JPH02137132A - Reproducing device for optical recording medium - Google Patents

Reproducing device for optical recording medium

Info

Publication number
JPH02137132A
JPH02137132A JP63289806A JP28980688A JPH02137132A JP H02137132 A JPH02137132 A JP H02137132A JP 63289806 A JP63289806 A JP 63289806A JP 28980688 A JP28980688 A JP 28980688A JP H02137132 A JPH02137132 A JP H02137132A
Authority
JP
Japan
Prior art keywords
recording medium
laser diode
optical recording
light
beam splitter
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
JP63289806A
Other languages
Japanese (ja)
Inventor
Hideyoshi Horigome
秀嘉 堀米
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP63289806A priority Critical patent/JPH02137132A/en
Publication of JPH02137132A publication Critical patent/JPH02137132A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To improve the degree of modulation by providing a beam splitter between an optical recording medium and a laser diode and detecting reflected light obtained through the beam splitter. CONSTITUTION:A laser light beam from the end face 11a of a laser diode 11 is reflected by the optical recording medium 20 through a lens 12, the beam splitter 13 and a lens 14. A part of the reflected light is separated by the beam splitter 13 through the lens 14 and enters a photodetector 16 through a lens 15. By detecting the change of the intensity of the separated light, the presence or absence of the pit of the optical recording medium 20 is read. Meanwhile, the rest of the light which passes through the beam splitter 13 is fed back to the end face 11a of the laser diode 11 through the lens 12. Self combining effect is generated in the laser diode 11 with the light which is fed back and the light output of the laser diode is increased. Thus, the degree of modulation is improved.

Description

【発明の詳細な説明】 (産業上の利用分野〕 本発明は、所謂自己結合型光学ピックアップを利用した
光記録媒体の再生装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an optical recording medium reproducing apparatus using a so-called self-coupling optical pickup.

〔発明の概要〕[Summary of the invention]

〔従来の技術〕 コンパクトディスクや光学ビデオディスク等の光学記録
媒体(ディスク)20は第3図に示すように、例えばポ
リカーボネイトから成る基板21の表面に所謂ピット2
2と呼ばれる一連の凹部が同心円状あるいは渦巻き状の
トラックに設けられており、ここに音楽等の情報がディ
ジタルデータとして記録されている。該光学記録媒体2
0は全面にわたってアルミニウムが蒸着されて反射膜2
3が形成されている。上記ピット22の深さはレーザ光
の波長の1/4に設定されており、レーザ光を上記光学
記録媒体に照射し、上記反射膜23で反射させ、該ピッ
ト22で起こる回折現象を利用し、光検出器で反射光の
強度変化を検出することで上記ディジタルデータが読み
取られ再生される。
[Prior Art] As shown in FIG. 3, an optical recording medium (disc) 20 such as a compact disc or an optical video disc has so-called pits 2 on the surface of a substrate 21 made of, for example, polycarbonate.
A series of recesses called 2 are provided in a concentric or spiral track, and information such as music is recorded here as digital data. The optical recording medium 2
0 is a reflective film 2 with aluminum vapor-deposited over the entire surface.
3 is formed. The depth of the pit 22 is set to 1/4 of the wavelength of the laser beam, and the laser beam is irradiated onto the optical recording medium, reflected by the reflective film 23, and the diffraction phenomenon occurring in the pit 22 is utilized. The digital data is read and reproduced by detecting changes in the intensity of the reflected light with a photodetector.

上記の光学記録媒体の再生装置の読み取りのための光ピ
ツクアップは第4図に示すように、光源としてのレーザ
ダイオード31と、レーザビームの直線偏光を円偏光に
変換するための1/4波長板32と、光学記録媒体から
の反射光を分離するためのビームスプリッタ33と、該
ビームスブリック33で分離された反射光学記録媒体を
検出するPINホトダイオード等の光検出器34と、シ
リンドリカルレンズ等の各種レンズ35.36.37と
から構成されている。上記光検出器34は光学記録媒体
上のピットの有無によって生じた反射光の強度変化を検
出し、光学記録媒体上に記録されているデータを読み取
ると共に、レーザビームのスポットが常に光学記録媒体
のトラック上に結像するように制御するための、所謂フ
ォーカシング及びトラッキング用信号の検出機能も有し
ている。
As shown in FIG. 4, the optical pickup for reading the optical recording medium reproducing apparatus described above includes a laser diode 31 as a light source and a quarter-wave plate for converting the linearly polarized light of the laser beam into circularly polarized light. 32, a beam splitter 33 for separating the reflected light from the optical recording medium, a photodetector 34 such as a PIN photodiode for detecting the reflected optical recording medium separated by the beam subrick 33, and various types such as a cylindrical lens. It is composed of lenses 35, 36, and 37. The photodetector 34 detects changes in the intensity of reflected light caused by the presence or absence of pits on the optical recording medium, and reads the data recorded on the optical recording medium. It also has a so-called focusing and tracking signal detection function for controlling the image formation on the track.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

