[go: up one dir, main page]

JPH01243252A - Medium and method for recording optical information - Google Patents

Medium and method for recording optical information

Info

Publication number
JPH01243252A
JPH01243252A JP63069079A JP6907988A JPH01243252A JP H01243252 A JPH01243252 A JP H01243252A JP 63069079 A JP63069079 A JP 63069079A JP 6907988 A JP6907988 A JP 6907988A JP H01243252 A JPH01243252 A JP H01243252A
Authority
JP
Japan
Prior art keywords
groove
transparent substrate
parts
optical information
recording medium
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
JP63069079A
Other languages
Japanese (ja)
Inventor
Michiharu Abe
通治 安倍
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP63069079A priority Critical patent/JPH01243252A/en
Publication of JPH01243252A publication Critical patent/JPH01243252A/en
Pending legal-status Critical Current

Links

Landscapes

  • Optical Record Carriers And Manufacture Thereof (AREA)

Abstract

PURPOSE:To improve sensitivity and recording quality by forming a groove on the plane on one side of a transparent substrate, constituting a part on which the groove is formed of a thermosoftening member, forming a light absorptive reflection layer on the plane where the groove of the substrate is formed, and setting a prescribed ratio of a reflecting level for a laser beam projecting the depth and the width of the groove at the part where the groove is formed to the part where no groove is formed. CONSTITUTION:Groove parts 7a, 7b, 7c... are formed on the plane on one side of an optical information recording medium 1, and the transparent substrate 2 in which the parts where the groove parts 7a, 7b, 7c... are formed are constituted of the thermosoftening member is used. On the plane where the groove parts 7a, 7b, 7c... are formed, the light absorptive reflection layer 3 and a protective layer 4 are formed sequentially. The depth and the width of the groove parts 7a, 7b, 7c... of the recording medium 1 constituted in such way that the reflected light levels of the groove parts 7a, 7b, 7c... for a laser convergence beam projected from the substrate 2 side are set at values of 10-50% of that of the parts where no groove part 7a, 7b, 7c... are formed.

Description

【発明の詳細な説明】 〔技術分野〕 本発明は、レーザー集光ビームで光学的に情報を記録す
る光ディスク等の光学的情報記録媒体および記録方法に
関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to an optical information recording medium, such as an optical disk, on which information is optically recorded using a focused laser beam, and a recording method.

〔従来技術〕[Prior art]

近年、映像および音声記録装置、コンピューター用外部
記憶装置等において光ディスクを用い直径1戸前後のレ
ーザー集光ビームで光学的に情報を記録することが行わ
れている。このような情報記録においては、従来、基板
上に光吸収反射性の薄膜を設け、レーザー集光ビームを
照射し、薄膜に小孔を形成して情報を記録する方法が採
られている。
2. Description of the Related Art In recent years, optical discs have been used in video and audio recording devices, external storage devices for computers, and the like to optically record information using a focused laser beam with a diameter of about one door. Conventionally, in such information recording, a method has been adopted in which a light-absorbing and reflective thin film is provided on a substrate, a focused laser beam is irradiated, and small holes are formed in the thin film to record information.

しかしながら、従来の光ディスクでは、光吸収反射性の
薄膜として金属、合金、有機色素が使われており、その
融点、蒸発温度、分解温度が200℃〜1000℃と高
いので、感度を高くすることができなかった。また、薄
膜に小孔を形成する際の除去物が信号品質を低下させる
という欠点があった。
However, in conventional optical discs, metals, alloys, and organic dyes are used as light-absorbing and reflective thin films, and their melting points, evaporation temperatures, and decomposition temperatures are as high as 200°C to 1000°C, making it difficult to increase sensitivity. could not. Furthermore, there is a drawback that the material removed when forming small holes in the thin film deteriorates signal quality.

〔目  的〕〔the purpose〕

本発明は、このような従来技術の欠点を解決するだめに
なされたものであって、感度および記録品質が向上した
光学的情報記録媒体および記録方法を提供することを目
的とする。
The present invention has been made to solve the drawbacks of the prior art, and an object of the present invention is to provide an optical information recording medium and a recording method with improved sensitivity and recording quality.

