JPS60257291A - Optical information recording member - Google Patents

Optical information recording member

Info

Publication number
JPS60257291A
JPS60257291A JP59113301A JP11330184A JPS60257291A JP S60257291 A JPS60257291 A JP S60257291A JP 59113301 A JP59113301 A JP 59113301A JP 11330184 A JP11330184 A JP 11330184A JP S60257291 A JPS60257291 A JP S60257291A
Authority
JP
Japan
Prior art keywords
germanium oxide
layer
recording
light
oxide 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
Application number
JP59113301A
Other languages
Japanese (ja)
Other versions
JPH0545434B2 (en
Inventor
Noboru Yamada
昇 山田
Kenichi Nishiuchi
健一 西内
Yoshito Ninomiya
二宮 義人
Masatoshi Takao
高尾 正敏
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP59113301A priority Critical patent/JPS60257291A/en
Publication of JPS60257291A publication Critical patent/JPS60257291A/en
Publication of JPH0545434B2 publication Critical patent/JPH0545434B2/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
    • G11B7/252Record 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
    • 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
    • G11B7/243Record 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 inorganic materials only, e.g. ablative layers
    • G11B7/2433Metals or elements of groups 13, 14, 15 or 16 of the Periodic System, e.g. B, Si, Ge, As, Sb, Bi, Se or Te
    • 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
    • G11B7/243Record 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 inorganic materials only, e.g. ablative layers
    • G11B2007/24302Metals or metalloids
    • G11B2007/24312Metals or metalloids group 14 elements (e.g. Si, Ge, Sn)
    • 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
    • G11B7/243Record 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 inorganic materials only, e.g. ablative layers
    • G11B2007/24302Metals or metalloids
    • G11B2007/24314Metals or metalloids group 15 elements (e.g. Sb, Bi)
    • 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
    • G11B7/243Record 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 inorganic materials only, e.g. ablative layers
    • G11B2007/24302Metals or metalloids
    • G11B2007/24316Metals or metalloids group 16 elements (i.e. chalcogenides, Se, Te)
    • 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
    • G11B7/243Record 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 inorganic materials only, e.g. ablative layers
    • G11B2007/24318Non-metallic elements
    • G11B2007/2432Oxygen

Abstract

PURPOSE:To contrive enhancement of recording sensitivity, erasing sensitivity or the like and durability in repeated use, by a method wherein a germanium oxide layer is provided on a base, and a recording layer capable of being heated by irradiating with light with the result of a change in an optical constant thereof is provided thereon. CONSTITUTION:The layer 2 of germanium oxide GeOx (x=2) is provided on the base 1 by vapor deposition, sputtering or other similar method. In this case, germanium oxide may have the composition of GeOx (xapprox.=2), depending on the condition. The recording layer 3 the optical constant of which is changed upon irradiation with light is provided on the layer 2. Accordingly, the intensity of reflected light reaches a minium, is then increased to a maximum, is reduced to a minimum, is increased to a maximum, and such increase and decrease are repeated to converge to a fixed value. In this case, all of the maxima, minima and the limit can be made to be small. Accordingly, by providing the germanium oxide layer 2 between the base 1 and the recording layer 3, it is possible to enhance the efficiency of incidence of light, and to enhance the overall recording sensitivity.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、レーザ光線等を用いて光学的に高密度な情報
を高速に記録、再生する光学情報記録部材特に光ディス
クに関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an optical information recording member, particularly an optical disk, which optically records and reproduces high-density information at high speed using a laser beam or the like.

従来例の構成とその問題点 レーザ光線を用いて、回転しているディスク上に高密度
な情報を高速に記録、再生する技術は、光デイスク装置
として既に幾つもの研究成果例、商品開発例の報告が有
シ、情報システムを構成するうえで不可欠のものとなり
2つある。
Conventional configurations and their problems The technology of recording and reproducing high-density information on a rotating disk at high speed using a laser beam has already been used in many research results and product development examples as an optical disk device. There are two types of reports that are essential to constructing an information system.

