JPS6142737A - Optical disk device - Google Patents

Optical disk device

Info

Publication number
JPS6142737A
JPS6142737A JP59164447A JP16444784A JPS6142737A JP S6142737 A JPS6142737 A JP S6142737A JP 59164447 A JP59164447 A JP 59164447A JP 16444784 A JP16444784 A JP 16444784A JP S6142737 A JPS6142737 A JP S6142737A
Authority
JP
Japan
Prior art keywords
energy
energy value
value
optical disk
waveform
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
JP59164447A
Other languages
Japanese (ja)
Inventor
Takeyoshi Koi
児井 武義
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
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 NEC Corp filed Critical NEC Corp
Priority to JP59164447A priority Critical patent/JPS6142737A/en
Publication of JPS6142737A publication Critical patent/JPS6142737A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording 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
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/125Optical 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
    • G11B7/126Circuits, methods or arrangements for laser control or stabilisation
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording 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
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/2407Tracks or pits; Shape, structure or physical properties thereof
    • G11B7/24085Pits

Landscapes

  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Recording Or Reproduction (AREA)

Abstract

PURPOSE:To obtain the optical disk device which is increased in storage capacity by increasing the bit density without causing any mutual interference of the output waveform of a playback signal even when bit intervals are narrowed down by allowing the waveform of write laser light to have a specific standard energy value at a leading and a trailing edge part. CONSTITUTION:A write signal 22 forms a bit 23 by irradiating an optical disk with laser light 22a having higher energy than readout laser light 22c having low energy. The waveform of the write signal 22 is not rectangular, but held at the 1st energy write signal 22 is not rectangular, but held at the 1st energy standard (22a) for a short time and then decreases monotonously to an energy value of a standard 22b in the middle between the 1st standard and the 2nd standard (22c). Therefore, the bit 23 has a semicircular part as the left half and a part thinner than a semicircle as the right half. Consequently, the output waveform of the playback signal has no mutual interference even when the bit density is increased, so the storage capacity can be increased.

Description

【発明の詳細な説明】 〔技術分野〕 不兄男に光ディスク装置に関し、特に光ヘッドから高エ
ネルギー値のレーザ光全照射することによって光ディス
ク上にピット6形成し、同一光学ヘッドから低エネルギ
ー値のレーザ光を照射してビットからの反射光を検出す
ることによって情報の書込みおよび読出しを行う構成を
有する光ディスフ装置に関する。
[Detailed Description of the Invention] [Technical Field] Regarding optical disk devices, in particular, pits 6 are formed on an optical disk by full irradiation of high-energy laser beams from an optical head, and low-energy laser beams are formed from the same optical head. The present invention relates to an optical disc device having a configuration for writing and reading information by irradiating laser light and detecting reflected light from bits.

〔従来技術〕[Prior art]

従来の書込み可能な光ディスク装置において情報を光デ
ィスク上に書込む場合に、高エネルギーのレーザ光を光
学レンズで極小のスボ、トに収斂して光ディスク上に照
射し、光ディスクの記憶媒体に溶融等の光学的状態変化
を生せしめることによってピットと呼ばれる穴状部分を
形成して情報を記録し、このど、トに対して読出し用の
低エネルギーのレーザを照射してその反射光を検知する
ことによって記録された情報の読出しを行5ように構成
されている。
When writing information onto an optical disk in a conventional writable optical disk device, a high-energy laser beam is focused onto the optical disk using an optical lens and is applied to the optical disk to cause melting or other damage to the storage medium of the optical disk. Information is recorded by forming a hole-like part called a pit by causing an optical state change, and then by irradiating the pit with a low-energy laser for reading and detecting the reflected light. The recorded information is read out in row 5.

このときのピットの形状は、第1図(a)t7tは(b
)に示すように、書込み用のレーザ光の波形を制御する
ことに工つて円形または長円形に形成され。
The shape of the pit at this time is as shown in Fig. 1 (a) t7t is (b
), it is formed into a circular or oval shape by controlling the waveform of the laser beam for writing.

これに対して情報の読出しは1円形ビットの場合はその
再生信号の出力波形のピーク点を、iた長円形ピットの
場合は再生信号の出力波形の幅を検出することによって
行われる。
On the other hand, information is read by detecting the peak point of the output waveform of the reproduced signal in the case of one circular bit, and by detecting the width of the output waveform of the reproduced signal in the case of i oblong pits.

