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JPH0443572B2 - - Google Patents
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JPH0443572B2 - - Google Patents

Info

Publication number
JPH0443572B2
JPH0443572B2 JP61008336A JP833686A JPH0443572B2 JP H0443572 B2 JPH0443572 B2 JP H0443572B2 JP 61008336 A JP61008336 A JP 61008336A JP 833686 A JP833686 A JP 833686A JP H0443572 B2 JPH0443572 B2 JP H0443572B2
Authority
JP
Japan
Prior art keywords
electron
group
optical recording
recording medium
substance
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 - Lifetime
Application number
JP61008336A
Other languages
Japanese (ja)
Other versions
JPS62165647A (en
Inventor
Takashi Yamadera
Toshinori Tagusari
Nobuyuki Hayashi
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.)
Resonac Corp
Original Assignee
Hitachi Chemical 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 Hitachi Chemical Co Ltd filed Critical Hitachi Chemical Co Ltd
Priority to JP61008336A priority Critical patent/JPS62165647A/en
Publication of JPS62165647A publication Critical patent/JPS62165647A/en
Publication of JPH0443572B2 publication Critical patent/JPH0443572B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • 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
    • G11B7/246Record 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
    • 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
    • G11B7/249Record 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 organometallic compounds
    • 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
    • G11B7/249Record 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 organometallic compounds
    • G11B7/2492Record 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 organometallic compounds neutral compounds
    • 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
    • G11B7/249Record 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 organometallic compounds
    • G11B7/2495Record 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 organometallic compounds as anions
    • 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
    • G11B7/249Record 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 organometallic compounds
    • G11B7/2498Record 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 organometallic compounds as cations

Landscapes

  • Chemical & Material Sciences (AREA)
  • Organic Chemistry (AREA)
  • Optical Record Carriers And Manufacture Thereof (AREA)
  • Non-Silver Salt Photosensitive Materials And Non-Silver Salt Photography (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は光記録媒体に関する。[Detailed description of the invention] (Industrial application field) The present invention relates to optical recording media.

