JPS60209940A - Optical recording medium - Google Patents

Optical recording medium

Info

Publication number
JPS60209940A
JPS60209940A JP59064213A JP6421384A JPS60209940A JP S60209940 A JPS60209940 A JP S60209940A JP 59064213 A JP59064213 A JP 59064213A JP 6421384 A JP6421384 A JP 6421384A JP S60209940 A JPS60209940 A JP S60209940A
Authority
JP
Japan
Prior art keywords
layer
recording medium
recording
refractive index
light
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
JP59064213A
Other languages
Japanese (ja)
Other versions
JPH0544739B2 (en
Inventor
Nobutoshi Asai
伸利 浅井
Shinichiro Tamura
眞一郎 田村
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 JP59064213A priority Critical patent/JPS60209940A/en
Publication of JPS60209940A publication Critical patent/JPS60209940A/en
Publication of JPH0544739B2 publication Critical patent/JPH0544739B2/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
    • 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
    • G11B7/252Record 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
    • G11B7/258Record 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 reflective layers
    • 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
    • G11B7/252Record 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
    • G11B7/253Record 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
    • G11B7/2531Record 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 glass

Landscapes

  • Optical Record Carriers And Manufacture Thereof (AREA)
  • Manufacturing Optical Record Carriers (AREA)

Abstract

PURPOSE:To improve the percentage modulation of recording sensitivity and recording signal by constituting a recording medium in such a way that the light absorptive layer thereof exists between the conventional reflecting layer and a noval layer having increased reflectivity. CONSTITUTION:A recording medium 1 has a substrate 2 made of glass having 0.2mm. thickness and 1.5 refractive index. The 1st reflecting layer 3 consisting of a ZnS film deposited by evaporation to have 860Angstrom thickness and 2.3 refractive index is provided as a coating layer having increased reflectivity on one surface of the substrate 2. A light absorptive layer 4 as a recording layer is provided on the exposed surface of the layer 3. The layer 4 is formed by mixing a spiropyrane compd. exhibiting a high absorption characteristic at a >=700nm wavelength region, i.e., 5'-methoxy-1'-n-hexyl-3',3'-dimethyl-6-nitro-8-methoxy spiropyrane and a vinyl chloride/vinylidene chloride copolymer at 1:2 by weight, dissolving the mixture in a solvent and forming the layer by spinner coating. The 2nd reflecting layer 5 consisting of an Ag layer deposited by evaporation to have 1,000Angstrom reflectivity and 0.85-15.35 refractive index is provided as a light reflecting layer on the exposed surface of the layer 4.

Description

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

背景技術とその問題点 透明な基板と光吸収層と光反射層′とからなる光学式記
録媒体iこおいて、記録感度および記録信号の変調度を
改善するために干渉効果を利用する方法は、光吸収層が
Teなどの金属薄膜である場合、あるいは光磁気記録媒
体においてよく研究されている(例えば、A、E、Be
l 1 、 F、W、Spong、 IEEE、J 。
BACKGROUND ART AND PROBLEMS There is a method of utilizing interference effects to improve the recording sensitivity and the degree of modulation of recording signals in an optical recording medium consisting of a transparent substrate, a light absorption layer, and a light reflection layer. , where the light absorption layer is a metal thin film such as Te, or which has been well studied in magneto-optical recording media (for example, A, E, Be
l1, F, W, Spong, IEEE, J.

Quantum Filectronics 14.p
、497)。
Quantum Filectronics 14. p
, 497).

