JPH0877596A - Optical information recording medium - Google Patents
Optical information recording mediumInfo
- Publication number
- JPH0877596A JPH0877596A JP6230671A JP23067194A JPH0877596A JP H0877596 A JPH0877596 A JP H0877596A JP 6230671 A JP6230671 A JP 6230671A JP 23067194 A JP23067194 A JP 23067194A JP H0877596 A JPH0877596 A JP H0877596A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- recording
- protective layer
- amorphous
- optical
- 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.)
- Pending
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 44
- 239000010410 layer Substances 0.000 claims abstract description 48
- 239000011241 protective layer Substances 0.000 claims abstract description 31
- 239000000758 substrate Substances 0.000 claims description 7
- 239000013078 crystal Substances 0.000 abstract description 8
- 238000001816 cooling Methods 0.000 abstract description 4
- 230000031700 light absorption Effects 0.000 abstract description 2
- 238000002310 reflectometry Methods 0.000 abstract description 2
- 238000010586 diagram Methods 0.000 description 8
- 229910004298 SiO 2 Inorganic materials 0.000 description 4
- 238000010521 absorption reaction Methods 0.000 description 4
- 230000000052 comparative effect Effects 0.000 description 3
- 238000005259 measurement Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 229920000515 polycarbonate Polymers 0.000 description 2
- 239000004417 polycarbonate Substances 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 238000004544 sputter deposition Methods 0.000 description 2
- KTTCLOUATPWTNB-UHFFFAOYSA-N 2-[2-[4-(6,7-dimethoxy-3,4-dihydro-1h-isoquinolin-2-yl)butylcarbamoyl]-4-methylphenoxy]ethyl methanesulfonate Chemical compound C1C=2C=C(OC)C(OC)=CC=2CCN1CCCCNC(=O)C1=CC(C)=CC=C1OCCOS(C)(=O)=O KTTCLOUATPWTNB-UHFFFAOYSA-N 0.000 description 1
- 229910000618 GeSbTe Inorganic materials 0.000 description 1
- 239000008186 active pharmaceutical agent Substances 0.000 description 1
- 230000008033 biological extinction Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000002425 crystallisation Methods 0.000 description 1
- 230000008025 crystallization Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000013028 medium composition Substances 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000001953 recrystallisation Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
Landscapes
- Optical Record Carriers And Manufacture Thereof (AREA)
Abstract
(57)【要約】
【目的】 波長670〜690nmの光ヘッドを用いた
マークエッジ記録において、オーバライトジッタの小さ
な光学情報記録媒体を提供する。
【構成】 反射層をSiとし、各層の膜厚をそれぞれ、
下部保護層を180〜260nm、記録層を10〜13
nm、上部保護層を13〜25nm、反射層を55〜6
5nmとする。波長690nm近傍において、非晶質と
結晶の反射率変化を大きくしたまま、結晶の吸収率を非
晶質の吸収率より高くすることが可能となるので、消去
率が高く、かつオーバライトによるジッタ増加の小さな
光学情報記録媒体を提供することが可能となる。また、
反射層での光吸収も小さいために、レーザ照射後の記録
層の冷却速度を遅くすることもなく、良好な非晶質マー
クを形成することができる。
(57) [Summary] [PROBLEMS] To provide an optical information recording medium with small overwrite jitter in mark edge recording using an optical head having a wavelength of 670 to 690 nm. [Structure] The reflective layer is Si, and the thickness of each layer is
The lower protective layer is 180 to 260 nm, and the recording layer is 10 to 13 nm.
nm, upper protective layer 13-25 nm, reflective layer 55-6
5 nm. In the vicinity of the wavelength of 690 nm, it is possible to make the absorptance of the crystal higher than the absorptivity of the amorphous while maintaining a large change in the reflectivity of the amorphous and the crystal. It is possible to provide an optical information recording medium whose increase is small. Also,
Since the light absorption in the reflective layer is also small, a good amorphous mark can be formed without slowing the cooling rate of the recording layer after laser irradiation.
Description
【0001】[0001]
【産業上の利用分野】本発明は、熱履歴の違いにより誘
起される相変化に伴う光学定数の変化を利用して情報の
記録・消去を行う光学情報記録媒体、すなわち相変化光
ディスクに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical information recording medium for recording and erasing information by utilizing a change in optical constants accompanying a phase change induced by a difference in thermal history, that is, a phase change optical disk.