ところで、上述のように形成されたピントを再生する場
合、光学系のレスポンス関数(OTF:0ptical
 Transfer Function)の絶対値(M
TF : Modulation transfer 
function)は第5図に示すようにピットの記録
密度が高くなると低下し、最後に零となる。これはピッ
トが小さくなると該ピットでの回折が大きくなり光検出
器への反射光が減少し、最後には該反射光が光学系の経
路から外れてしまい、ピットの読み取りができなくなる
ために起こるものである。すなわち、上記MTFは当該
光学記録媒体の記録密度の限界を表す一つの尺度である
。例えば一般の光学記録媒体の記録密度は該MTF値が
例えば約0.5以上の範囲が使用されている。
By the way, when reproducing the focus formed as described above, the response function of the optical system (OTF: 0ptical
Absolute value (M
TF: Modulation transfer
As shown in FIG. 5, the function) decreases as the recording density of the pits increases, and finally reaches zero. This happens because when the pit becomes smaller, the diffraction at the pit increases and the reflected light to the photodetector decreases, and eventually the reflected light deviates from the path of the optical system, making it impossible to read the pit. It is something. That is, the MTF is one measure representing the limit of the recording density of the optical recording medium. For example, the recording density of general optical recording media is such that the MTF value is, for example, about 0.5 or more.

ところで、上述の光学記録媒体は所定の角速度で回転さ
れている。このためディスクのピットは円周方向に対し
て外周になるほど長く、逆に内周になるほど短く形成さ
れている。換言すると、第5図に示すように内周になる
ほどピットが高密度で形成されおり、角速度一定で回転
される光学記録媒体の記録密度は内周のピットの大きさ
によって決定されることになる。
By the way, the above-mentioned optical recording medium is rotated at a predetermined angular velocity. For this reason, the pits of the disk are formed to be longer toward the outer circumference in the circumferential direction, and conversely to become shorter toward the inner circumference. In other words, as shown in Figure 5, the pits are formed at a higher density toward the inner periphery, and the recording density of an optical recording medium that is rotated at a constant angular velocity is determined by the size of the pits on the inner periphery. .

上述の技術は、再生時のレーザダイオードの出力が一定
であるために、上述のようにピットの長さが短くなると
MTFが低下して再生特性、例えばC/ N (Car
ier to No1se Ratio)が急激に低下
する。
In the above technology, since the output of the laser diode during reproduction is constant, when the length of the pit becomes shorter as described above, the MTF decreases and the reproduction characteristics, for example, C/N (Car
ier to No. 1se Ratio) decreases rapidly.

なお、上記MTFを向上させる方法として、対物レンズ
の開口数(N A : Numerical Aper
ture)をより大きくする方法、またはレーザ光の波
長をより短くする方法がある。しかしNAを大きくする
と、焦点深度が浅くなる、光軸の傾きによる収差量が大
きくなる、高価格になる等の弊害が生じる。また、レー
ザダイオードの短波長化には技術的に限界がある。した
がって別な方法での変調度改善が必要である。
Note that as a method for improving the MTF, the numerical aperture (NA: Numerical Aper.
There is a method of making the wavelength of the laser beam larger or a method of making the wavelength of the laser beam shorter. However, increasing the NA causes disadvantages such as the depth of focus becomes shallow, the amount of aberration due to the inclination of the optical axis increases, and the price increases. Furthermore, there is a technical limit to shortening the wavelength of a laser diode. Therefore, it is necessary to improve the modulation depth using another method.