〔構  成〕〔composition〕

本発明によれば、第1発明として、一方の面に溝が形成
されかつ少なくとも該溝が形成された部分は熱軟化性部
材からなる透明基板と、該透明基板の前記溝が形成され
た面上に設けられた光吸収反射層とから構成され、前記
溝の深さおよび幅が、前記透明基板側から照射されるレ
ーザー光に対する溝部分の反射光レベルが溝の形成され
ていない部分の反射光レベルの10%〜50%となるご
とき値に設定されていることを特徴とする光学的情報記
録媒体が提供される。
According to the present invention, a first aspect of the present invention includes a transparent substrate having a groove formed on one surface and at least a portion where the groove is formed is made of a thermosoftening material; and a surface of the transparent substrate where the groove is formed. and a light absorption/reflection layer provided on the transparent substrate, and the depth and width of the groove are such that the level of light reflected from the groove portion to the laser beam irradiated from the transparent substrate side is such that the level of light reflected from the groove portion is the same as the reflection of the portion where the groove is not formed. An optical information recording medium is provided, characterized in that the light level is set to a value of 10% to 50% of the light level.

また、第2発明として、上記光学情報記媒体の溝部分上
に設けられた光吸収反射層にレーザー集光ビームを透明
基板側から照射し、その熱作用で溝構造を変形させるこ
とにより情報記録を行うことを特徴とする記録方法が提
供される。
Further, as a second invention, information is recorded by irradiating the light absorbing and reflecting layer provided on the groove portion of the optical information recording medium with a focused laser beam from the transparent substrate side and deforming the groove structure by the heat effect. A recording method is provided that is characterized by performing the following steps.

次に、図面を参照して本発明の光学的情報記録媒体およ
び記録方法を説明する。第1図は本発明の光学的情報記
録媒体を示す、走査方向に垂直な断面図で、同図(a)
は未記録状態、同図(b)は記録状態を示している。第
1図において、1はたとえば光ティスフ等の光学的情報
記録媒体で、基本的に、一方の面に溝が形成された透明
基板2と、該透明基板2」二に設けられた光吸収反射層
3より構成される。本発明の光学的情報記録媒体1にお
いては、場合によっては、記録面を保護するために保護
層4を設けてもよい。なお図中、5は集光レンズ、6は
レーザー築光ビーム、7a 、 7b 、 7cは光吸
収反射層3の溝部分である。
Next, the optical information recording medium and recording method of the present invention will be explained with reference to the drawings. FIG. 1 is a sectional view perpendicular to the scanning direction showing the optical information recording medium of the present invention, and FIG.
shows an unrecorded state, and (b) shows a recorded state. In FIG. 1, reference numeral 1 denotes an optical information recording medium such as an optical disk, which basically includes a transparent substrate 2 with grooves formed on one surface, and a light absorbing/reflecting medium provided on the transparent substrate 2. Consists of layer 3. In the optical information recording medium 1 of the present invention, a protective layer 4 may be provided in order to protect the recording surface, depending on the case. In the figure, 5 is a condenser lens, 6 is a laser light forming beam, and 7a, 7b, and 7c are groove portions of the light absorption and reflection layer 3.

透明基板2はその全体が熱軟化性部材で構成されていて
もよいし、一部すなわち溝が形成される部分が熱軟化性
部材で構成されていてもよい。透明基板2に形成された
溝は第1図の場合、基板側に対して凹溝となっているが
、記録層側に対して凹溝すなわち基板側に対して凸状で
あってもよい。
The entire transparent substrate 2 may be made of a heat-softening material, or a portion, that is, a portion where the grooves are formed, may be made of a heat-softening material. In the case of FIG. 1, the grooves formed in the transparent substrate 2 are concave grooves toward the substrate side, but they may also be concave grooves toward the recording layer side, that is, convex grooves toward the substrate side.

この溝の概念は相対的なものであって、本明細書では両
者を含めて溝と称することとする。
This concept of groove is relative, and in this specification, both grooves will be collectively referred to as grooves.