【0002】[0002]
【従来の技術】レーザ光の照射によって情報の記録・消
去・再生を行う光学情報記録媒体としては、光磁気ディ
スクや相変化光ディスクなどが知られている。このう
ち、例えば相変化光ディスクでは、図2に示すように、
基板1上に下部保護層2、記録層3、上部保護層4、反
射層5がこの順に設けられた4層構成が通常用いられ
る。情報の記録・消去は、レーザ光の照射による昇温・
冷却の熱履歴の違いによって誘起される記録層の非晶質
・結晶間の相変化を利用して行われる。すなわち、記録
層を溶融し急冷することにより非晶質化させ記録を行
い、また、結晶化温度以上に一定時間保持することによ
り結晶化させ、消去を行う。信号の再生は非晶質・結晶
間の反射率差を利用して行われる。下部保護層2、記録
層3、上部保護層4および反射層5のそれぞれの膜厚
は、感度、C/N、消去率、書換可能繰り返し回数など
の観点から最適化される。2. Description of the Related Art Magneto-optical disks and phase change optical disks are known as optical information recording media for recording / erasing / reproducing information by irradiating laser light. Among them, for example, in a phase change optical disk, as shown in FIG.
A four-layer structure in which a lower protective layer 2, a recording layer 3, an upper protective layer 4, and a reflective layer 5 are provided in this order on a substrate 1 is usually used. Information is recorded / erased by heating with laser light
This is performed by utilizing the phase change between the amorphous and crystalline of the recording layer which is induced by the difference in thermal history of cooling. That is, the recording layer is melted and rapidly cooled to be amorphized for recording, and the recording layer is kept at a crystallization temperature or higher for a certain time to be crystallized and erased. Signal reproduction is performed by utilizing the difference in reflectance between amorphous and crystalline. The film thickness of each of the lower protective layer 2, the recording layer 3, the upper protective layer 4, and the reflective layer 5 is optimized from the viewpoint of sensitivity, C / N, erasing rate, rewritable repetition count, and the like.
【0003】高密度化には、記録マークの両端に情報を
持たせるマークエッジ記録が有効である。しかし、信号
の再生に結晶・非晶質間の反射率差を利用している相変
化光ディスクでは、結晶状態の吸収率と非晶質状態の吸
収率が異なる場合が多く、一般に、非晶質状態の吸収率
が結晶状態の吸収率より大きくなっている。このような
場合、形成されるマークの幅や長さは、新たに記録する
前の状態が結晶であったか、非晶質であったかによって
影響され、オーバライトによってジッタが大きく増加し
てしまう。従って、相変化光ディスクにおいてジッタを
低減し、マークエッジ記録を実現するには、非晶質状態
と結晶状態の吸収率を等しくする必要がある。結晶状態
の方が融解に伴う潜熱が大きいことを考慮すると、結晶
状態の吸収率が非晶質状態の吸収率より大きくなるよう
に設計するのが望ましい。このような媒体を提供する手
段として、特開平2−218334号公報に記載されて
いるSiのような透過性の反射層を用いた吸収率制御法
が有効であることが知られている。また、この方法を用
いて波長830nmにおいてオーバライトジッタを低減
した相変化光ディスクが報告されている(ISOM/O
DS '93 Conference Digest p.72)。[0005] To increase the recording density, mark edge recording in which information is provided at both ends of a recording mark is effective. However, in a phase-change optical disk that utilizes the difference in reflectance between crystalline and amorphous to reproduce a signal, the absorptance in the crystalline state and the absorptance in the amorphous state are often different. The absorptance of the state is higher than that of the crystalline state. In such a case, the width and length of the mark to be formed are affected by whether the state before new recording was crystalline or amorphous, and the jitter greatly increases due to overwriting. Therefore, in order to reduce the jitter and realize the mark edge recording in the phase change optical disk, it is necessary to make the absorptance of the amorphous state equal to that of the crystalline state. Considering that the latent heat associated with melting is higher in the crystalline state, it is desirable to design the absorptance of the crystalline state to be higher than that of the amorphous state. As a means for providing such a medium, it is known that the absorptance control method using a transmissive reflective layer such as Si described in JP-A-2-218334 is effective. Also, a phase change optical disc in which overwrite jitter is reduced at a wavelength of 830 nm using this method has been reported (ISOM / O
DS '93 Conference Digest p.72).
