JPS60214432A - Optical information recording and reproducing device - Google Patents
Optical information recording and reproducing deviceInfo
- Publication number
- JPS60214432A JPS60214432A JP59070628A JP7062884A JPS60214432A JP S60214432 A JPS60214432 A JP S60214432A JP 59070628 A JP59070628 A JP 59070628A JP 7062884 A JP7062884 A JP 7062884A JP S60214432 A JPS60214432 A JP S60214432A
- Authority
- JP
- Japan
- Prior art keywords
- light beam
- adjusting means
- recording
- information recording
- irradiating
- 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.)
- Granted
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 43
- 239000004065 semiconductor Substances 0.000 claims abstract description 22
- 230000001678 irradiating effect Effects 0.000 claims abstract description 16
- 230000010355 oscillation Effects 0.000 description 26
- 238000010586 diagram Methods 0.000 description 7
- 239000000463 material Substances 0.000 description 5
- 238000005259 measurement Methods 0.000 description 5
- 230000002542 deteriorative effect Effects 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000002238 attenuated effect Effects 0.000 description 1
- 230000008094 contradictory effect Effects 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 229920001169 thermoplastic Polymers 0.000 description 1
- 239000004416 thermosoftening plastic Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/12—Heads, e.g. forming of the optical beam spot or modulation of the optical beam
- G11B7/125—Optical beam sources therefor, e.g. laser control circuitry specially adapted for optical storage devices; Modulators, e.g. means for controlling the size or intensity of optical spots or optical traces
- G11B7/126—Circuits, methods or arrangements for laser control or stabilisation
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B19/00—Driving, starting, stopping record carriers not specifically of filamentary or web form, or of supports therefor; Control thereof; Control of operating function ; Driving both disc and head
- G11B19/02—Control of operating function, e.g. switching from recording to reproducing
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Recording Or Reproduction (AREA)
- Optical Head (AREA)
Abstract
Description
【発明の詳細な説明】
発明の技術分野
本発明は、ディスク状の光学記録媒体にレーザ発振器等
から出射する光ビームを照射して情報な記録再生する光
情報記録再生装置に係り、特に、記録又は再生動作の前
後においても媒体に光ビームを照射して所定のトラック
をトラッキング制御しつつ記録再生動作を待機する光情
報記録再生装置に関する。DETAILED DESCRIPTION OF THE INVENTION Technical Field of the Invention The present invention relates to an optical information recording/reproducing apparatus for recording and reproducing information by irradiating a disc-shaped optical recording medium with a light beam emitted from a laser oscillator or the like. Alternatively, the present invention relates to an optical information recording and reproducing apparatus that waits for a recording and reproducing operation while controlling tracking of a predetermined track by irradiating a light beam onto a medium before and after a reproducing operation.
従来技術と問題点
一般に、光情報記録再生装置では、記録すべき情報に応
じて光ビームを強弱に変調して記録媒体の所定の位置に
集光し前記媒体上に情報を記録する記録動作と、媒体上
の所定の位置に記録された情報を非破壊に再生する再生
動作とによって高密度かつ大量の情報の光学的記録や再
生を行なっている。特に、上記再生動作においては、媒
体に記録された情報を誤りなく再生し、かつ非破壊に情
報を再生することが、極めて重要である。Prior Art and Problems In general, optical information recording and reproducing devices perform a recording operation in which a light beam is modulated to be strong or weak depending on the information to be recorded, and is focused on a predetermined position on a recording medium to record information on the medium. , optical recording and reproduction of a large amount of information at high density is performed by a reproduction operation that non-destructively reproduces information recorded at a predetermined position on a medium. In particular, in the above-mentioned reproduction operation, it is extremely important to reproduce the information recorded on the medium without error and to reproduce the information non-destructively.
