JPS6361199B2 - - Google Patents

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Publication number
JPS6361199B2
JPS6361199B2 JP55181862A JP18186280A JPS6361199B2 JP S6361199 B2 JPS6361199 B2 JP S6361199B2 JP 55181862 A JP55181862 A JP 55181862A JP 18186280 A JP18186280 A JP 18186280A JP S6361199 B2 JPS6361199 B2 JP S6361199B2
Authority
JP
Japan
Prior art keywords
recording
track
optical
information
light
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
Application number
JP55181862A
Other languages
Japanese (ja)
Other versions
JPS57105394A (en
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 filed Critical
Priority to JP55181862A priority Critical patent/JPS57105394A/en
Publication of JPS57105394A publication Critical patent/JPS57105394A/en
Publication of JPS6361199B2 publication Critical patent/JPS6361199B2/ja
Granted 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
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • 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
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/252Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers
    • G11B7/253Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates
    • G11B7/2531Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates comprising glass
    • 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
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/252Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers
    • G11B7/253Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates
    • G11B7/2533Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates comprising resins

Landscapes

  • Optical Record Carriers And Manufacture Thereof (AREA)
  • Optical Recording Or Reproduction (AREA)
  • Thermal Transfer Or Thermal Recording In General (AREA)

Description

【発明の詳細な説明】 本発明は、熱によつて黒化する膜、例えば放電
重合膜、スパツタ膜または蒸着膜によつて形成し
た光学記録媒体およびこの記録媒体を用いて、記
録媒体上に光学的コントラストを有する記録トラ
ツクおよび情報を記録する光学記録方法に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides an optical recording medium formed of a film that is blackened by heat, such as a discharge polymerized film, a sputtered film, or a vapor-deposited film, and an optical recording medium formed by using this recording medium. The present invention relates to a recording track having optical contrast and an optical recording method for recording information.

レーザビーム等による光の熱的効果を利用する
ヒートモード記録方式は経年変化がなく実時間で
追加記録が可能である等の特長を有している。従
来、この種の光学記録を行う記録媒体としては、
基板上に染料およびバインダで記録層を形成した
もの(例えば、米国特許明細書第1117419号)や、
金属薄膜、金属酸化物またはカルコゲナイトガラ
ス層を記録層として用いる媒体(例えば、M.L、
Venene“Electron、Ion and Laser Beam Tech
nology”第11回シンポジウム記録(1969)、
Electronics誌1968、3、18日号p.50、特開昭50
−46317号公報)が知られている。
The heat mode recording method, which utilizes the thermal effect of light such as a laser beam, has features such as no deterioration over time and the ability to perform additional recording in real time. Conventionally, recording media for this type of optical recording are:
A recording layer formed with a dye and a binder on a substrate (for example, US Pat. No. 1,117,419),
Media that use a metal thin film, metal oxide or chalcogenite glass layer as the recording layer (e.g. ML,
Venene “Electron, Ion and Laser Beam Tech
"11th Symposium Record (1969),
Electronics magazine 1968, 3rd, 18th issue p.50, Japanese Patent Application Publication No. 1973
-46317) is known.

しかし、これらの記録媒体では記録に必要なエ
ネルギーが高く、大型のArレーザ等の高出力光
源、変調偏光器を必要とする欠点があつた。この
ような欠点を克服するために、小型で変調が電気
的に容易な半導体レーザに適用可能な高感度の光
学記録材料を開発すると共に、多層膜構造など媒
体構成上からも工夫をこらし、信号対雑音比、記
録安定性、取扱い性等に優れた記録媒体を得る試
みがなされている。
However, these recording media have disadvantages in that they require high energy for recording, require a high-output light source such as a large Ar laser, and a modulation polarizer. In order to overcome these drawbacks, we have developed highly sensitive optical recording materials that can be applied to semiconductor lasers that are small and electrically easy to modulate, and have also devised medium configurations such as multilayer structures to improve the signal strength. Attempts have been made to obtain recording media with excellent noise-to-noise ratio, recording stability, ease of handling, and the like.

このような光学記録媒体における情報密度およ
び書き込み・読み出し速度の向上を図るためには
記録ピツトを小さくするのみならず、記録部にト
ラツクを設けることが有効である。また、記録ト
ラツクが存在することにより書き込み・読み出し
ヘツドの追従も容易となる。そこで、機械的に記
録トラツクを設ける方式としてはレコード盤方式
の溝付きトレース方式があるが、これはランダム
アクセスの記録再生には困難である。したがつ
て、光学的な記録トラツクを容易に設けることが
でき、かつ高感度な光学記録媒体および記録方法
の開発が望まれていた。
In order to improve the information density and the writing/reading speed of such optical recording media, it is effective not only to make the recording pits smaller, but also to provide tracks in the recording section. Also, the presence of recording tracks makes it easier for write/read heads to follow. Therefore, as a method for mechanically providing recording tracks, there is a grooved trace method used in the record disc method, but this method is difficult for random access recording and reproduction. Therefore, it has been desired to develop a highly sensitive optical recording medium and recording method in which optical recording tracks can be easily provided.

