JPS6127291A - Laser recording medium and production thereof - Google Patents

Laser recording medium and production thereof

Info

Publication number
JPS6127291A
JPS6127291A JP59149040A JP14904084A JPS6127291A JP S6127291 A JPS6127291 A JP S6127291A JP 59149040 A JP59149040 A JP 59149040A JP 14904084 A JP14904084 A JP 14904084A JP S6127291 A JPS6127291 A JP S6127291A
Authority
JP
Japan
Prior art keywords
recording
laser
recording medium
recording layer
film
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.)
Granted
Application number
JP59149040A
Other languages
Japanese (ja)
Other versions
JPH0558913B2 (en
Inventor
Hikari Ishimoto
光 石本
Nobuyoshi Seto
瀬戸 順悦
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP59149040A priority Critical patent/JPS6127291A/en
Publication of JPS6127291A publication Critical patent/JPS6127291A/en
Publication of JPH0558913B2 publication Critical patent/JPH0558913B2/ja
Granted legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B41PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
    • B41MPRINTING, DUPLICATING, MARKING, OR COPYING PROCESSES; COLOUR PRINTING
    • B41M5/00Duplicating or marking methods; Sheet materials for use therein
    • B41M5/26Thermography ; Marking by high energetic means, e.g. laser otherwise than by burning, and characterised by the material used

Landscapes

  • Physics & Mathematics (AREA)
  • Optics & Photonics (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)

Abstract

PURPOSE:To ensure high sensitivity, high density and reversibility, by a construction wherein a recording layer is constituted of a built-up film of a J-associate of molecules of an organic coloring matter so that it has an absorption band in an oscillation wavelength range of laser. CONSTITUTION:The laser recording medium comprises a base, a reflective layer and the recording layer, in which the recording layer is constituted of a built-up film of the J-associate product of the molecules of an organic coloring matter and has an absorption band in the oscillation wavelength range of laser. The J-associate product is provided in the form of a built-up film by the Langmuir- Blodgett's method. First, a solution of a coloring matter of formula ( I ), wherein X is halogen, in an organic solvent (the dye may be mixed with arachic acid) is poured dropwise on a water surface in a water tank, and is spread to obtain a monomolecular film. Next, while compressing the monomolecular film under a fixed surface pressure, a substrate so disposed as to orthogonally traverse the water surface is repeatedly moved up and down a desired number of times, thereby transferring the film onto the substrate. Accordingly, the J-associate product in which the molecules of the coloring matter are oriented and arranged in a special aggregated condition can be obtained.

Description

【発明の詳細な説明】 産業上の利用分野 本発明はレーザ記録媒体及びその製造方法に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a laser recording medium and a method for manufacturing the same.

背景技術とその問題点 有機色素を用いたレーザ光記録媒体は従来多数試作され
ているが、これら記録媒体における記録原理は、色素が
レーザ光を吸収して生じる熱による記録媒体の形状変化
に基づいているため、実用するに当たって、記録層を直
接両面から密閉保護することが困難であり、エアーサン
ドインチ構造の採用などの対策を要し、記録媒体が複雑
な構造となる。また、これらの従来の記録媒体において
は、記録個所の形状変化を均一な形と微小な寸法゛のス
ポットに制御するための配慮を要する。このため1、こ
れらの記録媒体の記録原理自体が、最近強く要望されて
いる高密度化記録に対して障害となっている。さらに、
媒体の前記形状変化を起こすためには融解・気化のエネ
ルギーが最低限必要であり、且つこの形状変化は記録ピ
ントからの色素分子の離散を伴うものであり、従って可
逆性がない。
BACKGROUND TECHNOLOGY AND PROBLEMS A large number of laser beam recording media using organic dyes have been prototyped in the past, but the recording principle of these recording media is based on the change in shape of the recording medium due to the heat generated when the dye absorbs the laser beam. Therefore, in practical use, it is difficult to directly hermetically protect the recording layer from both sides, and measures such as the adoption of an air sandwich structure are required, resulting in a recording medium with a complicated structure. In addition, in these conventional recording media, consideration must be given to controlling the change in the shape of the recording location to a spot with a uniform shape and minute size. For this reason, (1) the recording principle of these recording media itself is an obstacle to high-density recording, which has been strongly desired recently. moreover,
A minimum amount of energy for melting and vaporization is required to cause the above-mentioned shape change of the medium, and this shape change is accompanied by the separation of dye molecules from the recording focus, and is therefore not reversible.