従って第1図(a)に例示する円形ピットの場合な。Therefore, in the case of the circular pit illustrated in FIG. 1(a).

書込み信号2によって形成されるピット3の間隔が一定
値より小さくなると、読出し用のレーザ光の波長が一定
であり従ってそのビーム径が一定であるため、再生i号
4に相互干渉が生じ(参照符号4b)、この再生信号4
と整形して得られる読出し情報信号5は誤り比信号とな
ることがめり。
When the interval between the pits 3 formed by the write signal 2 becomes smaller than a certain value, the wavelength of the reading laser beam is constant, and therefore the beam diameter is constant, so mutual interference occurs in the reproduction number I 4 (see 4b), this reproduced signal 4
The read information signal 5 obtained by shaping the signal is likely to be an error ratio signal.

従ってピット間の間隔を一定値以下にすることができな
いという欠点を有している。
Therefore, it has the disadvantage that the distance between the pits cannot be kept below a certain value.

また、第1図tb)に例示する長円形ピットの場合は、
ピット13の外形全形成する半円形の前縁部分および後
縁部分(エラジンの形状が不規則となる(レーザ光によ
る加熱のため記憶媒体が溶融されるとき、エツジ部分は
幾何学的な正しい半円形とにならず凹凸のある不規則な
形状となる)ため。
In addition, in the case of the oval pit illustrated in Figure 1 tb),
The semicircular leading and trailing edge portions that form the entire outer shape of the pit 13 (the shape of the elagin becomes irregular (when the storage medium is melted due to heating by laser light, the edge portion is shaped into a geometrically correct half). (It is not circular but has an irregular shape with uneven surfaces.)

このようなピット13からの再生信号14の出力波形は
第1図(b)の参照符号14′として点扉で例示する:
りに、−正規の位置からずれた波形となる。
The output waveform of the reproduced signal 14 from such a pit 13 is illustrated with a dot as reference numeral 14' in FIG. 1(b):
In other words, - the waveform deviates from the normal position.

このずれが大きくなると、再生信号の出力波形を整形し
て矩形波形とした読出し情報信号15の立上りおよび立
下りが読出しタイミングパルス16の正規のパルス位置
で正しく検出されない(すなわち読出し情報信号15の
幅Tが変化する)ことがあり、このため安定した情報の
読出しができないという欠点がある。
If this deviation becomes large, the rise and fall of the readout information signal 15, which has been shaped into a rectangular waveform by shaping the output waveform of the reproduced signal, will not be detected correctly at the regular pulse position of the readout timing pulse 16 (i.e., the width of the readout information signal 15). Therefore, there is a drawback that stable reading of information is not possible.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、上記の従来の技術の欠点を改良して、
ピット間隔を狭くしても再生信号の出力波形に相互干渉
が生じず、従りてピット密度を高くして同−元ディスク
の情報の記憶容量を増大させることのできる光ディスク
装置を提供することにある。
The purpose of the present invention is to improve the drawbacks of the above-mentioned conventional techniques, and
To provide an optical disc device that does not cause mutual interference in the output waveform of reproduced signals even when the pit interval is narrowed, and can therefore increase the pit density and increase the information storage capacity of the same original disc. be.

〔発明の構成〕[Structure of the invention]