【0004】[0004]
【発明が解決しようとする課題】現在、製品化されてい
る光ディスクの光ヘッド光源には、波長780〜830
nmのレーザダイオードが用いられている。さらに記録
密度を向上させるために、レーザダイオード短波長化が
計られており、波長690nm前後の高パワ赤色レーザ
ダイオードが実用化に供されつつある。相変化光ディス
クの記録層や反射層の光学定数は、780〜830nm
と690nmでは異なる値をもつ。そのため、780〜
830nmに適した従来構成の媒体では、690nmの
光ヘッドに対して良好なオーバライト特性を確保するこ
とが困難であり、オーバライトによってジッタが増加し
てしまうという問題があった。本発明は、波長690n
m近傍の光ヘッドを用いたマークエッジ記録において、
良好なオーバライト特性を得ることができる相変化光デ
ィスクを提供することを目的とする。Wavelengths of 780 to 830 are currently used as optical head light sources for optical disks that are currently being commercialized.
nm laser diodes are used. In order to further improve the recording density, the wavelength of the laser diode has been shortened, and a high power red laser diode with a wavelength of about 690 nm is being put to practical use. The optical constants of the recording layer and the reflective layer of the phase change optical disc are 780 to 830 nm.
And 690 nm have different values. Therefore, 780
In the medium having the conventional structure suitable for 830 nm, it is difficult to secure a good overwrite characteristic for the optical head of 690 nm, and there is a problem that the jitter increases due to the overwrite. The present invention has a wavelength of 690n
In mark edge recording using an optical head near m,
An object of the present invention is to provide a phase change optical disk that can obtain good overwrite characteristics.
【0005】[0005]
【課題を解決するための手段】本発明は、情報の記録・
消去・再生を行う相変化光ディスクにおいて、基板上に
下部保護層、記録層、上部保護層およびSiよりなる反
射層が順次形成された構造を有し、前記下部保護層の膜
厚が180〜260nm、前記記録層の膜厚が10〜1
3nm、前記上部保護層の膜厚が13〜25nm、前記
反射層の膜厚が55〜65nmであることを特徴とする
光学情報記録媒体である。ここで、相変化光ディスク
は、波長670〜695nmの光ヘッドを用いて、マー
クエッジ記録を利用し、情報の記録・消去・再生を行う
ものであることを好適とする。SUMMARY OF THE INVENTION The present invention is directed to recording / recording information.
An erasing / reproducing phase change optical disc has a structure in which a lower protective layer, a recording layer, an upper protective layer, and a reflective layer made of Si are sequentially formed on a substrate, and the lower protective layer has a thickness of 180 to 260 nm. , The thickness of the recording layer is 10 to 1
3 nm, the thickness of the upper protective layer is 13 to 25 nm, and the thickness of the reflective layer is 55 to 65 nm. Here, it is preferable that the phase change optical disc is one that records / erases / reproduces information by using mark edge recording by using an optical head having a wavelength of 670 to 695 nm.
【0006】本発明によれば、波長690nm近傍にお
いて、非晶質と結晶の反射率変化を大きくしたまま、結
晶の吸収率を非晶質の吸収率より高くすることが可能と
なるので、消去率が高く、かつオーバライトによるジッ
タ増加の小さな光学情報媒体を提供することが可能とな
る。According to the present invention, in the vicinity of a wavelength of 690 nm, it is possible to make the absorptance of the crystal higher than the absorptivity of the amorphous while maintaining a large change in the reflectivity of the amorphous and the crystal. It is possible to provide an optical information medium having a high rate and a small increase in jitter due to overwriting.
【0007】[0007]
【作用】記録層として一般に用いられているGeSbT
eの690nm近傍における光学定数の相変化に伴う変
化は、780〜830nm近傍に比べて小さい。例えば
Ge2Sb2Te5では、波長830nmにおける光学定
数(n,k)は、非晶質では(4.6,1.06)、結
晶では(5.89,3.47)である。これに対し、波
長690nmでは、非晶質では(4.36,1.7
2)、結晶では(4.46,4.0)であり、nの変化
が小さくなる。そのため、透過光を利用して吸収率を制
御するには、780〜830nmの時に比べて記録層の
膜厚を薄くしなければならない。ただし、感度・膜質の
観点から10nm以上は必要である。また、波長690
nmにおけるSiの光学定数(n,k)は、作成方法に
よって多少異なるが、(4.0〜4.6,0.1〜0.