光吸収層が光吸収性有機材料あるいは光吸収物質を分散
させた高分子結合剤を用いて形成されている場合、光吸
収層は一般に屈折率が1.5に近く、°また吸光度も比
較的小さいため、記録感度を向上させるためには層の厚
さをレーザ光の波長程度に厚くする必要かある。この場
合、光吸収層が空気に面するように構成された光記録媒
体では、光吸収層の2つの界面から反射される光の位相
を打ち消し合うように光吸収層の厚さを調整すれば、こ
の層での吸光率が向上し、反射率が低下して、記録感度
が改善される(例えば、K、Y、Law ; Appl
When the light-absorbing layer is formed using a light-absorbing organic material or a polymeric binder in which a light-absorbing substance is dispersed, the light-absorbing layer generally has a refractive index close to 1.5 and a relatively low absorbance. Since it is small, it is necessary to increase the thickness of the layer to the same extent as the wavelength of the laser beam in order to improve recording sensitivity. In this case, in an optical recording medium configured such that the light absorption layer faces the air, the thickness of the light absorption layer may be adjusted so that the phases of the light reflected from the two interfaces of the light absorption layer cancel each other out. , the absorbance in this layer increases, the reflectance decreases, and the recording sensitivity improves (for example, K, Y, Law; Appl
.

Phys、Let t 、 3(i Ql p、994
;D、G、Howe and J 、J 、Wrobe
l 。
Phys, Let t, 3(i Ql p, 994
; D, G, Howe and J, Wrobe
l.

J、Vac、8ci、Technol、18(1)p、
92) 。しかし、光吸収層(記録面)を保譲するため
に保繰層を設けたり、あるいは基板を通して記録再生を
行う場合、屈折率か1.5に近い光吸収層は、屈折率が
やはり1.5程度の基板または保護層に面するために、
界面での反射はほとんど起こらず、干渉効果が得られな
い。なお、基板または保護層に接する光吸収層の界面に
金属コーティング層を設ければ、強G1干渉効果は得ら
れるが、金属自身の光吸収が大きいため好ましくない。
J, Vac, 8ci, Technol, 18(1)p,
92). However, when a storage layer is provided to preserve the light absorption layer (recording surface), or when recording and reproduction are performed through a substrate, a light absorption layer with a refractive index close to 1.5 will still have a refractive index of 1.5. To face the substrate or protective layer of 5 degrees,
Almost no reflection occurs at the interface, and no interference effect is obtained. Note that if a metal coating layer is provided at the interface of the light absorption layer in contact with the substrate or the protective layer, a strong G1 interference effect can be obtained, but this is not preferable because the metal itself has a large light absorption.

発明の目的 本発明は、前記の点に鑑み、強い干渉効果が得られ、記
録感度および記録信号の変調度が改善された光学式記録
媒体を提供するものである。
OBJECTS OF THE INVENTION In view of the above points, the present invention provides an optical recording medium that provides a strong interference effect and has improved recording sensitivity and modulation degree of recorded signals.

発明の概要 本発明の光学式記録媒体は、透明基板と、第1反射層と
、光吸収層と、第2反射層とが積層されてなり、前記光
吸収層は第1反射層と第2反射層との間にあり、前記第
1反射層は光入射側にあって前記透明基板および前記光
吸収層の各屈折率より大きい屈折率を有する材料を用い
て厚さか”、(1+2m)(ここで、λはレーザ光の波
長、n nは第1反射層の屈折率、mは0または正の整数を表わ
す)であるように形成されている。
Summary of the Invention The optical recording medium of the present invention is formed by laminating a transparent substrate, a first reflective layer, a light absorption layer, and a second reflective layer, and the light absorption layer includes a first reflective layer and a second reflective layer. The first reflective layer is located between the transparent substrate and the light absorption layer, and is made of a material having a refractive index larger than the refractive index of the transparent substrate and the light absorption layer, and has a thickness of about 1.5 m (1+2 m). Here, λ is the wavelength of the laser beam, n is the refractive index of the first reflective layer, and m is 0 or a positive integer).

このように構成された本発明の光学式記録媒体において
は、第1反射層と光吸収層との界面における光の反射率
が増大しかつ強い干渉効果が得られ、記録感度と記録信
号の変調度が太き(改善される。
In the optical recording medium of the present invention configured in this way, the light reflectance at the interface between the first reflective layer and the light absorption layer increases and a strong interference effect is obtained, which improves the recording sensitivity and the modulation of the recording signal. The degree is thicker (improved).