本発明の光ディスク製置は、光学ヘッドから第一のエネ
ルギー水準のレーザ光を照射することによって光ディス
ク上にピットを形成し、前記光学ヘッドから前記第一の
エネルギー水準のエネルギー値より低いエネル“ギー値
の第二のエネルギー水準のレーザ先金前記光ディスクに
照射して前記ピットからの反射光を検知することに工っ
て情報の書込みおよび読出しを行う光ディスク装置にシ
いて、前記第一のエネルギー水準のレーザ光の信号波形
がその前縁部において高水準の第一のエネルギー値を有
し、かつその後縁部において前記第一のエネルギー値と
前記第二のエネルギー水準のエネルギー値との中間の値
を有する第二のエネルギー値を有し、前記第一のエネル
ギー値から前記第二のエネルギー値まで二次曲線に近似
する曲線または少くとも1段の階段状の形状に沿って減
少させるか、または前記第一のエネルギー水準のレーザ
光の信号波形が、その前縁部において前記第一のエネル
ギー値と前記第二のエネルギー水準のエネルギー値の中
間の値を有する第二のエネルギー値を有し、かつその後
縁部において高水準の第一のエネルギー値を有し、前記
第二のエネルギー値から前記第一のエネルギー値まで二
次曲線に近似する曲線または少くとも1段の階段状の形
状に沿って増大させて構成される。
In the optical disk manufacturing method of the present invention, pits are formed on the optical disk by irradiating a laser beam of a first energy level from an optical head, and an energy value lower than the energy value of the first energy level is emitted from the optical head. In an optical disc device that writes and reads information by irradiating the optical disc with a laser tip at a second energy level of a value and detecting light reflected from the pit, the laser tip has a second energy level. The signal waveform of the laser beam has a high level first energy value at its leading edge, and has a value intermediate between the first energy value and the second energy level energy value at the trailing edge. and decreases from the first energy value to the second energy value along a curve approximating a quadratic curve or at least one step-like shape, or the signal waveform of the laser beam at the first energy level has a second energy value at its leading edge having an intermediate value between the first energy value and the energy value at the second energy level; and has a first energy value at a high level at its rear edge, and extends from the second energy value to the first energy value along a curve approximating a quadratic curve or at least one step-like shape. It is configured by increasing the

〔実施例〕〔Example〕

以下1本発明について実施例を示す図面全参照して詳細
に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described in detail below with reference to all the drawings showing embodiments.

第2図は本発明の一実施例の書込み信号波形と。FIG. 2 shows a write signal waveform according to an embodiment of the present invention.

それによって形成される媒体上のビットの形状およびそ
のビットからの反射光によって生成される再生信号なら
びにこの再生信号を整形して矩形波とした読出し情報信
号の波形とt−読出しタイミングパルスと共に示した図
面である。
The shape of the bit on the medium formed thereby, the reproduced signal generated by the reflected light from the bit, the waveform of the read information signal that has been shaped into a rectangular wave, and the t-read timing pulse. It is a drawing.

図に示すエフに1本実施例の書込み信号22は、参照符
号22cで示す低エネルギー値(以下これ全第二のエネ
ルギー水準と称する)の読出し用レーザ光に対して参照
符号22aで示す高エネルギー([(以下第一のエネル
ギー水準と称する)のレーザ光を光ディスクに照射する
ことによってピット23を形成するが、このときの書込
み信号22の波形は従来のような矩形波(第1図参照)
と異りて、第一エネルギー水準の値に短時間保持された
のち参照符号22bで示すような第一および第二のエネ
ルギー水準の中間の大きさのエネルギー値まで、2次曲
線唸たはOれに近似した曲線に沿って単調に減少する形
状を有している。なお図において参照符号2Zdはエネ
ルギー値Oのレベル?示している(第1図および第3図
も同じ)。
The write signal 22 of this embodiment shown in FIG. (The pits 23 are formed by irradiating the optical disc with a laser beam of (hereinafter referred to as the first energy level), but the waveform of the write signal 22 at this time is a conventional rectangular wave (see Fig. 1).
, the quadratic curve curve O It has a shape that decreases monotonically along a curve that approximates this. In the figure, reference symbol 2Zd is the level of energy value O? (The same applies to Figures 1 and 3).

このような舊込み信号波形金有するレーザ光の照射によ
って形成されるビット23の形状は、轟然に第1図(a
)に示す従来の円形と異った形状となる。すなわち、ビ
ットの左手分はほぼ半円形となるが、右半分は半円形を
形成するのに充分なエネルギーが供給されていないため
半円形りりやせ細って参照符号23aに示す工うな三角
形に近似した形状となる。
The shape of the bit 23 formed by irradiation with laser light having such a cutting signal waveform is dramatically similar to that shown in FIG.
) The shape is different from the conventional circular shape shown in ). In other words, the left hand portion of the bit is approximately semicircular, but the right half is not supplied with enough energy to form a semicircle, so the semicircular shape becomes thinner and thinner, resulting in a shape that approximates the rough triangle shown by reference numeral 23a. becomes.