(従来の技術) 光記録方式は、安価、大容量の記録媒体が得ら
れるため開発がさかんな分野である。従来この分
野では無機系金属薄膜を記録膜として、半導体レ
ーザの近赤外出力を一度熱に変換し、その熱を利
用して記録膜に穴をあけ、或いは相変化を生じさ
せてこれによる表面反射率の変化を読みとるいわ
ゆるヒートモードの光記録方式が実用化されてき
た。さらに近年有機染料を記録膜とするヒートモ
ード光記録方式が新たに提案されている。しか
し、ヒートモードを用いた光記録方法では、半導
体レーザの出力を熱に変換する際に基板等を通じ
て熱が発散するために感度に限界があり、又、穴
をあける方式に基づくものでは情報の消去が困難
である。これらの観点より、吸収した光を熱とし
て発散することが少なく記録膜の変形をも防ぐ方
法として、吸収した光を光子エネルギーとしてそ
のまま利用し、引きつづき起こる光反応を情報の
記録再生に用いようという、フオトンモードの光
記録方法が提案されており、特に情報の消去が可
能な可逆型光記録材料を得るための手段として精
力的に研究が行われている。これらの目的のため
にフオトクロミツク材料を記録膜材料とする提案
がなされており、例えば特開昭57−59956号公報
には直鎖アルキル基を有するスピロピラン誘導体
が、特開昭60−123838号公報には同様のスピロピ
ラン化合物の化学蒸着膜を記録層とする提案がな
されている。又同様の目的により、ヘラー(A.
Heller)らはジヤーナルオブケミカルソサエテイ
ーパーキンI(J.Chem.Soc Perkin I)、202頁
(1981)においてフルジドと称されるフオトクロ
ミツク化合物の特性とその光記録材料への応用に
つき述べている。これらの化合物の光記録方法に
ついては種々提案されているが、一般的には紫外
光線を全面に照射してスピロピラン類、フルジド
化合物等のフオトクロミツク化合物を強く着色さ
せて初期化を行い、次いで、フオトクロミツク化
合物の変色域にあわせた可視光線照射によつて情
報の記録,読み出しを行つている。これらは一般
に紫外〜可視光線の領域で行われるが、最近、半
導体レーザの発振波長域にマツチングしたスピロ
ピラン類の発表(例えば日本化学会第50春季年会
予稿集I,P259(1985))もなされている。
(Prior Art) Optical recording systems are a field of active development because they allow inexpensive, large-capacity recording media to be obtained. Conventionally, in this field, an inorganic metal thin film is used as a recording film, and the near-infrared output of a semiconductor laser is converted into heat, and the heat is used to make a hole in the recording film or to cause a phase change to change the surface. A so-called heat mode optical recording method that reads changes in reflectance has been put into practical use. Furthermore, in recent years, a new heat mode optical recording method using an organic dye as a recording film has been proposed. However, optical recording methods using heat mode have a limit in sensitivity because heat is dissipated through the substrate etc. when converting the output of a semiconductor laser into heat, and methods based on drilling holes have limitations on the sensitivity. Difficult to erase. From these points of view, as a method to prevent the absorbed light from dissipating as heat and preventing deformation of the recording film, it is possible to use the absorbed light as it is as photon energy and use the subsequent photoreactions to record and reproduce information. A photon mode optical recording method has been proposed and is being actively researched as a means to obtain reversible optical recording materials that can erase information. For these purposes, proposals have been made to use photochromic materials as recording film materials; for example, spiropyran derivatives having a linear alkyl group are disclosed in JP-A-57-59956, and JP-A-60-123,838 discloses spiropyran derivatives having a linear alkyl group. A proposal has been made to use a chemical vapor deposited film of a similar spiropyran compound as the recording layer. For the same purpose, Heller (A.
Heller et al., Journal of Chemical Society Perkin I, p. 202 (1981), describe the properties of a photochromic compound called fulgide and its application to optical recording materials. Various methods for optical recording of these compounds have been proposed, but in general, photochromic compounds such as spiropyrans and fulgide compounds are initialized by irradiating the entire surface with ultraviolet light to strongly color the photochromic compounds, and then photochromic recording is performed. Information is recorded and read out by irradiating visible light that matches the color change area of the compound. These are generally carried out in the ultraviolet to visible light range, but recently there have been publications on spiropyrans that match the oscillation wavelength range of semiconductor lasers (for example, in Proceedings of the 50th Spring Annual Meeting of the Chemical Society of Japan, I, p. 259 (1985)). ing.

(発明が解決しようとする問題点) しかしながら、従来のフオトクロミツク化合物
を光記録材料として用いる際の問題点としてあげ
られるものはこれらフオトクロミツク化合物によ
る情報の読み出し破壊である。これは、フオトク
ロミツク化合物の初期状態および着色状態は共通
ないしは高い確率で交差した励起状態を有してお
り、着色種の吸収に光照射をして情報を記録する
ことと、後に読み出し光による情報の読みとりと
は同値の励起状態に至り、読み出し破壊が避けら
れないことによる。この問題を回避する方法とし
て通常読み出し光の光強度を弱くする方法がとら
れるが、光励起そのものが唯一の反応過程である
ため、しきい値による区別は不可能であり、常に
一定程度の確率で読み出し破壊が起こりうるた
め、情報のくり返し読み出しの際に問題を生じ
る。
(Problems to be Solved by the Invention) However, one of the problems when using conventional photochromic compounds as optical recording materials is that these photochromic compounds destroy information when read. The initial state and colored state of a photochromic compound have a common or crossed excited state with a high probability, and information can be recorded by irradiating the absorption of the colored species with light, and information can later be read out using light. This is due to the fact that the excitation state is the same as that of the readout, and readout destruction is unavoidable. A method to avoid this problem is usually to weaken the light intensity of the readout light, but since optical excitation itself is the only reaction process, it is impossible to differentiate based on the threshold value, and there is always a certain probability that Read corruption can occur, creating problems when repeatedly reading information.