しかるに、前記光ビームなレーザ発振器のレーザ光によ
る場合には、低出力発振時に量子ショット雑音や発光閾
値雑音あるいは、媒体からの反射光による干渉による雑
音等を発生し出力のゆらぎを生じ再生信号のシヘ比を悪
くする欠点を有している。以下、半導体レーザな例に説
明する。第1図は半導体レーザの発振出力と順方向駆動
電流の関係を示し、横軸は駆動電流、縦軸は発振出力を
それぞれ示す。図中(イ)の領域はLED領域、(ロ)
は、コヒーレンシイの優れたレーザ発振領域を示し、第
1図の例ではレーザ発振を開始する発振閾値電流は約6
0 mAである。第2図は第3図の後述する測定光学系
で実測した上記半導体レーザの発振出力と発振出力に生
じる雑音(出力のゆらぎ)の関係を示し、横軸はレーザ
発振出力、縦軸は発振出力に生じる雑音量をそれぞれ示
す。第2図で低出力発振域に生じる大きな雑音は第1図
でのレーザ発振領域(ロ)の発振閾値近傍部に相当して
おり、発振出力の増加とともに上記雑音は減少する事が
わかる。かかる雑音は、再生動作時に光ビーム強度のゆ
らぎを生じるため、再生信号のSβ比を悪化させ再生時
の誤り率を高くする問題を生じる。かかる問題の解消の
ためには、発振出力を前記雑音を含まぬ充分に大きな値
とする事により、(第2図の例では発振出力を1mW以
上)再生信号のシ公比を良好に得ることによっている。However, when the laser beam from a laser oscillator is used as the light beam, quantum shot noise, emission threshold noise, or noise due to interference due to reflected light from the medium is generated during low-output oscillation, resulting in fluctuations in the output and deterioration of the reproduced signal. It has the disadvantage of worsening the shedding ratio. An example of a semiconductor laser will be explained below. FIG. 1 shows the relationship between the oscillation output and forward drive current of a semiconductor laser, where the horizontal axis shows the drive current and the vertical axis shows the oscillation output. In the diagram, the area (a) is the LED area, and (b)
indicates a laser oscillation region with excellent coherency, and in the example shown in Fig. 1, the oscillation threshold current for starting laser oscillation is approximately 6
0 mA. Figure 2 shows the relationship between the oscillation output of the semiconductor laser and the noise (output fluctuation) generated in the oscillation output, which was actually measured using the measurement optical system shown in Figure 3, which will be described later. The horizontal axis is the laser oscillation output, and the vertical axis is the oscillation output. shows the amount of noise generated in each case. The large noise generated in the low output oscillation region in FIG. 2 corresponds to the area near the oscillation threshold in the laser oscillation region (b) in FIG. 1, and it can be seen that the noise decreases as the oscillation output increases. Such noise causes fluctuations in the optical beam intensity during the reproduction operation, resulting in a problem of deteriorating the Sβ ratio of the reproduced signal and increasing the error rate during reproduction. In order to solve this problem, it is necessary to obtain a good common ratio of the reproduced signal by setting the oscillation output to a sufficiently large value that does not include the above-mentioned noise (in the example of Fig. 2, the oscillation output is 1 mW or more). I am by.
第3図は上記雑音を検出する測定光学系を示す。FIG. 3 shows a measurement optical system for detecting the above noise.
半導体レーザ1の光ビームはコリメータレンズ2で平行
ビームとしへ山フミラー3により1部は半導体レーザ雑
音測定用光検出器9に受光され、他は偏光ビームスプリ
ッタ4、回転式V4λ板5を通過した後、集光レンズ6
で集光し光軸の軸方向に振動するミラー1に照射し、反
射光は再びレンズ6、V4λ板5、偏光ビームスプリッ
タ4を通過し、八−7ミラー3により1部は戻り光測定
用光検出器8に、更に1部はレンズ2を経て半導体レー
ザ1に至る。The light beam of the semiconductor laser 1 is made into a parallel beam by a collimator lens 2, and one part is received by a photodetector 9 for semiconductor laser noise measurement by a mirror 3, and the other part passes through a polarizing beam splitter 4 and a rotating V4λ plate 5. Rear, condenser lens 6
The reflected light is focused on the mirror 1 that vibrates in the axial direction of the optical axis, and the reflected light passes through the lens 6, the V4λ plate 5, and the polarizing beam splitter 4 again, and a part of the light is returned by the 8-7 mirror 3 for measurement of the returned light. A portion of the light passes through the photodetector 8 and the lens 2 and then reaches the semiconductor laser 1 .