本発明の目的は、上述した従来の欠点を除去し
て、光学的コントラストを有する記録トラツクを
形成し、その記録トラツク上に情報ピツトを記録
することができる光学記録媒体を提供することに
ある。
SUMMARY OF THE INVENTION It is an object of the present invention to provide an optical recording medium capable of eliminating the above-mentioned conventional drawbacks, forming a recording track having optical contrast, and recording information pits on the recording track.

本発明の他の目的は、上述した従来の問題点を
解決するために、光学記録媒体上に容易に光学的
コントラストを有する記録トラツクを設けること
ができ、次いでその記録トラツク上への情報ピツ
トの記録感度を向上させることのできる光学記録
媒体の情報記録方法を提案することにある。
Another object of the present invention is to easily provide a recording track having optical contrast on an optical recording medium, and then to place information pits on the recording track, in order to solve the above-mentioned conventional problems. The object of the present invention is to propose an information recording method for an optical recording medium that can improve recording sensitivity.

本発明光学記録媒体は、基板を有し、基板上に
熱によつて黒化する膜による記録層を被着し、記
録層に黒化に必要なエネルギー密度を持つトラツ
ク記録光を照射することによりトラツク記録光照
射部分に黒化したストライプ状の記録トラツクを
形成し、記録トラツク上にトラツク記録光より高
いエネルギー密度を持つ情報ピツト記録光を照射
することにより情報ピツト記録光照射部分を溶融
蒸発させて情報ピツトを記録可能となしたことを
特徴とする。
The optical recording medium of the present invention has a substrate, a recording layer made of a film that is blackened by heat is deposited on the substrate, and the recording layer is irradiated with track recording light having an energy density necessary for blackening. A blackened striped recording track is formed on the track recording light irradiated area, and by irradiating the information pit recording light with a higher energy density than the track recording light onto the recording track, the information pit recording light irradiated area is melted and evaporated. The invention is characterized in that the information pit can be recorded.

本発明光学記録方法では、熱によつて黒化する
膜により形成した記録層を有する光学記録媒体上
に、黒化に必要なエネルギー密度のトラツク記録
光で記録すべき記録トラツクのパタンを走査し、
パタンに沿つて黒化により光学的コントラストを
有するストライプ状の記録トラツクを形成し、次
いで、書き込み・読み出しヘツドを記録トラツク
に追従させながらトラツク記録光よりも高いエネ
ルギー密度の情報ピツト記録光パルスにより記録
トラツク上の記録層を溶融蒸発させて情報ピツト
を記録することを特徴とする。
In the optical recording method of the present invention, a recording track pattern to be recorded is scanned on an optical recording medium having a recording layer formed of a film that is blackened by heat using track recording light having an energy density necessary for blackening. ,
A striped recording track with optical contrast is formed by blackening along the pattern, and then recording is performed using an information pit recording light pulse having a higher energy density than the track recording light while making the write/read head follow the recording track. It is characterized by recording information pits by melting and evaporating the recording layer on the track.

以下、図面について本発明を詳細に説明する。 Hereinafter, the invention will be explained in detail with reference to the drawings.

第1図は本発明の記録に用いる媒体の一例を示
し、ここで、11は基板、12は熱によつて黒化
する膜としての放電重合膜あるいはスパツタ膜で
ある。基板11としてはガラスまたは透明プラス
チツク板を用いることができる。熱によつて黒化
する放電重合膜あるいはスパツタ膜12において
は、薄膜自身が記録光を吸収する性質を持つてい
る。
FIG. 1 shows an example of a medium used for recording according to the present invention, where 11 is a substrate, and 12 is a discharge polymerized film or a sputtered film as a film that is blackened by heat. As the substrate 11, a glass or transparent plastic plate can be used. In the discharge polymerized film or sputtered film 12 which is blackened by heat, the thin film itself has the property of absorbing recording light.

本発明では、この媒体上に、まず低いエネルギ
ー密度の記録光で記録すべき記録トラツクのパタ
ンを走査する。この記録光によつて薄膜12は黒
化現象を起こして、第2図に示すように、媒体上
にストライプ状の光学的コントラストを持つたト
ラツク23が形成される。かかるトラツク23の
記録を行うにあたつては、情報ピツト24の記録
光より低いエネルギー密度の記録光を低速度で走
査する。それによつて光学記録媒体には情報ピツ
ト24の記録閾値の数倍程度のエネルギーが加え
られるが、単位時間あたりに加えられるエネルギ
ー量が少ないために、媒体には昇華や蒸発のよう
な現象は起こらず、黒化のみが起こり、熱によつ
て黒化したストライプ状のトラツク23のみが形
成される。このようなストライプ状のコントラス
トの発生により記録したトラツク部分は、未記録
部分より高い吸収係数を持つことが可能となり、
以下の情報ピツト24の記録の際に記録トラツク
23上では情報ピツト24の記録感度が高められ
る。なお、トラツク記録に用いられる黒化現象は
薄膜の性質変化に基づくもので、表面形状などの
幾何学的変化を伴うものではない。
In the present invention, a recording track pattern to be recorded is first scanned onto the medium using recording light of low energy density. This recording light causes the thin film 12 to undergo a blackening phenomenon, and as shown in FIG. 2, tracks 23 having a stripe-like optical contrast are formed on the medium. When recording such a track 23, recording light having a lower energy density than the recording light of the information pit 24 is scanned at a low speed. As a result, energy several times the recording threshold of the information pit 24 is applied to the optical recording medium, but since the amount of energy applied per unit time is small, phenomena such as sublimation and evaporation do not occur in the medium. At first, only blackening occurs, and only striped tracks 23 blackened by heat are formed. Due to the generation of such striped contrast, the recorded track portion can have a higher absorption coefficient than the unrecorded portion.
During the following recording of the information pits 24, the recording sensitivity of the information pits 24 on the recording track 23 is increased. Note that the blackening phenomenon used in track recording is based on changes in the properties of the thin film, and is not accompanied by geometric changes such as surface shape.