ところで、光学ピックアップとしては、小型軽量化の要
望が強く、この要望に応じてレーザダイオードの自己結
合効果を利用した所謂自己結合型光学ピックアップ(S
 COOP : 5elf Coupled 0pti
cal Pickup)が知られている。該5COOP
の構成を第6図に示す。該5coopは、光学記録媒体
20で反射されたレーザビームをレーザダイオード41
に積極的に返し、該光学記録媒体20とレーザダイオー
ド41で構成される外部共振器で外部共振状態を起こし
、レーザダイオード41の後方に設けられた光検出器4
2でこの共振状態の変化、すなわちレーザダイオード4
1の後方光出力強度変化を検出することによって、上述
の光ピツクアップと同様に光学記録媒体上に記録されて
いるデータを読み取るようにしたものである。
By the way, there is a strong demand for smaller and lighter optical pickups, and in response to this demand, so-called self-coupled optical pickups (S
COOP: 5elf Coupled 0pti
cal Pickup) is known. The 5 COOP
The configuration is shown in FIG. The 5coop converts the laser beam reflected by the optical recording medium 20 into a laser diode 41.
The external resonator formed by the optical recording medium 20 and the laser diode 41 generates an external resonance state, and the photodetector 4 provided behind the laser diode 41 generates an external resonance state.
2, this change in resonance state, that is, the laser diode 4
By detecting the change in the rear light output intensity of No. 1, the data recorded on the optical recording medium is read in the same manner as the above-mentioned optical pickup.

この技術によれば、レーザダイオードの後方出力を検出
するために、上記のサーボ制御用の信号検出ができず、
別の検出手段を設ける必要がある。
According to this technology, since the rear output of the laser diode is detected, the above-mentioned servo control signal detection cannot be performed.
It is necessary to provide another detection means.

そこで、本発明は、上述の如き従来の問題点に鑑み、メ
調度を改善することのできる光学記録媒体の再生装置を
提供することを目的とするものである。
SUMMARY OF THE INVENTION In view of the above-mentioned conventional problems, it is an object of the present invention to provide an optical recording medium reproducing apparatus that can improve the quality of playback.

〔課題を解決するための手段〕[Means to solve the problem]

本発明は、上述の!IBを解決するために、レーザダイ
オードからの光を光学記録媒体に照射し該照射光の反射
光を上記レーザダイオードに戻す光学系を有し、上記反
射光の一部を取り出すビームスプリッタを上記光学記録
媒体とレーザダイオードの間に設け、該ビームスプリッ
タを介して得られる反射光を検出する光検出器からなる
ことを特徴とするものである。
The present invention is based on the above! In order to solve IB, an optical system is provided that irradiates light from a laser diode onto an optical recording medium and returns the reflected light of the irradiated light to the laser diode, and a beam splitter that takes out a part of the reflected light is connected to the optical system. It is characterized by comprising a photodetector that is provided between the recording medium and the laser diode and detects reflected light obtained through the beam splitter.

〔作 用〕[For production]

かかる構成によれば、光学記録媒体上のピットの有無に
よる光学記録媒体からの反射光の強度変化が、レーザダ
イオードの自己結合効果によって強調され、変調度が改
善される。
According to this configuration, changes in the intensity of reflected light from the optical recording medium due to the presence or absence of pits on the optical recording medium are emphasized by the self-coupling effect of the laser diode, and the degree of modulation is improved.

〔実施例〕〔Example〕

以下、本発明に係る光学記録媒体の再生装置の一実施例
について図面を参照しながら説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of an optical recording medium reproducing apparatus according to the present invention will be described below with reference to the drawings.

本発明の実施例となる光学ピックアップの構成を第1図
に示す。この第1図において、レーザダイオード11の
端面11aからのレーザ光はレンズ12、ビームスプリ
ッタ13及びレンズ14を介して、光学記録媒体20で
反射される。この反射光は上記レンズ14を介して、上
記ビームスプリッタ13で一部の光が分離されレンズ1
5を介して光検出器16に入り、この分離された光の強
度変化を検出することで光学記録媒体のピットの有無を
読み取る。一方上記ビームスプリック13を通過した残
りの光はレンズ12を介してレーザダイオード11の当
該端面11aに帰還される。
FIG. 1 shows the configuration of an optical pickup according to an embodiment of the present invention. In FIG. 1, laser light from an end face 11a of a laser diode 11 is reflected by an optical recording medium 20 via a lens 12, a beam splitter 13, and a lens 14. This reflected light passes through the lens 14, and a part of the light is separated by the beam splitter 13, and the lens 1
The separated light enters the photodetector 16 via the light beam 5, and detects the change in intensity of the separated light to read the presence or absence of pits in the optical recording medium. On the other hand, the remaining light that has passed through the beam sprick 13 is returned to the end surface 11a of the laser diode 11 via the lens 12.