一方、上記した光情報記録再生装置の記録媒体には、サ
ーモプラスチックス光記録材料、アモルファス光記録材
料、あるいはMnB1等の磁気光学記録材料等が用いら
れるが、これ等の記録材料は固有な光物性が照射される
光ビームのエネルギーに感応して変化することを利用し
て媒体への情報の記録もしくは記録情報の再生を行なう
ことによっており、その結果、低出力の光ビームであっ
ても長時間に渡って上記媒体の同一トラックを照射しつ
づけた場合には、記録材料に変化を来たし媒体を損傷せ
しめることが知られていた。この関係を第4図に示して
いる。On the other hand, thermoplastic optical recording materials, amorphous optical recording materials, magneto-optical recording materials such as MnB1, etc. are used as the recording medium of the above-mentioned optical information recording/reproducing device, but these recording materials have unique optical properties. Information is recorded on the medium or reproduced by utilizing the fact that physical properties change in response to the energy of the irradiated light beam. As a result, even a low-power light beam can be used for a long time. It has been known that continued irradiation of the same track on the medium over time can cause changes in the recording material and damage the medium. This relationship is shown in FIG.
94図は、一定強度の光ビームを所定のトラックC二継
続して照射した場合に生じる再生信号の雑音量増加特性
を示す。横軸は光ビームを同一トラックに照射してトラ
ッキング制御を行なうトラッキング時間、縦軸は前記継
続トラッキングの結果再生信号に発生する雑音量の増加
をそれぞれ示す。FIG. 94 shows the noise increase characteristic of the reproduced signal when two predetermined tracks C are continuously irradiated with a light beam of constant intensity. The horizontal axis shows the tracking time during which tracking control is performed by irradiating the same track with a light beam, and the vertical axis shows the increase in the amount of noise generated in the reproduced signal as a result of the continuous tracking.
囚は半導体レーザの発振出力を1.25 mW、 (B
)は15mW、(C)は1.75 mW、 (D)は2
mWとした場合の雑音増加特性をそれぞれ示しており
、本図中(3)は1.25mWの発振出力においても、
100時間の同一トラックへの光ビーム照射によって、
再生信号の雑音量が増加し、媒体を損傷しはじめている
事がわかる。なお、上記(A)の発振出力は、第2図で
閾値雑音が低下した部分に対応しており、媒体の損傷を
防止すべく更に発振出力を低下せしめると、前記閾値雑
音が増大し、再生信号の9比を悪くする問題点を生じる
ことが示されている。The oscillation output of the semiconductor laser is 1.25 mW, (B
) is 15 mW, (C) is 1.75 mW, (D) is 2
The noise increase characteristics are shown for each mW, and (3) in this figure shows that even at an oscillation output of 1.25mW
By irradiating the same track with a light beam for 100 hours,
It can be seen that the amount of noise in the reproduced signal increases and begins to damage the medium. Note that the oscillation output in (A) above corresponds to the part where the threshold noise has decreased in FIG. It has been shown that this causes a problem of deteriorating the 9-ratio of the signal.
上記背反的な問題点を解決する為に、従来光学系の途中
にフィルターを挿入し、再生時には前記雑音が発生しな
い充分な発振出力を有するレーザ光を前記フィルターで
減衰させて媒体に照射して良好なS/N比の再生信号を
得る方法等が提案されているが、高出力でレーザな発振
させることによるレーザ自体の寿命の短縮や、光学系を
含めた光情報記録再生装置の構造が複雑化するなど、更
に別な問題を発生し、実用上、多くの欠点を有するもの
となっていた。In order to solve the above-mentioned contradictory problems, conventionally a filter is inserted in the middle of the optical system, and a laser beam with sufficient oscillation output that does not generate the noise during reproduction is attenuated by the filter and irradiated onto the medium. Methods have been proposed to obtain reproduction signals with a good S/N ratio, but the life of the laser itself is shortened due to high-output laser oscillation, and the structure of the optical information recording and reproducing device including the optical system is affected. Further problems such as complication arise, resulting in many practical drawbacks.
