JPS6236878B2 - - Google Patents
Info
- Publication number
- JPS6236878B2 JPS6236878B2 JP54120138A JP12013879A JPS6236878B2 JP S6236878 B2 JPS6236878 B2 JP S6236878B2 JP 54120138 A JP54120138 A JP 54120138A JP 12013879 A JP12013879 A JP 12013879A JP S6236878 B2 JPS6236878 B2 JP S6236878B2
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- dye
- optical recording
- dyes
- substrate
- 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
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/242—Record 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
- G11B7/244—Record 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
- G11B7/246—Record 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 dyes
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/242—Record 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
- G11B7/244—Record 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
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/252—Record 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
- G11B7/253—Record 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
- G11B7/2533—Record 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
- G11B7/2535—Record 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 polyesters, e.g. PET, PETG or PEN
Landscapes
- Heat Sensitive Colour Forming Recording (AREA)
- Thermal Transfer Or Thermal Recording In General (AREA)
- Non-Silver Salt Photosensitive Materials And Non-Silver Salt Photography (AREA)
- Optical Record Carriers And Manufacture Thereof (AREA)
Description
本発明は光学記録用媒体、更に詳細にはレー
ザ、特に記録読み出し系を小型にすることのでき
る半導体レーザの発振波長に適合するような比較
的長波長の光エネルギを用いて、物質変化又は熱
的な融解、蒸発昇華等の状態変化を利用した光学
記録用媒体に関する。
従来、この種の記録媒体にはカルコゲナイト系
非晶質ガラス(特公昭54−20136号公報参照)、
Te酸化物(特公昭54−3725号公報参照)、カーボ
ンブラツク分散型自己酸化性バインダ(特公昭51
−35144号公報参照)、フルオレセイン(IEEE、
Spectrum August 1978、第20頁)等が用いられ
ていた。
カルコゲナイト系非晶質ガラスは光学記録用材
料として蒸着膜の状態で用いられる。この材料は
非晶状態、結晶状態において安定であるが、蒸着
等の方法で薄膜を得る場合所定の成分を真空中で
固溶させて急冷し、均一な原材料を得るという製
造過程が必要である。又成分元素が多種であるた
め組成の均一な原料を得て薄膜化することは困難
である。更にカルコゲナイト系非晶質ガラスの薄
膜は未記録状態の初期光学的濃度が大きく、コン
トラスト比を高く取ると、読み出し効率が著しく
低いという欠点を有する。
カルコゲナイト系非晶質ガラスに比べ高感度を
有するTe酸化物薄膜の場合はTeO2を蒸着して製
造されるが、薄膜を形成する主成分はTeOX(X
は0<X<2)とされ、蒸着条件によつて薄膜の
組成が変化して均一な薄膜の製造はかなり困難で
ある。又Te酸化物薄膜の感光波長域は350〜600n
mであつて、記録用光源を長波長域に求めた場合
本質的に感度を有していないという欠点を有す
る。
染料分散型の有機薄膜はニトロセルロース等の
自己酸化性材料をバインダとして用いると感度的
には、上記の無機薄膜を凌ぐ可能性を有してい
る。しかし媒体の製造法として溶液からのスピン
コート法及びキヤステイング法をとらねばならな
いので光学記録用媒体を大型化する場合これらの
方法で均一な薄膜を作成することは非常に困難で
ある。更に溶液状態で染料等の吸収体とバインダ
を均一に分散させることは困難で、染料等の分散
の不均一性のために解像度が悪いという欠点を有
する。
フルオレセインの薄膜は蒸着によつて得られ
Te酸化物と同等の感度分解能を有する。しかし
吸収波長が480nmの可視部にあるため、書込
み、読み出しの光源が限定され記録・再生装置の
小型化に適している半導体レーザの発振波長に対
応できないという欠点を有している。吸収波長が
長波長の色素の蒸着が容易に類推されるが、通常
の長波長光吸収色素は熱安定性、昇華性に欠点を
持ち、薄膜を形成させることは一般に困難であ
る。(共立全書「写真化学」第62頁)
本発明は前記現状に鑑みてなされたもので、そ
の目的は比較的長波長帯に光吸収能のあるスクア
リリウム色素を基板上に薄膜として設けた光学記
録用媒体を提供することであり、又他の目的は薄
膜組成の再現性及び薄膜の均一性において優れた
光学記録用媒体を提供することである。
前記目的を達成する本発明の光学記録用媒体は
基板上に一般式
The present invention utilizes optical recording media, more specifically lasers, and in particular, optical energy with a relatively long wavelength that is compatible with the oscillation wavelength of a semiconductor laser, which allows the recording/reading system to be miniaturized. This invention relates to optical recording media that utilize state changes such as natural melting, evaporation, and sublimation. Conventionally, this type of recording medium has been made of chalcogenite-based amorphous glass (see Japanese Patent Publication No. 54-20136),
