JPH0241288A - Optical recording medium and optical recording method - Google Patents
Optical recording medium and optical recording methodInfo
- Publication number
- JPH0241288A JPH0241288A JP63192532A JP19253288A JPH0241288A JP H0241288 A JPH0241288 A JP H0241288A JP 63192532 A JP63192532 A JP 63192532A JP 19253288 A JP19253288 A JP 19253288A JP H0241288 A JPH0241288 A JP H0241288A
- Authority
- JP
- Japan
- Prior art keywords
- recording
- layer
- wavelength
- light
- recording layer
- 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
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 27
- 238000000034 method Methods 0.000 title claims description 13
- 238000010521 absorption reaction Methods 0.000 claims abstract description 28
- 230000003595 spectral effect Effects 0.000 claims abstract description 12
- 238000002835 absorbance Methods 0.000 claims description 4
- 238000002310 reflectometry Methods 0.000 abstract 5
- 230000009102 absorption Effects 0.000 abstract 2
- 239000010410 layer Substances 0.000 description 46
- 239000000975 dye Substances 0.000 description 13
- 239000000463 material Substances 0.000 description 7
- 239000000758 substrate Substances 0.000 description 5
- 150000001875 compounds Chemical class 0.000 description 4
- 238000000576 coating method Methods 0.000 description 3
- 239000011521 glass Substances 0.000 description 3
- 238000004528 spin coating Methods 0.000 description 3
- 239000012780 transparent material Substances 0.000 description 3
- HEDRZPFGACZZDS-UHFFFAOYSA-N Chloroform Chemical compound ClC(Cl)Cl HEDRZPFGACZZDS-UHFFFAOYSA-N 0.000 description 2
- 239000004372 Polyvinyl alcohol Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 229920002451 polyvinyl alcohol Polymers 0.000 description 2
- 239000011241 protective layer Substances 0.000 description 2
- 239000000243 solution Substances 0.000 description 2
- 238000003860 storage Methods 0.000 description 2
- LFQSCWFLJHTTHZ-UHFFFAOYSA-N Ethanol Chemical compound CCO LFQSCWFLJHTTHZ-UHFFFAOYSA-N 0.000 description 1
- 229930192627 Naphthoquinone Natural products 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- 239000007864 aqueous solution Substances 0.000 description 1
- 125000000751 azo group Chemical group [*]N=N[*] 0.000 description 1
- 230000008033 biological extinction Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- OEYIOHPDSNJKLS-UHFFFAOYSA-N choline Chemical compound C[N+](C)(C)CCO OEYIOHPDSNJKLS-UHFFFAOYSA-N 0.000 description 1
- 229960001231 choline Drugs 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000003618 dip coating Methods 0.000 description 1
- CZZYITDELCSZES-UHFFFAOYSA-N diphenylmethane Chemical compound C=1C=CC=CC=1CC1=CC=CC=C1 CZZYITDELCSZES-UHFFFAOYSA-N 0.000 description 1
- 230000031700 light absorption Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 125000001434 methanylylidene group Chemical group [H]C#[*] 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- LKKPNUDVOYAOBB-UHFFFAOYSA-N naphthalocyanine Chemical compound N1C(N=C2C3=CC4=CC=CC=C4C=C3C(N=C3C4=CC5=CC=CC=C5C=C4C(=N4)N3)=N2)=C(C=C2C(C=CC=C2)=C2)C2=C1N=C1C2=CC3=CC=CC=C3C=C2C4=N1 LKKPNUDVOYAOBB-UHFFFAOYSA-N 0.000 description 1
- 150000002791 naphthoquinones Chemical class 0.000 description 1
- 239000011368 organic material Substances 0.000 description 1
- 229920000620 organic polymer Polymers 0.000 description 1
- 238000007699 photoisomerization reaction Methods 0.000 description 1
- 239000001007 phthalocyanine dye Substances 0.000 description 1
- 239000002861 polymer material Substances 0.000 description 1
- 239000001008 quinone-imine dye Substances 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- ANRHNWWPFJCPAZ-UHFFFAOYSA-M thionine Chemical compound [Cl-].C1=CC(N)=CC2=[S+]C3=CC(N)=CC=C3N=C21 ANRHNWWPFJCPAZ-UHFFFAOYSA-M 0.000 description 1
- AAAQKTZKLRYKHR-UHFFFAOYSA-N triphenylmethane Chemical compound C1=CC=CC=C1C(C=1C=CC=CC=1)C1=CC=CC=C1 AAAQKTZKLRYKHR-UHFFFAOYSA-N 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
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
- G11B7/004—Recording, reproducing or erasing methods; Read, write or erase circuits therefor
- G11B7/0045—Recording
- G11B7/00455—Recording involving reflectivity, absorption or colour changes
-
- 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
- G11B7/2403—Layers; Shape, structure or physical properties thereof
- G11B7/24035—Recording layers
- G11B7/24038—Multiple laminated recording layers
-
- 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
- G11B2007/24618—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 two or more dyes in two or more different layers, e.g. one dye absorbing at 405 nm in layer one and a different dye absorbing at 650 nm in layer two
Abstract
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及び光記録方法に関する。[Detailed description of the invention] Industrial applications The present invention relates to an optical recording medium and an optical recording method.
