JPH06301979A - Method and device for reproducing information - Google Patents

Method and device for reproducing information

Info

Publication number
JPH06301979A
JPH06301979A JP5087608A JP8760893A JPH06301979A JP H06301979 A JPH06301979 A JP H06301979A JP 5087608 A JP5087608 A JP 5087608A JP 8760893 A JP8760893 A JP 8760893A JP H06301979 A JPH06301979 A JP H06301979A
Authority
JP
Japan
Prior art keywords
amplitude
light rays
information
interference
ultrasonic
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
Application number
JP5087608A
Other languages
Japanese (ja)
Other versions
JP3189242B2 (en
Inventor
Manabu Yamamoto
学 山本
Kikuji Kato
喜久次 加藤
Hidetoshi Tatemichi
英俊 立道
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.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone 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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP08760893A priority Critical patent/JP3189242B2/en
Publication of JPH06301979A publication Critical patent/JPH06301979A/en
Application granted granted Critical
Publication of JP3189242B2 publication Critical patent/JP3189242B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Optical Recording Or Reproduction (AREA)

Abstract

PURPOSE:To obtain an information reproducing method by which the packing density of a recording medium can be increased by driving an ultrasonic deflector by means of amplitude-modulated signals and reproducing information by using moving interference fringes generated by the interference between a plurality of simultaneously generated diffracted light rays. CONSTITUTION:An amplitude modulator 6 outputs carrier signals inputted from a carrier generator 8 to an ultrasonic deflector 2 after modulating the carrier signals in amplitude by using sine wave signals inputted from a sine wave signal generator 7. The deflector 2 generates two diffracted light rays 9 by simultaneously diffracting a laser beam from a semiconductor laser 100 in two directions. The diffracted light rays 9 are made incident to a recording medium 108 through a lens 101, beam splitter 103, and lens 102 so as to generate reflected light rays 107. The reflected light rays 107 are made incident to a detector 105 and the information recorded on the medium 108 is reproduced by using interference fringes formed by interference between the diffracted light rays 9. When such a constitution is used, the track pitch of the medium can be reduced and an information reproducing method by which the packing density of the medium can be increased is obtained.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、高密度光ディスク装置
を実現する情報再生方法及び装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an information reproducing method and device for realizing a high density optical disk device.

【0002】[0002]

【従来の技術】従来のこの種装置の記録再生方法を図4
(a),(b)で説明する。図4(a)は記録再生装置
を示し、図4(b)はディスク媒体を示す。図4
(a),(b)において、100は半導体レーザ、10
1,102,104はレンズ、103はビームスプリッ
タ、105は検出器、106は記録再生用のレーザ光、
107はディスク媒体からの反射光、108はディスク
媒体、109はトラック、110は記録された領域であ
る。半導体レーザ100からのレーザ光106は、レン
ズ101,ビームスプリッタ103,レンズ102を介
してディスク媒体108に入射して、記録が行われる。
一方、再生する場合は、半導体レーザ100からの光1
06が、レンズ101,ビームスプリッタ103,レン
ズ102を介してディスク媒体108に入射し、ディス
ク媒体108からの反射光107がレンズ102,ビー
ムスプリッタ103,レンズ104を介して検出器10
5に入射して、再生が行われる。
2. Description of the Related Art A conventional recording / reproducing method of this kind of apparatus is shown in FIG.
This will be described with reference to (a) and (b). 4A shows a recording / reproducing device, and FIG. 4B shows a disk medium. Figure 4
In (a) and (b), 100 is a semiconductor laser, 10
1, 102 and 104 are lenses, 103 is a beam splitter, 105 is a detector, 106 is a recording / reproducing laser beam,
Reference numeral 107 is the reflected light from the disk medium, 108 is the disk medium, 109 is the track, and 110 is the recorded area. Laser light 106 from the semiconductor laser 100 enters the disk medium 108 via the lens 101, the beam splitter 103, and the lens 102, and recording is performed.
On the other hand, when reproducing, light 1 from the semiconductor laser 100
06 enters the disk medium 108 through the lens 101, the beam splitter 103, and the lens 102, and the reflected light 107 from the disk medium 108 passes through the lens 102, the beam splitter 103, and the lens 104, and the detector 10
Upon incidence on 5, reproduction is performed.

【0003】従来この種装置では、記録再生用のレーザ
光106の強度分布はガウシャン分布であり、ディスク
媒体108上ではほぼ円形で集光されている。その記録
の形態としては、レーザ光106のエネルギーにより、
穴を開けたり、結晶と非晶質状態の相変化を利用するこ
とによって、記録媒体の反射率を変化させて情報を書き
込む場合と、磁気バイアスを記録媒体に加えておき、レ
ーザ光106のオン,オフにより磁化を反転させて情報
を書き込む場合とがある。
Conventionally, in this type of apparatus, the intensity distribution of the laser light 106 for recording and reproduction has a Gaussian distribution, and is condensed in a substantially circular shape on the disk medium 108. As the form of recording, the energy of the laser beam 106 causes
When the information is written by changing the reflectance of the recording medium by making a hole or by utilizing the phase change between the crystalline state and the amorphous state, a magnetic bias is added to the recording medium and the laser beam 106 is turned on. In some cases, the information is written by reversing the magnetization when turned off.

【0004】[0004]

【発明が解決しようとする課題】上記記録の形態のいず
れの場合もディスク媒体108上のレーザ光106は波
長が0.8μm付近である場合は半値幅でせいぜい0.
8μm程度が限界であり記録密度はこの集光ビーム径で
制限されることになる。例えば130mm径のディスク
媒体では、記録されたピットの間隔は最短距離で約1.
5μm程度であり、このようなピットの間隔を再生する
場合には、再生時の信号出力は波形干渉により1/2程
度に低減する。S/N条件より1/2程度の低減が限界
であり、従来のこの種装置では、5.25インチの媒体
で片面の容量は325MBに制限される。
In any of the above recording modes, the laser beam 106 on the disk medium 108 has a full width at half maximum of at most 0.8 when the wavelength is near 0.8 μm.
The limit is about 8 μm, and the recording density is limited by this focused beam diameter. For example, on a disk medium having a diameter of 130 mm, the shortest distance between recorded pits is about 1.
It is about 5 μm, and when reproducing such a pit interval, the signal output during reproduction is reduced to about 1/2 due to waveform interference. The limit is about 1/2 reduction from the S / N condition, and the conventional device of this type limits the capacity of one side to 325 MB with a medium of 5.25 inches.

【0005】本発明の目的は、従来の光ディスク装置に
比べ高密度化が可能な情報再生方法及び装置を提供する
ことにある。
It is an object of the present invention to provide an information reproducing method and an apparatus capable of achieving higher density than a conventional optical disk apparatus.

【0006】[0006]

【課題を解決するための手段】上記課題を解決するため
に本発明の情報再生方法は、超音波偏向器から同時に発
生する複数の回折光の干渉によって形成される干渉縞に
よって、記録された情報の再生を行なうことを特徴とす
るものである。
In order to solve the above-mentioned problems, the information reproducing method of the present invention is such that the information recorded by the interference fringes formed by the interference of a plurality of diffracted lights simultaneously generated from the ultrasonic deflector. Is performed.

【0007】又、本発明の情報再生装置は、再生用光源
と、所定波長の搬送波信号を発生する搬送波信号発生手
段と、前記搬送波信号とは異なる波長の振幅変調用入力
信号を発生する入力信号発生手段と、前記搬送波信号を
前記入力信号により振幅変調する振幅変調手段と、前記
振幅変調手段による振幅変調信号により前記再生用光源
による光ビームを複数方向に回折する超音波偏向器と、
前記超音波偏光器による複数回折光を記録媒体に入射さ
せる手段と、前記複数回折光の記録媒体からの反射光を
検出器に入射させる手段とを備えたことを特徴とするも
のである。
Further, the information reproducing apparatus of the present invention includes a reproducing light source, a carrier signal generating means for generating a carrier signal of a predetermined wavelength, and an input signal for generating an amplitude modulating input signal of a wavelength different from the carrier signal. Generating means, amplitude modulating means for amplitude-modulating the carrier signal with the input signal, and an ultrasonic deflector for diffracting the light beam from the reproduction light source in a plurality of directions by the amplitude-modulating signal by the amplitude modulating means,
It is characterized by comprising means for causing a plurality of diffracted lights from the ultrasonic polarizer to enter a recording medium, and means for causing a reflected light of the plurality of diffracted lights from the recording medium to enter a detector.

【0008】更に、本発明の情報再生装置は、前記検出
器に空間遮蔽板を配置し、移動干渉縞の一部を検出する
ことを特徴とするものである。
Further, the information reproducing apparatus of the present invention is characterized in that a space shielding plate is arranged on the detector to detect a part of the moving interference fringes.

【0009】[0009]

【作用】上記手段により本発明は、進行超音波よりなる
超音波偏向器を振幅変調信号で駆動し、同時に発生する
複数の回折光の干渉によって生ずる移動干渉縞によって
情報の再生を行うことを特徴とする。
According to the above-mentioned means, the present invention is characterized in that the ultrasonic deflector composed of traveling ultrasonic waves is driven by the amplitude modulation signal, and the information is reproduced by the moving interference fringes generated by the interference of a plurality of diffracted lights which are simultaneously generated. And

【0010】[0010]

【実施例】本発明の実施例を図1、図2および図3を用
いて説明する。図1〜図3の部分中、図4の部分と同様
の部分は同一番号を付してその説明を省略する。図1に
おいて、2は超音波偏向器、6は振幅変調器である。7
は正弦波信号発生器であり、周波数は例えば1〜10M
Hz程度である。8は超音波を駆動する振幅変調信号用
の搬送波発生器であり、周波数は100MHz程度であ
る。9は超音波偏向器2から同時に発生する2本の回折
光、10は2本の回折光の干渉によって形成される干渉
縞、1001は検出器105上の干渉縞、11は干渉縞
10が移動する方向、12はディスク媒体108の回転
方向、13はディスク媒体108上のビームパターン、
1301は検出器105上のビームパターンである。
Embodiments of the present invention will be described with reference to FIGS. 1, 2 and 3. 1 to 3, those parts which are the same as those corresponding parts in FIG. 4 are designated by the same reference numerals, and a description thereof will be omitted. In FIG. 1, 2 is an ultrasonic deflector, and 6 is an amplitude modulator. 7
Is a sine wave signal generator, and the frequency is, for example, 1 to 10M.
It is about Hz. Reference numeral 8 denotes a carrier wave generator for an amplitude modulation signal which drives ultrasonic waves, and has a frequency of about 100 MHz. Reference numeral 9 denotes two diffracted lights simultaneously generated from the ultrasonic deflector 2, 10 denotes an interference fringe formed by the interference of the two diffracted lights, 1001 denotes an interference fringe on the detector 105, and 11 denotes the interference fringe 10. Direction, 12 is the rotation direction of the disk medium 108, 13 is the beam pattern on the disk medium 108,
1301 is a beam pattern on the detector 105.

【0011】即ち、正弦波信号発生器7は例えば周波数
が1〜10MHz程度の振幅変調用正弦波信号を発生し
て振幅変調器6へ出力する。また、搬送波発生器8は周
波数が100MHz程度の搬送波信号を発生して振幅変
調器6へ出力する。この振幅変調器6は搬送波発生器8
から入力された搬送波信号を正弦波信号発生器7から入
力された正弦波信号により振幅変調して超音波偏向器2
へ出力する。この超音波偏向器2は振幅変調器6から入
力された振幅変調信号により、半導体レーザ100から
発生したレーザ光ビームを同時に二方向に回折して二つ
の回折光9を発生する。超音波偏向器2から同時に発生
した二つの回折光9はレンズ101,ビームスプリッタ
103,レンズ102を介してディスク媒体108に入
射される。ディスク媒体108は超音波偏向器2から入
射された二つの回折光9に基づく反射光107を発生
し、この反射光107はレンズ102,ビームスプリッ
タ103,レンズ104を介して検出器105に入射さ
れる。しかして、超音波偏向器2から同時に発生する二
つの回折光9の干渉によって形成される干渉縞10によ
って、ディスク媒体108に記録された情報の再生を行
なうことができる。
That is, the sine wave signal generator 7 generates a sine wave signal for amplitude modulation having a frequency of, for example, about 1 to 10 MHz and outputs it to the amplitude modulator 6. The carrier wave generator 8 also generates a carrier wave signal having a frequency of about 100 MHz and outputs it to the amplitude modulator 6. This amplitude modulator 6 is a carrier wave generator 8
The carrier wave signal input from the ultrasonic wave deflector 2 is amplitude-modulated by the sine wave signal input from the sine wave signal generator 7.
Output to. The ultrasonic deflector 2 simultaneously diffracts the laser light beam generated from the semiconductor laser 100 in two directions by the amplitude modulation signal input from the amplitude modulator 6 to generate two diffracted lights 9. Two diffracted lights 9 generated simultaneously from the ultrasonic deflector 2 are incident on the disk medium 108 via the lens 101, the beam splitter 103, and the lens 102. The disk medium 108 generates reflected light 107 based on the two diffracted lights 9 incident from the ultrasonic deflector 2, and the reflected light 107 is incident on the detector 105 via the lens 102, the beam splitter 103, and the lens 104. It Therefore, the information recorded on the disk medium 108 can be reproduced by the interference fringes 10 formed by the interference of the two diffracted lights 9 simultaneously generated from the ultrasonic deflector 2.

【0012】超音波偏向器2は図2に示される周波数帯
域14を持ち、搬送波信号が正弦波信号によって振幅変
調されるため、超音波偏向器2を駆動する信号のスペク
タルは図2に示すように搬送波周波数f0 及び上側波帯
信号f0 +fi と下側波帯信号f0 −fi よりなる。こ
こで上側波帯信号f0 +fi は超音波偏向器2の周波数
帯域14外にあるように設定すると、超音波偏向器2を
実質的に駆動する信号は搬送波信号f0 と下側波帯信号
0 −fi になる。この二つの信号に対応して超音波の
回折光も二つとなる。この二つの回折光が干渉すると正
弦波信号の周波数に比例したピッチの干渉縞10が形成
される。また、定在波ではなく進行波の超音波によって
回折された光の干渉では干渉縞10が一定の速度MVa
で移動する。ここで、M=fc/foである。
The ultrasonic deflector 2 has the frequency band 14 shown in FIG. 2, and since the carrier wave signal is amplitude-modulated by the sine wave signal, the spectrum of the signal for driving the ultrasonic deflector 2 is as shown in FIG. consisting of the carrier frequency f 0 and an upper sideband signal f 0 + f i and a lower sideband signal f 0 -f i to. If the upper sideband signal f 0 + f i is set outside the frequency band 14 of the ultrasonic deflector 2, the signals that substantially drive the ultrasonic deflector 2 are the carrier wave signal f 0 and the lower sideband. It will signal f 0 -f i. There are two ultrasonic diffracted lights corresponding to these two signals. When these two diffracted lights interfere, an interference fringe 10 having a pitch proportional to the frequency of the sine wave signal is formed. Further, in the interference of light diffracted by a traveling wave ultrasonic wave instead of a standing wave, the interference fringe 10 has a constant velocity MVa.
To move. Here, M = fc / fo.

【0013】このような移動干渉縞10で情報を再生す
る方法を図3(a),(b),(c)を用いて説明す
る。図において、20は空間遮蔽板である。図3(a)
に示すように、記録された情報パターン110において
黒色パターン1101はトラック109の記録情報であ
り、白色パターン1102は隣設トラックの記録情報で
ある。本方法では干渉縞移動速度MVaとディスク媒体
108の回転速度Vdを一致させ、図3(a),(b)
に示すように、干渉縞10の位置と記録情報のパターン
1101の位置を同期させて情報を再生する。両者を同
期させる方法としては、例えば、あらかじめディスク媒
体108上に形成されている情報パターン110を再生
し、その信号出力が最大となるよう超音波偏向器駆動用
の正弦波信号の周波数を調節して、干渉縞10の位置と
記録情報パターン1101の位置を同期させるなどの方
法が考えられる。再生用の検出器105上でも干渉縞1
001は移動するが、図3(c)に示すように、常に最
大ピークの干渉縞のみを空間遮蔽板20を用いて選別す
れば記録情報が1ビット単位で検出できることになる。
ここで、干渉縞の間隔はディスク媒体108上ではサブ
ミクロンから数ミクロンの値であるが、検出器105上
では反射光集光光学系の倍率を大きくすることによっ
て、10μm以上数100μm程度まで拡大することが
可能であり、空間遮蔽板20の透過領域をそのような長
さに設定して容易に高密度記録の再生が可能であった。
実験ではガラス板にクロム蒸着により20ミクロン程度
のスリット部を形成し、高密度記録の信号再生を行なっ
た。
A method of reproducing information using such moving interference fringes 10 will be described with reference to FIGS. 3 (a), 3 (b) and 3 (c). In the figure, 20 is a space shielding plate. Figure 3 (a)
In the recorded information pattern 110, the black pattern 1101 is the recording information of the track 109, and the white pattern 1102 is the recording information of the adjacent track as shown in FIG. In this method, the moving speed MVa of the interference fringes and the rotating speed Vd of the disk medium 108 are made equal to each other, and the moving speed MVa shown in FIGS.
As shown in, the information is reproduced by synchronizing the position of the interference fringe 10 and the position of the pattern 1101 of the recorded information. As a method of synchronizing the two, for example, the information pattern 110 previously formed on the disk medium 108 is reproduced, and the frequency of the sine wave signal for driving the ultrasonic deflector is adjusted so that the signal output thereof becomes maximum. Then, a method of synchronizing the position of the interference fringe 10 and the position of the recording information pattern 1101 can be considered. Interference fringe 1 on the detector 105 for reproduction
Although 001 moves, as shown in FIG. 3C, if only the interference fringe having the maximum peak is always selected using the space shield plate 20, the recorded information can be detected in 1-bit units.
Here, the interval of the interference fringes is a value from submicron to several microns on the disk medium 108, but on the detector 105, by increasing the magnification of the reflected light condensing optical system, it is expanded from 10 μm to several hundred μm. It is possible to set the length of the transmission region of the space shield plate 20 to such a level, and it is possible to easily reproduce high density recording.
In the experiment, a slit portion of about 20 μm was formed on the glass plate by vapor deposition of chromium, and signal reproduction for high density recording was performed.

【0014】この方法によればトラック109の情報の
みが検出され、隣設トラックの情報は極めて近接されて
いても再生されることはなく、光ディスク媒体の狭トラ
ックピッチ化が図れる。本方法によれば、既に市販され
ている光ディスク媒体の再生も容易であり、メモリにお
ける下位互換性も確保できる。記録媒体としては、既存
の光磁気媒体、相変化媒体などが適用可能である。
According to this method, only the information of the track 109 is detected, the information of the adjacent track is not reproduced even if it is extremely close, and the track pitch of the optical disk medium can be narrowed. According to this method, it is easy to reproduce an optical disc medium that is already on the market, and it is possible to secure backward compatibility in the memory. As the recording medium, an existing magneto-optical medium, phase change medium or the like can be applied.

【0015】[0015]

【発明の効果】以上説明したように、本発明によれば、
光ディスク媒体の狭トラックピッチ化が可能なため、高
密度光ディスク装置を実現できる。
As described above, according to the present invention,
Since the track pitch of the optical disk medium can be narrowed, a high density optical disk device can be realized.

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

【図1】本発明の一実施例を示す構成説明図である。FIG. 1 is a structural explanatory view showing an embodiment of the present invention.

【図2】本発明に係る超音波偏向器の周波数帯域および
振幅変調信号のスペクトルの一例を示す特性図である。
FIG. 2 is a characteristic diagram showing an example of a spectrum of a frequency band and an amplitude modulation signal of the ultrasonic deflector according to the present invention.

【図3】本発明における信号再生方法の一例を示す説明
図である。
FIG. 3 is an explanatory diagram showing an example of a signal reproducing method according to the present invention.

【図4】従来の光ディスク装置の記録再生方法を示す構
成説明図である。
FIG. 4 is a structural explanatory view showing a recording / reproducing method of a conventional optical disc device.

【符号の説明】[Explanation of symbols]

100…半導体レーザ、101,102,104…レン
ズ、103…ビームスプリッタ、105…検出器、10
6…レーザ光、107…ディスク媒体からの反射光、1
08…ディスク媒体、109…トラック、110…記録
された領域、2…超音波偏向器、6…振幅変調器、7…
正弦波信号発生器、8…搬送波発生器、9…回折光、1
0…干渉縞、1001…検出器上の干渉縞、11…干渉
縞が移動する方向、12…ディスク媒体の回転方向、1
3…ディスク媒体上のビームパターン、1301…検出
器上のビームパターン、14…超音波偏向器の周波数帯
域、20…空間遮蔽板。
100 ... Semiconductor laser, 101, 102, 104 ... Lens, 103 ... Beam splitter, 105 ... Detector, 10
6 ... Laser light, 107 ... Reflected light from the disk medium, 1
08 ... Disk medium, 109 ... Track, 110 ... Recorded area, 2 ... Ultrasonic deflector, 6 ... Amplitude modulator, 7 ...
Sine wave signal generator, 8 ... Carrier wave generator, 9 ... Diffracted light, 1
0 ... Interference fringes, 1001 ... Interference fringes on the detector, 11 ... Direction of movement of interference fringes, 12 ... Rotation direction of disk medium, 1
3 ... Beam pattern on disk medium, 1301 ... Beam pattern on detector, 14 ... Frequency band of ultrasonic deflector, 20 ... Space shield plate.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 超音波偏向器から同時に発生する複数の
回折光の干渉によって形成される干渉縞によって、記録
された情報の再生を行なうことを特徴とする情報再生方
法。
1. An information reproducing method characterized in that recorded information is reproduced by interference fringes formed by interference of a plurality of diffracted lights simultaneously generated from an ultrasonic deflector.
【請求項2】 再生用光源と、所定波長の搬送波信号を
発生する搬送波信号発生手段と、前記搬送波信号とは異
なる波長の振幅変調用入力信号を発生する入力信号発生
手段と、前記搬送波信号を前記入力信号により振幅変調
する振幅変調手段と、前記振幅変調手段による振幅変調
信号により前記再生用光源による光ビームを複数方向に
回折する超音波偏向器と、前記超音波偏光器による複数
回折光を記録媒体に入射させる手段と、前記複数回折光
の記録媒体からの反射光を検出器に入射させる手段とを
備えたことを特徴とする情報再生装置。
2. A reproducing light source, a carrier signal generating means for generating a carrier signal of a predetermined wavelength, an input signal generating means for generating an amplitude modulating input signal of a wavelength different from the carrier signal, and the carrier signal. Amplitude modulation means for amplitude-modulating by the input signal, an ultrasonic deflector for diffracting the light beam by the reproduction light source in a plurality of directions by the amplitude-modulation signal by the amplitude modulation means, and a plurality of diffracted light by the ultrasonic polarizer. An information reproducing apparatus comprising: a unit for causing a recording medium to enter; and a unit for causing reflected light of the plurality of diffracted lights from the recording medium to enter a detector.
【請求項3】 検出器に空間遮蔽板を配置し、移動干渉
縞の一部を検出することを特徴とする請求項2記載の情
報再生装置。
3. The information reproducing apparatus according to claim 2, wherein a space shield plate is arranged on the detector to detect a part of the moving interference fringes.
JP08760893A 1993-04-14 1993-04-14 Information reproducing method and apparatus Expired - Fee Related JP3189242B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP08760893A JP3189242B2 (en) 1993-04-14 1993-04-14 Information reproducing method and apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP08760893A JP3189242B2 (en) 1993-04-14 1993-04-14 Information reproducing method and apparatus

Publications (2)

Publication Number Publication Date
JPH06301979A true JPH06301979A (en) 1994-10-28
JP3189242B2 JP3189242B2 (en) 2001-07-16

Family

ID=13919686

Family Applications (1)

Application Number Title Priority Date Filing Date
JP08760893A Expired - Fee Related JP3189242B2 (en) 1993-04-14 1993-04-14 Information reproducing method and apparatus

Country Status (1)

Country Link
JP (1) JP3189242B2 (en)

Also Published As

Publication number Publication date
JP3189242B2 (en) 2001-07-16

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