JPS5862096A - Optical information recording medium - Google Patents

Optical information recording medium

Info

Publication number
JPS5862096A
JPS5862096A JP56161632A JP16163281A JPS5862096A JP S5862096 A JPS5862096 A JP S5862096A JP 56161632 A JP56161632 A JP 56161632A JP 16163281 A JP16163281 A JP 16163281A JP S5862096 A JPS5862096 A JP S5862096A
Authority
JP
Japan
Prior art keywords
layer
substrate
recording
light
reproduction
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP56161632A
Other languages
Japanese (ja)
Inventor
Masahiro Orukawa
正博 尾留川
Hideji Kawabata
川端 秀次
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP56161632A priority Critical patent/JPS5862096A/en
Publication of JPS5862096A publication Critical patent/JPS5862096A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24Record 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
    • G11B7/242Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
    • G11B7/244Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising organic materials only
    • G11B7/245Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising organic materials only containing a polymeric component
    • 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
    • G11B7/257Record 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 layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers
    • G11B7/2572Record 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 layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of organic materials
    • G11B7/2575Record 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 layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of organic materials resins

Landscapes

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

Abstract

PURPOSE:To provide an optical information recording medium capable of reproducing information by the interference between reflected light from a written part and that from a non-written part without requiring any developing process, by providing a substrate and a recording material layer in the manner that their reflectances for a laser beam used in reproduction are in a specified ratio. CONSTITUTION:The first high polymeric binder layer 2 containing a light absorber is formed on the substrate 1 as a recording layer, and the second high polymeric binder layer 3 not containing any light absorber is formed thereon to constitute the titled recording medium. In this case, the reflectance I1 of the substrate 1 the reflectance I2 of the recording material layer, for the laser beam source used in reproduction, are set to satisfy the relationship of 0.32<I2<I1< 2.0. When the medium is irradiated with the laser beam for recording, the first layer 2 generates heat, whereby both the first layer 2 and the second layer 3 are decomposed and evaporated, and a written bit as shown is formed, resulting in that the substrate 1 is exposed at the written part. At the time of reproduction, the signal is reproduced with a high degree of modulation by the interference between the reflected light from the second layer 3 and that from the substrate 1.

Description

【発明の詳細な説明】 本発明はレーザー光を用いて情報の記録再生がなされる
光情報記録担体に関するものであり、その目的とすると
ころは現像過程を要−することなく書込部と非書込部に
おける反射光の相互干渉による再生ができる光情報記録
担体を提供することにある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical information recording carrier on which information is recorded and reproduced using a laser beam, and its purpose is to form a writing section and a non-contact recording medium without requiring a developing process. An object of the present invention is to provide an optical information recording carrier that can be reproduced by mutual interference of reflected light in a writing section.

一般に、レーザー光による情報の記録再生を行なう場合
、レーザー光を用いて記録部材を蒸発あるいは気化させ
ることによって情報の記録を行なうヒートモード記録方
法が知られており、この記録方法は高密度記録が可能で
ある点で有利である。
Generally, when recording and reproducing information using laser light, a heat mode recording method is known in which information is recorded by evaporating or vaporizing the recording material using laser light, and this recording method is capable of high-density recording. This is advantageous in that it is possible.

そして、記録材料としてムlなどの金属薄膜を用いたデ
ィスクをヒートモード記録のために利用する方法は、ビ
デオディスクの原板作製などにすでに応用されている。
The method of using a disk using a thin metal film such as mulch as a recording material for heat mode recording has already been applied to the production of a master plate for a video disk.

しかしながら、一般的に金属薄膜は高融点であり、記録
に大規模なレーザーを必要とするため、ユーザー側で記
録を行なうには不向きである゛。これに対し、Bi膜、
Te系薄膜などの低融点金属膜、低融点金属膜によるヒ
ートモード記録は、記録パワーの低減化が図られている
点で有利であるが、さらに低パワー記録が可能なものが
望まれている。一方、カーボンブラック。
However, metal thin films generally have a high melting point and require a large-scale laser for recording, making them unsuitable for users to perform recording. On the other hand, Bi film,
Heat mode recording using a low melting point metal film such as a Te-based thin film or a low melting point metal film is advantageous in that recording power can be reduced, but there is a desire for something that can perform even lower power recording. . On the other hand, carbon black.