光学的情報記録媒体1への情報の記録は次のようにして
行われる。第1図(a)に示すように、集光レンズ5に
よってたとえば光吸収反射層3の溝部分7bに、直径1
μm前後のスポット径とされかつ所定値以上のパワーの
レーザー集光ビーム6を照射する。レーザー集光ビーム
6は光吸収反射層3によって吸収され、溝部分7bの温
度が上昇するとともにその付近の熱軟化性部材が軟化し
、表面張力によって溝部分7bは第1図(b)の7b’
のように低下すなわち浅くなる。なお、7b’は溝構造
が完全に消失した状態となってもよい。第1図(b)の
7b’が記録状態であり、レーザー照射パワーが所定値
以上になったときに記録される。レーザー照射パワーが
所定値より小さいときは変形温度に達しないため溝部分
の形状変化は生じない。したがって、レーザー集光ビー
ム6のパワーの強弱により、第2図(b)に示すように
溝からなるトラック10上に溝構造の消失あるいは低下
した部分11a、llb、llc・・・を形成し、情報
記録を行うことができる。
Information is recorded on the optical information recording medium 1 as follows. As shown in FIG. 1(a), for example, the condenser lens 5 creates a groove with a diameter of 1
A focused laser beam 6 with a spot diameter of around μm and a power of a predetermined value or more is irradiated. The laser focused beam 6 is absorbed by the light absorption/reflection layer 3, and as the temperature of the groove portion 7b rises, the heat-softening material in the vicinity thereof softens, and the groove portion 7b becomes 7b in FIG. 1(b) due to surface tension. '
It decreases, that is, becomes shallower. Note that 7b' may be in a state where the groove structure completely disappears. 7b' in FIG. 1(b) is a recording state, and recording is performed when the laser irradiation power exceeds a predetermined value. When the laser irradiation power is lower than a predetermined value, the deformation temperature is not reached, so no change in shape of the groove portion occurs. Therefore, depending on the strength of the power of the laser focused beam 6, portions 11a, llb, llc... where the groove structure disappears or is reduced are formed on the track 10 made of grooves as shown in FIG. Information can be recorded.

光学情報記録媒体1から情報を読み出すには、溝構造を
変化させないレベルの低い照射パワーのレーザー集光ビ
ームでトラックをなぞることにより反射光の強弱として
読みとることができる。たとえば第2図(b)の如きト
ラックをなぞった場合、溝構造の消失あるいは低下した
部分11a、ilb、1.1cに対応して、第2図(a
)の9a、9b、9cのような反射光信号となる。図中
8は溝部分による反射光レベルである。すなわち溝部分
では回折作用のため反射光レベルが低くなるが、溝構造
の消失あるいは低下した部分では反射光レベルが高くな
る。したがって本発明では、溝の深さおよび幅は、溝の
反射光レベルが溝のない部分(ミラー面)の反射光レベ
ルの10%〜50%、好ましくは20%〜40%になる
ように設定しておく必要がある。そのためには溝の実効
深さは0.13λ〜0.24λ(λは光波長)、溝の半
値幅は集光スポット径(半値全幅)の0.2〜0.5倍
が好ましい。溝の最大深さは溝の形状によって多少異な
り、矩形状の場合実効深さの1倍、V字状の場合実効深
さの1.6倍が適当である。
To read information from the optical information recording medium 1, a track is traced with a focused laser beam of low irradiation power that does not change the groove structure, and the intensity of the reflected light can be read. For example, when tracing a track as shown in FIG. 2(b), corresponding to the parts 11a, ilb, and 1.1c where the groove structure has disappeared or deteriorated, the groove structure shown in FIG.
) are reflected light signals such as 9a, 9b, and 9c. 8 in the figure is the level of light reflected by the groove portion. That is, the reflected light level is low in the groove portion due to the diffraction effect, but the reflected light level is high in the portion where the groove structure has disappeared or decreased. Therefore, in the present invention, the depth and width of the groove are set such that the level of reflected light from the groove is 10% to 50%, preferably 20% to 40%, of the level of reflected light at the portion without the groove (mirror surface). It is necessary to do so. For this purpose, the effective depth of the groove is preferably 0.13λ to 0.24λ (λ is the wavelength of light), and the half width of the groove is preferably 0.2 to 0.5 times the focused spot diameter (full width at half maximum). The maximum depth of the groove varies somewhat depending on the shape of the groove, and in the case of a rectangular groove, 1 times the effective depth is appropriate, and in the case of a V-shape, 1.6 times the effective depth is appropriate.

第3図に、レーザービームの半値全幅の0.2〜0.4
倍の半値幅を有する溝の最大深さと反射光比の関係の例
を示す。同図(a)は矩形溝の場合、同図(b)はV字
溝の場合である。深さ0.2λの矩形溝の場合、レーザ
ー光照射により、0.1λの溝になることにより反射光
比が0.35から0.85に上昇する。V字溝の場合、
0.26λの溝がレーザー光照射により、0゜1λにな
ることにより反射光比が0.4から0.85に上昇する
Figure 3 shows the full width at half maximum of 0.2 to 0.4 of the laser beam.
An example of the relationship between the maximum depth of a groove having double the half width and the reflected light ratio is shown. The figure (a) shows the case of a rectangular groove, and the figure (b) shows the case of a V-shaped groove. In the case of a rectangular groove with a depth of 0.2λ, the reflected light ratio increases from 0.35 to 0.85 by turning the groove into a 0.1λ groove by laser beam irradiation. In the case of a V-shaped groove,
By irradiating a 0.26λ groove with a laser beam, the groove becomes 0°1λ, thereby increasing the reflected light ratio from 0.4 to 0.85.