この帰還された光でレーザダイオード11に自己結合効
果が発生し、同じ駆動電流であっても自己結合効果が無
い場合に比較してレーザダイオードの光出力は増大する
This feedback light causes a self-coupling effect in the laser diode 11, and even with the same drive current, the optical output of the laser diode increases compared to a case where there is no self-coupling effect.

第2図はレーザダイオードへの戻り光をパラメータとし
た場合のレーザダイオードの駆動11流光出力特性を示
す。上述のように、光学記録媒体の反射率はピットの有
無によって、高(rl)、低(r2)の2値となるため
、本実施例の駆動電流−出力特性は第2図に示すように
、戻り光が大(ピットが無く、光学記録媒体の反射率が
高い)の場合の曲線A、と戻り光が小(ピットが有り、
光学記録媒体の反射率が低い)の場合の曲線A2の2本
の曲線で表される。なお曲線A0はレーザダイオードへ
の戻り光が無い場合の駆動電流−出力特性を示す、すな
わち、レーザダイオードへの戻り光が大になるほどレー
ザダイオードの出力が大になる。
FIG. 2 shows the light output characteristics of the laser diode drive 11 when the return light to the laser diode is used as a parameter. As mentioned above, the reflectance of an optical recording medium has two values, high (rl) and low (r2), depending on the presence or absence of pits, so the drive current-output characteristics of this example are as shown in Figure 2. , curve A when the returned light is large (no pits, high reflectance of the optical recording medium), and curve A when the returned light is small (with pits,
It is represented by two curves, curve A2 in the case where the reflectance of the optical recording medium is low). Note that the curve A0 shows the drive current-output characteristic when there is no light returning to the laser diode, that is, the larger the light returning to the laser diode, the larger the output of the laser diode.

例えば一定の駆動電流■に対してピットが無い場合には
レーザダイオードの光出力はり、となり、ピットがある
場合にはレーザダイオードの光出力はL2となる。この
レーザダイオード出力の変化が光学記録媒体で反射され
、上記のビームスプリッタを介して光検出器において検
出される。この結果、自己結合効果が無い場合に検出さ
れる光の強弱の幅よりも、上記のような自己結合効果が
有る場合に検出される光の強弱の幅、が大になり、換言
するとピットの有無によって生じる光の強弱の比率が大
になり、ピットの有無の判別が余裕を持ってできること
となる。すなわちピットが無い場合の光学記録媒体での
反射光は、ピットがある場合の反射光よりも自己結合効
果によって、より強められ結果となり、上述の変調度が
改善される。
For example, for a constant drive current (2), if there are no pits, the optical output of the laser diode will be L2, and if there are pits, the optical output of the laser diode will be L2. This change in laser diode output is reflected by the optical recording medium and detected by the photodetector via the beam splitter. As a result, the width of the intensity of light detected when there is a self-coupling effect as described above becomes larger than the width of the intensity of light detected when there is no self-coupling effect. The ratio of the intensity of light caused by the presence or absence of pits becomes large, and the presence or absence of pits can be determined with ample margin. In other words, the reflected light on the optical recording medium without pits is stronger due to the self-coupling effect than the reflected light in the presence of pits, and the above-mentioned degree of modulation is improved.

また、上述のC/Nは、ノイズ成分は一定であって、信
号成分のみがレーザダイオードの自己結合効果によって
増大する結果良好なものとなる。
Further, the above-mentioned C/N is good because the noise component is constant and only the signal component increases due to the self-coupling effect of the laser diode.

なお、上記の光検出器の内部に、例えば所謂3ビーム法
等のトラッキング用の信号検出機能と、シリンドリカル
レンズを用いた非点収差によるフォーカシング用の信号
検出機能を設けることにより、トラッキングサーボ制御
及びフォーカシングサーボ制御が一つの光学系で可能と
なる。
Note that by providing a signal detection function for tracking such as the so-called three-beam method and a signal detection function for focusing using astigmatism using a cylindrical lens inside the photodetector, tracking servo control and Focusing servo control is possible with a single optical system.