染料などの光吸収体にニトロセルロースをノ(イングー
として混合して作製した薄膜は、高分子膜が低温で分解
、気化してしまうため、記録に要するエネルギーは極め
て小さく、ヒートモード記録のだめに有利である。そし
て、これらの記録材料に情報を記録したとき、非書込部
は反射率の小さい光吸収体で被覆されており、書込部は
光吸収体が除去され、基板が露出しでいる。したがって
、再生時に高い変調度を得るためには、基板の反射率を
できるだけ大きくすることが必要である。そのだめに、
基板にムe薄膜を形成させることなども考えられている
が、これらの工夫は、ムl薄嘆の熱体、導がよいために
熱拡散を助長し、記録エネルギーが大きくなる欠点を有
する。また、高い変調度を得るために、書込部と非書込
部において反射される光の相互、干渉を用いる方法も提
案されているが、この方式を実現するためには、光吸収
体を紫外線などに露光させ漂白するといつだ現像過程を
必要とする欠点があった。
Thin films made by mixing nitrocellulose with a light absorber such as a dye are decomposed and vaporized at low temperatures, so the energy required for recording is extremely small, making them advantageous for heat mode recording. When information is recorded on these recording materials, the non-writing area is covered with a light absorber with low reflectance, and the writing area is covered with a light absorber, leaving the substrate exposed. Therefore, in order to obtain a high degree of modulation during reproduction, it is necessary to increase the reflectance of the substrate as much as possible.
Although it has been considered to form a thin film on the substrate, these methods have the drawback that the thin heat source and good conductivity promote thermal diffusion and increase the recording energy. In addition, in order to obtain a high degree of modulation, a method has been proposed that uses mutual interference between the light reflected in the writing section and the non-writing section, but in order to realize this method, a light absorber is required. Bleaching by exposure to ultraviolet light has the disadvantage of requiring a developing process.

本発明はこれらの欠点を除くだめになされたものであり
、再生時におけるレーザー光源に対し、基板の反射強度
工1と記録材料層の反射強度工2の間に0.32 (I
2/II (2,0なる関係を満足するように構成した
ものである。かかる構成によれば、書込部と非書込部の
反射率を揃えて現像過程を経ずに相互干渉により高変調
度での再生を行なうことができる利点を有する。
The present invention has been made in order to eliminate these drawbacks, and there is a gap of 0.32 (I
2/II (This is a structure that satisfies the relationship 2,0. According to this structure, the reflectance of the written area and the non-written area are made equal and the reflectance is increased due to mutual interference without going through the development process. It has the advantage of being able to perform reproduction with a modulation degree.

以下、本発明について実施例の図面と共に説明する。第
1図は本発明の光情報記録担体の一実施・例を示してお
り、第1図において、記録担体は高分子バインダーと同
程度の反射率を有する基板1の上に、光吸収体を含む第
1高分子バインダ一層2を記録層!として設け、さらに
第1高分子バインダ一層2上に光吸収体を含まない高分
子バインダーから−なる第2高分子バインダ一層3を設
けることによって構成される。この記録担体に記録のだ
めのレーザー光を照射すると、一部は前記第2高分子バ
インダ一層3と空気の界面で反射し、残りの光は透過し
た後に前記第1高分子バインダ一層2にて吸収される。
The present invention will be described below with reference to drawings of embodiments. FIG. 1 shows an example of an optical information recording carrier according to the present invention. In FIG. The recording layer contains the first polymer binder layer 2! The first polymer binder layer 2 is further provided with a second polymer binder layer 3 made of a polymer binder containing no light absorber. When this record carrier is irradiated with a recording laser beam, part of the light is reflected at the interface between the second polymer binder layer 3 and air, and the remaining light is absorbed by the first polymer binder layer 2 after passing through. be done.