(問題点を解決するための手段) 本発明はこのような問題に鑑みてなされたもの
であり、従来のフオトクロミツク材料と異なり、
読み出し破壊を起こさずに情報の記録再生を行う
ことのできる光記録媒体を提供するものである。
(Means for solving the problems) The present invention was made in view of the above problems, and unlike conventional photochromic materials,
An object of the present invention is to provide an optical recording medium on which information can be recorded and reproduced without causing reading damage.

本発明は、光増感剤、電子供与性物質および電
子受容性物質を含有し、かつ前記電子供与性物質
および前記電子受容性物質の少なくとも一方を混
合原子価状態をとりうる物質としてなる光記録媒
体に関する。
The present invention provides an optical recording medium containing a photosensitizer, an electron-donating substance, and an electron-accepting substance, and at least one of the electron-donating substance and the electron-accepting substance is a substance capable of taking a mixed valence state. Regarding the medium.

本発明になる光記録媒体においては書き込み光
によつて記録を行う分子となる光増感剤と、読み
とり分子となる電子供与性物質および/又は電子
受容性物質並びにそれらが光増感剤の光励起状態
との相互作用によつて、電子供与性物質から電子
受容性物質に電子を移動した反応生成物とは異な
る分子であり、両者の励起状態は区別でき、読み
出し光は書き込み光と完全に区別することがで
き、読み出し破壊は原理的に回避される。これを
図示したのが第1図1である。第1図1では光増
感剤Sが書き込み光により励起型の光増感剤S*
となる。
In the optical recording medium of the present invention, a photosensitizer is used as a molecule that performs recording by writing light, an electron-donating substance and/or an electron-accepting substance that is used as a reading molecule, and the photo-excitation of the photosensitizer by these substances. This is a different molecule from the reaction product in which electrons are transferred from an electron-donating substance to an electron-accepting substance through interaction with the state, and the excited states of the two can be distinguished, and the read light can be completely distinguished from the write light. Therefore, read corruption can be avoided in principle. This is illustrated in FIG. 1. In Figure 1, the photosensitizer S is an excited type photosensitizer S * by the writing light.
becomes.

S*は活性であり、電子受容性物質Aに電子を
受けわたしてそれぞれ酸化型S+
S * is active and transfers electrons to electron-accepting substance A to form oxidized S +

Claims (1)