発明の目的
本発明の目的は上記の従来技術のもつ間え に着目し、
高密度かつ大容量に情報を記録再生する光情報記録再生
装置において、記録あるいは再生時の光ビーム強度調整
手段と媒体の所定のトラックに光ビームを照射してトラ
ッキング制御を行い待機する光ビーム照射エネルギー調
整手段を設けることによって、信頼性に優れた実用的な
光情報記録再生装置を提供しようとするものである。Purpose of the Invention The purpose of the present invention is to focus on the limitations of the above-mentioned prior art,
In an optical information recording and reproducing device that records and reproduces information with high density and large capacity, a light beam intensity adjustment means and a light beam irradiation device that performs tracking control and waits by irradiating a light beam onto a predetermined track of a medium during recording or reproduction. By providing energy adjustment means, the present invention aims to provide a highly reliable and practical optical information recording/reproducing device.
発明の構成 以下、本発明を実施例を参照して詳細に説明する。Composition of the invention Hereinafter, the present invention will be explained in detail with reference to Examples.
第5図は、本発明による光情報記録再生装置の主要部の
概略構成を示す図である。半導体レーザ1による光ビー
ムはレンズ2によって平行光となりハーフミラ−3,1
/4λ板5′、対物レンズ6を通ってディスク10上に
集光される。反射光は再びレンズ6、V4λ板5′を通
ってハーフミラ−3によって光検出器8に受光され、デ
ィスク10に記録されている情報の検出やトラッキング
制御等が行なわれる。半導体レーザ1を駆動する駆動回
路11は、待機、記録、再生それぞれの動作に応じて選
択される待機時の第1の光ビーム照射エネルギー調整手
段12、記録時の第2の光ビーム照射強度調整手段13
、再生時の第3の光ビーム照射強度調整手段14によっ
て所望の駆動信号を半導体レーザに印加し、発振出力を
得ることができる。なお、本発明の第1の光ビーム照射
エネルギー調整手段12は、前記第3の光ビーム強度調
整手段14が半導体レーザ1を駆動して得る光ビーム照
射強度より低い出力で連続的に半導体レーザを発振させ
る回路構成でもよく、又、前記第3の光ビーム強度調整
手段14により得られる光く−ム強度と同程度のピーク
光強度を有する変調された発振状態で半導体レーザな発
振させる回路構成によってもよい。FIG. 5 is a diagram showing a schematic configuration of the main parts of the optical information recording/reproducing apparatus according to the present invention. The light beam from the semiconductor laser 1 is turned into parallel light by the lens 2 and is converted into a parallel beam by the half mirrors 3 and 1.
The light passes through the /4λ plate 5' and the objective lens 6 and is focused onto the disk 10. The reflected light passes through the lens 6 and the V4λ plate 5' again and is received by the photodetector 8 by the half mirror 3, where information recorded on the disc 10 is detected and tracking control is performed. A drive circuit 11 that drives the semiconductor laser 1 includes a first light beam irradiation energy adjustment means 12 during standby and a second light beam irradiation intensity adjustment means during recording, which are selected according to each operation of standby, recording, and reproduction. Means 13
During reproduction, a desired drive signal is applied to the semiconductor laser by the third light beam irradiation intensity adjusting means 14, and an oscillation output can be obtained. The first light beam irradiation energy adjusting means 12 of the present invention continuously operates the semiconductor laser at an output lower than the light beam irradiation intensity obtained by driving the semiconductor laser 1 by the third light beam intensity adjusting means 14. Alternatively, a circuit configuration that causes a semiconductor laser to oscillate in a modulated oscillation state having a peak light intensity comparable to the optical beam intensity obtained by the third light beam intensity adjusting means 14 may be used. Good too.