実施例 以下、本発明の光学式記録媒体の実施例につき図面を参
照しながら説明する”。
EXAMPLES Hereinafter, examples of the optical recording medium of the present invention will be explained with reference to the drawings.

第1図は本実施例による記録媒体1の構造を示す断面図
である。記録媒体1は、ガラスを材料として作られた厚
さ0.2 rom 、屈折率1.5の基板2を有する。
FIG. 1 is a sectional view showing the structure of a recording medium 1 according to this embodiment. The recording medium 1 has a substrate 2 made of glass with a thickness of 0.2 rom and a refractive index of 1.5.

基板2の片面には反射率強化コーティング層として、厚
ざs 60 X%屈折率2.3のZnS蒸着膜の第1反
射層3が設けられている。第1反射層3の露出面上には
記録層としての光吸収層4か設けられている。この光吸
収層4は、7000m以上の波長域に高い吸収特性を示
す次式のスピロピラン化合物、即ち5′−メトキシ−1
′−n−へキシル−3’、 3 ’−レジメチル−6−
二トロ−8−メトキシスピロ(2H−1−ベンゾチオビ
ラン−2,2′−インドリン〕と塩化ビニル−塩化ビニ
リデン共重合体(電気化学工業社製デンカビニル$10
00W)とを重量比1:2で混合し、溶剤(テトラヒド
ロフラン:シクロへキサノン=1:1)に溶解させてス
ピンナ塗布により形成させた層であり、厚さ0.7μm
および屈折率1.5である。光吸収層4は紫外線照射に
より発色し、波長780〜8000mの半導体レーザ光
を吸収して記録を行い、可視光照射あるいは加熱により
消色する。
On one side of the substrate 2, a first reflective layer 3 of a ZnS vapor-deposited film having a thickness s 60 X% and a refractive index of 2.3 is provided as a reflectance-enhancing coating layer. A light absorption layer 4 as a recording layer is provided on the exposed surface of the first reflective layer 3. This light absorption layer 4 is made of a spiropyran compound of the following formula, which exhibits high absorption characteristics in a wavelength range of 7000 m or more, that is, 5'-methoxy-1
'-n-hexyl-3', 3'-redimethyl-6-
Nitro-8-methoxyspiro (2H-1-benzothiobilane-2,2'-indoline) and vinyl chloride-vinylidene chloride copolymer (Denkabinyl $10, manufactured by Denki Kagaku Kogyo Co., Ltd.)
00W) at a weight ratio of 1:2, dissolved in a solvent (tetrahydrofuran: cyclohexanone = 1:1), and formed by spinner coating, with a thickness of 0.7 μm.
and a refractive index of 1.5. The light absorption layer 4 develops a color when irradiated with ultraviolet rays, performs recording by absorbing semiconductor laser light with a wavelength of 780 to 8000 m, and is decolored by irradiation with visible light or heating.

光吸収層4の露出面上には光反射層として、厚き1oo
oX、屈折率0.085〜i5.35のAg蒸着層の第
2反射層5が設けられている。
A 10mm thick layer is formed on the exposed surface of the light absorption layer 4 as a light reflection layer.
A second reflective layer 5 is provided, which is an Ag vapor deposited layer with oX and a refractive index of 0.085 to i5.35.

このように構成された記録媒体1の緒特性を測定するた
め、基板2側から紫外線を照射して光吸収層4を発色さ
せた。このためには、soow超高圧水銀灯(ウシオ電
気社製)を用い、東芝製フ付近の紫外線を選択的に照射
した。照度は約15mW/c〆である。次に、この発色
した光吸収層4に基板2側から半導体レーザ光を照射し
た。
In order to measure the characteristics of the recording medium 1 constructed as described above, ultraviolet rays were irradiated from the substrate 2 side to cause the light absorption layer 4 to develop color. For this purpose, a SOOW ultra-high-pressure mercury lamp (manufactured by Ushio Electric Co., Ltd.) was used to selectively irradiate ultraviolet rays in the vicinity of Toshiba's fu. The illumination intensity is about 15 mW/c〆. Next, this colored light absorption layer 4 was irradiated with semiconductor laser light from the substrate 2 side.