有機色素分子、例えばシアニン色素は水溶液中での色素
の濃度が高くなると、色素の単分子による吸収帯及びこ
れより短波長側の二量体吸収帯と多分子会合体吸収帯の
外に、単分子吸収帯より長波長側に吸収強度が大きく、
半値幅の非常に狭い吸収帯をもつ。この吸収帯はJ−吸
収帯と呼ばれ、J−会合体と呼ばれる色素の集合状態に
属することが知られている。
When the concentration of organic dye molecules, such as cyanine dyes, increases in an aqueous solution, in addition to the absorption band of a single dye molecule, the dimer absorption band and the multimolecular association absorption band on the shorter wavelength side, The absorption intensity is large on the longer wavelength side than the molecular absorption band,
It has an absorption band with a very narrow half-width. This absorption band is called a J-absorption band, and is known to belong to an aggregated state of dyes called a J-aggregate.

本発明者らは、このJ−会合体が加熱によって解離し、
解離前後で吸収スペクトルが大きく変化することに着目
し、J−会合体の累積膜を記録層に利用することによっ
て本発明を完成するに牟った。
The present inventors discovered that this J-aggregate dissociates upon heating,
Noting that the absorption spectrum changes significantly before and after dissociation, the present invention was completed by utilizing a cumulative film of J-aggregates as a recording layer.

発明の目的 本発明は、前記の点に潅み、高感度、高密度及び可逆性
の各特性を有する、有機色素を用いたレーザ光記録媒体
及びその製造方法を提供するものである。
OBJECTS OF THE INVENTION The present invention addresses the above points and provides a laser beam recording medium using an organic dye and a method for manufacturing the same, which has characteristics of high sensitivity, high density, and reversibility.

発明の概要 本発明に係るレーザ記録媒体は、基板と、反射層と、記
録層とを有するレーザ記録媒体において、前記記録層が
有機色素分子のJ−会合体の累積膜であり且つレーザの
発振波長域に吸収帯を有するものであることを特徴とす
る。
Summary of the Invention A laser recording medium according to the present invention includes a substrate, a reflective layer, and a recording layer, in which the recording layer is a cumulative film of J-aggregates of organic dye molecules, It is characterized by having an absorption band in the wavelength range.

また、本発明に係る前記レーザ記録媒体の製造方法は、
前記、J−会合体をラングミュア・ブロジェット法(以
下、LB法と記す)により累積膜として形成することを
特徴とする。
Further, the method for manufacturing the laser recording medium according to the present invention includes:
The J-aggregate is formed as a cumulative film by the Langmuir-Blodgett method (hereinafter referred to as LB method).

本発明のレーザ記録媒体における各層の積層順序は、(
a)基板−反射層−記録層及び(b)基板−記録層−反
則層のいずれであってもよい。前記(b)の積層順序に
よれは、両側から密閉保護された記録層に記録すること
ができる。
The lamination order of each layer in the laser recording medium of the present invention is (
Either a) substrate-reflection layer-recording layer or (b) substrate-recording layer-fouling layer may be used. Depending on the lamination order in (b) above, recording can be performed on a recording layer that is hermetically protected from both sides.

前記有機色素分子としては、例えば次式(I)(式中、
Xはハロゲンを表す) のシアニン色素が挙げられる。
As the organic dye molecule, for example, the following formula (I) (wherein,
X represents a halogen).