上記のように構成した光情報記録再生装置によれば、必
要な情報の記録または再生を待機する状態においては、
媒体上に記録された情報を破壊したり未記録状態の媒体
に無用なトラッキング痕跡を残さぬ、かつ、所定のトラ
ックにトラッキング制御を可能とする充分に低い照射エ
ネルギーの光ビームを第1の光ビーム照射エネルギー調
整手段12によって駆動回路11を介して半導体レーザ
1から発振せしめ、媒体からの反射光又は透過光を光検
出器8で検出し、所定のトラッキング制御を行いつつ次
の記録や再生の命令を長時間にわたって待機することが
できる。According to the optical information recording/reproducing apparatus configured as described above, in a state of waiting for recording or reproduction of necessary information,
The first light beam is a light beam with sufficiently low irradiation energy to enable tracking control on a predetermined track without destroying information recorded on the medium or leaving unnecessary tracking traces on an unrecorded medium. The beam irradiation energy adjustment means 12 causes the semiconductor laser 1 to oscillate via the drive circuit 11, and the reflected light or transmitted light from the medium is detected by the photodetector 8, and predetermined tracking control is performed while the next recording or reproduction is performed. Can wait for instructions for a long time.
また、記録や再生の命令によって、駆動回路11を介し
て半導体レーザな記録時の第2の光ビーム強度調整手段
13によって記録すべき信号に応じて変調し媒体に情報
を記録する充分な発振出力で発振させ、あるいは、再生
時の第3の光ビーム強度調整手段14によってS/N比
の良好な閾値ノイズの少ない発振出力範囲で発振させ、
最適な記録または再生を行うことができる。In addition, in response to a recording or reproduction command, the second light beam intensity adjusting means 13 at the time of recording, such as a semiconductor laser, modulates the signal to be recorded via the drive circuit 11 and generates sufficient oscillation output to record information on the medium. or oscillate in an oscillation output range with a good S/N ratio and less threshold noise by the third light beam intensity adjustment means 14 during reproduction,
Optimal recording or playback can be performed.
発明の詳細
な説明したごとく本発明によれば、ディスク状の光学記
録媒体に光ビームを照射して情報を記録再生する光情報
記録再生装置において、情報の記録または再生の命令を
待機する際には、長時間にわたって同一トラック上に光
ビームを照射しても媒体を損傷させることのない低エネ
ルギーの光ビームを照射する第1の光ビーム照射エネル
ギー調整手段を有し、記録の際には、媒体に安定かつ確
実に情報を記録する第2の光ビーム強度調整手段を備え
、再生にあたっては、低出力な光ビームに固有な光強度
のゆらぎの少ない良質な光ビームを照射する第3戸の光
ビーム強度調整手段を具備することによって良好ない比
の再生信号を得、それぞれ適宜選択することによって、
信頼性に優れた実用的な光情報記録再生装置を提供する
ことができる。DETAILED DESCRIPTION OF THE INVENTION According to the present invention, in an optical information recording and reproducing apparatus that records and reproduces information by irradiating a light beam onto a disk-shaped optical recording medium, when waiting for a command to record or reproduce information, has a first light beam irradiation energy adjustment means for irradiating a low energy light beam that does not damage the medium even if the light beam is irradiated onto the same track for a long time; It is equipped with a second light beam intensity adjustment means that stably and reliably records information on the medium, and during reproduction, a third door that irradiates a high quality light beam with less fluctuation in light intensity inherent to low output light beams. By providing a light beam intensity adjustment means, a reproduced signal with a good ratio can be obtained, and by selecting each appropriately,
A highly reliable and practical optical information recording/reproducing device can be provided.
なお、前述した実施例では、記録再生を行いうる光情報
記録再生装置について例示して説明したが、光情報記録
装置もしくは光情報再生装置について本発明の技術的思
想を適用することは勿論可能であり、本発明を逸脱する
ものではない。また、第1の光ビーム照射エネルギー調
整手段、第2の光ビーム強度調整手段、第3の光ビーム
強度調整手段及び駆動回路の固々の構成は、本発明の技
術範囲内で自由になし得るものである。In the above-mentioned embodiments, an optical information recording and reproducing device capable of recording and reproducing was explained as an example, but it is of course possible to apply the technical idea of the present invention to an optical information recording device or an optical information reproducing device. Yes, it does not depart from the present invention. Moreover, the specific configurations of the first light beam irradiation energy adjustment means, the second light beam intensity adjustment means, the third light beam intensity adjustment means, and the drive circuit can be freely configured within the technical scope of the present invention. It is something.