これら光ディスクに用いる記録材料としては、穴や泡等
の形状変化を生じさせることで光の反射率変化、透過率
変化を得るものと、光年的性質(屈折率n、消衰係数k
)を変えて反射率変化。
The recording materials used for these optical discs include those that change the reflectance and transmittance of light by creating shapes such as holes and bubbles, and those that change the reflectance and transmittance of light (refractive index n, extinction coefficient k).
) to change the reflectance.

透過率変化を得るものがあるが・後者のタイプのものが
、密着した保護層を設けられる点、原理的に変化が可逆
的で書き換え可能なものが得られるという点で有利であ
り、光ディスクの主流になると考えられる。
Although there are devices that change the transmittance, the latter type is advantageous in that it can be provided with a protective layer that adheres tightly, and that changes are reversible in principle and rewritable. It is thought that it will become mainstream.

このタイプの光ディスクとして代表的なものに、[Te
0x(0(X<2):] を用いたものがある◇これは
PMMA等の樹脂基材上に、紫外線硬化樹脂を用いて光
ガイド用のトランク溝を形成し、その上に〔TeOx・
〕薄膜を蒸着等の方法で設置し、更に基材と同様の樹脂
基材をはり合わせた構造をしている。この光ディスクは
既に静止画ファイル。
A typical optical disc of this type is [Te
0x (0 (X < 2):] ◇This method involves forming a trunk groove for light guide using ultraviolet curing resin on a resin base material such as PMMA, and then forming a trunk groove for light guide on the resin base material such as PMMA.
] It has a structure in which a thin film is installed by a method such as vapor deposition, and then a resin base material similar to the base material is glued together. This optical disc already contains still image files.

文書・ファイル等のシステム機器へ応用されているが、
この〔Te0X〕を主材料として用い今後例えば、大型
化、書き換え可能化等、更に発展させた形態にするため
には幾つかの問題が残されている。
It is applied to system equipment such as documents and files, but
Several problems remain if this [Te0X] is to be used as the main material in a more advanced form, such as larger size and rewritability.

つまり現状のままの構造では、くシ返し使用することに
よって基材と記録層の界面付近で基材がダメージを受け
やすく記録信号の品質が低下してしまう点、更に容量を
上げるためにディスク形状を大きくする、あるいは転送
レートを上げるために回転速度を上げるというような試
みに対しては、現状の半導体レーザーの出力では記録感
度が不足する心配がある点、等の理由から何らかの対策
を必要とする。
In other words, with the current structure, the base material is easily damaged near the interface between the base material and the recording layer due to the use of combs, and the quality of the recorded signal deteriorates. Attempts to increase the rotation speed in order to increase the transfer rate or to increase the transfer rate require some kind of countermeasure, as there is a concern that the recording sensitivity may be insufficient with the current output of semiconductor lasers. do.

発明の目的 本発明は光ディスクの構造を改良して、記録感度、消去
感度等を向上するとともに繰り返し使用してもダメージ
を受けにくい光ディスクを提供することを目的とする。
OBJECTS OF THE INVENTION An object of the present invention is to improve the structure of an optical disc to improve recording sensitivity, erasing sensitivity, etc., and to provide an optical disc that is less susceptible to damage even after repeated use.

発明の構成 本発明による光学情報記録部材は、基材上に酸化ゲルマ
ニウム層を設け、その上に光照射によって加熱昇温し、
その光学定数を変化する性質を有する性質を有する記録
層番積層したことを特徴とする。
Structure of the Invention The optical information recording member according to the present invention provides a germanium oxide layer on a base material, heats the layer on the germanium oxide layer by irradiating it with light,
It is characterized in that a recording layer number having a property of changing its optical constant is laminated.

酸化ゲルマニウム層は、レーザ光の入射効率を高めて見
かけ上の記録感度を高めるとともに、基材に対する防護
層として作用し、くり返し使用による基材の損傷を防止
する。
The germanium oxide layer increases the incidence efficiency of laser light and increases the apparent recording sensitivity, and also acts as a protective layer for the base material to prevent damage to the base material due to repeated use.

実施例の説明′ 以下図面を参照しつつ本発明の詳細な説明する。Description of Examples' The present invention will be described in detail below with reference to the drawings.