L B法による前記、J−会合体累積膜の形成は次の通
り行うことができる。まず、水槽の水面に有機溶媒に熔
解した前記一般式(1)の色素(他の成膜分子、例えば
アラキン酸と混合してもよい)を滴下、展開して単分子
膜を得る。次にこの単分子膜を一定表血圧下で圧縮しな
がら、水面を垂直に横切る基板を繰返し所望回数上下動
させてこれに移し採る。こうして、色素分子が配向、配
列して特殊な集合状態のJ−会合体が形成される。この
色素分子のJ−会合体においては、熱による微小な集合
状態の変化に伴って、光吸収スペクトルが大きく変化す
る。本発明のレーザ記録媒体はこの色素分子の集合状態
のレーザ光による微小な変化を記録原理としている。
The formation of the J-aggregate cumulative film by the LB method can be performed as follows. First, the dye of general formula (1) dissolved in an organic solvent (which may be mixed with other film-forming molecules, such as arachidic acid) is dropped onto the water surface of a water tank and spread to obtain a monomolecular film. Next, while compressing this monomolecular film under a constant pressure, it is transferred onto a substrate that vertically crosses the water surface by repeatedly moving it up and down a desired number of times. In this way, the dye molecules are oriented and arranged to form a J-aggregate in a special state of assembly. In this J-aggregate of dye molecules, the light absorption spectrum changes greatly as a result of minute changes in the state of assembly caused by heat. The laser recording medium of the present invention uses the recording principle of minute changes in the aggregated state of dye molecules caused by laser light.

本発明のレーザ記録媒体における記録層は、記録原理か
ら理解できるように、記録ピントからの色素の離散を伴
わないため、原理的に可逆的であり、書換えが可能であ
る。
As can be understood from the recording principle, the recording layer in the laser recording medium of the present invention is reversible and rewritable in principle since the dye does not disperse from the recording focus.

以下に、本発明の実施例につき図面を参照しながら説明
する。
Embodiments of the present invention will be described below with reference to the drawings.

実施例1  ′ 第1図に本実施例のレーザ記録媒体1を示す。Example 1 ′ FIG. 1 shows a laser recording medium 1 of this embodiment.

この記録媒体1は、硝子基板2、アルミニラ1、反射膜
3 (厚さ約2,000人)及び記録層4(厚さ約1、
.600人)が図示の順序に積層されてなる。記録層4
は、次式(II) で示されるシアニン色素とアラキン酸(C1qH3qc
OOtl)との累積膜から成り、この膜中で前記シアニ
ン色素は、J−会合体として存在している。この記録媒
体lは次のようにして製造することができる。
This recording medium 1 includes a glass substrate 2, an aluminum laminate 1, a reflective film 3 (about 2,000 layers thick), and a recording layer 4 (about 1 layer thick).
.. 600 people) were stacked in the order shown. Recording layer 4
is a cyanine dye represented by the following formula (II) and arachidic acid (C1qH3qc
The cyanine dye is present as a J-aggregate in this film. This recording medium 1 can be manufactured as follows.