4)であり、780〜830nmに比べて消衰係数kが
大きくなる。Si反射層での光吸収は、レーザ光反射後
の記録層の冷却速度を遅くし、良好な非晶質マーク形成
を阻害する要因となるので、できるだけ低くする必要が
ある。従って、690nm近傍ではSiの膜厚を薄くし
なければならない。Function: GeSbT generally used as a recording layer
The change of e with the phase change of the optical constant in the vicinity of 690 nm is smaller than that in the vicinity of 780 to 830 nm. For example, with Ge 2 Sb 2 Te 5 , the optical constant (n, k) at a wavelength of 830 nm is (4.6, 1.06) in the amorphous state and (5.89, 3.47) in the crystalline state. On the other hand, at a wavelength of 690 nm, (4.36, 1.7
2), the crystal has (4.46, 4.0), and the change of n is small. Therefore, in order to control the absorptance by utilizing the transmitted light, the film thickness of the recording layer must be made smaller than that in the case of 780 to 830 nm. However, from the viewpoint of sensitivity and film quality, 10 nm or more is necessary. Also, the wavelength 690
The optical constants (n, k) of Si in nm are slightly different depending on the manufacturing method, but are (4.0 to 4.6, 0.1 to 0.
4), and the extinction coefficient k becomes larger than that of 780 to 830 nm. Light absorption in the Si reflection layer slows down the cooling rate of the recording layer after the laser light reflection and hinders the formation of a good amorphous mark. Therefore, it is necessary to reduce the thickness of Si in the vicinity of 690 nm.
【0008】図1にSiを反射層とした相変化光ディス
クの690nmにおける光学特性の例を示す。媒体構成
は、Si(60nm)反射層/ZnS−SiO2(18
nm)上部保護層/GeSbTe(13nm)記録層/
ZnS−SiO2下部保護層/ポリカーボネート基板で
ある。図中、Acは結晶の吸収率、Aaは非晶質の吸収
率、Rcは結晶の反射率、Raは非晶質の反射率を示
す。記録層を13nmと薄くすることによって、下部保
護層の広い膜厚範囲にわたって結晶の吸収率を非晶質の
吸収率より高くすることが可能となっている。FIG. 1 shows an example of optical characteristics at 690 nm of a phase change optical disk having Si as a reflection layer. The medium composition is Si (60 nm) reflective layer / ZnS—SiO 2 (18
nm) upper protective layer / GeSbTe (13 nm) recording layer /
A ZnS-SiO 2 lower protective layer / polycarbonate substrate. In the figure, Ac represents a crystal absorption rate, Aa represents an amorphous absorption rate, Rc represents a crystal reflectance, and Ra represents an amorphous reflectance. By making the recording layer as thin as 13 nm, it is possible to make the absorptance of crystals higher than the absorptivity of amorphous over a wide thickness range of the lower protective layer.
【0009】[0009]
【実施例】以下、本発明の実施例について、図面に基づ
いて説明する。 実施例1 図2は本発明に係る光学情報記録媒体の断面を示す図で
ある。基板1上に下部保護層2、記録層3、上部保護層
4、反射層5を順次積層した構成である。基板1として
ポリカーボネート(PC)を用い、下部保護層2として
ZnS−SiO2を240nm、記録層3としてGe2S
b2Te5を12nm、上部保護層4としてZnS−Si
O2を18nm、反射層5としてSiを60nmを順次
スパッタリングにより積層した。この構成では、非晶質
状態の記録層の吸収率および結晶状態の記録層の吸収率
はそれぞれ50%と63%であった。上記ディスクを線
速10m/sで回転させ、波長690nmの半導体レー
ザを用いて記録・消去を行った。1.88MHz,du
ty=50%の信号に3.03MHz,duty=50
%の信号をオーバライトして、C/N、消去率、ジッタ
を測定した。図3に示すように、オーバライト後でもジ
ッタは3ns以下と良好な値を示した。Embodiments of the present invention will be described below with reference to the drawings. Example 1 FIG. 2 is a diagram showing a cross section of an optical information recording medium according to the present invention. In this configuration, a lower protective layer 2, a recording layer 3, an upper protective layer 4, and a reflective layer 5 are sequentially laminated on a substrate 1. Polycarbonate (PC) is used as the substrate 1, ZnS—SiO 2 is 240 nm as the lower protective layer 2, and Ge 2 S is as the recording layer 3.