比較例として、第1図の記録媒体1における第1反射層
3が設けられていないこと以外は前記記録媒体1と同じ
様に構成された記録媒体6(第2図)についても、前記
と同様に紫外線および半導体レーザ光の照射を行った。
As a comparative example, a recording medium 6 (FIG. 2) having the same structure as the recording medium 1 of FIG. 1 except that the first reflective layer 3 is not provided is also used. was irradiated with ultraviolet light and semiconductor laser light.

各記録媒体の特性として次の結果を得た。The following results were obtained regarding the characteristics of each recording medium.

1、紫外線照射時間に対する半導体レーザ光の反射率変
化(第3図および第4図) 紫外線の照射時間を0.5,15.60秒と変化させて
、光吸収層4でのスピロビラ発色iこ伴うレレーザ光の
各波長における反射率の変化を測定し、第3図に本実施
例の記録媒体11こよる結果を実線で、比較例の記録媒
体6による結果を点線で示した。
1. Change in reflectance of semiconductor laser light with respect to ultraviolet irradiation time (Figs. 3 and 4) The spirovir color development in the light absorption layer 4 was observed by changing the ultraviolet irradiation time to 0.5 and 15.60 seconds. Changes in reflectance at each wavelength of the accompanying laser light were measured, and in FIG. 3, the results for the recording medium 11 of this example are shown by a solid line, and the results for the recording medium 6 of the comparative example are shown by a dotted line.

第3図から明らかなように、記録媒体1は記録媒体6に
比べて、少ない紫外線照射量で波長780〜800nm
付近の反射率が低下し、牛導体レーザ光がより吸収され
易くなっていることがわかる。
As is clear from FIG. 3, compared to recording medium 6, recording medium 1 requires less ultraviolet irradiation and has a wavelength of 780 to 800 nm.
It can be seen that the reflectance in the vicinity has decreased and the cow conductor laser beam is more easily absorbed.

逆に、配置媒体1は600〜yoonm付近で反射率の
低下が少なく、この波長範囲の光が吸収されにくくなっ
ている。
On the other hand, the placement medium 1 exhibits little decrease in reflectance in the vicinity of 600-yoonm, making it difficult for light in this wavelength range to be absorbed.

才た、@3図における波長7801mでの反射率変化を
、紫外線照射時間に対してプロットして第4図に示した
。第4図からも本実施例の記録媒体1が比較例の記録媒
体6に比べて少ない紫外線照射量で反射率の低下が大き
いことが明らかである。
The change in reflectance at a wavelength of 7801 m in Figure 3 is plotted against the ultraviolet irradiation time and shown in Figure 4. It is also clear from FIG. 4 that the reflectance of the recording medium 1 of this example is significantly reduced by a smaller amount of ultraviolet irradiation than the recording medium 6 of the comparative example.

2、記録感度(第5図) 記録媒体1および6の各試料に前記と同様の紫外線を 
照射して光吸収層4を 発色させ、次いで半導体レーザ光を照射し、この照射(
記録)前後の反射率変化を測定した。
2. Recording sensitivity (Figure 5) Each sample of recording media 1 and 6 was exposed to the same ultraviolet rays as above.
The light absorption layer 4 is colored by irradiation, and then the semiconductor laser light is irradiated, and this irradiation (
Recording) Changes in reflectance before and after were measured.

記録条件二レーザ光の波長=780nmレーザパワー=
9mW(試料上) レーザビーム直径=1.2μm(牛値@う、パルス幅=
0.1〜7μs 得られた結果を第5図に示す。
Recording conditions 2 Laser light wavelength = 780 nm Laser power =
9mW (on sample) Laser beam diameter = 1.2μm (value @, pulse width =
0.1 to 7 μs The results obtained are shown in FIG.