第1図は、本発明の光学情報記録部材の基本的構成の断
面図を示したものである。図中1は、基材であって、P
MMA 、塩化ビニール、ポリカーボネイト等のプラス
チック、又はガラス等を使用目的に応じて用いることが
できる。2は本発明の根幹をなす酸化ゲルマニウムGe
0x(x−2又はx = 2 )の層であって蒸着、ス
パッタリング等の方法を用いて形成する。膜形成に際し
ては蒸着用ソース材料あるいはスパッタリングのターゲ
ノ)It’llとして二酸化ゲルマニウムGe○2を用
いる。蒸着あるいはスパッタリングの条件によってはや
や○がはずれてGe0x(xユ2)となる場合があるが
本発明においては、はぼ同様の効果を得ることが可能で
ある。
FIG. 1 shows a sectional view of the basic structure of the optical information recording member of the present invention. 1 in the figure is a base material, P
Plastics such as MMA, vinyl chloride, polycarbonate, glass, etc. can be used depending on the purpose of use. 2 is germanium oxide Ge, which forms the basis of the present invention.
It is a layer of 0x (x-2 or x = 2) and is formed using a method such as vapor deposition or sputtering. When forming the film, germanium dioxide Ge2 is used as a source material for vapor deposition or as a target material for sputtering. Depending on the conditions of vapor deposition or sputtering, the circle may deviate slightly and become Ge0x (xyu2), but in the present invention, it is possible to obtain the same effect.

膜厚としては、基材1側から光を入射した時の反射光量
が干渉効果として極大値を示す時の膜厚に設定すること
ができる。設定方法としては、例えば特開昭59−17
139に提案されている反射率測定方法を用いて行なう
ことができる一ヶ第2図は、前述の方法を用いて酸化ゲ
ルマニウム薄膜を堆積していった時の膜厚と基材側から
の反射率との関係を示したものである。反射光強度は、
基材表面からの反射光と、基材と酸化ゲルマニウム層の
界面からの反射光との間の多重干渉の結果、図のように
膜厚の増加に従って増大し、極大値をとった後、減少す
ることがわかった。酸化ゲルマニウムのように透明で光
がほとんど吸収されない物質の場合には、極大値をとる
場合の膜厚dと屈折率n、波長λの間には、nd−λ/
4のような近似式が成立し、酸化ゲルマニウム薄膜の屈
折率n=1.6.光源の波長λ=840nmとすると、
反射光強度が極大をとる膜厚d。は、約130nmとな
る。
The film thickness can be set to a film thickness at which the amount of reflected light when light is incident from the base material 1 side shows a maximum value as an interference effect. As a setting method, for example, JP-A-59-17
Figure 2 shows the film thickness and reflection from the substrate side when a germanium oxide thin film was deposited using the method described above. This shows the relationship with the rate. The reflected light intensity is
As a result of multiple interference between the reflected light from the substrate surface and the reflected light from the interface between the substrate and the germanium oxide layer, as shown in the figure, it increases as the film thickness increases, reaches a maximum value, and then decreases. I found out that it does. In the case of a transparent material such as germanium oxide that absorbs almost no light, the relationship between the film thickness d, the refractive index n, and the wavelength λ at its maximum value is nd-λ/
4 is established, and the refractive index of the germanium oxide thin film is n=1.6. Assuming that the wavelength of the light source is λ=840 nm,
Film thickness d at which the reflected light intensity is maximum. is approximately 130 nm.

第1図において3は記録層を示す。上述のように設計し
た酸化ゲルマニウム層2の上に記録層゛3を堆積させる
場合、記録膜3の屈折率が酸化ゲルマニウム2の屈折率
よシも大であれば、記録層3を含めた全体の系として、
基材側1からの反射光強度を、酸化ゲルマニウム層2の
無い場合に比べてはるかに小さくすることが可能であり
光の入射効率を高めることができる。
In FIG. 1, numeral 3 indicates a recording layer. When depositing the recording layer 3 on the germanium oxide layer 2 designed as described above, if the refractive index of the recording film 3 is higher than the refractive index of the germanium oxide 2, the whole including the recording layer 3 will be deposited. As a system of
The intensity of reflected light from the base material side 1 can be made much smaller than in the case without the germanium oxide layer 2, and the light incidence efficiency can be increased.