従来の技術
光記録媒体は大容量でありビット当りのコストが安いと
いう特徴のゆえに、外部記憶媒体として発展が期待され
ている。しかしながら、今日実用化されている光記録媒
体はいずれも二次元記録であるため、記録密度は記録に
用いるレーザーの波長で限界があり、ld当り108ビ
ツトが上限とされている。この記録密度でも文書情報の
ファイリングのような用途には充分な記憶容量が得られ
るが、画像特に動画を記憶する場合には、決して充分な
記録密度とは言えず、このためさらに高密度の記録媒体
がこれらの目的のために必要とされいる。高密度化の一
つの方法は多層化であり、積層膜を用いた多層記録が提
案されている。(特開昭58−209594号公報)ま
た、フォトケミカルホールバーニングも提案されている
。2. Description of the Related Art Optical recording media are expected to develop as external storage media because of their large capacity and low cost per bit. However, since all optical recording media put into practical use today are two-dimensional recording, the recording density is limited by the wavelength of the laser used for recording, and the upper limit is 108 bits per ld. Although this recording density provides sufficient storage capacity for applications such as filing document information, it is by no means sufficient for storing images, especially moving images, and for this reason even higher-density recording is required. A medium is required for these purposes. One method for increasing density is multilayering, and multilayer recording using laminated films has been proposed. (Japanese Unexamined Patent Publication No. 58-209594) Photochemical hole burning has also been proposed.
発明が解決しようとする課題
上記した多重記録の方法ではいずれも、再生時にも記録
に用いたと同じ波長の光が必要とされるため、再生の装
置でも複数の光源を用意しなけれはならい、複数の光源
を用いた再生装置は大変複雑な光学系が必要とされるた
め非常に高価な装置になってしまう0本発明は、民生用
に、安価な再生装置で再生できる高密度光ディスクを提
供しようとするものである。Problems to be Solved by the Invention In all of the above-mentioned multiplex recording methods, light of the same wavelength as that used for recording is required during playback, so the playback device must also prepare multiple light sources. A playback device using such a light source requires a very complicated optical system, resulting in a very expensive device.The present invention provides a high-density optical disc for consumer use that can be played with an inexpensive playback device. That is.
課題を解決するための手段
本発明は、画像の記録のように大容量の情報を高密度記
録出来、しかも単一の波長の光源での再生を可能ならし
めるというものであり、そのために本発明の光記録方式
は、記録層の各層が互いに異なった波長で分光吸収極大
値を示し、各層が吸収極大を示す波長では他の記録層の
吸収率が充分に低い値となる多層構造の光記録媒体を用
いて、吸収極大を示す波長の近傍の特定波長の記録光で
一つの記録層の反射率のみを変化せしめ、前記記録層の
吸収極大を示す波長以外の波長をもち、かつその波長で
は各記録層が互いに異なった開存の反射率を示す光を再
生光として用い、各記録層毎の反射率変化を識別して検
出することを特徴とする。Means for Solving the Problems The present invention is capable of recording a large amount of information at high density, such as recording an image, and also enables reproduction using a light source of a single wavelength. The optical recording method uses a multilayer structure in which each layer of the recording layer exhibits a maximum spectral absorption value at a different wavelength, and at the wavelength at which each layer exhibits maximum absorption, the absorption rate of other recording layers is sufficiently low. Using a medium, only the reflectance of one recording layer is changed by recording light of a specific wavelength near the wavelength showing the absorption maximum, and the reflectance of the recording layer has a wavelength other than the wavelength showing the absorption maximum, and at that wavelength. The present invention is characterized in that light in which each recording layer exhibits a different open reflectance is used as reproduction light, and changes in reflectance for each recording layer are identified and detected.