保護層4は記録面を保護するものであり、記録情報の損
傷を防ぐために有効であり、過度のレーザー光照射時に
光吸収反射層3の一部が飛散することを防ぐためにも有
効である。保護層4は光吸収反射層3の面が汚染されな
いような状態(例えばエアーサンドインチ構造の空隙内
に開放されている場合など)になっていれば必ずしも必
要でないこともある。
The protective layer 4 protects the recording surface and is effective for preventing damage to recorded information, and is also effective for preventing part of the light absorbing reflective layer 3 from scattering during excessive laser beam irradiation. The protective layer 4 may not necessarily be necessary if the surface of the light-absorbing reflective layer 3 is not contaminated (for example, when it is open in the air gap of an air sandwich structure).

本発明の光学的情報記録媒体1の透明基板2を構成する
材料としては、たとえばガラス、透明プラスチック(ア
クリル樹脂(PMMA)、ポリカーボネート樹脂、ポリ
エステル樹脂、ポリ塩化ビニル樹脂、ナイロン樹脂、ポ
リオレフィン樹脂、ポリスチレン樹脂、エポキシ樹脂、
シリコン樹脂、など)が用いられるが、少なくともその
溝形成部には熱軟化性透明樹脂を選択する必要がある。
Examples of materials constituting the transparent substrate 2 of the optical information recording medium 1 of the present invention include glass, transparent plastics (acrylic resin (PMMA), polycarbonate resin, polyester resin, polyvinyl chloride resin, nylon resin, polyolefin resin, polystyrene). resin, epoxy resin,
silicone resin, etc.), but it is necessary to select a heat-softening transparent resin at least for the groove forming portion.

光吸収反射層3を構成する材料としては、たとえばTe
 、 Bi 、 Se 、 Ti 、 Pb 、 Sn
等の金属、合金、酸化物;シアニン色素、メロシアニン
色素、トリフェニルメタン色素、フタロシアニン色素、
スクワリリウム色素、ピリリウム色素等の有機色素が用
いられる。
Examples of the material constituting the light absorption and reflection layer 3 include Te.
, Bi, Se, Ti, Pb, Sn
Metals, alloys, oxides such as cyanine dyes, merocyanine dyes, triphenylmethane dyes, phthalocyanine dyes,
Organic dyes such as squarylium dyes and pyrylium dyes are used.

保護層4を構成する材料としては、たとえばAp。The material constituting the protective layer 4 is, for example, Ap.

Au、Ag、Pdなどの金属、合金;Sin、MgF、
SiN、などの金属酸化物、金属弗化物、金属窒化物;
アクリル樹脂(PMMA)、ポリカーボネート樹脂、ポ
リエステル樹脂、ポリ塩化ビニル樹脂、ナイロン樹脂、
エポキシ樹脂、シリコン樹脂、ゼラチン、ポリスチレン
樹脂などの樹脂が用いられる。また保護層4には潤滑剤
、安定剤、顔料、色素などを含有させることができる。
Metals and alloys such as Au, Ag, Pd; Sin, MgF,
Metal oxides, metal fluorides, metal nitrides such as SiN;
Acrylic resin (PMMA), polycarbonate resin, polyester resin, polyvinyl chloride resin, nylon resin,
Resins such as epoxy resin, silicone resin, gelatin, and polystyrene resin are used. Further, the protective layer 4 can contain a lubricant, a stabilizer, a pigment, a dye, and the like.

〔効  果〕〔effect〕

=7− 本発明によれば、レーザー集光ビームを用いて溝構造を
変形(消失ある′いは低下)させることにより情報を記
録するようにしたので、小孔形成方式の記録よりも低温
で記録できるため、感度が向上する。また、記録膜(光
吸収反射層)が記録時に飛散しなくなるので、記録膜表
面が異物で汚染されなくなり、信頼性が向上する。さら
に、エアーサンドインチ構造にする必要がないため、製
造コストが低減でき、外気圧の影響によるそりが発生し
なくなる。
=7- According to the present invention, information is recorded by deforming (disappearing or lowering) the groove structure using a focused laser beam, so it is possible to record information at a lower temperature than the small hole formation method. Since it can be recorded, sensitivity is improved. Furthermore, since the recording film (light absorbing and reflecting layer) is not scattered during recording, the surface of the recording film is not contaminated with foreign matter, improving reliability. Furthermore, since there is no need for an air sand inch structure, manufacturing costs can be reduced and warping due to the influence of external pressure will not occur.