前記式(II)のシアニン色素とアラキン酸とをモル比
1=4でジクロロメタン/メタノール(4:1)に溶解
し、アラキン酸の濃度カ月mg/mβになるように溶液
を調製した。この溶液を16℃の蒸留水の水面に、アラ
キン酸の占有断面積が1分子当り25人2になるまで滴
下して単分子膜を展開した後、水面の仕切りを動かして
表面圧が106yne/ Cmになるまで圧縮し、15
分間放置後、さらに40 dyne/ cmまで圧縮し
た。この単分子膜をり、 r3 法テ、厚さ約2,00
0 人のアルミニウム反射膜3の伺いノこカラス基板2
に50層累積させて厚さ約1,600 Aの記録層4を
形成し、乾燥して記録媒このようにして作製した記録媒
体lの記録層4側から光を照射して反射吸収スペクトル
を測定したところ、第2図の曲線Aを得た。一方、前記
(II)式のシアニン色素の単分子の吸収スペクトル(
10−’Mメタノール溶液で測定)は第2図の曲線Bに
示す通りであった。曲線Aを曲線Bと比較することによ
り、曲線Aの785nmにおける吸収帯はJ−会合体と
いわれる色素の集合状態に属するものであることが確認
でき、記録層4内の前記シアニン色素がJ−会合体で存
在していることかわかる。この記録層4にフラッジJ、
光を照射して瞬間的に加熱したところ、J−会合体の集
合状態が乱されるために、第2図の破線Cに示すように
785nmの吸収帯が消えた。
The cyanine dye of formula (II) and arachidic acid were dissolved in dichloromethane/methanol (4:1) at a molar ratio of 1=4, and a solution was prepared such that the concentration of arachidic acid was 1 mg/mβ. This solution was dropped onto the surface of distilled water at 16°C until the occupied cross-sectional area of arachidic acid became 25 yne/molecule per molecule to develop a monomolecular film, and then the partition on the water surface was moved to increase the surface pressure to 106 yne/2. Compress until cm, 15
After standing for a minute, it was further compressed to 40 dyne/cm. This monomolecular film is coated with R3 method and has a thickness of approximately 2,000 mm.
0 People's Aluminum Reflective Film 3 Inquiry Saw Crow Substrate 2
A recording layer 4 with a thickness of about 1,600 A was formed by accumulating 50 layers, and the recording medium L was dried and irradiated with light from the side of the recording layer 4 of the thus prepared recording medium 1 to obtain a reflection/absorption spectrum. As a result of the measurement, curve A shown in FIG. 2 was obtained. On the other hand, the absorption spectrum of a single molecule of the cyanine dye of formula (II) (
(measured with a 10-'M methanol solution) was as shown in curve B of FIG. By comparing curve A with curve B, it can be confirmed that the absorption band at 785 nm of curve A belongs to the aggregation state of the dye called J-aggregate, and the cyanine dye in the recording layer 4 is J-aggregate. It can be seen that it exists as an aggregate. In this recording layer 4, Fludge J,
When the material was instantaneously heated by irradiation with light, the aggregation state of the J-aggregates was disturbed, so that the absorption band at 785 nm disappeared as shown by the broken line C in FIG.

第3図に、記録層4に波長785nmの半導体レーザ光
を1.6μm径に7 、5mWのパワー(記録層4上)
でパルス照射して得られた反射率変化をグラフで示す。
In Figure 3, a semiconductor laser beam with a wavelength of 785 nm is applied to the recording layer 4 with a diameter of 1.6 μm, and a power of 5 mW (on the recording layer 4).
The graph shows the change in reflectance obtained by pulse irradiation.

この反射率変化はパルス照射(書込み)に用いたレーザ
の出力を弱くして、パルス照射前後の反射光強度を測定
して求めた。その結果、最大レーザ出力(7,5mW 
)で0.1 μsのパルス照射で15%の反射率変化(
10%→25%)が得られた。これは約0.03 J 
/cm2の感度になり、半導体レーザを用いた実時間ビ
デオ信号記録用媒体に必要な感度にほぼ匹敵する。
This reflectance change was determined by weakening the output of the laser used for pulse irradiation (writing) and measuring the reflected light intensity before and after pulse irradiation. As a result, the maximum laser output (7,5mW
), a 15% reflectance change (
10% → 25%) was obtained. This is about 0.03 J
/cm2, which is almost comparable to the sensitivity required for a real-time video signal recording medium using a semiconductor laser.

実h1!!例2 この実施例では、第4図に示す通り、カラス基板2トに
実施例1と同様な手順で直接記録層4(厚さ約1,60
0人)を形成し、その」二にアルミニウム反射膜(厚さ
約1..000人)を設けてレーザ記録媒体5を得た。
Real h1! ! Example 2 In this example, as shown in FIG. 4, a recording layer 4 (with a thickness of approximately 1.60 mm
A laser recording medium 5 was obtained by forming an aluminum reflective film (about 1.000 mm thick) on the second layer.

従って、記録層4ば両側から保護されている。Therefore, the recording layer 4 is protected from both sides.

この記録媒体5について、半導体レーザ光を、ガラス基
板2側から照1・1する以外は実施例1の場合と同様に
して照射して、第5図のグラフに示した反躬率変1ヒを
得た。このように、本実施例の記録媒体5の構成によれ
ば、両側から密閉保護さた記録層4に記録することがで
きる。
This recording medium 5 was irradiated with semiconductor laser light in the same manner as in Example 1 except that it was irradiated from the glass substrate 2 side, and the reflux rate change 1 curve shown in the graph of FIG. I got it. As described above, according to the configuration of the recording medium 5 of this embodiment, recording can be performed on the recording layer 4 which is hermetically protected from both sides.