次に、このストライプ状に黒化したトラツク2
3上に光パルスによつて情報ピツト24を記録す
る。この場合の情報ピツト記録光としては、先に
述べたトラツク記録光より高いエネルギー密度で
あり、しかも持続時間の極めて短いパルス光を用
いる。パルス光照射された媒体薄膜は昇華、蒸発
あるいは融解して、小孔状のピツト24を形成す
る。この情報ピツト24はその周囲部分に対して
透過率または反射率の差異が著しい。
Next, track 2, which is blackened in stripes,
3, information pits 24 are recorded by light pulses. As the information pit recording light in this case, pulsed light having a higher energy density than the track recording light described above and an extremely short duration is used. The medium thin film irradiated with pulsed light sublimates, evaporates or melts, forming small pore-like pits 24. This information pit 24 has a significant difference in transmittance or reflectance with respect to its surrounding parts.

第3図は本発明による情報記録の過程において
得られた透過光読み出し形での光学コントラスト
を示す。31は未記録の光記録媒体の光学的コン
トラスト、32はトラツク23の記録後の光学的
コントラスト、33はピツト24の書き込み後の
光記録媒体の光学的コントラストを示す。
FIG. 3 shows the optical contrast obtained in the process of recording information according to the present invention in a transmitted light readout mode. 31 shows the optical contrast of the unrecorded optical recording medium, 32 shows the optical contrast of the optical recording medium after the tracks 23 are recorded, and 33 shows the optical contrast of the optical recording medium after the pits 24 are written.

第4図は本発明の光学記録に用いる媒体の他の
例を示し、ここで、41は基板、42は基板41
上に形成した反射層、43は反射層42上の放電
膜あるいは蒸着膜、44は膜43に被着した保護
層である。基板41としては、ガラス板、プラス
チツク板、アルミニウム板、セラミツク板等を用
いることができる。
FIG. 4 shows another example of the medium used for optical recording of the present invention, where 41 is a substrate, and 42 is a substrate 41.
The reflective layer 43 formed on the reflective layer 42 is a discharge film or a vapor deposited film, and 44 is a protective layer deposited on the film 43. As the substrate 41, a glass plate, a plastic plate, an aluminum plate, a ceramic plate, etc. can be used.

第5図は第4図示の記録媒体にトラツクおよび
ピツトを記録したトラツクおよびピツトの形成状
態を示し、ここで、53は記録トラツク部分、5
4は記録ピツトであり、それぞれ上述したように
して形成する。
FIG. 5 shows the formation state of tracks and pits recorded on the recording medium shown in FIG. 4, where 53 is a recorded track portion;
Reference numeral 4 indicates recording pits, each of which is formed as described above.

第6図は本発明光学式記録方法の過程において
得られた反射光読み出し形での光学的コントラス
トを示す。61は未記録の光記録媒体の光学的コ
ントラスト、62はトラツク記録後の光学的コン
トラスト、63はピツト書き込み後の光学的コン
トラストをそれぞれ示す。
FIG. 6 shows the optical contrast in the reflected light readout method obtained in the process of the optical recording method of the present invention. 61 shows the optical contrast of an unrecorded optical recording medium, 62 shows the optical contrast after track recording, and 63 shows the optical contrast after pit writing.

なお、反射形読み出しの光学記録媒体では、記
録層43と反射層42との間に光干渉層を介在さ
せて形成した無反射構造の光学記録媒体を用いて
も、本発明による情報記録方法を用いることがで
きる。
In addition, in a reflective readout optical recording medium, even if an optical recording medium with a non-reflective structure formed by interposing an optical interference layer between the recording layer 43 and the reflective layer 42 is used, the information recording method according to the present invention can be applied. Can be used.

本発明によつて記録されたトラツクおよび情報
ピツトを読み出す原理は次の通りである。
The principle of reading tracks and information pits recorded according to the present invention is as follows.

透過読み出し形では、記録された光学記録媒体
は第3図に示した光学コントラスト33を持つの
で、トラツク23の自動追従機構(トラツキン
グ・サーボ)は情報ピツト24の幅より外側のト
ラツク余剰部で最低透過光量を得るように作動し
て、情報ピツト24が読み出される。
In the transmission readout type, the recorded optical recording medium has the optical contrast 33 shown in FIG. The information pit 24 is read out by operating to obtain the amount of transmitted light.