〔実施例〕〔Example〕

次に、本発明の詳細な説明するがこれに限定されるもの
ではない。
Next, the present invention will be explained in detail, but it is not limited thereto.

実施例1 ポリカーボネート樹脂に溝幅0.3μm、深さ0.12
戸の台形状で少しダした溝をトラックピッチ1.6ρで
らせん状に形成した光デイスク用基板を用い、光吸収反
射層として5eTeの膜を厚さ400人に蒸着した。更
にその上に厚さ10μmのシリコン樹脂を塗布して保護
膜を形成した。そして波長780nmの半導体レーザー
を用い開口数0.47の集光レンズにより半値全@0.
9μmのスポットにレーザー光を集光し、記録媒体に照
射した。線速度2.1.m/see、照射パワー2.3
dで記録した結果、C/N比50dBが得られた。この
とき5eTeの膜には孔は形成されず、基板の溝が浅く
なっていた。
Example 1 Groove width 0.3 μm, depth 0.12 in polycarbonate resin
Using an optical disk substrate in which a trapezoidal groove with a slightly rounded shape was spirally formed at a track pitch of 1.6ρ, a 5eTe film was deposited to a thickness of 400 mm as a light absorbing and reflecting layer. Furthermore, a 10 μm thick silicone resin was applied thereon to form a protective film. Then, using a semiconductor laser with a wavelength of 780 nm and a condensing lens with a numerical aperture of 0.47, the full half maximum @ 0.
Laser light was focused on a 9 μm spot and irradiated onto the recording medium. Linear velocity 2.1. m/see, irradiation power 2.3
As a result of recording at d, a C/N ratio of 50 dB was obtained. At this time, no holes were formed in the 5eTe film, and the grooves in the substrate became shallow.

実施例2 実施例1と同じ基板に次の構造式のシアニン色素を厚さ
0.05証で塗布し、その上にSiOの保護膜を0.0
7μmの厚さで蒸着した。
Example 2 A cyanine dye having the following structural formula was coated on the same substrate as in Example 1 to a thickness of 0.05 mm, and a protective film of SiO was coated on it to a thickness of 0.05 mm.
It was deposited to a thickness of 7 μm.

そして上記と同様のレーザー光の集光を行い、線速度2
.1m/see、照射パワー2.2mWで記録した結果
、C/N比52dBが得られた。このとき色素の膜には
孔は形成されず、基板の溝が浅くなっていた。保護膜と
して厚さ30μmのゼラチンの層を塗布した場合にも同
様の結果が得られた。
Then, the same laser beam as above is focused, and the linear velocity is 2
.. As a result of recording at 1 m/see and irradiation power of 2.2 mW, a C/N ratio of 52 dB was obtained. At this time, no holes were formed in the dye film, and the grooves in the substrate became shallow. Similar results were obtained when a layer of gelatin with a thickness of 30 μm was applied as a protective film.

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

第1図は本発明に係る光学的情報記録媒体の構成を示す
図で、第1図(a)は未記録状態、第1図(b)は記録
状態を示す。第2図は本発明に係る光学的情報記録媒体
からの情報読み出しの説明図で、第2図(a)は溝部分
および溝構造の消失もしくは低下した部分に対応する反
射光レベルを示し、第2図(b)はトラック上の信号パ
ターンを示す。第3図は溝の最大深さと反射光比の関係
を示すグラフで、第3図(a)は矩形溝の場合、第3図
(b)はV字溝の場合を示す。 1・・・光学的情報記録媒体 2・・・透明基板    3・・光吸収反射層4・・保
護層     6・・・レーザー集光ビーム7a 、 
7b 、 7cm溝部分
FIG. 1 is a diagram showing the structure of an optical information recording medium according to the present invention, with FIG. 1(a) showing an unrecorded state and FIG. 1(b) showing a recorded state. FIG. 2 is an explanatory diagram of information reading from the optical information recording medium according to the present invention, and FIG. FIG. 2(b) shows the signal pattern on the track. FIG. 3 is a graph showing the relationship between the maximum depth of the groove and the reflected light ratio. FIG. 3(a) shows the case of a rectangular groove, and FIG. 3(b) shows the case of a V-shaped groove. 1... Optical information recording medium 2... Transparent substrate 3... Light absorption reflective layer 4... Protective layer 6... Laser condensed beam 7a,
7b, 7cm groove part

