laser beams separated by PBS 7 can be easily changed. There is no need to readjust the optical components from the PBS 7 to the lens actuator 15 because the optical axis of the laser beam does not change. It is possible to change the intensity ratio of the two beams by changing the intensity ratio of the two beams.It is also possible to make the intensity of the recording laser beam on the substrate exactly equal, or it is possible to set the intensity ratio to an arbitrary value as needed. When recording an information signal on a substrate with a groove formed on it, there is a force required to record the signal along the groove (recording can be done by replacing the mirror 14 with a tracking mirror and adding a tracking control system to the focus control system). For example, the push-pull method involves a lens and a photodetector divided into two parts. Based on the signal obtained by the photodetector, the angle of the tracking mirror is changed and tracking control is performed so that the groove is always being tracked. In the case where we also have a tracking control system, k
The apparatus for producing an optical disk master according to the present invention is capable of precisely equalizing the intensity of recording laser beams on the substrate.It is also possible to set the intensity ratio to any desired intensity ratio as required.Effects of the Invention Apparatus of the present inventionFor recording It has means for changing the polarization state of the laser beam and a polarizing beam splitter, and by dividing the recording laser beam into two by the polarizing beam splitter, the polarization state of the recording laser beam is changed and the polarizing beam splitter is formed.・Although it is possible to change the ratio of the amount of light transmitted by the vine to the amount of reflected light, there is no need to change the polarization state of the recording laser beam and readjust the optical components from the polarizing beam splitter to the lens actuator. t~ This number It is possible to easily equalize the intensities of two recording laser beams on the optical disc master, and to obtain an easy-to-maintain and highly reliable optical disc master production apparatus.

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

第1医 第2図は本発明の光ディスク原盤の作成装置の
第1、第2の実施例の構成図 第3図は光ディスク原盤
の作成装置の従来例の構成図であム ト・・基K 4・・・記録用レーザ装置 6・・・波長
板7・・・偏光ビームスプリッタ−0 代理人の氏名 弁理士 粟野重孝 はか1名第 図 (a−) (b) Sミラ
1. Fig. 2 is a block diagram of the first and second embodiments of the optical disc master production apparatus of the present invention. Fig. 3 is a block diagram of a conventional example of the optical disc master production apparatus of the present invention. ... Recording laser device 6 ... Wave plate 7 ... Polarizing beam splitter - 0 Name of agent Patent attorney Shigetaka Awano Figure 1 (a-) (b) S Mira

Claims (5)

【特許請求の範囲】[Claims] (1)フォトレジストを塗布した光ディスク基板に記録
信号により強度変調したレーザー光を照射する工程を有
する、記録信号を記録した光ディスク原盤の作成装置で
あって、記録用レーザー光の偏光状態を変化させる手段
と偏光ビームスプリッターを有し、前記偏光ビームスプ
リッターで記録用レーザー光を二つに分けることを特徴
とする光ディスク原盤の作成装置。
(1) An apparatus for producing an optical disc master on which a recording signal is recorded, which has a process of irradiating an optical disc substrate coated with a photoresist with a laser beam whose intensity is modulated according to a recording signal, and which changes the polarization state of the recording laser beam. 1. An apparatus for producing an optical disc master, comprising: a means for producing an optical disc master; and a polarizing beam splitter, the polarizing beam splitter splitting a recording laser beam into two.
(2)フォトレジストを塗布した光ディスク基板に記録
信号により強度変調したレーザー光を照射する工程を有
する、記録信号を記録した光ディスク原盤の作成装置で
あって、直線偏光したレーザー光を波長板を用いて偏光
状態を変化させた後偏光ビームスプリッターで偏波面が
90度異なる二つの記録レーザー光に分けることを特徴
とする光ディスク原盤の作成装置
(2) A device for producing an optical disk master recording a recording signal, which includes a step of irradiating an optical disk substrate coated with a photoresist with laser light whose intensity is modulated according to the recording signal, and which uses a wavelength plate to emit linearly polarized laser light. An apparatus for producing an optical disc master, characterized in that the polarization state is changed using a polarizing beam splitter, and then the recording laser beam is divided into two recording laser beams with polarization planes different by 90 degrees.
(3)波長板として1/2波長板を用いることを特徴と
する請求項(2)記載の光ディスク原盤の作成装置
(3) The apparatus for producing an optical disc master according to claim (2), characterized in that a 1/2 wavelength plate is used as the wavelength plate.
(4)波長板を調整し楕円偏光の楕円度を変えて偏光ビ
ームスプリッターの透過光量と反射光量の割合を変化さ
せることにより、二つの記録レーザー光の光ディスク原
盤上での強度を等しくなすことを特徴とする請求項(2
)もしくは(3)記載の光ディスク原盤の作成装置
(4) By adjusting the wavelength plate and changing the ellipticity of the elliptically polarized light to change the ratio between the amount of transmitted light and the amount of reflected light from the polarizing beam splitter, the intensity of the two recording laser beams on the optical disk master can be made equal. Claim (2)
) or the optical disc master production device described in (3)
(5)フォトレジストを塗布した光ディスク基板に、記
録信号により強度変調したレーザー光を照射する工程を
有する、記録信号を記録した光ディスク原盤の作成装置
であって、直線偏光した記録用レーザー光を発生させる
レーザー装置を記録用レーザー光の光軸を中心として回
転可能にし、前記記録用レーザー光を偏光ビームスプリ
ッターで偏波面が90度異なる二つの記録用レーザー光
に分けることを特徴とする光ディスク原盤の作成装置。
(5) A device for producing an optical disc master on which a recording signal is recorded, which has a process of irradiating an optical disc substrate coated with a photoresist with a laser beam whose intensity is modulated according to the recording signal, and generates a linearly polarized recording laser beam. The optical disc master is characterized in that a laser device is rotatable around the optical axis of a recording laser beam, and the recording laser beam is split into two recording laser beams with polarization planes different by 90 degrees by a polarizing beam splitter. Creation device.
JP21104290A 1990-08-08 1990-08-08 Producing device for master optical disk Pending JPH0495243A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21104290A JPH0495243A (en) 1990-08-08 1990-08-08 Producing device for master optical disk

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21104290A JPH0495243A (en) 1990-08-08 1990-08-08 Producing device for master optical disk

Publications (1)

Publication Number Publication Date
JPH0495243A true JPH0495243A (en) 1992-03-27

Family

ID=16599415

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21104290A Pending JPH0495243A (en) 1990-08-08 1990-08-08 Producing device for master optical disk

Country Status (1)

Country Link
JP (1) JPH0495243A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2019333A1 (en) * 2007-07-25 2009-01-28 Singulus Mastering B.V. Production of stamps, masks or templates for semiconductor device manufacturing

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03122844A (en) * 1989-10-06 1991-05-24 Nec Corp Optical disk master disk exposing method

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03122844A (en) * 1989-10-06 1991-05-24 Nec Corp Optical disk master disk exposing method

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2019333A1 (en) * 2007-07-25 2009-01-28 Singulus Mastering B.V. Production of stamps, masks or templates for semiconductor device manufacturing
WO2009013028A1 (en) * 2007-07-25 2009-01-29 Singulus Mastering B. V. Production of stamps, masks or templates for semiconductor device manufacturing

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