Te oxide (see Japanese Patent Publication No. 54-3725), carbon black dispersed self-oxidizing binder (Japanese Patent Publication No. 51
-35144), fluorescein (IEEE,
Spectrum August 1978, p. 20) etc. were used. Chalcogenite amorphous glass is used in the form of a vapor-deposited film as an optical recording material. This material is stable in both the amorphous and crystalline states, but in order to obtain a thin film using methods such as vapor deposition, a manufacturing process is required in which predetermined components are dissolved in a solid solution in vacuum and then rapidly cooled to obtain a uniform raw material. . Furthermore, since there are many kinds of component elements, it is difficult to obtain a raw material with a uniform composition and form a thin film. Furthermore, a thin film of chalcogenite-based amorphous glass has a large initial optical density in an unrecorded state, and has the disadvantage that when the contrast ratio is set high, the readout efficiency is extremely low. Te oxide thin films, which have higher sensitivity than chalcogenite amorphous glasses, are manufactured by vapor-depositing TeO2 , but the main component forming the thin film is TeOX (X
is assumed to be 0<X<2), and the composition of the thin film changes depending on the deposition conditions, making it quite difficult to manufacture a uniform thin film. Also, the sensitive wavelength range of Te oxide thin film is 350 to 600n.
m, and has the disadvantage that it essentially has no sensitivity when a recording light source is used in a long wavelength region. When a dye-dispersed organic thin film uses a self-oxidizing material such as nitrocellulose as a binder, it has the potential to surpass the above-mentioned inorganic thin film in terms of sensitivity. However, since the medium must be manufactured using a spin coating method from a solution or a casting method, it is very difficult to create a uniform thin film using these methods when increasing the size of an optical recording medium. Furthermore, it is difficult to uniformly disperse absorbers such as dyes and binders in a solution state, and there is a drawback that resolution is poor due to non-uniformity of dispersion of dyes etc. Thin films of fluorescein are obtained by vapor deposition.
It has the same sensitivity resolution as Te oxide. However, since the absorption wavelength is in the visible region of 480 nm, the light source for writing and reading is limited, and it has the disadvantage that it cannot correspond to the oscillation wavelength of semiconductor lasers, which are suitable for downsizing recording and reproducing devices. The vapor deposition of dyes with long absorption wavelengths is easily inferred, but ordinary long wavelength light-absorbing dyes have drawbacks in thermal stability and sublimability, and it is generally difficult to form thin films. (Kyoritsu Zensho Photo Chemistry, p. 62) The present invention was made in view of the above-mentioned current situation, and its purpose is to provide optical recording using a thin film on a substrate of squarylium dye, which has the ability to absorb light in a relatively long wavelength range. Another object of the present invention is to provide an optical recording medium that is excellent in reproducibility of thin film composition and uniformity of thin film. The optical recording medium of the present invention which achieves the above object has a general formula on a substrate.