作用
このように本発明の光記録媒体を用いた光記録方式にお
いては、単位面積当りの記録密度が従来よりも著しく高
くできるため、大容量が必要とされる長時間の動画でも
比較的小面積に格納できる。As described above, in the optical recording method using the optical recording medium of the present invention, the recording density per unit area can be significantly higher than conventional methods, so even long videos that require a large capacity can be recorded in a relatively small area. can be stored in
また、記録材料として300nmから900nmの間で
は単一の吸収極大波長を有する有機色素を選択して用い
ることができるため、製造コストの安い湿式塗布法が使
える。加えて、再生用には単一の光源を用いることがで
きるため、再生機の低価格化にも有利である。Further, since an organic dye having a single absorption maximum wavelength between 300 nm and 900 nm can be selected and used as a recording material, a wet coating method with low manufacturing cost can be used. In addition, since a single light source can be used for reproduction, it is advantageous for reducing the cost of the reproduction machine.
実施例 以下に本発明の一実施例を図面を用いて説明する。Example An embodiment of the present invention will be described below with reference to the drawings.
第1図には一例として三層系光記録媒体の模式図を示し
た。すなわち、基体上に三層の記録層A、B、Cが形成
されており、各記録層は第2図に示すように各々λ1.
λ2.λ3に吸収極大値を持つ、第2図から明らかなよ
うに記録NAの吸収極大を示す波長λ、においては記録
層B、Cの吸収率は十分に小さな値であり波長λ1の光
では記録層Aのみが変化する。同様に、λ2の光では記
録層Bのみが変化し、λ8の光では記録1cのみが変化
する9次に再生方法について説明する。FIG. 1 shows a schematic diagram of a three-layer optical recording medium as an example. That is, three recording layers A, B, and C are formed on the substrate, and each recording layer has a wavelength of λ1.
λ2. As is clear from FIG. 2, the absorption coefficients of the recording layers B and C are sufficiently small at the wavelength λ, which has an absorption maximum value at λ3, which indicates the absorption maximum value of the recording NA, and the absorption coefficients of the recording layers B and C are sufficiently small for light of the wavelength λ1. Only A changes. Similarly, a ninth-order reproduction method will be described in which only the recording layer B changes with the light of λ2, and only the recording layer 1c changes with the light of λ8.
第3図に示すように、積層化した状態での各記録層A、
B、Cの、未記録状態での再生光の波長での反射率が各
々R,,R2,R3であり、全反射率が(R1+R2+
R,)であるとする、記録層Aが記録によってΔR8変
化するとすれば記録後の全反射率は((R,+R2+R
,)−R,lとなる。同様に、記録層B、Cは各々記録
後にΔR2゜ΔR8変化するとして、ΔR8≠ΔR2≠
ΔR3とすれば記録後の全反射率は記録層A、 B、
Cの記録状態によりへ種類の異なった値をとることにな
り、各記録層の記録状態を一種類の光で検出できること
になる。ここで本発明の光記録媒体の各構成要素毎に必
要な性質を述べる。記録層を形成する材料としては光を
吸収して一定量の反射率変化を生じる性質があればよく
、変化の形態としてはヒートモードでもフォントモード
でも構わない。As shown in FIG. 3, each recording layer A in a laminated state,
The reflectances of B and C at the wavelength of the reproduction light in an unrecorded state are R, , R2, and R3, respectively, and the total reflectance is (R1+R2+
R,), and if the recording layer A changes by ΔR8 due to recording, the total reflectance after recording is ((R, +R2+R
, )-R,l. Similarly, assuming that recording layers B and C change by ΔR2°ΔR8 after recording, ΔR8≠ΔR2≠
If ΔR3 is assumed, the total reflectance after recording is recording layer A, B,
Since C takes different values depending on the recording state of C, the recording state of each recording layer can be detected with one type of light. Here, properties required for each component of the optical recording medium of the present invention will be described. The material forming the recording layer need only have the property of absorbing light and causing a certain amount of change in reflectance, and the form of change may be either heat mode or font mode.