【特許請求の範囲】 1 光増感剤,電子供与性物質および電子受容性
物質を含有し、かつ前記電子供与性物質および前
記電子受容性物質のうちの少なくとも一方を下記
の一般式(),()または()で示される化
合物の中から選ばれる遷移金属錯体であつて第1
の酸化還元電位が−0.5V〜+0.8V(対飽和カロメ
ル電極)のものとし、前記光増感剤をその基底エ
ネルギー準位での酸化還元電位が前記電子供与性
物質の酸化還元電位より低く、その励起エネルギ
ー準位での酸化還元電位が前記電子受容性物質の
酸化還元電位よりも高いものである光記録媒体。 式()および()において、ZはO,S及
びNR(Rは水素又はアルキル基)から選ばれる
原子又は原子団であり各位置において相違してい
てもよく,X及びX′は水素,アルキル基,置換
アルキル基,ハロゲン,アルコキシ基,アルキル
アミノ基,ニトロ基又はシアノ基から選ばれ、X
及びX′は同一でもよく,nは1〜4の整数,m
は+2〜−2の整数、Aはmによつて規定される
電荷を中和するに必要な電荷数を有するアニオ
ン,カチオン又はその群およびMは遷移金属イオ
ンを表わす(ただし、mが0の場合にはAは存在
しない)。 式()において、Z′はS及びNR(Rは水素
又はアルキル基)から選ばれ各位置において相違
していてもよく、Yは水素,アルキル基,置換ア
ルキル基,フエニル基,置換フエニル基及びシア
ノ基から選ばれ、各位置において相違していても
よく、mは+2〜−2の整数、Aはmによつて規
定される電荷を中和するに必要な電荷数を有する
アニオン,カチオン又はその群およびMは遷移金
属イオンを表わす(ただし、mが0の場合にはA
は存在しない)。 2 電子供与性物質および電子受容性物質が実質
的に分離されている特許請求の範囲第1項記載の
光記録媒体。 3 光記録媒体が電子供与性物質又はこれを含有
する層,光増感剤又はこれを含有する層及び電子
受容性物質又はこれを含有する層をこの順に積層
したものである特許請求の範囲第1項又は第2項
記載の光記録媒体。 4 光記録媒体が、反射層を有する特許請求の範
囲第1項,第2項又は第3項記載の光記録媒体。
[Scope of Claims] 1. Contains a photosensitizer, an electron-donating substance, and an electron-accepting substance, and at least one of the electron-donating substance and the electron-accepting substance is represented by the following general formula (), A transition metal complex selected from the compounds represented by () or (), and the first
has a redox potential of −0.5 V to +0.8 V (vs. saturated calomel electrode), and the redox potential of the photosensitizer at its base energy level is lower than the redox potential of the electron donating substance. , an optical recording medium whose redox potential at its excitation energy level is higher than the redox potential of the electron-accepting substance. In formulas () and (), Z is an atom or atomic group selected from O, S and NR (R is hydrogen or an alkyl group), and may be different at each position, and X and X' are hydrogen, alkyl group, substituted alkyl group, halogen, alkoxy group, alkylamino group, nitro group or cyano group,
and X′ may be the same, n is an integer from 1 to 4, m
is an integer from +2 to -2, A is an anion, cation, or a group thereof having the number of charges required to neutralize the charge specified by m, and M is a transition metal ion (provided that when m is 0, A does not exist in that case). In formula (), Z' is selected from S and NR (R is hydrogen or an alkyl group) and may be different at each position, and Y is hydrogen, an alkyl group, a substituted alkyl group, a phenyl group, a substituted phenyl group, and selected from cyano groups, which may be different at each position, where m is an integer from +2 to -2, and A is an anion, cation, or The group and M represent transition metal ions (provided that when m is 0, A
does not exist). 2. The optical recording medium according to claim 1, wherein the electron-donating substance and the electron-accepting substance are substantially separated. 3. Claims No. 3 in which the optical recording medium has an electron-donating substance or a layer containing the same, a photosensitizer or a layer containing the same, and an electron-accepting substance or a layer containing the same, laminated in this order. The optical recording medium according to item 1 or 2. 4. The optical recording medium according to claim 1, 2 or 3, wherein the optical recording medium has a reflective layer.
JP61008336A 1986-01-18 1986-01-18 Optical recording medium Granted JPS62165647A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61008336A JPS62165647A (en) 1986-01-18 1986-01-18 Optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61008336A JPS62165647A (en) 1986-01-18 1986-01-18 Optical recording medium

Publications (2)

Publication Number Publication Date
JPS62165647A JPS62165647A (en) 1987-07-22
JPH0443572B2 true JPH0443572B2 (en) 1992-07-17

Family

ID=11690350

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61008336A Granted JPS62165647A (en) 1986-01-18 1986-01-18 Optical recording medium

Country Status (1)

Country Link
JP (1) JPS62165647A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02275944A (en) * 1988-09-22 1990-11-09 Agency Of Ind Science & Technol Optical recording material
JP2715600B2 (en) * 1989-11-30 1998-02-18 日立化成工業株式会社 Optical function element
JP2715601B2 (en) * 1989-11-30 1998-02-18 日立化成工業株式会社 How to convert light intensity changes into electrical signals

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5872929A (en) * 1981-10-28 1983-05-02 Toshiba Corp Optical conversion element
JPS6083029A (en) * 1983-10-13 1985-05-11 Mitsui Toatsu Chem Inc Optical recording medium

Also Published As

Publication number Publication date
JPS62165647A (en) 1987-07-22

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