反射読み出し形では、第6図に示した光学コン
トラスト63を持つので、トラツク53のトラツ
キング・サーボは情報ピツト54の幅より外側の
トラツク余剰部で最低反射光量を得るように作動
して、情報ピツト54が読み出される。
Since the reflective readout type has the optical contrast 63 shown in FIG. 6, the tracking servo of the track 53 operates to obtain the minimum amount of reflected light in the surplus portion of the track outside the width of the information pit 54. 54 is read out.

次に、本発明により情報記録を行つた記録媒体
における情報のトラツク方向における記録状態を
第8図および第9図に示す。第8図は反射光読み
出し形の記録媒体の例を示し、ここで81は未記
録部分、82はトラツク記録部、83は情報記録
部を示す。トラツク記録部82中のトラツク方向
で最初のピツトブロツク84はトラツク自体の識
別用情報を記録したヘツデイング用情報ピツトで
あり、この情報ピツト84に引続いて記録すべき
情報が情報ピツト85に書き込まれている。第9
図は透過光読み出し形の記録媒体の例を示し、こ
こで91は未記録部分、92はトラツク記録部、
93は情報記録部を示す。トラツク記録部92中
のトラツク方向で最初のピツトブロツク94はト
ラツク自体の識別用情報を記録したヘツデイング
用情報ピツトであり、この情報ピツト94に引続
いて記録すべき情報が情報ピツト95に書き込ま
れている。
Next, FIGS. 8 and 9 show the recording state of information in the track direction on a recording medium on which information is recorded according to the present invention. FIG. 8 shows an example of a reflective light readout type recording medium, where 81 is an unrecorded portion, 82 is a track recording section, and 83 is an information recording section. The first pit block 84 in the track direction in the track recording section 82 is a heading information pit in which identification information of the track itself is recorded. Information to be recorded following this information pit 84 is written in an information pit 85. There is. 9th
The figure shows an example of a transmitted light readout type recording medium, where 91 is an unrecorded part, 92 is a track recording part,
93 indicates an information recording section. The first pit block 94 in the track direction in the track recording section 92 is a heading information pit in which identification information of the track itself is recorded. Information to be recorded following this information pit 94 is written in an information pit 95. There is.

次に、本発明方法を実施するにあたつて用いた
記録媒体の具体例について述べる。
Next, a specific example of the recording medium used in carrying out the method of the present invention will be described.

実施例 1 基板としてガラスを用い、CS2ガスを1×
10-2Torr導入した容器中で、電極に13.56MHzの
高周波放電を行つた。その放電は、放電電力
120W、基板温度50℃、ガス流量10c.c./分で10分
間行つた。この放電中に1.5Å/secの蒸着速度で
Teを蒸着したところ、Teを含有した膜厚約0.2μ
mの薄膜が形成された。
Example 1 Using glass as the substrate, 1x CS2 gas
A high frequency discharge of 13.56 MHz was applied to the electrode in a container introduced with 10 -2 Torr. Its discharge is the discharge power
The test was carried out for 10 minutes at 120W, substrate temperature 50°C, and gas flow rate 10c.c./min. During this discharge, at a deposition rate of 1.5 Å/sec,
When Te was deposited, the film thickness containing Te was approximately 0.2μ.
A thin film of m was formed.

このようにして得られた記録前の薄膜の吸収ス
ペクトルは第7図の曲線aに示すようになつた。
次に、この薄膜を加熱して黒化させた。記録後の
黒化部の吸収スペクトルは第7図の曲線bに示す
ようになつた。第7図からわかるように、レーザ
光加熱によるトラツク記録操作により、光学コン
トラストの大きい良好なトラツク記録を行うこと
ができることが確認できた。実際に、パワー0.6
mWの半導体レーザ光(波長830nm)を約100m
J/cm2照射することによりトラツクを記録でき
た。このようにして記録したトラツク上に出力6
mWの半導体レーザ光パルス(1.2×2.0μm径)
を照射すると、持続時間100nsecのパルスで情報
ピツトの記録が可能であつた。これはエネルギー
密度に換算すると、約30mJ/cm2の感度であつ
た。記録したトラツク以外の場所に直接情報ピツ
トを記録する場合の感度は約40mJ/cm2に相当し
ていた。
The absorption spectrum of the thin film thus obtained before recording was as shown by curve a in FIG. 7.
Next, this thin film was heated to blacken it. The absorption spectrum of the blackened area after recording was as shown by curve b in FIG. As can be seen from FIG. 7, it was confirmed that good track recording with high optical contrast could be performed by the track recording operation using laser beam heating. In fact, power 0.6
mW semiconductor laser light (wavelength 830nm) about 100m
Tracks could be recorded by irradiating with J/cm 2 . Output 6 on the track recorded in this way.
mW semiconductor laser light pulse (1.2 x 2.0 μm diameter)
When irradiated with , it was possible to record information pits with a pulse duration of 100 ns. This was a sensitivity of approximately 30 mJ/cm 2 when converted into energy density. The sensitivity when directly recording information pits in locations other than the recorded tracks was equivalent to approximately 40 mJ/cm 2 .