【式】又は[Formula] or
【式】
(式中Xは発色団を示す)で表わされるスクアリ
リウム色素からなる有機薄膜を設けたことを特徴
とするものである。
本発明について詳細に説明すると、本発明にお
いて有機薄膜を形成させる前記一般式で表わされ
るスクアリリウム色素はスクアリツク酸(3・4
−ジヒドロキシ−3−シクロブテン−1・2−ジ
オン)と対応する発色団を有する化合物とを縮合
反応させることにより得られる化合物である。
次に本発明において使用されるスクアリリウム
色素の若干の具体例を次表に示す。It is characterized by providing an organic thin film made of a squarylium dye represented by the formula: (wherein X represents a chromophore). To explain the present invention in detail, in the present invention, the squarylium dye represented by the general formula above that forms an organic thin film is squaric acid (3.4
-dihydroxy-3-cyclobutene-1,2-dione) and a compound having a corresponding chromophore. Next, some specific examples of squarylium dyes used in the present invention are shown in the following table.
【表】【table】
【表】
スクアリリウム色素は比較的長波長帯に光吸収
能を有するが、通常の染料に比較して保存性、耐
熱性に優れており、昇華操作に耐え得るという特
性を有する。
これらの色素が鋭い融解性及び昇華性を有する
一例を第1図に示した。第1図において曲線11
は表に示す色素のうち(4)−(a)の熱重量変化曲線
TGであり、280℃前後で著しい重量減を示してい
る。一方曲線12は同じ色素の示差走査熱量曲壁
DSCであり、13は312℃においてこの色素が融
点を有することを示し、14は370℃以上で色素
が分解することを示している。図に示すように、
この色素は280℃前後の狭い温度範囲で昇華性が
あることは明らかである。又昇華・分解温度間
に、温度的余裕があり、基板上に容易に蒸着で
き、蒸着膜へのレーザ記録も解像度よく行なうこ
とができることを示している。
したがつて、本発明においてはスクアリリウム
色素をポリエステルフイルム、テフロン等のプラ
スチツク類、ガラス又は金属等の基板上に直接蒸
着することにより薄膜組成の再現性及び薄膜の均
一性を達成できる。
又スクアリリアム色素はその種類によりその有
機色素特有の吸収帯を有するので、記録用光源の
種類、波長に応じてスクアリリウム色素を選択す
ることにより非常に大きな薄膜の吸収係数が得ら
れ、したがつて従来の材料に比較して感度の向上
と信号/雑音(S/N)比の向上を達成できる。
次に本発明を実施例について説明するが、本発
明はこれによりなんら限定されるものではない。
実施例 1
前記表の(1)の構造の色素500mgを蒸着用Moボー
トに入れ1×10-6mmHg以下に排気した後パイレ
ツクス(登録商標、以下略)基板に蒸着する。蒸
着中は真空室内の圧力が10-5mmHg以上に上昇し
ないようにヒーターを制御する。こうしてパイレ
ツクス基板の光学記録用媒体を作製した。
前記光学記録用媒体に波長632nmのHe−Neレ
ーザを照射すると露光部分は昇華して、露光部の
薄膜は消失した。第2図の曲線22及び21に(1)
の色素を厚さ0.2μmに蒸着した媒体のHe−Neレ
ーザ照射前及び照射後の可視近赤外部の透過率を
示す。これにより650〜750nm帯に発振波長を有
するレーザにより記録可能なことは明らかであ
る。He−Neレーザ光に対する記録感度は約50m
J/cm2であつた。
実施例 2
実施例1と同様にして前記表の(4)−(a)の色素を
Al蒸着した基板上に厚さ0.2μmに蒸着して光学
記録用媒体を作製した。これにHe−Neレーザ照
射し、媒体の反射光を測定し、その結果を第3図
に示す。曲線32及び曲線31はそれぞれレーザ
照射前及び照射後の反射スペクトルを示す。第3
図から明らかなように反射モードでも露光部と未
露光部のコントラストが十分にとれる。記録感度
は約40mJ/cm2であつた。
実施例 3
実施例1、2と同様にして前記表の(5)−(a)の色
素をパイレツクス基板上に厚さ0.15μmに蒸着し
て光学記録用媒体を作製した。これに830nmの
半導体レーザを照射した。媒体の透過光を測定
し、その結果を第4図に示す。曲線42及び曲線
41はそれぞれレーザ照射前及び照射後の透過率
を示す。色素(1)、色素(4)−(a)より吸収はブロード
になるが830nmの光に対して記録可能なことは
明らかである。半導体レーザに対する記録感度は
約50mJ/cm2であつた。
上記実施例から明らかなように、本発明はスク
アリリウム色素を使用することにより次の利点を
有する。
(1) 製造法が容易
組成が単一の有機色素であり、蒸着その他の
方法で容易に均一かつ良質の薄膜が得られる。
又媒体の基板材料としてガラス、金属の他に、
蒸着が容易で基板温度の上昇が小さいためにプ
ラステイツク、紙なども基板材料として使用で
きる。
(2) 感度が高い
実施例で示したように、記録用光源の波長に
応じた色素を選択することにより、記録用光源
の種類に拘わらず高い感度を有する。感度的に
は金属薄膜、カルコゲナイト系ガラスの数分の
1、Te酸化物薄膜と同等である。
(3) コントラスト比が高い
透過モード、反射モードで記録の読み出しを
行なう場合、媒体上の物質が完全に除去される
ため露光前後のコントラスト比は極めて大き
い。
(4) 解像度が高い
有機物色素は元来熱伝導率が低く、実施例で
示したような記録を行なう場合、解像度は薄膜
の熱伝導率に依存するが、この点で優れてい
る。また第1図に示したようにスクアリリウム
色素の熱特性は変化部が非常に鋭く、照射エネ
ルギによる変化のしきい値が明確であつて1000
ライン/cm以上の解像度を有している。
(5) 安定性が高い
コントラスト比が非常に大きいために、読み
出し用の光エネルギは小さくとどめることが可
能なために長期の使用に対しても極めて安定性
が高い。又吸収波長域が他の光学記録用媒体に
対して狭いため、吸収域以外の光に対しての安