但し、記録による変化で光の透過を妨げる様な材料は適
切でない、すなわち、光を吸収して酸化分解し脱色して
もよいし、光の吸収に伴う発熱により分解し気泡を形成
してもよいし、また熱により発色したり結晶相が変化す
るものでもよく、光異性化してもよい、多くの場合には
記録時に発熱を伴うため、第4図に示したように隣接す
る記録層11と12との間には透明な断熱層13を設け
ることが好ましい、また、記録1i14のうえから直接
、保護層15を形成してもよいし、よく知られているよ
うないわゆるエアーギャップ方式の保護形態としてもよ
い。光記録材料は、300nmから900nmの波長領
域において分光吸収曲線に単一の吸収極大値をもち、か
つその吸収極大波長で一定量の反射率を有するものであ
ればよい。好ましくは、吸収極大波長でのモル吸光係数
が1×104以上の色素が記録感度および反射率特性の
点から望ましい、記録層自体はこの様な色素単体からな
っていてもよいし透明材料との組成物の形態としても良
い、これらの観点から、具体的な色素としては、シアニ
ン色素、スクワリリウム色素。However, materials that change due to recording and impede the transmission of light are not suitable; in other words, they may absorb light and oxidize and decompose and decolorize, or they may decompose and form bubbles due to the heat generated due to light absorption. It may also be one that develops color or changes its crystalline phase when heated, or may undergo photoisomerization.In many cases, heat is generated during recording, so as shown in FIG. 4, the adjacent recording layer 11 It is preferable to provide a transparent heat insulating layer 13 between the recording layer 1i14 and the recording layer 12. Also, the protective layer 15 may be formed directly on the recording layer 1i14, or a well-known so-called air gap method may be used. It may also be used as a form of protection. The optical recording material may be any material as long as it has a single absorption maximum value in its spectral absorption curve in the wavelength range from 300 nm to 900 nm, and has a certain amount of reflectance at the absorption maximum wavelength. Preferably, a dye having a molar extinction coefficient of 1 x 104 or more at the absorption maximum wavelength is desirable from the viewpoint of recording sensitivity and reflectance characteristics.The recording layer itself may be composed of such a dye alone or may be composed of a transparent material. From these viewpoints, specific dyes that may be used in the form of a composition include cyanine dyes and squalirium dyes.
メチン系色素、ナフトキノン系色素、キノンイミン系色
素、ジフェニルメタン系色素、トリフェニルメタン系色
素、フタロシアニン系色素、ナフタロシアニン系色素、
スピロピラン系化合物、フルギド系化合物、アゾ化合物
、コリン系色素などが使用できる。これらを分散する場
合には、透明材料としては、用いる色素との適合性と溶
解性とによって選択すればよい、また、各記録層間に断
熱層を設ける場合は、既に塗布されている記録層に悪影
響を与えない限り、有機材料であろうと無機系透明材料
であろうと基本的には構わないが、断熱層形成時の記録
材料への影響を考えると、透明な有機高分子材料が好ま
しい。その形成法としては回転塗布、浸漬塗布、ウェッ
ブコーティングなどに加えて、プラズマ重合膜も用いる
ことができる。記録層についても前記の湿式塗布性以外
に蒸着によっても形成できる。Methine dyes, naphthoquinone dyes, quinoneimine dyes, diphenylmethane dyes, triphenylmethane dyes, phthalocyanine dyes, naphthalocyanine dyes,
Spiropyran compounds, fulgide compounds, azo compounds, choline dyes, etc. can be used. When dispersing these materials, the transparent material may be selected depending on its compatibility with the dye used and its solubility.Also, when providing a heat insulating layer between each recording layer, Basically, it does not matter whether it is an organic material or an inorganic transparent material as long as it does not have any adverse effects, but in consideration of the influence on the recording material when forming the heat insulating layer, a transparent organic polymer material is preferable. In addition to spin coating, dip coating, web coating, etc., a plasma polymerized film can also be used as a forming method. The recording layer can also be formed by vapor deposition in addition to the above-mentioned wet coating method.
以下、具体例によってさらに詳細な説明を行なう。A more detailed explanation will be given below using specific examples.