第5図から明らかなように、本実施例の記録媒体1は比
較例の記録媒体6に比べて、小さなエネルギーで大きな
反射率変化が得られ、例えば反射率変化20%を得るた
めのエネルギー密度は第1表に示す通り、比較例の場合
の約1/2になっている。なお。
As is clear from FIG. 5, compared to the recording medium 6 of the comparative example, the recording medium 1 of this example can obtain a large change in reflectance with a small amount of energy; for example, the energy density required to obtain a change in reflectance of 20% is As shown in Table 1, it is about 1/2 of that of the comparative example. In addition.

この結果は各試料について、光吸収層4の発色条件をい
ろいろに変えて測定したうちの最良の場合を比較したも
ので、第1表にそのときの紫外線照射量と記録前の反射
率が示しである。
These results are a comparison of the best case measurements of each sample under various coloring conditions of the light absorption layer 4. Table 1 shows the amount of ultraviolet irradiation and the reflectance before recording. It is.

本実施例の記録媒体1による記録感度の向上は、第1反
射N3と光吸収層4との界面での反射率を高めたことに
より、光吸収層4と第2反射層5の界面からの光と強い
干渉を起こし、入射したレーザ光か光吸収層4に一層集
中し、反射する光量が減少するためであると考えられる
The recording sensitivity of the recording medium 1 of this embodiment is improved by increasing the reflectance at the interface between the first reflection layer N3 and the light absorption layer 4. This is thought to be because strong interference occurs with the light, and the incident laser light is further concentrated on the light absorption layer 4, reducing the amount of reflected light.

本実施例において、ざらに、基板2の厚さを変えた以外
は記録媒体1および6の各種構成を有する光ディスクを
次のように作製し、キャリアの記録、再生特性を測定し
た。
In this example, optical disks having various configurations of the recording media 1 and 6 except that the thickness of the substrate 2 was changed were fabricated as follows, and the recording and reproducing characteristics of the carriers were measured.

光ディスクの形状: 直径8 cm +ガラス製基板厚さ= 1.3 mm 
;プリグループなし。
Shape of optical disc: diameter 8 cm + glass substrate thickness = 1.3 mm
;No pregroup.

記録条件=(紫外#(360nm)照射量: 1.QJ
/cm )基板側からレーザ光照射;レーザ光の波長=
78Qnm;レーザパワー=53mW(試料上);レン
ズNA=0.5;キャリア周波数1fvl)iz;デユ
ーティ比50%の方形波使用;記録線速度=2.6m/
S;記録波長=2.6μm;トラックピッ千=約5μm
0 こうして記録された各党ディスクから、家庭用コンパク
トディスクプレーヤを利用した再生装置により得られた
再生信号(ディスク1周分)のエンベロープは第6図(
実施例の光ディスク;曲線−L L l −ys二! 
’l j+ L V16th)ETA / II M 
all M m rノスク;曲線Cとdとで示す)の通
りであった。これらの図において、縦軸の0.5V単位
は反射率で20%に相当する。本実施例の構成を有する
光ディスクのエンベロープは比較例の光ディスクのエン
ベロープに比べて信号振幅か約2倍であり、キャリアレ
ベルが6dB向上していることがわかる。
Recording conditions = (ultraviolet # (360 nm) irradiation amount: 1.QJ
/cm) Laser light irradiation from the substrate side; wavelength of laser light =
78Qnm; Laser power = 53mW (on sample); Lens NA = 0.5; Carrier frequency 1fvl)iz; Use of square wave with duty ratio of 50%; Recording linear velocity = 2.6m/
S; recording wavelength = 2.6 μm; track pitch = approximately 5 μm
0 The envelope of the playback signal (for one round of the disk) obtained from each party's disk recorded in this way by a playback device using a home compact disk player is shown in Figure 6 (
Optical disc of Example; Curve-L L l -ys2!
'l j+ L V16th) ETA/II M
all M m r nosk; shown by curves C and d). In these figures, a unit of 0.5V on the vertical axis corresponds to 20% in reflectance. It can be seen that the envelope of the optical disc having the configuration of this example has a signal amplitude approximately twice that of the envelope of the optical disc of the comparative example, and the carrier level has improved by 6 dB.