実施例 2 アクリル基板上に実施例1と同様の条件でCS2
ガスを導入して高周波放電を行つた。その放電中
に、1.4Å/secの蒸着速度でBiを蒸着してBiを含
有した膜厚約0.2μmの薄膜を形成した。この薄膜
について反射光を測定すると、波長830nmで約
30%であつた。この媒体上に実施例1と同様にし
てトラツクを記録した。その黒化によつてトラツ
ク上の反射率は50%に上昇した。更にレーザパル
スによる情報ピツトを実施例1と同様にして記録
した。記録部の溶融蒸発によつて反射率は5%に
低下した。トラツク記録の感度は100mJ/cm2
情報ビツトの感度は50mJ/cm2であつた。
Example 2 CS 2 was deposited on an acrylic substrate under the same conditions as Example 1.
A high-frequency discharge was performed by introducing gas. During the discharge, Bi was deposited at a deposition rate of 1.4 Å/sec to form a thin film containing Bi with a thickness of about 0.2 μm. When measuring the reflected light of this thin film, at a wavelength of 830 nm, approximately
It was 30%. Tracks were recorded on this medium in the same manner as in Example 1. Due to the blackening, the reflectance on the track increased to 50%. Furthermore, information pits were recorded using laser pulses in the same manner as in Example 1. The reflectance decreased to 5% due to melting and evaporation of the recorded portion. The sensitivity of track recording is 100mJ/cm 2 ,
The sensitivity of the information bit was 50 mJ/cm 2 .

実施例 3 基板としてガラス板を用い、反射層としてAl
を約5000Åの厚さに蒸着した。この上にCS2の放
電重合膜を3000Åの厚さに形成し、更に実施例1
と同様にTeを含有したCS2放電重合膜を約100Å
の膜厚に形成した。その結果、光学記録媒体は多
重干渉を利用した無反射構造となり、波長830n
mでの反射率は約20%となつた。この光学記録媒
体に波長830nmでパワー0.6mWの半導体レーザ
光によりトラツクを記録した。かかるトラツクの
記録によつてトラツク上での反射率は5%以下に
低下し、トラツクの記録感度は50mJ/cm2であつ
た。次に、トラツク上に情報ピツトを記録した。
その場合に、波長830nm、ビーム径1.2×2.0μm、
パワー6mWの半導体レーザを用いると持続時間
15nsecのパルスで記録が可能であつた。これはエ
ネルギー密度にして約5m/Jcm2の感度であつ
た。
Example 3 A glass plate was used as the substrate, and Al was used as the reflective layer.
was deposited to a thickness of approximately 5000 Å. On top of this, a discharge polymerized film of CS 2 was formed to a thickness of 3000 Å, and then Example 1
Similarly, a CS 2 discharge polymerized film containing Te is approximately 100 Å thick.
It was formed to a film thickness of . As a result, the optical recording medium has a non-reflection structure that utilizes multiple interference, and has a wavelength of 830n.
The reflectance at m was about 20%. Tracks were recorded on this optical recording medium using a semiconductor laser beam with a wavelength of 830 nm and a power of 0.6 mW. By recording on such a track, the reflectance on the track was reduced to 5% or less, and the recording sensitivity of the track was 50 mJ/cm 2 . Next, information pits were recorded on the track.
In that case, the wavelength is 830 nm, the beam diameter is 1.2 x 2.0 μm,
When using a semiconductor laser with a power of 6mW, the duration
Recording was possible with a pulse of 15 nsec. This had a sensitivity of about 5 m/Jcm 2 in terms of energy density.

実施例 4 基板としてガラス板を用い、As8Te75G17の組
成を持つカルコゲナイトガラスをターゲツトと
し、容器中にArを10-2Torr導入し、13.56MHzの
高周波でスパツタリングを行つて基板上に
As7Te77G16の組成のカルコゲナイトガラスの薄
膜を約2000Åの厚さに形成した。これを光学記録
媒体として、波長830nmでパワー1mWの半導
体レーザ光でトラツクを記録した。トラツク記録
の感度は300mJ/cm2であつた。更に、このトラ
ツク上に波長830nm、ビーム径1.2×2.0μm径、
パワー6mWの半導体レーザを用いて情報ピツト
を記録した。情報ピツトの記録感度は約100m
J/cm2であつた。記録したトラツク以外の場所に
直接に情報ピツトを記録した場合の感度は約200
mJ/cm2であつた。
Example 4 Using a glass plate as a substrate, targeting chalcogenite glass with a composition of As 8 Te 75 G 17 , introducing Ar into a container at 10 -2 Torr and performing sputtering at a high frequency of 13.56 MHz to prepare the substrate. above
A thin film of chalcogenite glass having a composition of As 7 Te 77 G 16 was formed to a thickness of about 2000 Å. Using this as an optical recording medium, tracks were recorded using a semiconductor laser beam with a wavelength of 830 nm and a power of 1 mW. The sensitivity of track recording was 300 mJ/cm 2 . Furthermore, on this track, a beam with a wavelength of 830 nm and a beam diameter of 1.2 x 2.0 μm,
Information pits were recorded using a semiconductor laser with a power of 6 mW. The recording sensitivity of the information pit is approximately 100m.
It was J/ cm2 . The sensitivity is approximately 200 when recording information pits directly in a location other than the recorded track.
It was mJ/ cm2 .