Claims (2)

【特許請求の範囲】[Claims] (1)一方の面に溝が形成されかつ少なくとも該溝が形
成された部分は熱軟化性部材からなる透明基板と、該透
明基板の前記溝が形成された面上に設けられた光吸収反
射層とから構成され、前記溝の深さおよび幅が、前記透
明基板側から照射されるレーザー光に対する溝部分の反
射光レベルが溝の形成されていない部分の反射光レベル
の10%〜50%となるごとき値に設定されていること
を特徴とする光学的情報記録媒体。
(1) A transparent substrate with grooves formed on one surface and at least the portion where the grooves are formed is made of a thermosoftening material, and a light absorbing/reflecting substrate provided on the surface of the transparent substrate where the grooves are formed. The depth and width of the groove are such that the level of light reflected at the groove portion with respect to the laser beam irradiated from the transparent substrate side is 10% to 50% of the level of light reflected at the portion where the groove is not formed. An optical information recording medium characterized by being set to a value such that .
(2)請求項1記載の光学的情報記録媒体の溝部分に設
けられた光吸収反射層にレーザー集光ビームを透明基板
側から照射し、その熱作用で溝構造を変形させることに
より情報記録を行うことを特徴とする記録方法。
(2) Information is recorded by irradiating the light absorbing and reflecting layer provided in the groove portion of the optical information recording medium according to claim 1 with a focused laser beam from the transparent substrate side and deforming the groove structure by the heat effect. A recording method characterized by performing the following.
JP63069079A 1988-03-23 1988-03-23 Medium and method for recording optical information Pending JPH01243252A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63069079A JPH01243252A (en) 1988-03-23 1988-03-23 Medium and method for recording optical information

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63069079A JPH01243252A (en) 1988-03-23 1988-03-23 Medium and method for recording optical information

Publications (1)

Publication Number Publication Date
JPH01243252A true JPH01243252A (en) 1989-09-27

Family

ID=13392219

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63069079A Pending JPH01243252A (en) 1988-03-23 1988-03-23 Medium and method for recording optical information

Country Status (1)

Country Link
JP (1) JPH01243252A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5714748A (en) * 1992-10-02 1998-02-03 Goldstar Co., Ltd. Magnetic cards employing optical recording material

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5714748A (en) * 1992-10-02 1998-02-03 Goldstar Co., Ltd. Magnetic cards employing optical recording material

Similar Documents

Publication Publication Date Title
US4385372A (en) Reflective optical data storage and laser recording media having grooved dielectric encoded prerecorded information
US4918682A (en) Ablative and bump-forming optical recording media including a metallic reflective layer
JPH0158079B2 (en)
KR101083199B1 (en) Method of recording information, information recording medium and manufacturing method of information recording medium
US5079758A (en) Single polymer layer recordable/erasable optical media
JPH0776171A (en) Write-once optical disc
JPH01243252A (en) Medium and method for recording optical information
US5728441A (en) Recordable/replayable optical recording medium and optical recording method therefor
US20020057646A1 (en) Optical information recording medium and method of manufacturing the same
JP3082143B2 (en) Optical information recording medium and recording method thereof
JP2985100B2 (en) Optical information recording medium and recording method thereof
JP2741101B2 (en) Optical information recording medium
JP3106318B2 (en) Optical information recording medium and recording method thereof
US5088087A (en) Dual-metal reflective layer recordable/erasable optical media
JP2866022B2 (en) Optical information recording medium and reproducing method thereof
JPS63298837A (en) Optical recording medium
JP2001134981A (en) Multilayer optical disc
JP2811603B2 (en) Optical information recording medium
JP2982329B2 (en) Information optical recording medium and recording / reproducing method thereof
JP2847977B2 (en) Optical recording medium and manufacturing method thereof
JP3099275B2 (en) Optical information recording medium and recording method thereof
JPH083912B2 (en) Novel optical recording medium and manufacturing method thereof
JP2793516B2 (en) Optical information recording medium and reproducing method thereof
JP2859599B2 (en) Optical information recording medium
JPH02187939A (en) Optical recording medium and optical recording and reproducing method