定性は特に優れている。[Table] Squarylium dyes have the ability to absorb light in a relatively long wavelength range, but compared to ordinary dyes, they have excellent storage stability and heat resistance, and have the characteristics of being able to withstand sublimation operations. An example of these dyes having sharp melting and sublimation properties is shown in FIG. In Figure 1, curve 11
is the thermogravimetric change curve of (4)−(a) among the pigments shown in the table.
TG, and shows a significant weight loss at around 280℃. On the other hand, curve 12 is the differential scanning calorimetry curve of the same dye.
DSC, 13 indicates that the dye has a melting point at 312°C, and 14 indicates that the dye decomposes above 370°C. As shown in the figure,
It is clear that this dye is sublimable in a narrow temperature range around 280°C. It also shows that there is a temperature margin between the sublimation and decomposition temperatures, making it possible to easily deposit the film on the substrate and to perform laser recording on the deposited film with good resolution. Therefore, in the present invention, reproducibility of the thin film composition and uniformity of the thin film can be achieved by directly depositing the squarylium dye onto a substrate such as a polyester film, plastics such as Teflon, glass, or metal. Furthermore, squarylium dyes have absorption bands specific to the organic dye depending on their type, so by selecting a squarylium dye according to the type and wavelength of the recording light source, a very large thin film absorption coefficient can be obtained. It is possible to achieve improved sensitivity and improved signal/noise (S/N) ratio compared to conventional materials. Next, the present invention will be described with reference to Examples, but the present invention is not limited thereto in any way. Example 1 500 mg of the dye having the structure shown in Table (1) above was placed in a Mo boat for vapor deposition, evacuated to below 1 x 10 -6 mmHg, and then vapor deposited on a Pyrex (registered trademark, hereinafter omitted) substrate. During deposition, the heater is controlled so that the pressure in the vacuum chamber does not rise above 10 -5 mmHg. In this way, a Pyrex substrate optical recording medium was produced. When the optical recording medium was irradiated with a He--Ne laser having a wavelength of 632 nm, the exposed area sublimated and the thin film at the exposed area disappeared. Curves 22 and 21 in Figure 2 (1)
This figure shows the transmittance in the visible and near-infrared region before and after irradiation with a He-Ne laser for a medium on which a dye of 0.2 μm is deposited to a thickness of 0.2 μm. It is clear that recording can be performed using a laser having an oscillation wavelength in the 650-750 nm band. Recording sensitivity for He-Ne laser light is approximately 50m
It was J/ cm2 . Example 2 The dyes (4)-(a) in the table above were prepared in the same manner as in Example 1.