実施例 5 基板としてガラス板を用い、Te80Ge14Sb3S3
組成を持つカルコゲナイトガラスをターゲツトと
し、実施例4と同様にスパツタリングを行つて、
基板上にTe81Ge15Sb2S2の組成を持つカルコゲナ
イトガラスの薄膜を約2000Åの厚さに形成した。
この光学記録媒体に実施例4と同様にして半導体
レーザ光でトラツクを記録したところ、トラツク
記録感度300mJ/cm2を得た。更に、実施例4と
同様にして情報ピツトを記録したところ、その感
度は100mJ/cm2であつた。
Example 5 Using a glass plate as a substrate and targeting chalcogenite glass having a composition of Te 80 Ge 14 Sb 3 S 3 , sputtering was performed in the same manner as in Example 4.
A thin film of chalcogenite glass having a composition of Te 81 Ge 15 Sb 2 S 2 was formed on a substrate to a thickness of about 2000 Å.
When tracks were recorded on this optical recording medium using a semiconductor laser beam in the same manner as in Example 4, a track recording sensitivity of 300 mJ/cm 2 was obtained. Furthermore, when information pits were recorded in the same manner as in Example 4, the sensitivity was 100 mJ/cm 2 .

実施例 6 基板としてガラス板を用い、反射層としてAl
を約5000Åの厚さに蒸着した。この上にCS2の放
電重合膜を2800Åの厚さに形成し、更に実施例1
と同様にTeを含有したCS2の放電重合膜を約100
Åの膜厚に形成した。その結果、光学記録媒体は
多重干渉を利用した無反射構造となり、波長
750nmでの反射率は5%以下となつた。波長
830nmでの反射率は約20%であつた。この光学
記録媒体に波長750nmの半導体レーザ(ビーム
径3.0mmφ、パワー1mW)を用いてトラツクを
記録した。この記録感度は50mJ/cm2であつた。
これによつてトラツク部の波長750nmでの反射
率は約20%に増加したが、波長830nmでの反射
率は5%以下に減少した。次に、このトラツク上
に波長830nmの半導体レーザ(ビーム径1.2×
2.0μm、パワー6mW)を用いて情報ピツトをパ
ルス光で記録した。持続時間15nsecのパルスで記
録が可能であつた。これはエネルギー密度にして
約5mJ/cm2の感度であつた。
Example 6 A glass plate was used as the substrate, and Al was used as the reflective layer.
was deposited to a thickness of approximately 5000 Å. On top of this, a discharge polymerized film of CS 2 was formed to a thickness of 2800 Å, and further Example 1
Similarly, about 100% of the discharge polymerized film of CS 2 containing Te was
The film was formed to a film thickness of 1.5 Å. As a result, the optical recording medium has a non-reflective structure that utilizes multiple interference, and the wavelength
The reflectance at 750 nm was less than 5%. wavelength
The reflectance at 830 nm was about 20%. Tracks were recorded on this optical recording medium using a semiconductor laser with a wavelength of 750 nm (beam diameter 3.0 mmφ, power 1 mW). The recording sensitivity was 50 mJ/cm 2 .
As a result, the reflectance of the track portion at a wavelength of 750 nm increased to approximately 20%, but the reflectance at a wavelength of 830 nm decreased to less than 5%. Next, a semiconductor laser with a wavelength of 830 nm (beam diameter 1.2 ×
Information pits were recorded with pulsed light using a beam of 2.0 μm and a power of 6 mW. Recording was possible with a pulse duration of 15 nsec. This had a sensitivity of about 5 mJ/cm 2 in terms of energy density.

実施例 7 基板としてガラスを用い、スチレン・モノマを
ガス状にして1×10-2Torr導入した容器中で、
電極に13.56MHzの高周波放電を行つた。放電は
放電電力120W、基板温度を室温としてガス流量
15c.c./分で10分間行つた。この放電中に1.5Å/
secの蒸着温度でTeを蒸着したところ、Teを含
有した膜厚約0.2μmの薄膜が形成された。この
Teを含有したスチレンプラズマ重合膜に波長
830nmの半導体レーザ光を0.6mWのパワーで約
100mJ/cm2照射することによつてトラツクを記
録した。このトラツク上にパワー6mWの半導体
レーザ光のパルス(1.2×2.0μm径)を照射する
と、持続時間150nsecのパルスで情報ピツトを記
録できた。これはエネルギー密度に換算して約45
mJ/cm2の感度であつた。
Example 7 Using glass as a substrate, styrene monomer was made into a gas and introduced at 1×10 -2 Torr in a container.
A high frequency discharge of 13.56MHz was applied to the electrode. The discharge power is 120W, the substrate temperature is room temperature, and the gas flow rate is
It ran for 10 minutes at 15c.c./min. 1.5Å/during this discharge
When Te was deposited at a deposition temperature of sec, a thin film containing Te with a thickness of about 0.2 μm was formed. this
Wavelength of Te-containing styrene plasma polymerized film
Approximately 830nm semiconductor laser light with 0.6mW power
Tracks were recorded by irradiating with 100 mJ/cm 2 . When this track was irradiated with a pulse of semiconductor laser light (1.2 x 2.0 μm diameter) with a power of 6 mW, information pits could be recorded with a pulse duration of 150 nsec. This is approximately 45 in terms of energy density.
The sensitivity was mJ/cm 2 .