従ってこの工うな異形のビットからの反射光による再生
信号24の波形は、従来のような円形のビットからの波
形に比してその後半の出力値が急速に減少しく参照符号
24a)、前半と後半とが非対象な形状金有する波形と
なる。この几め2個のピットが近接したとき、この2個
のピットからの再生信号24の出力波形の相互干渉は、
従来のもの(第1図(a)参照符号4b)に比して小さ
くな〕、第2図参照符号24bの如くなる。従ってこの
再生信号24を整形して矩形波とした読出し情報信号2
5は上記の近接し九2個のビットのそれぞれに対応した
独立の矩形波となって正しい読出し動作が行われるため
、2個のビットの近接距離全従来に比して短くすること
が可能となフ、その分だけ情報の記憶密度を高めること
ができる。
Therefore, in the waveform of the reproduced signal 24 caused by the reflected light from this oddly shaped bit, the output value in the latter half decreases rapidly compared to the waveform from the conventional circular bit. The second half is a waveform with an asymmetrical shape. When these two pits are close to each other, the mutual interference between the output waveforms of the reproduced signal 24 from these two pits is as follows:
It is smaller than the conventional one (see reference numeral 4b in FIG. 1(a)), as shown in FIG. 2, reference numeral 24b. Therefore, the readout information signal 2 is shaped into a rectangular wave by shaping the reproduced signal 24.
5 becomes an independent rectangular wave corresponding to each of the 92 adjacent bits mentioned above, and a correct read operation is performed, so it is possible to shorten the distance between two bits compared to the conventional method. Therefore, the storage density of information can be increased accordingly.

書込み信号の波形は1M2図に示すような単調な曲線に
沿って減少するものの外に、第3図に示すような各種の
階段状の形状に沿って減少するように構成することもで
きる。すなわち、第3図(a)は2段の階段状に、第2
図tb)に3段の階段状に順次減少する場合金示し、第
3図(C)は中間が最終段ニジ低い特殊の形状の場合を
示してbる。これらのいずれの場合も、媒体上に形成さ
れるビットの形状は第2図の場合と酷似した形状となる
のでその動作および作用は上記の説明と全く同様である
The waveform of the write signal may be configured not only to decrease along a monotonous curve as shown in FIG. 1M2 but also to decrease along various step-like shapes as shown in FIG. In other words, in FIG. 3(a), the second
Fig. 3 (b) shows a case in which the number decreases sequentially in a stepwise manner with three steps, and Fig. 3 (C) shows a case in which the intermediate part is a special shape that is lower than the final step. In any of these cases, the shape of the bit formed on the medium is very similar to that shown in FIG. 2, and its operation and effect are exactly the same as described above.

なお、上述の実施例はすべて書き込み信号の波形が、前
縁部において高水準のエネルギー値を有し、後縁部にお
いて中間の大きさのエネルギー値を有する場合金示した
が、この関係を反転させて。
Note that all of the above embodiments show cases where the write signal waveform has a high level energy value at the leading edge and an intermediate level energy value at the trailing edge, but this relationship can be reversed. Let me.

前縁部において中間の大きさのエネルギー値とし。An energy value of intermediate magnitude at the leading edge.

後縁部において高水準のエネルギー値とし、この間を2
次曲線またはこれに近似するFtfI線に沿って単調に
増大させるか、あるいは少くとも1段の階段上の形状に
沿りて増大させるよう構成することによって、前述の実
施例と全く同様の作用および効果が得られる。
The energy value is at a high level at the trailing edge, and 2
By configuring the structure to increase monotonically along a curve of Effects can be obtained.

〔発明の効果〕〔Effect of the invention〕

以上詳細に説明したように1本発明の光ディスク装置を
用いることによシ、媒体上のビ、ト間隔を従来に比して
狭めることができるため、同一寸法の光ディスクを用い
て情報の記憶容量の大きな光ディスク装置が得られると
いう効果がある。
As explained in detail above, by using the optical disk device of the present invention, the bit spacing on the medium can be narrowed compared to the conventional one, so that the information storage capacity can be reduced using an optical disk of the same size. This has the effect that a large optical disk device can be obtained.