第1反射層は、屈折率が通常のガラス、間分子樹脂など
の屈折率と大きく具なる方が効果的であり、また透明で
あることが好ましく、前記実施例におけるZn8 (7
)他に、TiO2、Zr(J2、Y2O3などλ に、膜厚−5(1+ 2 m ’)の高屈折率層と低屈
折率層とを交互に重ねた多層構造であってもよい。なお
前記mの値は特に制限はないが、実用上θ〜3の整数で
あるのが好ましい。
It is more effective for the first reflective layer to have a refractive index higher than that of ordinary glass, interlayer resin, etc., and is preferably transparent.
) In addition, a multilayer structure in which high refractive index layers and low refractive index layers with a film thickness of -5 (1+2 m') are alternately stacked on λ such as TiO2, Zr (J2, Y2O3, etc.) may also be used. The value of m is not particularly limited, but is preferably an integer between θ and 3 for practical purposes.

第2反射層は、不発明において屈折率が1.5に近い材
料で効果が高く、スピロピラン化合物の他に各種の色素
、金属微粒子などを高分仔結合剤に分散させて得た材料
を使用することができる。
The second reflective layer is a highly effective material with a refractive index close to 1.5, and uses a material obtained by dispersing various pigments, metal particles, etc. in a polymeric binder in addition to spiropyran compounds. can do.

基板は第1反射層に面しているか、あるいは第2反射層
に面しているか、いずれでもよい。
The substrate may face either the first reflective layer or the second reflective layer.

発明の効果 光学式記録媒体において、光吸収層が従来の反射層と本
発明における新規な反射率強化層との開基こ存在するよ
うに構成することにより、光吸収層における記録感度の
向上した光学式記録媒体を得ることができる。また、光
吸収層がスピロピラン系フォトクロミック化合物を材料
として形成されている場合、記録に先立って必要な発色
のための紫外線の量を減少させることができ、光吸収層
が長寿命化し、書き換え回数が増加した光学式記録媒体
を得ることができる。さらに、記録媒体の吸光度変化だ
けでなく、屈折率変化や体積変化記録再生方式において
も反射率を大きく変化させることができる。また、レー
ザ光の波長以外の波長の光に対しては、光吸収層の吸光
率が低くなるので、光化学的変化に基づく記録媒体では
記録の保存性を向上させることができる。
Effects of the Invention In an optical recording medium, by configuring the light absorption layer to be a combination of the conventional reflection layer and the novel reflectance-enhancing layer of the present invention, an optical recording medium with improved recording sensitivity in the light absorption layer can be obtained. A type recording medium can be obtained. Additionally, if the light absorption layer is made of a spiropyran-based photochromic compound, the amount of ultraviolet rays required for color development prior to recording can be reduced, extending the lifespan of the light absorption layer and reducing the number of rewrites. Increased optical recording media can be obtained. Furthermore, the reflectance can be greatly changed not only by changing the absorbance of the recording medium but also by changing the refractive index or by changing the volume of the recording/reproducing method. Further, since the absorbance of the light absorption layer is low for light having a wavelength other than the wavelength of laser light, the storage stability of recording can be improved in a recording medium based on photochemical change.

【図面の簡単な説明】 第1図は本発明の一実施例の光学式記録媒体の構成、第
2図は比較例の光学式記録媒体の構成、執3図〜第5図
はレーザ光の反射率変化、第6図は本発明の一実施例の
光ディスクによる再生信号のエンベロープおよび第7図
は比較例の光ディスクによる再生信号のエンベロープを
示す。 なお図面に用いられた符号において、 1・・・・・・・・・・・・記録媒体 2・・・・・・・・・・・・基板 3・・・・・・・・・・・・第1反射層4・・・・・・
・・・・・・光吸収層 5・・・・・・・・・・・・第2反射層6・・・・・・
・・・・・・記録媒体 である。 代理人 土星 勝 I 常包芳男
[Brief Description of the Drawings] Figure 1 shows the configuration of an optical recording medium according to an embodiment of the present invention, Figure 2 shows the configuration of an optical recording medium according to a comparative example, and Figures 3 to 5 show the configuration of an optical recording medium according to an example of the present invention. FIG. 6 shows the envelope of the reproduced signal from the optical disc according to the embodiment of the present invention, and FIG. 7 shows the envelope of the reproduced signal from the optical disc according to the comparative example. In addition, in the symbols used in the drawings: 1... Recording medium 2... Substrate 3...・First reflective layer 4...
......Light absorption layer 5......Second reflective layer 6...
...It is a recording medium. Agent: Masaru Saturn Yoshio Tsunekami