第3図に、記録層材料としてTe−Tea2系薄膜全薄
膜た場合において、酸化ゲルマニウム層2が有る場合(
、)、と無い場合(b)における反射光強度の相違を示
す。酸化ゲルマニウム層2が無い(b)の場合において
は、反射光強度は膜厚の増加とともに増大し、極大値4
をとった後、減少し、その後、極小5.極大6と増減を
くシ返しながら一定の値に収束する。これに対して酸化
ゲルマニウム層2が有る場合においては反射光強度は小
さい極小値7をとった後、増大し極大8をとb、その後
減少し極4z9.極大1oと増減をくシ返しながら一定
の値に収束する。このとき、酸化ゲルマニウム層2が有
る場合には、各極大値、極小値、又収束値とも無い場合
に比べて全体に低くすることができることがわかった。
Figure 3 shows a case where a Te-Tea2-based thin film is used as the recording layer material and a germanium oxide layer 2 is present (
, ), and (b) without the reflected light intensity are shown. In case (b) without the germanium oxide layer 2, the reflected light intensity increases as the film thickness increases, reaching a maximum value of 4.
After taking , it decreases and then reaches a minimum of 5. It converges to a constant value while repeating increases and decreases to a maximum of 6. On the other hand, in the case where the germanium oxide layer 2 is present, the reflected light intensity takes a small minimum value 7, increases to a maximum value 8, and then decreases to a minimum value 4z9. It converges to a constant value while repeating increases and decreases from a maximum of 1o. At this time, it has been found that when the germanium oxide layer 2 is present, the overall maximum value, minimum value, and convergence value can be made lower than when there is no convergence value.

従って基材1と記録膜3との間に酸化ゲルマニウム層2
を設けることで光の入射効率を高めることが可能となシ
、全体として記録感度の向上が計れるものである。
Therefore, between the base material 1 and the recording film 3, there is a germanium oxide layer 2.
By providing this, it is possible to increase the light incidence efficiency, and it is possible to improve the recording sensitivity as a whole.

酸化ゲルマニウム層2の膜厚としては、前述の近似式で
反射光強度が最大となるように選ぶ場合においそ上述の
反射率低減の効果を最大限得ることができるものである
が、反射光強度が最大でない場合においても類似の効果
を得ることは可能であり、この場合においては記録層3
を含めた光の反射率は、第3図aとbの中間の値をとる
ものである。
The thickness of the germanium oxide layer 2 can be selected to maximize the reflected light intensity using the approximation formula described above, so that the effect of reducing the reflectance described above can be maximized. It is possible to obtain a similar effect even when the
The reflectance of light, including , takes a value between a and b in FIG.

記録層3としては、上記以外にもSb2Te3 。As the recording layer 3, in addition to the above, Sb2Te3 may be used.

、Sb 2 S e 3等、やはり記録前後で光学的特
性を変化するもの、あるいは’f e−C系薄膜、Pb
−To−5e系薄膜等の穴を形成するような材料もその
まま適用が可能である。
, Sb 2 S e 3, etc., which also change optical characteristics before and after recording, 'f e-C thin film, Pb
Materials that form holes, such as -To-5e thin films, can also be applied as they are.

次に、記録層3としてTe−Ge−5n−0系薄膜(特
願昭58−58’158記載)を用いて、くり返し記録
、消去を行った場合の実施例について説明する。この系
の記録薄膜は、その使用方法として膜をあらかじめ反射
率の高い状態にしておき、光を照射して反射率の低い状
態に変化させることで記録しようというものであるから
、記録時の光の入射効率を高めるという意味で、酸化ゲ
ルマニウム層による反射率低減効果は非常に有用である
Next, an example will be described in which a Te-Ge-5n-0 thin film (described in Japanese Patent Application No. 58-58-158) is used as the recording layer 3 and recording and erasing are performed repeatedly. The method of using this type of recording thin film is to record by first setting the film in a high reflectance state and changing it to a low reflectance state by irradiating it with light. The reflectance reduction effect of the germanium oxide layer is very useful in terms of increasing the incidence efficiency of the light.