具体例
第4図に示すように、5C1lX5C11のガラス基板
ll上に化合物(1)のクロロホルム溶液を回転塗布に
より形成し、厚さ60nmの第1の記録層12を形成し
た。この上にポリビニルアルコールの水溶液を同じく回
転塗布して200nm厚の透明層13を形成した。さら
にその上から、ビクトリアブルーのアルコール溶液によ
り50nmの第2の記録層14を形成した。最後にもう
一度ポリビニルアルコールを300nm形成して保護層
15とした。各記録層毎の分光吸収曲線は第5図に示す
様に、一方の記録層の吸収極大波長では他方の吸収が非
常に小さい値を持つ、また、未記録状態での各層毎の分
光反射率は第6図に示すが、記録jW12.14の吸収
が少ない830nmでも充分な反射率を有している。第
4図のように完成した光記録媒体において再生光として
830nmのレーザー光を用いると、未記録状態では全
体の反射率は22%であった。出力30mWで波長78
0nmのレーザーを、ガラス基板11をとうして化合物
(1)からなる第1の記録層12上に直径3μmのスポ
ットに集光したところ反射率は10%となった。すなわ
ち、反射率の変化量は12%であった。つぎに、別の位
置に30mWで波長633nmのHe −N eレーザ
ーを同じようにガラス基板11を通してビクトリアブル
ーからなる第2の記録層14上に直径3μmのスポット
に集光したところ反射率は15%となった。すなわち、
反射率の変化量は7%となった0次に、あらかじめ63
3 nmで記録した同一の位置に780nmの光ぞ照射
したところ反射率は8%まで低下した。一方、予め、7
80nmで記録後に633nmで書き加えたところ反射
率はやはり8%となった0以上に示したように、二層の
記録膜をもつ本具体例に於ては、記録の状態によって反
射率は、三種類の異なった変化量を示すためどの層に記
録されているかを容易に識別して検出することが出来た
。Specific Example As shown in FIG. 4, a chloroform solution of compound (1) was formed on a 5C11×5C11 glass substrate 11 by spin coating to form a first recording layer 12 with a thickness of 60 nm. A transparent layer 13 having a thickness of 200 nm was formed by spin coating an aqueous solution of polyvinyl alcohol thereon. Furthermore, a 50 nm second recording layer 14 was formed thereon using a Victoria Blue alcohol solution. Finally, polyvinyl alcohol was formed once again to a thickness of 300 nm to form a protective layer 15. As shown in Figure 5, the spectral absorption curve for each recording layer shows that at the absorption maximum wavelength of one recording layer, the absorption of the other layer is extremely small, and that the spectral reflectance of each layer in the unrecorded state is As shown in FIG. 6, recording jW12.14 has sufficient reflectance even at 830 nm, where absorption is low. When a laser beam of 830 nm was used as the reproduction light in the completed optical recording medium as shown in FIG. 4, the overall reflectance was 22% in the unrecorded state. Wavelength 78 with output 30mW
When a 0 nm laser was focused onto a spot with a diameter of 3 μm on the first recording layer 12 made of compound (1) through the glass substrate 11, the reflectance was 10%. That is, the amount of change in reflectance was 12%. Next, when a He-Ne laser with a wavelength of 633 nm and a power of 30 mW was focused on a spot with a diameter of 3 μm on the second recording layer 14 made of Victoria Blue through the glass substrate 11 at another position, the reflectance was 15. %. That is,
The amount of change in reflectance is 7% at the 0th order, and 63% in advance.
When the same position recorded at 3 nm was irradiated with 780 nm light, the reflectance decreased to 8%. On the other hand, in advance, 7
When additional writing was performed at 633 nm after recording at 80 nm, the reflectance was still 8%. As shown above, in this specific example with a two-layer recording film, the reflectance varies depending on the recording state. Because it showed three different amounts of change, it was possible to easily identify and detect which layer it was recorded in.
発明の効果
以上の実施例で説明したように、本発明の光記録媒体お
よび光記録方法は同一の位置に多重記録することができ
、しかも単一の再生光で検出できると言う優れた特徴を
持っている。Effects of the Invention As explained in the above embodiments, the optical recording medium and optical recording method of the present invention have the excellent feature that multiple recording can be performed at the same position and detection can be performed with a single reproduction beam. have.