Claims (1)

【特許請求の範囲】 透明基板と、第1反射層き、光吸収層と、第2反射層と
が積層されてなり、前記光吸収層は第1反射層と第2反
射層との間にあり、前記第1反射層は光入射側にあって
、前記透明基板お、よび前記光吸収・層の各屈折率より
大きい屈折率を有する材λ 料を用いて厚さが 4.(1+2m)(ここで、λはレ
ーザ光の波長、nは第1反射層の屈折率、mは0〜また
は正の整数を表わず)であるように形成されてなること
を特徴とする光学式記録媒体。
[Claims] A transparent substrate, a first reflective layer, a light absorbing layer, and a second reflective layer are laminated, and the light absorbing layer is provided between the first reflective layer and the second reflective layer. 4. The first reflective layer is on the light incident side and is made of a material having a refractive index larger than the refractive index of the transparent substrate and the light absorbing layer. (1+2m) (where λ is the wavelength of the laser beam, n is the refractive index of the first reflective layer, and m is not 0 or more or a positive integer). Optical recording medium.
JP59064213A 1984-03-31 1984-03-31 Optical recording medium Granted JPS60209940A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59064213A JPS60209940A (en) 1984-03-31 1984-03-31 Optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59064213A JPS60209940A (en) 1984-03-31 1984-03-31 Optical recording medium

Publications (2)

Publication Number Publication Date
JPS60209940A true JPS60209940A (en) 1985-10-22
JPH0544739B2 JPH0544739B2 (en) 1993-07-07

Family

ID=13251579

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59064213A Granted JPS60209940A (en) 1984-03-31 1984-03-31 Optical recording medium

Country Status (1)

Country Link
JP (1) JPS60209940A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0458604A2 (en) * 1990-05-22 1991-11-27 Canon Kabushiki Kaisha Method and apparatus for recording and reproducing information in cells using multiple interference
JPH08315422A (en) * 1995-05-15 1996-11-29 Nec Corp Optical information medium

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5437740A (en) * 1977-08-29 1979-03-20 Rca Corp Laser beam recording media
JPS5778649A (en) * 1980-10-30 1982-05-17 Teijin Ltd Laminated material for optical memory
JPS586541A (en) * 1981-07-02 1983-01-14 Sharp Corp Magnetooptic storage element
JPS598150A (en) * 1982-07-02 1984-01-17 Sharp Corp Magnetooptical storage element
JPH0226299A (en) * 1988-07-15 1990-01-29 Matsushita Electric Works Ltd Stepping motor

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5437740A (en) * 1977-08-29 1979-03-20 Rca Corp Laser beam recording media
JPS5778649A (en) * 1980-10-30 1982-05-17 Teijin Ltd Laminated material for optical memory
JPS586541A (en) * 1981-07-02 1983-01-14 Sharp Corp Magnetooptic storage element
JPS598150A (en) * 1982-07-02 1984-01-17 Sharp Corp Magnetooptical storage element
JPH0226299A (en) * 1988-07-15 1990-01-29 Matsushita Electric Works Ltd Stepping motor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0458604A2 (en) * 1990-05-22 1991-11-27 Canon Kabushiki Kaisha Method and apparatus for recording and reproducing information in cells using multiple interference
JPH08315422A (en) * 1995-05-15 1996-11-29 Nec Corp Optical information medium

Also Published As

Publication number Publication date
JPH0544739B2 (en) 1993-07-07

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