更にくシ返し使用する際には樹脂基材1が熱的に変形し
、ノイズレベルが増大することが考えられるが、酸化ゲ
ルマニウムという無機材質層を介することでその変形を
押さえることができるものである。特願昭58−581
58記載のT e e o S n 1sG e s 
O2゜薄膜を用いて、酸化ゲルマニウム/i di有る
場合と無い場合との両方の光ディスクを試作し、やはシ
特願昭58−58158記載の記録消去方法を用いてく
シ返し記録消去実験を行なった。
Furthermore, when used repeatedly, the resin base material 1 may be thermally deformed and the noise level may increase, but this deformation can be suppressed by interposing the inorganic material layer of germanium oxide. be. Patent application 58-581
T e o S n 1s G e s described in 58
Using an O2° thin film, optical discs with and without germanium oxide/IDI were prototyped, and repeated recording erasure experiments were conducted using the recording erasing method described in Japanese Patent Application No. 58-58158. Ta.

第4図は酸化ゲルマニウム層を設けて試作した光ディス
クの断面図、第5図は光デイスク作成時の各工程におけ
るディスクの反射率を連続的に示しだものである。
FIG. 4 is a cross-sectional view of an optical disk prototyped with a germanium oxide layer provided thereon, and FIG. 5 is a continuous graph showing the reflectance of the disk at each step during the production of the optical disk.

基材11は1.2叫厚のPMMAを用い、そのうえに酸
化ゲルマニウム層12を反射率が極太となるように蒸着
し、その上にTe6o S、n 1s Ge 5020
薄膜層13を、その反射率が極小となるようにこれも蒸
着して形成する。更に、この場合はくり返し使用時にお
けるゴミ、キズ等の影響を避けるため記録膜の上に更に
もう一層、酸化ゲルマニウム層14を反射率が極小とな
るように蒸着し、紫外線硬化樹脂を爪いて、1.1tr
rIn厚のPMMA基材16をはり合わせて光ディスク
とする。
The base material 11 is made of PMMA with a thickness of 1.2 mm, on which a germanium oxide layer 12 is vapor-deposited so that the reflectance is extremely thick, and on top of that, Te6o S, n 1s Ge 5020 is used.
The thin film layer 13 is also formed by vapor deposition so that its reflectance is minimal. Furthermore, in this case, in order to avoid the influence of dust, scratches, etc. during repeated use, one more germanium oxide layer 14 is vapor-deposited on top of the recording film so that the reflectance is minimal, and an ultraviolet curing resin is applied. 1.1tr
The rIn-thick PMMA base material 16 is glued together to form an optical disc.

第6図は、これらの光ディスクを用いて、記録パワー、
消去パワーをそれぞれ8mW、12mW、消去レーザー
ビーム長を半値巾で15μmとして同一トラック上にく
り返し記録消去を行なった場合のC/Hの変化の様子を
示したものである。記録周波数は5 MHz 、ディス
クの周速は15 ml Bである。このとき、酸化ゲル
マニウム層を備えた光ディスクavcおいては、光の吸
収効率が良いだめに初期C/Nが高く、同時にくシ返し
使用時においてもC/Nの劣化がごく微かでしかなかっ
た。それに比して、酸化ゲルマニウム層の無い光ディス
クbにおいては、aJC/Nがやや低く、くり返し使用
するとノイズレベルの上昇に伴ない、C/Nが低下する
減少が観察された。
Figure 6 shows the recording power,
This figure shows the change in C/H when recording and erasing is repeatedly performed on the same track with the erasing power being 8 mW and 12 mW, respectively, and the erasing laser beam length being 15 μm at half-width. The recording frequency was 5 MHz, and the circumferential speed of the disk was 15 ml B. At this time, the optical disc AVC equipped with a germanium oxide layer had a high initial C/N due to its high light absorption efficiency, and at the same time, there was only a slight deterioration in the C/N even when it was used repeatedly. . In comparison, in optical disc b without a germanium oxide layer, aJC/N was somewhat low, and when used repeatedly, a decrease in C/N was observed as the noise level increased.