そのとき、光吸収体を含む第1高分子バインダ一層2は
発熱し、ある温度に達すると第1高分子バインダ一層2
.第2高分子バインダ一層3が共に分解、気化し、第2
図に示す書込ビットが形成される。その結果、書込部で
は基板1の面が露出される。このとき、第1高分子バイ
ンダ一層2.第2高分子バインダ一層3の合計膜厚を、
再生レーザー波長λに対し、(2n+1)λ/4 (n
 :整数)と設定する。したが9て、再生時は第2高分
子バインダ一層3で反射される一部の光と、基板1にて
反射される一部の光との干渉により、高い変調度として
信号再生を行なうことができる。
At that time, the first polymer binder layer 2 containing the light absorber generates heat, and when it reaches a certain temperature, the first polymer binder layer 2
.. The second polymer binder layer 3 decomposes and vaporizes, and the second polymer binder layer 3 decomposes and vaporizes.
The write bit shown in the figure is formed. As a result, the surface of the substrate 1 is exposed in the writing section. At this time, the first polymer binder layer 2. The total film thickness of the second polymer binder layer 3 is
(2n+1)λ/4 (n
: integer). Therefore, during reproduction, signal reproduction is performed with a high degree of modulation due to interference between part of the light reflected by the second polymer binder layer 3 and part of the light reflected by the substrate 1. I can do it.

第4図に基板面からの再生光反射強度工1と記録材料表
面からの再生光反射強度工2の比に対する変調度の変化
を示す。この図から、基板面と記録材料面両面からの再
生光反射強度が完全に一致する理想的な場合の変調度に
対し、 0.32 < I2/II (2,0 なる範囲で70チ以上の変調度が得られることがわかる
FIG. 4 shows the change in the degree of modulation with respect to the ratio of the reproduction light reflection intensity factor 1 from the substrate surface to the reproduction light reflection intensity factor 2 from the recording material surface. From this figure, it can be seen that for the modulation degree in an ideal case where the reproduction light reflection intensities from both the substrate surface and the recording material surface are completely equal, 0.32 < I2/II (70 inches or more in the range of 2,0). It can be seen that the modulation degree can be obtained.

具体的には、外径120mmの透明なアクリル基板をエ
チルアルコールで約1時間超音波洗浄した後、高速スピ
ナーで回転し乾燥させた。。次に、高速スピナーにディ
スクを保持し回転させた捷ま、1.5y−のメチレンブ
ルーと、2y−のニトロセルロースを100m5の溶剤
に溶かした溶液を用いて回転塗布を行なった。さらに高
速スピナーの回転数を2倍にし、1y−のニトロセルロ
ースヲ同じく100 mlの溶剤に溶かした溶液を用い
て回転塗布を行なった。このとき、塗布した膜の厚みは
、第1層、第2層合わせて約60oO人であった。
Specifically, a transparent acrylic substrate with an outer diameter of 120 mm was ultrasonically cleaned with ethyl alcohol for about 1 hour, and then dried by spinning with a high-speed spinner. . Next, the disk was held in a high-speed spinner and rotated, and a solution of 1.5y-methylene blue and 2y-nitrocellulose dissolved in 100 m5 of a solvent was used for spin coating. Further, the rotation speed of the high-speed spinner was doubled, and a solution of 1y-nitrocellulose dissolved in 100 ml of the solvent was used for spin coating. At this time, the thickness of the coated film was approximately 6000 mm in total for the first layer and the second layer.

この厚みは、再生に用いた半導体レーザー波長8100
人の約V4波長である。また、アクリル基板の表面の半
導体レーザー波長での反射率は、実測した結果4.8チ
であった。一方、作製した塗布膜の反射率は4.0%で
あった。このようにして作製したディスクを1100O
rpで回転させなが□ ら出力smWのH81’ieレ
ーザーを約1.2μm径に絞り、1周記録を行なった結
果、全周にわたって約1μmの溝ができた。次に、ビー
ム径約2,6μmに集光した出力04mWの半導体レー
ザーを用いて、第3図に示す光学系により反射光強度を
測定した。
This thickness is based on the semiconductor laser wavelength 8100 used for reproduction.
This is approximately the V4 wavelength of humans. Furthermore, the reflectance of the surface of the acrylic substrate at the semiconductor laser wavelength was actually measured to be 4.8 inches. On the other hand, the reflectance of the prepared coating film was 4.0%. The disk produced in this way was heated to 1100O
While rotating at RP, an H81'ie laser with an output of smW was focused to a diameter of about 1.2 μm, and as a result of one round recording, a groove of about 1 μm was formed over the entire circumference. Next, using a semiconductor laser with an output of 04 mW focused to a beam diameter of about 2.6 μm, the intensity of reflected light was measured using the optical system shown in FIG.