以上説明したように、本発明による光学記録媒
体の光学式情報記録方法によれば、光学的コント
ラストを有するトラツクを容易に作製でき、かつ
記録したトラツク上の情報ピツトの記録感度をも
向上させることができる。すなわち、本発明によ
れば、幾何学的形状変化を伴うことなく光学記録
媒体にトラツクを形成することができるので、か
かるトラツクにより情報の読み出し、書き込み時
に記録媒体上の各点へ容易にランダムアクセスす
ることが可能となる。
As explained above, according to the optical information recording method for an optical recording medium according to the present invention, a track having optical contrast can be easily produced, and the recording sensitivity of information pits on the recorded track can also be improved. I can do it. That is, according to the present invention, a track can be formed on an optical recording medium without changing the geometric shape, so that it is possible to easily randomly access each point on the recording medium using such a track when reading or writing information. It becomes possible to do so.

また、本発明によれば、記録したトラツク上の
情報ピツト記録感度が向上するので、情報記録を
より高速に行えると同時に、トラツク部以外への
露光等の記録ミスも少なくすることができる利点
がある。
Further, according to the present invention, the sensitivity for recording information pits on recorded tracks is improved, so information can be recorded at a higher speed, and at the same time, recording errors such as exposure to areas other than the track areas can be reduced. be.

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

第1図は本発明光学記録媒体の構成の一例を示
す断面図、第2図は第1図示の光学記録媒体に本
発明によりトラツクおよび情報ピツトを記録した
状態を示す斜視図、第3図は透過光読み出し形の
記録状態の光学的コントラストを示す図、第4図
は本発明光学記録媒体の他の例を示す断面図、第
5図は第4図示の光学記録媒体に本発明によりト
ラツクおよび情報ピツトを記録した状態を示す斜
視図、第6図は反射光読み出し形の記録状態の光
学的コントラストを示す図、第7図は加熱黒化部
のスペクトル変化を示す特性曲線図、第8図およ
び第9図は本発明により情報を光学記録媒体に記
録した状態を示す図である。 11……基板、12……熱によつて黒化する物
質を含む放電重合膜あるいは蒸着膜、23……記
録されたトラツク部、24……記録された情報ピ
ツト、31……未記録媒体の光学的コントラス
ト、32……トラツク記録後の記録媒体の光学的
コントラスト、33……情報記録後の記録媒体の
光学的コントラスト、41……基板、42……反
射層、43……熱によつて黒化する物質を含む放
電重合膜あるいは蒸着膜、44……保護層、53
……記録されたトラツク部、54……記録された
ピツト、61……未記録媒体の光学的コントラス
ト、62……トラツク記録後の記録媒体の光学的
コントラスト、63……情報記録後の記録媒体の
光学的コントラスト、81……未記録部、82…
…トラツク記録部、83……情報記録部、84…
…トラツク用情報ピツト(ヘツデイング)、85
……情報記録用ピツト、91……未記録部、92
……トラツク記録部、93……情報記録部、94
……トラツク用情報ピツト(ヘツデイング)、9
5……情報記録用ピツト。
FIG. 1 is a cross-sectional view showing an example of the structure of the optical recording medium of the present invention, FIG. 2 is a perspective view showing the state in which tracks and information pits are recorded on the optical recording medium shown in FIG. 1 according to the present invention, and FIG. FIG. 4 is a sectional view showing another example of the optical recording medium of the present invention, and FIG. 5 is a diagram showing the optical contrast of the recorded state of the transmitted light readout type. FIG. FIG. 6 is a perspective view showing the state in which information pits are recorded. FIG. 6 is a diagram showing the optical contrast of the recorded state of reflected light readout type. FIG. and FIG. 9 is a diagram showing a state in which information is recorded on an optical recording medium according to the present invention. DESCRIPTION OF SYMBOLS 11...Substrate, 12...Discharge polymerized film or vapor deposited film containing a substance that blackens by heat, 23...Recorded track portion, 24...Recorded information pit, 31...Unrecorded medium Optical contrast, 32... Optical contrast of the recording medium after track recording, 33... Optical contrast of the recording medium after information recording, 41... Substrate, 42... Reflective layer, 43... By heat discharge polymerized film or vapor deposited film containing a blackening substance, 44...protective layer, 53
... Recorded track portion, 54 ... Recorded pit, 61 ... Optical contrast of unrecorded medium, 62 ... Optical contrast of recording medium after track recording, 63 ... Recording medium after information recording optical contrast, 81... unrecorded area, 82...
...Track recording section, 83... Information recording section, 84...
...Truck information pit (heading), 85
... Information recording pit, 91 ... Unrecorded section, 92
...Track recording section, 93...Information recording section, 94
...Truck information pit (heading), 9
5... Pit for information recording.