なお、前記各実施例において、反射層と記録層との間に
透明層、例えばアラキン酸累積膜を設りて、記録層の累
積層数を減少させてもよい。
In each of the above embodiments, a transparent layer, for example, an arachidic acid cumulative film, may be provided between the reflective layer and the recording layer to reduce the cumulative number of recording layers.

発明の効果 以上のように、本発明の記録媒体は記録層がイ1機色素
分子のJ−会合体であるために、本発明によって次の効
果が得られる。
Effects of the Invention As described above, in the recording medium of the present invention, since the recording layer is a J-aggregate of monochromatic dye molecules, the following effects can be obtained by the present invention.

(1)、J−会合体の集合状態の変化は色素分子数個〜
数十個を単位として起こるものであるため、記録を担う
媒体の単位が非常に小さく、均一な形と微小な寸法の記
録スポットが得られ、従って高密度記録が可能となる。
(1), the change in the assembly state of the J-aggregate is caused by several dye molecules ~
Since the recording occurs in units of several tens, the unit of the medium responsible for recording is extremely small, and recording spots with uniform shapes and minute dimensions can be obtained, thus enabling high-density recording.

(2)、記録媒体の大きな形状変化を伴わないため、記
録層を両面から保護することが可能となり、実用に当た
って記録媒体の構造が簡単で済む。
(2) Since there is no major change in the shape of the recording medium, it is possible to protect the recording layer from both sides, and the structure of the recording medium is simple in practical use.

(3)、記録原理が色素分子の集合状態の微小な変化に
伴う吸収スペクトルの変化を利用したものであるため、
記録過程に要するエネルギーが小さくて済み、従って高
い記録感度を得ることができる。
(3) The recording principle utilizes changes in the absorption spectrum due to minute changes in the aggregated state of dye molecules;
The energy required for the recording process is small, and therefore high recording sensitivity can be obtained.

(4)、更に、記録原理が記録ピントからの色素の離散
を伴わないため、可逆的な書換え可能な記録媒体となり
得る。
(4) Furthermore, since the recording principle does not involve dispersion of the dye from the recording focus, it can be a reversible and rewritable recording medium.

また、本発明の方法によれば、記録層を形成するJ−会
合体はL B法により累積膜として作製されるので、記
録層の膜1ν、を精度よく制御することができる。
Furthermore, according to the method of the present invention, since the J-aggregates forming the recording layer are produced as a cumulative film by the LB method, the film 1ν of the recording layer can be controlled with high precision.

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

第1図は本発明のレーザ記録媒体の第1実施態様の断面
図、第2図は吸収スペクトルを示すグラフ、第3図は第
1実施態様における反射率変化を示すグラフ、第4図は
本発明の第2実施態様の断面図及び第5図は第2実施態
様における反射率変化を示すグラフである。 なお図面に用いられた符号において、 1−・・−−−−−−−−一一−−−−−記録媒体2−
−−−−−−−−−−−−一基板 3−−−−一−−−・−−−−一−−反射膜4−−−−
・−−−−−−−一記録層 5−−−−−−−・−−−−−−−・記録媒体6−・−
−−−−−−一−−−−・−反射膜である。 第1図 第2図
FIG. 1 is a cross-sectional view of the first embodiment of the laser recording medium of the present invention, FIG. 2 is a graph showing the absorption spectrum, FIG. 3 is a graph showing reflectance changes in the first embodiment, and FIG. A cross-sectional view of the second embodiment of the invention and FIG. 5 are graphs showing reflectance changes in the second embodiment. In addition, in the symbols used in the drawings, 1-...-----11--Recording medium 2-
-----------1--Substrate 3----1-----・---1--Reflecting film 4--
---------One recording layer 5------------Recording medium 6--
---------1-----It is a reflective film. Figure 1 Figure 2

Claims (1)