An optical recording medium was prepared by depositing Al to a thickness of 0.2 μm on a substrate. This was irradiated with a He--Ne laser and the reflected light from the medium was measured. The results are shown in FIG. Curve 32 and curve 31 show the reflection spectra before and after laser irradiation, respectively. Third
As is clear from the figure, even in the reflection mode, there is sufficient contrast between the exposed and unexposed areas. The recording sensitivity was approximately 40 mJ/cm 2 . Example 3 In the same manner as in Examples 1 and 2, the dyes (5) to (a) in the table above were deposited on a Pyrex substrate to a thickness of 0.15 μm to prepare an optical recording medium. This was irradiated with an 830 nm semiconductor laser. The transmitted light of the medium was measured and the results are shown in FIG. Curve 42 and curve 41 show the transmittance before and after laser irradiation, respectively. Although the absorption is broader than that of dye (1) and dye (4)-(a), it is clear that recording is possible for light of 830 nm. The recording sensitivity to the semiconductor laser was approximately 50 mJ/cm 2 . As is clear from the above examples, the present invention has the following advantages by using squarylium dye. (1) Easy to manufacture Since the composition is a single organic dye, uniform and high-quality thin films can be easily obtained by vapor deposition or other methods.
In addition to glass and metal, media substrate materials include
Plastics, paper, etc. can also be used as substrate materials because vapor deposition is easy and the rise in substrate temperature is small. (2) High sensitivity As shown in the examples, by selecting a dye according to the wavelength of the recording light source, high sensitivity can be achieved regardless of the type of recording light source. In terms of sensitivity, it is a fraction of that of metal thin films and chalcogenite glass, and is equivalent to Te oxide thin films. (3) High contrast ratio When reading records in transmission mode or reflection mode, the contrast ratio before and after exposure is extremely high because the substance on the medium is completely removed. (4) High resolution Organic dyes inherently have low thermal conductivity, and when recording as shown in the examples, the resolution depends on the thermal conductivity of the thin film, but they are excellent in this respect. In addition, as shown in Figure 1, the thermal properties of squarylium dye have very sharp changes, and the threshold for change due to irradiation energy is clear.
It has a resolution of lines/cm or higher. (5) High stability Because the contrast ratio is extremely high, the light energy for reading can be kept small, so it is extremely stable even for long-term use. Furthermore, since the absorption wavelength range is narrower than that of other optical recording media, the stability against light outside the absorption range is particularly excellent.
第1図は発明の詳細な説明の欄に記載した表の
(4)−(a)のスクアリリウム色素の熱特性図、第2図
は同表の(1)のスクアリリウム色素の光記録特性、
第3図は同表の(4)−(a)のスクアリリウム色素の光
記録特性、第4図は同表の(5)−(a)のスクアリリウ
ム色素の光記録特性を示す。
Figure 1 shows the table described in the detailed description of the invention.
(4)-(a) Thermal characteristics diagram of the squarylium dye, Figure 2 shows the optical recording characteristics of the squarylium dye shown in (1) of the same table.
FIG. 3 shows the optical recording characteristics of the squarylium dyes shown in (4)-(a) of the same table, and FIG. 4 shows the optical recording characteristics of the squarylium dyes shown in (5)-(a) of the same table.