発明の効果 本発明によれば、酸化ゲルマニウム層を基材と記録層と
の間に備えることで、反射率が低減化され、全体の系と
して記録感度が高く、しかも基材を保護する効果を伴っ
て、くり返し使用時の耐久性に優れた光学情報記録部材
を提供することができる・
Effects of the Invention According to the present invention, by providing a germanium oxide layer between the base material and the recording layer, the reflectance is reduced, the recording sensitivity is high as a whole system, and the effect of protecting the base material is achieved. Accordingly, it is possible to provide an optical information recording member with excellent durability during repeated use.

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

第1図は、本発明の光学情報記録部材の基本構成の断面
図、第2図は酸化ゲルマニウム層の膜厚と反射率の関係
を示すグラフ、第3図は、酸化ゲルマニウム層が有る場
合と無い場合の記録材料の反射率の差異を示すグラフ、
第4図は書き換え可能な材料を用いて、はり合わせた構
造の本発明の一実施例における光学情報記録部材の断面
図、第5図は、ディスク作成時の各工程におけるディス
クの反射率の連続的な変化を示すグラフ、第6図は、酸
化ゲルマニウム層の有無によるくり返し使用時のC/N
の変化の相違を示すグラフである。 1・・・・・・基材、2・・・・・・酸化ゲルマニウム
層、3・・・・・・記録層。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 第2図 躾 厚 d(ty島 第3図 (Cl) 月叉 4 d(npn) (b) 躾4 d(n川 第4図 第5図 ceら冴 記僧#軒層 6eρ2層 頑 4 n’tn
FIG. 1 is a cross-sectional view of the basic structure of the optical information recording member of the present invention, FIG. 2 is a graph showing the relationship between the thickness of the germanium oxide layer and the reflectance, and FIG. A graph showing the difference in reflectance of recording materials in the absence of
Fig. 4 is a cross-sectional view of an optical information recording member according to an embodiment of the present invention, which has a structure in which rewritable materials are bonded together, and Fig. 5 shows the continuation of the reflectance of the disc at each step during disc production. Figure 6 is a graph showing changes in C/N during repeated use with and without a germanium oxide layer.
It is a graph showing the difference in the change. 1...Base material, 2...Germanium oxide layer, 3...Recording layer. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 Discipline Thickness d (Ty Island Figure 3 (Cl) Moon 4 d (npn) (b) Discipline 4 d (n River Figure 4 Figure 5 CE et al. n'tn

Claims (3)

【特許請求の範囲】[Claims] (1)基材上に酸化ゲルマニウムGemx(x = 2
又はx = 2 )層を設け、その上に光照射によって
昇温し、その光学定数が変化する性質を有する記録層を
積層した光学情報記録部材。
(1) Germanium oxide Gemx (x = 2
or x = 2) layer, and a recording layer having a property of changing its optical constants when heated by light irradiation is laminated thereon.
(2)記録層として、光照射によって昇温させた後、急
冷することでその光学定数が減少し、徐冷することでそ
の光学定数が増大する性質を備えた薄膜を用いることを
特徴とする特許請求の範囲第1項記載の光学情報記録部
材。
(2) The recording layer is characterized by using a thin film whose optical constant decreases when the temperature is raised by light irradiation and then rapidly cools, and whose optical constant increases when slowly cooled. An optical information recording member according to claim 1.
(3)基材側から光を入射させた時その光の波長に応じ
て、その反射率が極大になるように第1の酸化ゲルマニ
ウム層の膜厚を選び、反射率が極小となるように記録層
の膜厚を選んだことを特徴とする特許請求の範囲第1項
記載の光学情報記録部材。
(3) The thickness of the first germanium oxide layer is selected so that when light is incident from the base material side, the reflectance is maximized according to the wavelength of the light, and the reflectance is minimized. The optical information recording member according to claim 1, characterized in that the thickness of the recording layer is selected.
JP59113301A 1984-06-01 1984-06-01 Optical information recording member Granted JPS60257291A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59113301A JPS60257291A (en) 1984-06-01 1984-06-01 Optical information recording member