第1図は半導体レーザの発振出力と駆動電流の特性図、
第2図は半導体レーザの出力雑音特性図、第3図は雑音
特性の測定光学系概略構成図、第4図は媒体のトラッキ
ングによる雑音増加特性図、第5図は本発明になる光情
報記録再生装置の主要部構成図を示す。
1・・・・・・半導体レーザ
2・・・・・・コリメータレンズ
3・・・・・・八−フミラー
4・・・・・・偏光ビームスプリッタ
5・・・・・・回転式V4λ板
5′・・・・・・v4λ板
B・・・・・・集光レンズ
7・・・・・・ミラー
8・・・・・・戻り光測定用光検出器
B・・・・・・雑音測定用光検出器
10・・・・・・ディスク
11・・・・・・駆動回路
12・・・・・・光ビーム照射エネルギー調整手段13
・・・・・・光ビーム強度調整手段14・・・・・・光
ビーム強度調整手段第1図
0501o。
・・11すL14宅丸 (“4)
第2図
do1
発撮式方 (mWlFigure 1 is a characteristic diagram of the oscillation output and drive current of a semiconductor laser.
Figure 2 is a diagram of output noise characteristics of a semiconductor laser, Figure 3 is a schematic diagram of the optical system for measuring noise characteristics, Figure 4 is a diagram of noise increase characteristics due to tracking of the medium, and Figure 5 is an optical information recording according to the present invention. The main part configuration diagram of the playback device is shown. 1...Semiconductor laser 2...Collimator lens 3...Eight mirror 4...Polarizing beam splitter 5...Rotating V4λ plate 5 '...v4λ plate B...Condensing lens 7...Mirror 8...Photodetector for measuring returned light B...Noise measurement Photodetector 10...Disk 11...Drive circuit 12...Light beam irradiation energy adjustment means 13
. . . Light beam intensity adjustment means 14 . . . Light beam intensity adjustment means Fig. 1 0501o. ...11S L14 Takumaru (“4) Figure 2 do1 Shooting method (mWl
Claims (4)
の記録又は再生を行う光情報記録再生装置(=おいて、
光ビームを照射する手段と、媒体の所定のトラックに光
ビームを照射しつつ待機する第1の光ビーム照射エネル
ギー調整手段と、媒体の所定の位置に光ビームを照射し
て情報を記録する第2の光ビーム強度調整手段及び又は
、媒体に光ビームを照射して記録された情報を再生する
第3の光ビーム強度調整手段を備えてなることを特徴と
する光情報記録再生装置。(1) Optical information recording and reproducing device that records or reproduces information by irradiating a light beam onto a disk-shaped recording medium (=
means for irradiating a light beam; a first light beam irradiation energy adjusting means for waiting while irradiating a predetermined track of a medium with a light beam; and a first light beam irradiation energy adjusting means for irradiating a predetermined position of a medium with a light beam to record information. 1. An optical information recording/reproducing apparatus comprising: a second light beam intensity adjusting means; and/or a third light beam intensity adjusting means for reproducing recorded information by irradiating a medium with a light beam.
その光源とすることを特徴とする特許請求の範囲第1項
に記載の光情報記録再生装置。(2) The optical information recording and reproducing apparatus according to claim 1, wherein the means for irradiating the light beam is a light source such as a semiconductor laser.
.前記第3の光ビーム強度調整手段により照射される光
ビーム強度よりも低強度の光ビームを照射するようにし
た事を特徴とする特許請求の範囲第1項に記載の光情報
記録再生装置。(3) The first light beam irradiation energy adjusting means is 1
.. 2. The optical information recording and reproducing apparatus according to claim 1, wherein the optical information recording and reproducing apparatus is configured to irradiate a light beam with a lower intensity than the light beam intensity irradiated by the third light beam intensity adjusting means.