第3図において、4は半導体レーザ、5,8゜10は集
光レンズ、6は偏光ビームスプリータ、7は1/4波長
板、9は光ディスク、11は受光器である。その結果、
再生ビームを記録した溝の上に位置させた時の反射光強
度が0.6μWであったのに対し、再生ビームを記録し
た溝からはずした時の光強度は1.8μWであっだ0 また、−外径120朋のガラス基板を用い、高分子バイ
ンダーとしてポリメタクリル酸メチル、染料としてメチ
レンブルーを用い、上述のディスクと同様のディスクを
作製した。このディスクにおいて、記録光源として20
 mWのH6N、レーザーを用いたことを一除いて、第
3図に示す再生光学系と同様の記録再生を行なった結果
、同様の再生結果が得られた。
In FIG. 3, 4 is a semiconductor laser, 5, 8.degree. 10 is a condenser lens, 6 is a polarizing beam splitter, 7 is a quarter wavelength plate, 9 is an optical disk, and 11 is a light receiver. the result,
The reflected light intensity when the playback beam was positioned above the recorded groove was 0.6 μW, while the light intensity when the playback beam was removed from the recorded groove was 1.8 μW. A disk similar to the disk described above was prepared using a glass substrate having an outer diameter of 120 mm, polymethyl methacrylate as a polymer binder, and methylene blue as a dye. In this disc, 20
Recording and reproduction were carried out in the same manner as in the reproduction optical system shown in FIG. 3, except that a mW H6N laser was used, and as a result, similar reproduction results were obtained.

尚、上記の実施例では、光吸収体としてメチレンブルー
、記録用光源としてaeNeレー尤−を用いたが、本発
明は、記録用光源波長に対し光吸収性を有し、高分子バ
インダーと相溶性を有する染料において有効である。ま
だ、本発明は、記録用光源波長に対し光吸収性を有し、
高分子バインダーを溶かす溶剤に対しに好な分散性を有
する顔料において有効である。+1上記の実施例では再
生時において、書込部からの反射光と非書込部からの反
射光との間に干渉を起こさせるべく両者の反射率を揃え
るために2層構造としたが、これは単層構造、あるいは
多層構造、もしくは連続的な分布を持たせた構造におい
ても、反射率を揃えることにより有効である。
In the above embodiment, methylene blue was used as the light absorber and aeNe laser was used as the recording light source, but the present invention uses methylene blue as the light absorber and aeNe light as the recording light source. It is effective for dyes with Still, the present invention has light absorption property for the wavelength of the recording light source,
It is effective for pigments that have good dispersibility in solvents that dissolve polymeric binders. +1 In the above embodiment, a two-layer structure was used in order to equalize the reflectance of the reflected light from the written part and the reflected light from the non-written part in order to cause interference between the reflected light from the written part and the reflected light from the non-written part during reproduction. This is effective even in a single layer structure, a multilayer structure, or a structure with continuous distribution by making the reflectance uniform.

以上のように本発明によれば、再生時に用いるレーザー
光源に対し、基板の反射彊度工1と、高分子バインダー
と光吸収体からなる記録層の反射強度工2の間に0.3
2 (I2/I+ < 2.0なる関係が満足されるよ
うに、2層膜構造にするなどして記録層の面での反射率
と基板面との反射率を揃えることにより、現像過程を必
要としない干渉利用型ヒートモード記録体が実現できる
。したがって、記録装置の簡素化ばかりでなく、ユーザ
ーサイドでの追加書込みなどが簡単に行なえる利点を有
するものである。
As described above, according to the present invention, with respect to the laser light source used during reproduction, there is a difference of 0.3 between the reflection strength 1 of the substrate and the reflection strength 2 of the recording layer made of a polymer binder and a light absorber.
2 (In order to satisfy the relationship I2/I+ < 2.0, the development process can be improved by aligning the reflectance on the recording layer surface and the reflectance on the substrate surface, such as by creating a two-layer film structure. It is possible to realize an interference-based heat mode recording medium that does not require the use of interference.Therefore, it has the advantage of not only simplifying the recording apparatus but also allowing additional writing to be easily performed on the user's side.