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59113301A JPS60257291A (en) 1984-06-01 1984-06-01 Optical information recording member

Related Child Applications (1)

Application Number Title Priority Date Filing Date
JP27697390A Division JPH03141054A (en) 1990-10-15 1990-10-15 Production of optical information recording medium

Publications (2)

Publication Number Publication Date
JPS60257291A true JPS60257291A (en) 1985-12-19
JPH0545434B2 JPH0545434B2 (en) 1993-07-09

Family

ID=14608744

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59113301A Granted JPS60257291A (en) 1984-06-01 1984-06-01 Optical information recording member

Country Status (1)

Country Link
JP (1) JPS60257291A (en)

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61287058A (en) * 1985-06-10 1986-12-17 エナ−ジ−・コンバ−シヨン・デバイセス・インコ−ポレ−テツド Optical data memory device and making thereof
JPS62226446A (en) * 1986-03-28 1987-10-05 Toshiba Corp Optical recording medium
US4787077A (en) * 1985-08-15 1988-11-22 International Business Machines Corporation Process for optically storing information using materials having a single phase in both the crystalline state and the amorphous state
JPS63300441A (en) * 1987-05-29 1988-12-07 Nippon Columbia Co Ltd Optical information recording medium
JPH0264936A (en) * 1988-08-30 1990-03-05 Hitachi Ltd Optical information recording medium
JPH03141054A (en) * 1990-10-15 1991-06-17 Matsushita Electric Ind Co Ltd Production of optical information recording medium
US5187052A (en) * 1987-04-08 1993-02-16 Hitachi, Ltd. Optical recording medium
US5268254A (en) * 1989-02-28 1993-12-07 Fuji Xerox Co., Ltd. Optical recording medium
US5273861A (en) * 1987-12-04 1993-12-28 Matsushita Electric Industrial Co., Ltd. Optical information recording medium, method of making an optical information recording medium and method of recording/reproducing optical information
CN100385541C (en) * 2004-04-28 2008-04-30 索尼株式会社 One time write optical recording media
WO2008091018A1 (en) * 2007-01-26 2008-07-31 Sony Corporation Optical recording medium and method for manufacturing the same

Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61287058A (en) * 1985-06-10 1986-12-17 エナ−ジ−・コンバ−シヨン・デバイセス・インコ−ポレ−テツド Optical data memory device and making thereof
US4787077A (en) * 1985-08-15 1988-11-22 International Business Machines Corporation Process for optically storing information using materials having a single phase in both the crystalline state and the amorphous state
JPS62226446A (en) * 1986-03-28 1987-10-05 Toshiba Corp Optical recording medium
US5187052A (en) * 1987-04-08 1993-02-16 Hitachi, Ltd. Optical recording medium
JPS63300441A (en) * 1987-05-29 1988-12-07 Nippon Columbia Co Ltd Optical information recording medium
US5273861A (en) * 1987-12-04 1993-12-28 Matsushita Electric Industrial Co., Ltd. Optical information recording medium, method of making an optical information recording medium and method of recording/reproducing optical information
US5449589A (en) * 1987-12-04 1995-09-12 Matsushita Electric Industrial Co., Ltd. Method of making an optical information recording medium and method of recording/reproducing optical information
JPH0264936A (en) * 1988-08-30 1990-03-05 Hitachi Ltd Optical information recording medium
US5268254A (en) * 1989-02-28 1993-12-07 Fuji Xerox Co., Ltd. Optical recording medium
JPH03141054A (en) * 1990-10-15 1991-06-17 Matsushita Electric Ind Co Ltd Production of optical information recording medium
CN100385541C (en) * 2004-04-28 2008-04-30 索尼株式会社 One time write optical recording media
WO2008091018A1 (en) * 2007-01-26 2008-07-31 Sony Corporation Optical recording medium and method for manufacturing the same
US8119215B2 (en) 2007-01-26 2012-02-21 Sony Corporation Optical recording medium and method for manufacturing the same

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