Claims (1)
り光学的濃度変化を得る光学記録媒体において、
基板上に一般式 【式】又は【式】 (式中Xは発色団を示す)で表わされるスクアリ
リウム色素からなる有機薄膜を設けたことを特徴
とする光学記録用媒体。[Claims] 1. An optical recording medium that obtains an optical density change by applying optical or thermal energy,
An optical recording medium characterized in that an organic thin film made of a squarylium dye represented by the general formula [Formula] or [Formula] (wherein X represents a chromophore) is provided on a substrate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12013879A JPS5646221A (en) | 1979-09-20 | 1979-09-20 | Optically recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12013879A JPS5646221A (en) | 1979-09-20 | 1979-09-20 | Optically recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5646221A JPS5646221A (en) | 1981-04-27 |
| JPS6236878B2 true JPS6236878B2 (en) | 1987-08-10 |
Family
ID=14778898
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12013879A Granted JPS5646221A (en) | 1979-09-20 | 1979-09-20 | Optically recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5646221A (en) |
Families Citing this family (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| NL8301632A (en) * | 1983-05-09 | 1984-12-03 | Philips Nv | REGISTRATION HOLDER IN WHICH INFORMATION CAN BE REGISTERED AND READ OUT BY OPTICAL ROAD. |
| JPH0822618B2 (en) * | 1986-12-16 | 1996-03-06 | 富士ゼロックス株式会社 | Method for manufacturing optical information storage medium |
| JPH0822617B2 (en) * | 1986-12-16 | 1996-03-06 | 富士ゼロックス株式会社 | Method for manufacturing optical information storage medium |
| JPH0730300B2 (en) * | 1988-04-01 | 1995-04-05 | 三井東圧化学株式会社 | Alkyl phthalocyanine near infrared absorber and display / recording material using the same |
| CA2033821A1 (en) * | 1990-01-12 | 1991-07-13 | Evan D. Laganis | Photopolymerizable compositions sensitive to longer wavelength visible actinic radiation |
| US6063467A (en) * | 1997-02-24 | 2000-05-16 | Fuji Electric Co., Ltd. | Optical recording medium |
| US6103331A (en) * | 1997-09-26 | 2000-08-15 | Fuji Electric Co., Ltd. | Optical recording medium comprising organic dye thin film |
| JP3097628B2 (en) * | 1997-11-11 | 2000-10-10 | 富士電機株式会社 | Optical recording medium |
| DE10196853B4 (en) * | 2001-10-23 | 2005-02-17 | Council Of Scientific And Industrial Research | Squarain-based dyes and methods of making the same |
-
1979
- 1979-09-20 JP JP12013879A patent/JPS5646221A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5646221A (en) | 1981-04-27 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US4492750A (en) | Ablative infrared sensitive devices containing soluble naphthalocyanine dyes | |
| JPS58112792A (en) | Optical information recording medium | |
| JPH0749231B2 (en) | Optical recording body | |
| JPS6387282A (en) | Medium for optical recording | |
| JPS6236878B2 (en) | ||
| JPS61146595A (en) | Medium for optical recording | |
| JPS5816888A (en) | Lasers-recording film | |
| JPH0696347B2 (en) | Optical recording body | |
| JP2685054B2 (en) | Naphthoquinone methide compounds | |
| EP0381210A2 (en) | Optical recording media and process for preparing same | |
| JPS59144056A (en) | Optical recording medium and its production | |
| JPH0139916B2 (en) | ||
| JPH0152192B2 (en) | ||
| JPS5911292A (en) | Recording medium | |
| JPH0155118B2 (en) | ||
| JPS6364794A (en) | Optical recording medium | |
| JPS63164037A (en) | Optical information recording medium | |
| JPS63199759A (en) | Dioxazinaphthopentacene derivatives and optical recording media using the derivatives | |
| JPS58217391A (en) | Optical recording medium | |
| JP4158553B2 (en) | Optical recording method | |
| JPS615441A (en) | Optical recording and reading out method | |
| JPS62216795A (en) | Optical recording medium | |
| JPS62164594A (en) | Optical information recording medium | |
| JPS62193886A (en) | Optical information-recording medium | |
| JPS62193885A (en) | Optical information-recording medium |