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

第1図(a)お工び(b)は1円形および長円形ビット
を形成する場合の従来の光ディスク装置の畳込み信号、
読出し情報信号等の波形図、第2図は本発明の第一の実
施例の書込み信号、読出し情報信号等の波形図、第3図
(a)、 (b)、 (C)はそれぞれ本発明の第二、
第三お工び第四の実施例の書込み信号の波形図である。 図において。 2・・・・・・書込み信号、3・・・・・・ピット、4
・・・・・・再生信号、5・・・・・・読出し情報信号
、12・・・・・・書込み信号、13・・・・・・ビッ
ト、14・・・・・・再生信号、15・・・・・・読出
し情報信号、16・・・・・・読出しタイミングノくル
ス、22・・・・・・書込み信号、23・・・・・・媒
体上のピ、)、24・・・・・・再生信号、25・・・
・・・読出し情報信号、32,42.52・・・・・・
書込み信号。 蜆広しダイミンブノVルス  −11トmlり 予 /I!1
FIG. 1(a) and FIG. 1(b) show convolution signals of a conventional optical disk device when forming one circular and oval bits,
FIG. 2 is a waveform diagram of the write signal, read information signal, etc. of the first embodiment of the present invention, and FIGS. 3(a), (b), and (C) are waveform diagrams of the read information signal, etc. Second,
It is a waveform diagram of the write signal of the third and fourth embodiments. In fig. 2...Write signal, 3...Pit, 4
...Reproduction signal, 5 ...Read information signal, 12 ...Write signal, 13 ...Bit, 14 ...Reproduction signal, 15 ... Read information signal, 16 ... Read timing node, 22 ... Write signal, 23 ... Pi on medium, ), 24 ... ...Reproduction signal, 25...
...Read information signal, 32, 42.52...
write signal. Daimin Buno V Luss -11 ml /I! 1

Claims (1)

【特許請求の範囲】[Claims] 光学ヘッドから第一のエネルギー水準のレーザ光を照射
することによって光ディスク上にピットを形成し、前記
光学ヘッドから前記第一のエネルギー水準のエネルギー
値より低いエネルギー値の第二のエネルギー水準のレー
ザ光を前記光ディスクに照射して前記ピットからの反射
光を検知することによって情報の書込みおよび読出しを
行う光ディスク装置において、前記第一のエネルギー水
準のレーザ光の信号波形が、その前縁部において高水準
の第一のエネルギー値を有し、かつその後縁部において
前記第一のエネルギー値と前記第二のエネルギー水準の
エネルギー値との中間の値を有する第二のエネルギー値
を有し、前記第一のエネルギー値から前記第二のエネル
ギー値まで二次曲線に近似する曲線または少くとも1段
の階段状の形状に沿って減少するか、または前記第一の
エネルギー水準のレーザ光の信号波形が、その前縁部に
おいて前記第一のエネルギー値と前記第二のエネルギー
水準のエネルギー値の中間の値を有する第二のエネルギ
ー値を有し、かつその後縁部において高水準の第一のエ
ネルギー値を有し、前記第二のエネルギー値から前記第
一のエネルギー値まで二次曲線に近似する曲線または少
くとも1段の階段状の形状に沿って増大することを特徴
とする光ディスク装置。
forming pits on the optical disk by irradiating laser light of a first energy level from the optical head, and laser light of a second energy level having an energy value lower than the energy value of the first energy level from the optical head; In an optical disk device that writes and reads information by irradiating the laser beam onto the optical disk and detecting the reflected light from the pit, the signal waveform of the laser beam having the first energy level has a high level at its leading edge. and has a second energy value at its trailing edge having a value intermediate between the energy value of the first energy level and the energy value of the second energy level; The signal waveform of the laser light at the first energy level decreases from the energy value to the second energy value along a curve approximating a quadratic curve or at least one step-like shape, or a second energy value at its leading edge having a value intermediate between the energy values of said first energy level and said second energy level; and a first energy value of a higher level at its trailing edge. an optical disc device, wherein the energy value increases from the second energy value to the first energy value along a curve approximating a quadratic curve or at least one step-like shape.
JP59164447A 1984-08-06 1984-08-06 Optical disk device Pending JPS6142737A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59164447A JPS6142737A (en) 1984-08-06 1984-08-06 Optical disk device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59164447A JPS6142737A (en) 1984-08-06 1984-08-06 Optical disk device

Publications (1)

Publication Number Publication Date
JPS6142737A true JPS6142737A (en) 1986-03-01

Family

ID=15793337

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59164447A Pending JPS6142737A (en) 1984-08-06 1984-08-06 Optical disk device

Country Status (1)

Country Link
JP (1) JPS6142737A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0206824A2 (en) * 1985-06-26 1986-12-30 International Business Machines Corporation Apparatus for thermally recording data

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0206824A2 (en) * 1985-06-26 1986-12-30 International Business Machines Corporation Apparatus for thermally recording data
EP0206824A3 (en) * 1985-06-26 1988-10-19 International Business Machines Corporation Apparatus for thermally recording data apparatus for thermally recording data

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