Claims (1)

【特許請求の範囲】 1 基板を有し、該基板上に熱によつて黒化する
膜による記録層を被着し、該記録層に黒化に必要
なエネルギー密度を持つトラツク記録光を照射す
ることによりトラツク記録光照射部分に黒化した
ストライブ状の記録トラツクを形成し、前記記録
トラツク上に前記トラツク記録光より高いエネル
ギー密度を持つ情報ピツト記録光を照射すること
により情報ピツト記録光照射部分を溶融蒸発させ
て情報ピツトを記録可能となしたことを特徴とす
る光学記録媒体。 2 特許請求の範囲第1項記載の光学記録媒体に
おいて、前記記録層をTeまたはBi含有二硫化炭
素またはスチレン放電重合膜で形成したことを特
徴とする光学記録媒体。 3 特許請求の範囲第1項記載の光学記録媒体に
おいて、前記記録層をカルコゲナイトガラスで形
成したことを特徴とする光学記録媒体。 4 特許請求の範囲第1項、第2項及び第3項の
いずれかの項に記載の光学記録媒体において、前
記基板と前記記録層との間に反射層を介在させた
ことを特徴とする光学記録媒体。 5 特許請求の範囲第4項記載の光学記録媒体に
おいて、前記記録層と前記反射層との間に光干渉
層を介在させたことを特徴とする光学記録媒体。 6 熱によつて黒化する膜により形成した記録層
を有する光学記録媒体上に、黒化に必要なエネル
ギー密度のトラツク記録光で記録すべき記録トラ
ツクのパタンを走査し、該パタンに沿つて黒化に
より光学的コントラストを有するストライプ状の
記録トラツクを形成し、次いで、書き込み・読み
出しヘツドを前記記録トラツクに追従させながら
前記トラツク記録光よりも高いエネルギー密度の
情報ピツト記録光パルスにより前記記録トラツク
上の前記記録層を溶融蒸発させて情報ピツトを記
録することを特徴とする光学記録方法。
[Claims] 1. A device having a substrate, a recording layer made of a film that is blackened by heat is deposited on the substrate, and the recording layer is irradiated with track recording light having an energy density necessary for blackening. By doing so, a blackened stripe-like recording track is formed in the area irradiated with the track recording light, and by irradiating the information pit recording light having a higher energy density than the track recording light onto the recording track, the information pit recording light is formed. An optical recording medium characterized in that information pits can be recorded by melting and evaporating the irradiated portion. 2. The optical recording medium according to claim 1, wherein the recording layer is formed of Te or Bi-containing carbon disulfide or styrene discharge polymerized film. 3. The optical recording medium according to claim 1, wherein the recording layer is made of chalcogenite glass. 4. The optical recording medium according to any one of claims 1, 2, and 3, characterized in that a reflective layer is interposed between the substrate and the recording layer. optical recording medium. 5. The optical recording medium according to claim 4, characterized in that an optical interference layer is interposed between the recording layer and the reflective layer. 6. On an optical recording medium having a recording layer formed of a film that blackens with heat, scan a pattern of recording tracks to be recorded with track recording light having an energy density necessary for blackening, and record along the pattern. A striped recording track with optical contrast is formed by blackening, and then, while the write/read head is made to follow the recording track, the recording track is covered with an information pit recording light pulse having a higher energy density than the track recording light. An optical recording method characterized by recording information pits by melting and evaporating the upper recording layer.
JP55181862A 1980-12-24 1980-12-24 Optical recording medium and optical recording method Granted JPS57105394A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP55181862A JPS57105394A (en) 1980-12-24 1980-12-24 Optical recording medium and optical recording method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP55181862A JPS57105394A (en) 1980-12-24 1980-12-24 Optical recording medium and optical recording method

Publications (2)

Publication Number Publication Date
JPS57105394A JPS57105394A (en) 1982-06-30
JPS6361199B2 true JPS6361199B2 (en) 1988-11-28

Family

ID=16108131

Family Applications (1)

Application Number Title Priority Date Filing Date
JP55181862A Granted JPS57105394A (en) 1980-12-24 1980-12-24 Optical recording medium and optical recording method

Country Status (1)

Country Link
JP (1) JPS57105394A (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5051733A (en) * 1973-09-07 1975-05-08
JPS545742A (en) * 1977-06-15 1979-01-17 Fuji Photo Film Co Ltd Recording material
JPS5461543A (en) * 1977-10-25 1979-05-17 Canon Inc Recording method

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5051733A (en) * 1973-09-07 1975-05-08
JPS545742A (en) * 1977-06-15 1979-01-17 Fuji Photo Film Co Ltd Recording material
JPS5461543A (en) * 1977-10-25 1979-05-17 Canon Inc Recording method

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JPS57105394A (en) 1982-06-30

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