第1図は本発明の光記録媒体の構造を模式的に説明する
断面図、第2図は本発明の光記録方式を説明するための
分光吸光度曲線を示すグラフ、第3図は本発明の光記録
方式を説明する分光反射率曲線を示すグラフ、第4図は
本発明の具体例となる二層多重光記録媒体の断面構造図
、第5図は具体例の分光吸光度曲線を示すグラフ、第6
図は具l・・・・・・記録層A、
2・・・・・・記録層B、
3・・・・・・記録
層C1
4・・・・・・基板。FIG. 1 is a cross-sectional view schematically explaining the structure of the optical recording medium of the present invention, FIG. 2 is a graph showing a spectral absorbance curve for explaining the optical recording method of the present invention, and FIG. 3 is a graph showing the spectral absorbance curve of the present invention. A graph showing a spectral reflectance curve to explain the optical recording method, FIG. 4 is a cross-sectional structural diagram of a two-layer multilayer optical recording medium that is a specific example of the present invention, and FIG. 5 is a graph showing a spectral absorbance curve of a specific example. 6th
The figure shows the following: 1...Recording layer A, 2...Recording layer B, 3...Recording layer C1 4...Substrate.
Claims (3)
層が積層された多層構造の光記録媒体で、一つの記録層
の吸収極大を示す波長では他の層分光吸度が充分に低く
、かつ各記録層がいずれも充分低い吸収率を示す波長域
に属する特定の波長の光に対して、記録による変化後も
前記の光を透過する性質を保持し、かつ各記録層が記録
の前後で互いに異なった固有の反射率変化量を示すこと
を特徴とする光記録媒体。(1) An optical recording medium with a multilayer structure in which recording layers having spectral absorption maximum values at different wavelengths are laminated, and at the wavelength where one recording layer shows the absorption maximum value, the spectral absorption of other layers is sufficiently low. In addition, each recording layer maintains the property of transmitting light of a specific wavelength belonging to a wavelength range showing a sufficiently low absorption rate even after changes due to recording, and An optical recording medium characterized in that it exhibits unique amounts of change in reflectance that are different from each other.
項(1)記載の光記録媒体。(2) The optical recording medium according to claim (1), wherein each recording layer is separated by a transparent layer.
大値を示し、各層が吸収極大値を示す波長では他の記録
層の吸光度が充分に低い値となる多層構造の光記録媒体
で、吸収極大値を示す波長の近傍の特定波長の記録光で
一つの記録層のみを変化せしめ、前記記録層の吸収極大
を示す波長以外の波長をもち、かつその波長では各記録
層の記録前後での反射率変化が互いに異なった固有の反
射率変化量を示す光を再生光として用い、各記録層毎の
反射率変化を識別して検出することを特徴とする光記録
方法。(3) An optical recording medium with a multilayer structure in which each layer of the recording layer exhibits a spectral absorption maximum value at a different wavelength, and the absorbance of other recording layers is sufficiently low at the wavelength at which each layer exhibits the absorption maximum value, Only one recording layer is changed by recording light of a specific wavelength near the wavelength showing the maximum absorption value, and the recording layer has a wavelength other than the wavelength showing the maximum absorption value, and at that wavelength, each recording layer is changed before and after recording. 1. An optical recording method characterized in that the reflectance changes of each recording layer are identified and detected by using, as reproduction light, light that exhibits unique reflectance change amounts that are different from each other.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63192532A JPH07114027B2 (en) | 1988-08-01 | 1988-08-01 | Optical recording medium and optical recording method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63192532A JPH07114027B2 (en) | 1988-08-01 | 1988-08-01 | Optical recording medium and optical recording method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0241288A true JPH0241288A (en) | 1990-02-09 |
JPH07114027B2 JPH07114027B2 (en) | 1995-12-06 |
Family
ID=16292846
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63192532A Expired - Lifetime JPH07114027B2 (en) | 1988-08-01 | 1988-08-01 | Optical recording medium and optical recording method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH07114027B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2006085515A1 (en) * | 2005-02-09 | 2006-08-17 | Kyoto University | Reflectance control optical device |
-
1988
- 1988-08-01 JP JP63192532A patent/JPH07114027B2/en not_active Expired - Lifetime
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2006085515A1 (en) * | 2005-02-09 | 2006-08-17 | Kyoto University | Reflectance control optical device |
JPWO2006085515A1 (en) * | 2005-02-09 | 2008-08-07 | 国立大学法人京都大学 | Reflectance control optical element and ultrathin film light absorption enhancing element |
JP4565197B2 (en) * | 2005-02-09 | 2010-10-20 | 国立大学法人京都大学 | Reflectance control optical element and ultrathin film light absorption enhancing element |
Also Published As
Publication number | Publication date |
---|---|
JPH07114027B2 (en) | 1995-12-06 |
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