【特許請求の範囲】 1、基板と、反射層と、記録層とを有するレーザ記録媒
体において、前記記録層が有機色素分子の、J−会合体
の累積膜であり且つレーザの発振波長域に吸収帯を有す
るものであることを特徴とするレーザ記録媒体。 2、基板と、反射層と、記録層とが、この記載の順序で
積層されている特許請求の範囲第1項記載のレーザ記録
媒体。 3、基板と、記録層と、反則層とが、この記載の順序で
積層されている特許請求の範囲第1項記載のレーザ記録
媒体。 4、基板と、反射層と、記録層とを有し、前記記録層が
有機色素分子のJ−会合体の累積膜であり且つレーザの
発振波長域に吸収帯を有するレーザ記録媒体の製造方法
において、前記J−会合体の累積膜をラングミュア・ブ
ロジェット法により形成することを特徴とするレーザ記
録媒体 の製造方法。 5、基板と、反射層と、記録層とが、この記載の順序で
積層される特許請求の範囲第4項記載の方法。 6、基板と、記録層と、反射層とが、この記載の順序で
積層される特許請求の範囲第4項記載の方法。
[Scope of Claims] 1. A laser recording medium having a substrate, a reflective layer, and a recording layer, wherein the recording layer is a cumulative film of J-aggregates of organic dye molecules, and is in the oscillation wavelength range of the laser. A laser recording medium characterized by having an absorption band. 2. The laser recording medium according to claim 1, wherein the substrate, the reflective layer, and the recording layer are laminated in the stated order. 3. The laser recording medium according to claim 1, wherein the substrate, the recording layer, and the anti-fouling layer are laminated in the stated order. 4. A method for manufacturing a laser recording medium having a substrate, a reflective layer, and a recording layer, the recording layer being a cumulative film of J-aggregates of organic dye molecules, and having an absorption band in the laser oscillation wavelength range. A method for manufacturing a laser recording medium, characterized in that the cumulative film of J-aggregates is formed by a Langmuir-Blodgett method. 5. The method according to claim 4, wherein the substrate, the reflective layer, and the recording layer are laminated in the stated order. 6. The method according to claim 4, wherein the substrate, recording layer, and reflective layer are laminated in the stated order.
JP59149040A 1984-07-18 1984-07-18 Laser recording medium and production thereof Granted JPS6127291A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59149040A JPS6127291A (en) 1984-07-18 1984-07-18 Laser recording medium and production thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59149040A JPS6127291A (en) 1984-07-18 1984-07-18 Laser recording medium and production thereof

Publications (2)

Publication Number Publication Date
JPS6127291A true JPS6127291A (en) 1986-02-06
JPH0558913B2 JPH0558913B2 (en) 1993-08-27

Family

ID=15466334

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59149040A Granted JPS6127291A (en) 1984-07-18 1984-07-18 Laser recording medium and production thereof

Country Status (1)

Country Link
JP (1) JPS6127291A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63129339A (en) * 1986-11-20 1988-06-01 Teijin Ltd Optical recording medium and optical recording and reproducing method
EP0321923A2 (en) * 1987-12-21 1989-06-28 EASTMAN KODAK COMPANY (a New Jersey corporation) Infrared absorbing cyanine dyes for dye-donor element used in laser-induced thermal dye transfer
JPH0289683A (en) * 1988-09-27 1990-03-29 Fuji Photo Film Co Ltd Information recording medium and recording method using the same

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63129339A (en) * 1986-11-20 1988-06-01 Teijin Ltd Optical recording medium and optical recording and reproducing method
JPH0451819B2 (en) * 1986-11-20 1992-08-20 Teijin Ltd
EP0321923A2 (en) * 1987-12-21 1989-06-28 EASTMAN KODAK COMPANY (a New Jersey corporation) Infrared absorbing cyanine dyes for dye-donor element used in laser-induced thermal dye transfer
JPH0289683A (en) * 1988-09-27 1990-03-29 Fuji Photo Film Co Ltd Information recording medium and recording method using the same

Also Published As

Publication number Publication date
JPH0558913B2 (en) 1993-08-27

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