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

第1図は未記録状態における本発明による光情報記録担
体の一実施例を示す構成図、第2図は同記録担体の既記
録状態を示す構成図、第3図は本発明の光情報記録担体
の再生光学系を示す構成図、第4図は同光情報記録担体
の反射強度比に対する変調度を示す特性図である。 1・・・・・・基板、2・・・・・・第1高分子バイン
ダ一層、3・・・・・・第2高分子バインダ一層。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 第2図 第3図 第4図 h /(t
FIG. 1 is a block diagram showing an embodiment of the optical information recording carrier according to the present invention in an unrecorded state, FIG. 2 is a block diagram showing the same record carrier in a recorded state, and FIG. 3 is a block diagram showing the optical information recording carrier according to the present invention. FIG. 4 is a block diagram showing the reproduction optical system of the carrier, and a characteristic diagram showing the degree of modulation with respect to the reflection intensity ratio of the optical information recording carrier. 1... Substrate, 2... One layer of first polymer binder, 3... One layer of second polymer binder. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 Figure 3 Figure 4 h /(t

Claims (2)

【特許請求の範囲】[Claims] (1)光の一部を反射する基板と、この基板上に薄膜状
に形成され、光吸収体と高分子バインダーからなりレー
ザー光の照射により蒸発または気化して情報の記録が行
なわれる記録材料層を備えてなり、再生時に用いるレー
ザー光源に対し、上記基板の反射強度工1と、上記記録
材料層の反射強度工2ノ間に0.32< I2/L 〈
2.Ofzる関係を満足するように上記基板と上記記録
材料層の反射率を揃えたことを特徴とする光情報記録担
体。
(1) A substrate that reflects a portion of light, and a recording material formed in the form of a thin film on this substrate, consisting of a light absorber and a polymer binder, which evaporates or vaporizes when irradiated with laser light to record information. 0.32<I2/L<
2. An optical information recording carrier characterized in that the substrate and the recording material layer have the same reflectance so as to satisfy the following relationship.
(2)記録材料層は基板側から光吸収体を含む高分子バ
インダ一層と光吸収体を含まない高分子バインダ一層の
積層構造としたことを特徴とする特許請求の範囲第1項
記録の光情報記録担体。
(2) The recording material layer has a laminated structure of one layer of a polymer binder containing a light absorber and one layer of a polymer binder not containing a light absorber from the substrate side. Information record carrier.
JP56161632A 1981-10-09 1981-10-09 Optical information recording medium Pending JPS5862096A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56161632A JPS5862096A (en) 1981-10-09 1981-10-09 Optical information recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56161632A JPS5862096A (en) 1981-10-09 1981-10-09 Optical information recording medium

Publications (1)

Publication Number Publication Date
JPS5862096A true JPS5862096A (en) 1983-04-13

Family

ID=15738872

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56161632A Pending JPS5862096A (en) 1981-10-09 1981-10-09 Optical information recording medium

Country Status (1)

Country Link
JP (1) JPS5862096A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4719615A (en) * 1983-08-22 1988-01-12 Optical Data, Inc. Erasable optical data storage medium
EP0272875A2 (en) * 1986-12-20 1988-06-29 Kyodo Printing Co., Ltd. Optical recording card and method of producing the same

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4719615A (en) * 1983-08-22 1988-01-12 Optical Data, Inc. Erasable optical data storage medium
EP0272875A2 (en) * 1986-12-20 1988-06-29 Kyodo Printing Co., Ltd. Optical recording card and method of producing the same
EP0486482A2 (en) * 1986-12-20 1992-05-20 Kyodo Printing Co., Ltd. Optical recording card and method of producing the same

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