なお、本件発明者が既に提案した特願昭63−5597
6号の明細書及び図面において開示された光学記録媒体
の再生装置に本発明を適用することによ。てレーザダイ
オードの雑音を抑圧したデータ読み取りが可能となる。
In addition, the patent application No. 63-5597 already proposed by the inventor of the present invention
By applying the present invention to the optical recording medium reproducing apparatus disclosed in the specification and drawings of No. 6. This makes it possible to read data while suppressing laser diode noise.

すなわち、第1図に示すレーザダイオード11の駆動回
路内にパルス発生器を設け、レーザ光の1回の照射時間
を上記光学記録媒体20からの反射光による誘起振動の
基本周期よりも短く設定して、上記レーザ光を所定の周
期で断続することによって、レーザダイオードの雑音を
抑圧したデータ読み取りが可能となる。
That is, a pulse generator is provided in the drive circuit of the laser diode 11 shown in FIG. By interrupting the laser beam at a predetermined period, it becomes possible to read data while suppressing the noise of the laser diode.

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

第1図は本発明に係る再生装置の一実施例の構成を示す
模式図、第2図はレーザダイオードの駆動電流−光出力
特性図、第3図は光学記録媒体の要部の構成を示す模式
図、第4図は従来の再生装置の光学ピックアップの模式
図、第5図は光学記録媒体の変調度特性図、第6図は他
の従来の再生装置の光学ピックアップの模式図である。 11・・・レーザダイオード 13・・・ビームスプリッタ 16・・・光検出器 20・・・光学記録媒体 (発明の効果〕 上述の実施例の説明からも明らかのように、本発明によ
れば、レーザダイオードの自己結合効果を有効に利用す
ることによって、再生性能が良好でかつ小型軽量な光ピ
ツクアップを提供ができる。
Fig. 1 is a schematic diagram showing the configuration of an embodiment of a reproducing device according to the present invention, Fig. 2 is a drive current-light output characteristic diagram of a laser diode, and Fig. 3 is a diagram showing the configuration of the main parts of an optical recording medium. 4 is a schematic diagram of an optical pickup of a conventional reproducing apparatus, FIG. 5 is a diagram of modulation degree characteristics of an optical recording medium, and FIG. 6 is a schematic diagram of an optical pickup of another conventional reproducing apparatus. 11...Laser diode 13...Beam splitter 16...Photodetector 20...Optical recording medium (Effects of the invention) As is clear from the description of the above embodiments, according to the present invention, By effectively utilizing the self-coupling effect of a laser diode, it is possible to provide a compact and lightweight optical pickup with good reproduction performance.

Claims (1)

【特許請求の範囲】[Claims] レーザダイオードからの光を光学記録媒体に照射し該照
射光の反射光を上記レーザダイオードに戻す光学系を有
し、上記反射光の一部を取り出すビームスプリッタを上
記光学記録媒体とレーザダイオードの間に設け、該ビー
ムスプリッタを介して得られる反射光を検出する光検出
器からなることを特徴とする光学記録媒体の再生装置。
It has an optical system that irradiates light from a laser diode onto an optical recording medium and returns reflected light of the irradiated light to the laser diode, and a beam splitter that takes out a part of the reflected light is provided between the optical recording medium and the laser diode. 1. A reproducing apparatus for an optical recording medium, comprising a photodetector provided in the beam splitter for detecting reflected light obtained through the beam splitter.
JP63289806A 1988-11-16 1988-11-16 Reproducing device for optical recording medium Pending JPH02137132A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63289806A JPH02137132A (en) 1988-11-16 1988-11-16 Reproducing device for optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63289806A JPH02137132A (en) 1988-11-16 1988-11-16 Reproducing device for optical recording medium

Publications (1)

Publication Number Publication Date
JPH02137132A true JPH02137132A (en) 1990-05-25

Family

ID=17748009

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63289806A Pending JPH02137132A (en) 1988-11-16 1988-11-16 Reproducing device for optical recording medium

Country Status (1)

Country Link
JP (1) JPH02137132A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58125245A (en) * 1982-01-22 1983-07-26 Hitachi Ltd Optical pickup device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58125245A (en) * 1982-01-22 1983-07-26 Hitachi Ltd Optical pickup device

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