前記第3の光ビーム強度調整手段により照射される光ビ
ームエネルギーよりも低強度の光ビームを照射する変調
光ビーム発生制御手段よりなる事を特徴とする特許請求
の範囲第1項に記載の光情報記録再生装置。(4) The first light beam irradiation energy adjustment means:
The light according to claim 1, further comprising modulated light beam generation control means for emitting a light beam with lower intensity than the light beam energy emitted by the third light beam intensity adjustment means. Information recording and reproducing device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59070628A JPH07118084B2 (en) | 1984-04-09 | 1984-04-09 | Optical information reproducing device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59070628A JPH07118084B2 (en) | 1984-04-09 | 1984-04-09 | Optical information reproducing device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60214432A true JPS60214432A (en) | 1985-10-26 |
| JPH07118084B2 JPH07118084B2 (en) | 1995-12-18 |
Family
ID=13437081
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59070628A Expired - Lifetime JPH07118084B2 (en) | 1984-04-09 | 1984-04-09 | Optical information reproducing device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH07118084B2 (en) |
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61142538A (en) * | 1984-12-13 | 1986-06-30 | Matsushita Electric Ind Co Ltd | Optical information recording and reproducing device |
| JPS61230626A (en) * | 1985-04-05 | 1986-10-14 | Matsushita Electric Ind Co Ltd | How to play optical information media |
| JPS62101125U (en) * | 1985-12-16 | 1987-06-27 | ||
| JPH02235224A (en) * | 1989-03-08 | 1990-09-18 | Fujitsu Ltd | Projection power control system for optical disk device |
| US5197059A (en) * | 1990-08-02 | 1993-03-23 | Fujitsu Limited | Laser diode current supply including a threshold current component subject to automatic power control |
| EP0774684A3 (en) * | 1995-11-16 | 1998-04-22 | Matsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
| US5960259A (en) * | 1995-11-16 | 1999-09-28 | Matsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5940333A (en) * | 1982-08-31 | 1984-03-06 | Toshiba Corp | Disk record reproducer |
| JPS59186143A (en) * | 1983-04-06 | 1984-10-22 | Toshiba Corp | Optical disc device |
| JPS59191149A (en) * | 1983-04-14 | 1984-10-30 | Sanyo Electric Co Ltd | Mechanism for controlling optical record |
-
1984
- 1984-04-09 JP JP59070628A patent/JPH07118084B2/en not_active Expired - Lifetime
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5940333A (en) * | 1982-08-31 | 1984-03-06 | Toshiba Corp | Disk record reproducer |
| JPS59186143A (en) * | 1983-04-06 | 1984-10-22 | Toshiba Corp | Optical disc device |
| JPS59191149A (en) * | 1983-04-14 | 1984-10-30 | Sanyo Electric Co Ltd | Mechanism for controlling optical record |
Cited By (13)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61142538A (en) * | 1984-12-13 | 1986-06-30 | Matsushita Electric Ind Co Ltd | Optical information recording and reproducing device |
| JPS61230626A (en) * | 1985-04-05 | 1986-10-14 | Matsushita Electric Ind Co Ltd | How to play optical information media |
| JPS62101125U (en) * | 1985-12-16 | 1987-06-27 | ||
| JPH02235224A (en) * | 1989-03-08 | 1990-09-18 | Fujitsu Ltd | Projection power control system for optical disk device |
| US5197059A (en) * | 1990-08-02 | 1993-03-23 | Fujitsu Limited | Laser diode current supply including a threshold current component subject to automatic power control |
| EP0774684A3 (en) * | 1995-11-16 | 1998-04-22 | Matsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
| US5835650A (en) * | 1995-11-16 | 1998-11-10 | Matsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
| US5960259A (en) * | 1995-11-16 | 1999-09-28 | Matsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
| US6067393A (en) * | 1995-11-16 | 2000-05-23 | Matsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
| US6069904A (en) * | 1995-11-16 | 2000-05-30 | Matsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
| US6298075B1 (en) | 1995-11-16 | 2001-10-02 | Matsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
| US6590915B1 (en) | 1995-11-16 | 2003-07-08 | Matsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
| US7133428B2 (en) | 1995-11-16 | 2006-11-07 | Mmatsushita Electric Industrial Co., Ltd. | Optical apparatus and method for producing the same |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH07118084B2 (en) | 1995-12-18 |
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| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |