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JP2571776B2 - How to record and erase information - Google Patents

How to record and erase information

Info

Publication number
JP2571776B2
JP2571776B2 JP62014161A JP1416187A JP2571776B2 JP 2571776 B2 JP2571776 B2 JP 2571776B2 JP 62014161 A JP62014161 A JP 62014161A JP 1416187 A JP1416187 A JP 1416187A JP 2571776 B2 JP2571776 B2 JP 2571776B2
Authority
JP
Japan
Prior art keywords
recording
erasing
signal
level
information
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.)
Expired - Fee Related
Application number
JP62014161A
Other languages
Japanese (ja)
Other versions
JPS63183624A (en
Inventor
哲也 西田
元康 寺尾
裕史 助田
憲雄 太田
義人 角田
敏光 賀来
圭吉 安藤
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP62014161A priority Critical patent/JP2571776B2/en
Priority to KR1019880000459A priority patent/KR910003039B1/en
Priority to DE3851239T priority patent/DE3851239T2/en
Priority to CN 90103304 priority patent/CN1017841B/en
Priority to CN88100345A priority patent/CN88100345A/en
Priority to EP88101099A priority patent/EP0276808B1/en
Publication of JPS63183624A publication Critical patent/JPS63183624A/en
Priority to US07/634,049 priority patent/US5404348A/en
Application granted granted Critical
Publication of JP2571776B2 publication Critical patent/JP2571776B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related 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
    • G11B7/007Arrangement of the information on the record carrier, e.g. form of tracks, actual track shape, e.g. wobbled, or cross-section, e.g. v-shaped; Sequential information structures, e.g. sectoring or header formats within a track
    • G11B7/013Arrangement of the information on the record carrier, e.g. form of tracks, actual track shape, e.g. wobbled, or cross-section, e.g. v-shaped; Sequential information structures, e.g. sectoring or header formats within a track for discrete information, i.e. where each information unit is stored in a distinct discrete location, e.g. digital information formats within a data block or sector
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10502Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing characterised by the transducing operation to be executed
    • G11B11/10504Recording
    • G11B11/10506Recording by modulating only the light beam of the transducer
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10502Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing characterised by the transducing operation to be executed
    • G11B11/10515Reproducing
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10502Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing characterised by the transducing operation to be executed
    • G11B11/10517Overwriting or erasing
    • 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
    • G11B7/004Recording, reproducing or erasing methods; Read, write or erase circuits therefor
    • G11B7/0045Recording
    • G11B7/00454Recording involving phase-change effects
    • 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
    • G11B7/004Recording, reproducing or erasing methods; Read, write or erase circuits therefor
    • G11B7/006Overwriting

Landscapes

  • Optical Recording Or Reproduction (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、相変化型等の原子配列変化により光学定数
が変化するのを利用した、アクセス時間を短縮するのに
好適な情報の記録および消去方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to recording of information suitable for shortening access time by utilizing a change in an optical constant due to a change in atomic arrangement such as a phase change type. It relates to an erasing method.

〔従来の技術〕[Conventional technology]

光ディスクに情報の記録を行いまたは記録された情報
の消去を行う場合、記録または消去しようとする情報
が、実際に記録または消去されているかどうかを確認す
る必要がある。上記確認の方法として、従来は、記録ま
たは消去したのちに、ディスクが1回転するのを待っ
て、読み出し光により確認を行っていた。また、穴開け
型1回書き込み型の光ディスクでは、記録光の反射光を
検出することにより記録の有無を確認する方法が、特許
第1264450号に開示されている。しかしながら、相変化
型等の原子配列の変化を利用した1回書き込み、または
書き換え可能型光ディスクでは、記録光の反射光波形が
上記穴開け型とは異なるため、記録光、消去光の反射光
を検出して、記録および消去の有無を確認した例がなか
った。
When recording information on an optical disc or erasing recorded information, it is necessary to check whether the information to be recorded or erased is actually recorded or erased. Conventionally, as a method of the above-described confirmation, after recording or erasing, the disc is waited for one rotation, and then confirmed by a reading light. Japanese Patent No. 1264450 discloses a method of confirming the presence or absence of recording by detecting reflected light of recording light in a perforated type write once optical disk. However, in a single-write or rewritable optical disk utilizing a change in the atomic arrangement such as a phase change type, the reflected light waveform of the recording light is different from that of the above-mentioned perforated type optical disc, so that the reflected light of the recording light and the erasing light is reflected. There was no example in which the presence and absence of the recording and erasure were detected.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

上記従来技術では、相変化型等の原子配列変化を利用
した光ディスクにおいて、記録または消去の確認のため
に、ディスク1回転分の時間(例えば1800rpmの場合は3
3ms)を余分に費しており、アクセス時間が長いという
問題を有していた。
In the above prior art, in an optical disk using an atomic arrangement change such as a phase change type, a time for one rotation of the disk (for example, 3
3ms), and the access time is long.

本発明は、アクセス時間が短い記録、消去方法を得る
ことを目的とする。
An object of the present invention is to provide a recording and erasing method with a short access time.

〔問題点を解決するための手段〕[Means for solving the problem]

上記目的は、照射パワーレベルを少なくとも消去レベ
ルと記録レベルの間で変化させた単一のレーザ光を記録
媒体に照射し、情報の記録および消去を行う情報の記録
および消去方法において、上記記録媒体からの反射光の
再生信号波形を形成し、上記再生信号波形をクロックの
タイミングに基づいて分割し、該分割した再生信号波形
から、上記レーザ光の記録レベルおよび消去レベルのそ
れぞれの照射時における再生信号波形をそれぞれ取り出
し、取り出した再生信号波形を別々に評価し、記録およ
び消去をそれぞれ確認することにより達成される。
The object is to irradiate a recording medium with a single laser beam whose irradiation power level is changed at least between an erasing level and a recording level to record and erase information. A reproduction signal waveform of the reflected light from the laser beam is formed, the reproduction signal waveform is divided based on the clock timing, and the reproduction at the time of irradiating the recording level and the erasing level of the laser light from the divided reproduction signal waveform is performed. This is achieved by extracting each signal waveform, separately evaluating the extracted reproduced signal waveforms, and confirming recording and erasing, respectively.

〔作用〕[Action]

本発明による情報の記録および消去法は、記録中また
は消去中に、記録光または消去光の反射レベルが、原子
配列の規則性が異なる複数の状態間で、レーザ照射によ
り記録または消去中に変化する記録膜の反射率に応じて
光学定数が変化するのを利用し、上記変化をリアルタイ
ムで電気信号として検出し、上記電気信号の波形および
強度の変化によって、正常な記録あるいは消去が行われ
たかどうかを確認する。上記原子配列の規則性が異なる
複数の状態のうち2つの状態を利用して検出するが、上
記2つの状態とは、規則性が高い状態と低い状態で、例
えば結晶状態と非結晶状態でもよいし、結晶形が異なる
2つの結晶状態、あるいは異なった形で乱れを有する2
つの結晶状態であってもよい。
According to the method for recording and erasing information according to the present invention, during recording or erasing, the reflection level of recording light or erasing light changes during recording or erasing by laser irradiation between a plurality of states having different atomic arrangement regularities. Utilizing that the optical constant changes according to the reflectance of the recording film to be detected, the change is detected as an electric signal in real time, and the normal recording or erasing was performed by the change in the waveform and intensity of the electric signal. Check if. Detection is performed by using two states among the plurality of states having different regularities of the atomic arrangement. The two states may be a state having a high regularity and a state having a low regularity, for example, a crystalline state and an amorphous state. And two crystal states with different crystal forms, or two with different forms of disorder.
It may be in one crystal state.

上記記録膜の2つの状態間のうち、どちら向きの原子
配列の変化を記録と考え、あるいは消去と考えるかは任
意であり、あらかじめ決めておけばよい。
It is optional to determine in which direction the change in the atomic arrangement between the two states of the recording film is considered as recording or erasing, and may be determined in advance.

1つのレーザ光照射により記録または消去を行う場合
は、記録光(高パワーレーザ光)、消去光(低パワーレ
ーザ光)の少なくとも一方の反射光をクロックにより取
り出し、記録または消去が確実に行われたかどうかを確
認する。この際、記録光および消去光のそれぞれの反射
光を、クロックにより取り出し、記録および消去をそれ
ぞれ確認する方法が好ましい。
When recording or erasing is performed by irradiating one laser beam, at least one reflected light of recording light (high-power laser light) or erasing light (low-power laser light) is extracted by a clock, and recording or erasing is performed reliably. Check if it is. At this time, it is preferable that the reflected light of the recording light and the reflected light of the erasing light be extracted by a clock to confirm the recording and the erasing, respectively.

〔実施例〕〔Example〕

つぎに本発明の実施例を図面とともに説明する。第1
図は本発明による情報の記録および消去方法に用いる情
報記録媒体を示す断面図、第2図は上記記録媒体に照射
する単一レーザ光の波形を示す図、第3図(a)〜
(e)はクロックで取り出した高パワーレーザ光の反射
光シグナル、(f)〜(j)は上記シグナルのエラー信
号をそれぞれ示す図、第4図(a)〜(e)はそれぞれ
安定なエラー信号を得る方法を示す図、第5図(a)〜
(d)はクロックで取り出した高パワーレーザ光の反射
光シグナルをそれぞれ示す図、第6図(a)〜(e)は
それぞれ安定なエラー信号を得る方法を示す図、第7図
(a)〜(c)はクロックで取り出した低パワーレーザ
光の反射光シグナル、(d)〜(f)は上記シグナルの
エラー信号をそれぞれ示す図である。
Next, embodiments of the present invention will be described with reference to the drawings. First
FIG. 2 is a cross-sectional view showing an information recording medium used for the method of recording and erasing information according to the present invention, FIG. 2 is a view showing a waveform of a single laser beam applied to the recording medium, and FIGS.
(E) shows a reflected light signal of the high-power laser light extracted by the clock, (f) to (j) show error signals of the above signals, and FIGS. 4 (a) to (e) show stable errors, respectively. FIG. 5A to FIG. 5D show a method for obtaining a signal.
(D) is a diagram showing a reflected light signal of a high-power laser beam taken out by a clock, FIGS. 6 (a) to (e) are diagrams showing a method of obtaining a stable error signal, and FIG. 7 (a). (C) is a diagram showing a reflected light signal of a low-power laser beam extracted by a clock, and (d) to (f) are diagrams showing an error signal of the signal.

実施例 1 第1図において、1は直径130mm、厚さ1.1mmのディス
ク状化学強化ガラスの表面に紫外線硬化樹脂によってト
ラッキング用の溝のレプリカを形成した基板、2は上記
基板1上にマグネトロンスパッタリング法によって形成
されたSiO2からなる保護層で、該保護層2の厚さは110n
mである。3は上記保護層2の上に形成された薄膜の記
録膜で、該記録膜3はGe,TeおよびSeをそれぞれ独立に
蒸発させて蒸着したものである。4は上記記録膜3上に
マグネトロンスパッタリング法によって形成されたSiO2
の保護層で、該保護層4の厚さは110nmである。上記の
ような情報記録媒体に半導体レーザ光の連続光を照射す
ると、上記記録膜3中の元素を十分に反応させることが
でき、初期化を行うことができる。
Example 1 In FIG. 1, reference numeral 1 denotes a substrate in which a replica of a tracking groove is formed on the surface of a disk-shaped chemically strengthened glass having a diameter of 130 mm and a thickness of 1.1 mm by an ultraviolet curable resin, and 2 denotes magnetron sputtering on the substrate 1 Is a protective layer made of SiO 2 formed by the method, and the thickness of the protective layer 2 is 110 n
m. Reference numeral 3 denotes a thin recording film formed on the protective layer 2. The recording film 3 is formed by evaporating Ge, Te and Se independently from each other. Reference numeral 4 denotes SiO 2 formed on the recording film 3 by a magnetron sputtering method.
The thickness of the protective layer 4 is 110 nm. When the above-mentioned information recording medium is irradiated with continuous light of the semiconductor laser light, the elements in the recording film 3 can be sufficiently reacted, and initialization can be performed.

つぎに、上記情報記録媒体に第2図に示すような単一
のレーザ光の矩形パルスを照射した場合、高パワーレー
ザ光および低パワーレーザ光に応じた変化を生じるかど
うかを確認した。高パワーレーザ光を照射した場合は、
照射前の状態が結晶状態(消去状態)であるか、非結晶
状態(記録状態)であるかの如何にかかわらず、非結晶
状態(低反射率)となり、低パワーレーザ光を照射した
場合には結晶状態(高反射率)になるはずである。そこ
で、クロックを利用して新たに記録する信号の1単位ご
とに反射レーザ光の強度信号を別々に取り出すと、それ
ぞれ第3図および第6図に示すようになる。高パワーレ
ーザ光を照射した時に、記録膜3が一旦融解したのちに
非晶質化がおこる場合は、第3図(a)あるいは(b)
に示した波形となり、融解状態が続く場合は第3図
(e)に示した波形となり、何も変化しない場合(エラ
ーの時)第3図(c),(d)に示した波形になる。図
における(a),(c)は初期が結晶状態であり、
(b),(d)は非結晶状態である。つぎに第3図にA
で示したようにコンパレータレベルを設定し、1単位の
入力信号が終る位置において、上記コンパレータレベル
よりも信号が大きい場合にエラー信号を発生するように
すると、(c),(d)の時にだけ(h),(i)に示
すようにエラー信号が発生する。上記方法では記録膜3
の形成の不均一や書き換えに起因する反射率変動に対し
てエラー率が高いため、何も変化しない第3図(c),
(d)のときにエラー信号が発生する方法としては、つ
ぎに記す方法の方がより好ましい。すなわち、反射光シ
グナル(第4図(a))に対して、上記反射光シグナル
のパルス幅の1/2だけ遅延したシグナルを第4図(b)
のように作る。つぎに上記2つのシグナルをコンパレー
タに通して、遅延したシグナルが元のシグナルよりも大
きい場合にコンパレータ出力が高いレベルになるように
すると、第4図(c)に示すコンパレータの出力シグナ
ルが得られる。コンパレータ出力の立上りから20ns以内
に、第4図(d)に示すようにレーザ駆動パルスが立下
るときにだけエラー信号が発生するようにすると、第4
図(e)に示すように第3図中の(c),(d)の場合
にエラー信号が現われる。しかし、上記の方法では第3
図(e)に示した場合にもエラー信号が発生するため、
前記のエラー検出方法と組合わせて用いることが必要で
ある。
Next, when the information recording medium was irradiated with a rectangular pulse of a single laser beam as shown in FIG. 2, it was confirmed whether or not a change according to the high-power laser beam and the low-power laser beam occurred. When irradiated with high power laser light,
Irrespective of whether the state before irradiation is a crystalline state (erased state) or a non-crystalline state (recorded state), the state becomes a non-crystalline state (low reflectivity), and when a low power laser beam is irradiated. Should be in a crystalline state (high reflectivity). Therefore, when the intensity signal of the reflected laser light is separately extracted for each unit of a newly recorded signal using a clock, the results are as shown in FIGS. 3 and 6, respectively. When the recording film 3 is once melted and becomes amorphous after irradiation with the high-power laser beam, FIG. 3 (a) or (b)
When the melting state continues, the waveform shown in FIG. 3E is obtained, and when no change occurs (when an error occurs), the waveforms shown in FIGS. 3C and 3D are obtained. . (A) and (c) in the figure are initially in a crystalline state,
(B) and (d) are in an amorphous state. Next, in FIG.
When the comparator level is set as shown in (2) and an error signal is generated at a position where one unit of the input signal ends and the signal is larger than the comparator level, only at the time of (c) and (d), An error signal is generated as shown in (h) and (i). In the above method, the recording film 3
Since the error rate is high with respect to the non-uniformity of the formation of the pattern and the change in the reflectance caused by the rewriting, nothing changes.
As a method for generating an error signal in the case of (d), the following method is more preferable. That is, a signal delayed by 1/2 of the pulse width of the reflected light signal with respect to the reflected light signal (FIG. 4 (a)) is shown in FIG. 4 (b).
Make like. Next, when the two signals are passed through a comparator so that the comparator output becomes a high level when the delayed signal is larger than the original signal, the output signal of the comparator shown in FIG. 4C is obtained. . If an error signal is generated only when the laser drive pulse falls within 20 ns from the rise of the comparator output, as shown in FIG.
As shown in FIG. 3E, an error signal appears in the cases of FIGS. 3C and 3D. However, in the above method, the third
Since an error signal is also generated in the case shown in FIG.
It is necessary to use it in combination with the above error detection method.

また、基礎実験によると、高パワーレーザ光の出力が
15mW以上と特に大きい場合には、クロックにより分割し
て取出した反射光の信号は第5図のようになる。非晶質
化がおこる場合は第5図(a),(b)に示した波形に
なり、何も変化しない場合(エラーのとき)は第5図
(c),(d)に示した波形になる。(c),(d)の
時だけエラー信号を発生する方法としてつぎに示す方法
を用いた。すなわち、第6図(a)に示す反射光シグナ
ルに対して、このパルス幅(情報の単位長さ)の1/2だ
け遅延したシグナルを作る(第6図(b))。つぎに、
上記2つのシグナルをコンパレータに通して、元のシグ
ナルが遅延したシグナルよりも大きい場合にコンパレー
タ出力が高レベルになるようにし、このコンパレータ出
力をパルス幅の1/2だけ遅延させると、第6図(c)に
示すシグナルが得られる。コンパレータ出力の立上りか
ら20ns以内に、第6図(d)に示すようにレーザ駆動パ
ルスが立下る時だけエラー信号が発生するようにする
と、第6図(e)に示すように、第5図中の(c),
(d)の場合にだけエラー信号が現われる。
According to basic experiments, the output of high-power laser light
In the case of a particularly large power of 15 mW or more, the reflected light signal divided and extracted by the clock is as shown in FIG. When amorphization occurs, the waveforms shown in FIGS. 5A and 5B are obtained, and when no change occurs (when an error occurs), the waveforms shown in FIGS. 5C and 5D are obtained. become. The following method was used as a method for generating an error signal only in cases (c) and (d). That is, a signal is produced which is delayed from the reflected light signal shown in FIG. 6 (a) by の of the pulse width (unit length of information) (FIG. 6 (b)). Next,
When the two signals are passed through a comparator so that the output of the comparator becomes high when the original signal is larger than the delayed signal, and the output of the comparator is delayed by 1/2 of the pulse width, FIG. The signal shown in (c) is obtained. If an error signal is generated within 20 ns from the rise of the comparator output only when the laser drive pulse falls as shown in FIG. 6 (d), as shown in FIG. 6 (e), FIG. (C),
An error signal appears only in case (d).

一方、低パワーレーザ光を照射したときに結晶化がお
こる場合は、第7図(a),(b)に示した波形とな
り、何も変化しない場合は第7図(c)に示した波形に
なる。つぎに第7図のBで示したレベルにコンパレータ
を設定し、情報の単位長が終る位置において、上記コン
パレータレベルよりも信号が低い場合にエラー信号が発
生するようにすると、(c)の場合にだけエラー信号が
現われる。
On the other hand, when crystallization occurs when a low-power laser beam is irradiated, the waveform shown in FIGS. 7A and 7B is obtained, and when no change occurs, the waveform shown in FIG. 7C is obtained. become. Next, the comparator is set to the level shown in FIG. 7B, and at the position where the unit length of information ends, an error signal is generated when the signal is lower than the comparator level. The error signal appears only at

上記の高パワーレーザ光照射時(非晶質化時)の確認
と低パワーレーザ光照射時(結晶化時)の確認を両方同
時に行った場合のエラーレートは1×10-6であった。一
方、片方だけを行う場合は、非晶質化時だけに確認を行
ったときにエラーレートが5×10-5であったのに対し、
結晶化時にだけ確認を行った時は7×10-5であった。こ
れは非晶質化の方が結晶化よりも、確実に行われる率が
高いからである。
The error rate was 1 × 10 −6 when both the above confirmation at the time of high-power laser light irradiation (at the time of amorphization) and the confirmation at the time of low-power laser light irradiation (at the time of crystallization) were performed simultaneously. On the other hand, when performing only one of them, the error rate was 5 × 10 −5 when the confirmation was performed only at the time of amorphization ,
When it was confirmed only at the time of crystallization, it was 7 × 10 -5 . This is because amorphization is more reliably performed than crystallization.

上記実施例の説明は、記録または消去中における反射
光を利用して、記録または消去の確認を行う方法につい
て記載したが、透過光を利用しても、装置が複雑化する
ことを別にすれば、同様の方法により記録または消去を
確認することが可能である。
In the description of the above embodiment, a method of confirming recording or erasing using reflected light during recording or erasing is described, but even if transmitted light is used, except that the apparatus becomes complicated, It is possible to confirm recording or erasing by the same method.

〔発明の効果〕〔The invention's effect〕

上記のように本発明による情報の記録および消去方法
は、照射パワーレベルを少なくとも消去レベルと記録レ
ベルの間で変化させた単一のレーザ光を記録媒体に照射
し、情報の記録および消去を行う情報の記録および消去
方法において、上記記録媒体からの反射光の再生信号波
形を形成し、上記再生信号波形をクロックのタイミング
に基づいて分割し、該分割した再生信号波形から、上記
レーザ光の記録レベルおよび消去レベルのそれぞれの照
射時における再生信号波形をそれぞれ取り出し、取り出
した再生信号波形を別々に評価し、記録および消去をそ
れぞれ確認することにより、従来のようにディスクの回
転待ちをすることなく、リアルタイムで記録または消去
の確認ができるため、アクセス時間を短縮することがで
きる。
As described above, in the information recording and erasing method according to the present invention, the recording medium is irradiated with a single laser beam whose irradiation power level is changed at least between the erasing level and the recording level, and the information is recorded and erased. In the information recording and erasing method, a reproduction signal waveform of the reflected light from the recording medium is formed, the reproduction signal waveform is divided based on a clock timing, and the recording of the laser light is performed based on the divided reproduction signal waveform. By extracting the reproduced signal waveforms at the time of each irradiation of the level and the erase level, evaluating the extracted reproduced signal waveforms separately, and confirming the recording and erasing, respectively, without having to wait for the rotation of the disk as in the conventional case. Since recording or erasing can be confirmed in real time, access time can be reduced.

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

第1図は本発明による情報の記録および消去方法に用い
る情報記録媒体を示す断面図、第2図は上記記録媒体に
照射する単一レーザ光の波形を示す図、第3図(a)〜
(e)はクロックで取り出した高パワーレーザ光の反射
光シグナル、(f)〜(j)は上記シグナルのエラー信
号をそれぞれ示す図、第4図(a)〜(e)はそれぞれ
安定なエラー信号を得る方法を示す図、第5図(a)〜
(d)はクロックで取り出した高パワーレーザ光の反射
光シグナルをそれぞれ示す図、第6図(a)〜(e)は
それぞれ安定なエラー信号を得る方法を示す図、第7図
(a)〜(c)はクロックで取り出した低パワーレーザ
光の反射光シグナル、(d)〜(f)は上記シグナルの
エラー信号をそれぞれ示す図である。 3……記録媒体 5,6……レーザスポット
FIG. 1 is a cross-sectional view showing an information recording medium used in the information recording and erasing method according to the present invention, FIG. 2 is a diagram showing a waveform of a single laser beam applied to the recording medium, and FIGS.
(E) shows a reflected light signal of the high-power laser light extracted by the clock, (f) to (j) show error signals of the above signals, and FIGS. 4 (a) to (e) show stable errors, respectively. FIG. 5A to FIG. 5D show a method for obtaining a signal.
(D) is a diagram showing a reflected light signal of a high-power laser beam taken out by a clock, FIGS. 6 (a) to (e) are diagrams showing a method of obtaining a stable error signal, and FIG. 7 (a). (C) is a diagram showing a reflected light signal of a low-power laser beam extracted by a clock, and (d) to (f) are diagrams showing an error signal of the signal. 3… Recording medium 5,6… Laser spot

───────────────────────────────────────────────────── フロントページの続き (72)発明者 太田 憲雄 国分寺市東恋ヶ窪1丁目280番地 株式 会社日立製作所中央研究所内 (72)発明者 角田 義人 国分寺市東恋ヶ窪1丁目280番地 株式 会社日立製作所中央研究所内 (72)発明者 賀来 敏光 国分寺市東恋ヶ窪1丁目280番地 株式 会社日立製作所中央研究所内 (72)発明者 安藤 圭吉 国分寺市東恋ヶ窪1丁目280番地 株式 会社日立製作所中央研究所内 (56)参考文献 特開 昭53−6516(JP,A) 特開 昭59−58633(JP,A) ──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Norio Ota 1-280 Higashi-Koigabo, Kokubunji City, Hitachi, Ltd. Central Research Laboratory Co., Ltd. 72) Inventor Toshimitsu Kaku 1-280 Higashi Koigabo, Kokubunji City, Hitachi, Ltd. Central Research Laboratory Co., Ltd. (72) Inventor Keikichi Ando 1-280 Higashi Koigabo, Kokubunji City, Hitachi Central Research Laboratory Co., Ltd. 53-6516 (JP, A) JP-A-59-558633 (JP, A)

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】照射パワーレベルを少なくとも消去レベル
と記録レベルの間で変化させた単一のレーザ光を記録媒
体に照射し、情報の記録および消去を行う情報の記録お
よび消去方法において、上記記録媒体からの反射光の再
生信号波形を形成し、上記再生信号波形をクロックのタ
イミングに基づいて分割し、該分割した再生信号波形か
ら、上記レーザ光の記録レベルおよび消去レベルのそれ
ぞれの照射時における再生信号波形をそれぞれ取り出
し、取り出した再生信号波形を別々に評価し、記録およ
び消去をそれぞれ確認することを特徴とする情報の記録
および消去方法。
An information recording and erasing method for irradiating a recording medium with a single laser beam whose irradiation power level is changed at least between an erasing level and a recording level to record and erase information. A reproduction signal waveform of the reflected light from the medium is formed, the reproduction signal waveform is divided based on the clock timing, and the divided reproduction signal waveforms are used to irradiate the recording level and the erasing level of the laser light, respectively. A method of recording and erasing information, comprising extracting a reproduced signal waveform, separately evaluating the extracted reproduced signal waveform, and confirming recording and erasing, respectively.
JP62014161A 1987-01-26 1987-01-26 How to record and erase information Expired - Fee Related JP2571776B2 (en)

Priority Applications (7)

Application Number Priority Date Filing Date Title
JP62014161A JP2571776B2 (en) 1987-01-26 1987-01-26 How to record and erase information
KR1019880000459A KR910003039B1 (en) 1987-01-26 1988-01-22 Record playback method of information
CN 90103304 CN1017841B (en) 1987-01-26 1988-01-26 Method for recording and reproducing information
CN88100345A CN88100345A (en) 1987-01-26 1988-01-26 Method of recording and reproducing information
DE3851239T DE3851239T2 (en) 1987-01-26 1988-01-26 Information recording and playback method.
EP88101099A EP0276808B1 (en) 1987-01-26 1988-01-26 Method of recording and reproducing information
US07/634,049 US5404348A (en) 1987-01-26 1990-12-26 Method for recording and reproducing information using at least two energy beams

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62014161A JP2571776B2 (en) 1987-01-26 1987-01-26 How to record and erase information

Publications (2)

Publication Number Publication Date
JPS63183624A JPS63183624A (en) 1988-07-29
JP2571776B2 true JP2571776B2 (en) 1997-01-16

Family

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JP62014161A Expired - Fee Related JP2571776B2 (en) 1987-01-26 1987-01-26 How to record and erase information

Country Status (1)

Country Link
JP (1) JP2571776B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4924436A (en) * 1987-06-22 1990-05-08 Energy Conversion Devices, Inc. Data storage device having a phase change memory medium reversible by direct overwrite and method of direct overwrite
JP2638149B2 (en) * 1988-10-21 1997-08-06 松下電器産業株式会社 Optical information recording / erasing method
US6252844B1 (en) 1996-09-13 2001-06-26 Nec Corporation Phase-change type optical recording medium and method of optically recording with the same

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS536516A (en) * 1976-07-08 1978-01-21 Matsushita Electric Ind Co Ltd Optical recording and reproducing unit
JPS5958633A (en) * 1982-09-29 1984-04-04 Hitachi Ltd Optical disc device

Also Published As

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