b 2 Te 5 of 12 nm, ZnS-Si as the upper protective layer 4
O 2 having a thickness of 18 nm and Si having a thickness of 60 nm as the reflection layer 5 were sequentially laminated by sputtering. In this structure, the absorptance of the recording layer in the amorphous state and the absorptance of the recording layer in the crystalline state were 50% and 63%, respectively. The disk was rotated at a linear velocity of 10 m / s, and recording / erasing was performed using a semiconductor laser having a wavelength of 690 nm. 1.88MHz, du
3.03 MHz for duty = 50% signal, duty = 50
% Signal was overwritten, and C / N, erasure rate, and jitter were measured. As shown in FIG. 3, the jitter was a good value of 3 ns or less even after overwriting.
【0010】比較例1 波長830nmにおいて良好な特性を示したディスクを
用いて、波長690nmにおけるオーバライト特性を測
定した。ディスクは、下部保護層2としてZnS−Si
O2を250nm、記録層3としてGe2Sb2Te5を1
5nm、上部保護層4としてZnS−SiO2を18n
m、反射層5としてSiを65nmを順次スパッタリン
グにより積層した構成である。この構成では、波長69
0nmにおける非晶質状態の吸収率および結晶状態の吸
収率はどちらも60%であり、結晶状態の吸収率を非晶
質状態の吸収率より高くすることはできなかった。上記
ディスクのオーバライト特性を実施例1と同じ条件で測
定した結果を図4に示す。ジッタは4nsであり、初記
録時のジッタ2nsに比べて大きく増加することが確認
された。Comparative Example 1 Using a disk showing good characteristics at a wavelength of 830 nm, the overwrite characteristics at a wavelength of 690 nm were measured. The disk has ZnS-Si as the lower protective layer 2.
O 2 is 250 nm, and Ge 2 Sb 2 Te 5 is used as the recording layer 3.
ZnS-SiO 2 as the upper protective layer 4 having a thickness of 5 nm
m, and the reflective layer 5 has a structure in which Si having a thickness of 65 nm is sequentially laminated by sputtering. In this configuration, the wavelength 69
Both the absorptance in the amorphous state and the absorptance in the crystalline state at 0 nm were 60%, and the absorptance in the crystalline state could not be made higher than that in the amorphous state. FIG. 4 shows the result of measuring the overwrite characteristics of the above-mentioned disk under the same conditions as in Example 1. It was confirmed that the jitter was 4 ns, which was significantly larger than the jitter of 2 ns at the time of initial recording.
【0011】比較例2 オーバライトジッタに及ぼす記録層の膜厚の影響を調べ
るため、実施例1とほぼ同様の構成で、記録層の膜厚を
15nmとしたディスクを作成し、オーバライト特性を
測定した。実施例1と同じ条件で、C/N、消去率、ジ
ッタを測定した結果を図5に示す。消去率はほぼ同等で
あり、C/Nは向上している。しかしながら、ジッタは
大きく増加しており、高密度化は困難である。Comparative Example 2 In order to investigate the influence of the film thickness of the recording layer on the overwrite jitter, a disk having a recording layer film thickness of 15 nm was prepared with almost the same structure as in Example 1, and the overwrite characteristics were evaluated. It was measured. FIG. 5 shows the results of measurement of C / N, erasure rate, and jitter under the same conditions as in Example 1. The erasing rates are almost the same and the C / N is improved. However, the jitter is greatly increased, and it is difficult to increase the density.
【0012】比較例3 再生信号品質に及ぼすSi反射層の膜厚の影響を調べる
ため、実施例1と同様の構成で、Siの膜厚を70n
m,80nmとしたディスクを作成し、再生波形を観察
した。図6はその結果を示したもので、図6(a)は6
0nm、図6(b)は70nm、図6(c)は80nm
の場合である。同図に示すように、Si反射層の膜厚が
厚くなるにつれ、再生波形の歪みが大きくなる。この歪
みは、冷却速度低下のために生じる記録非晶質マーク中
央部での再結晶化によるものであることが、TEM観察
から確認された。Comparative Example 3 In order to investigate the influence of the film thickness of the Si reflective layer on the reproduced signal quality, the Si film thickness was set to 70 n in the same configuration as in Example 1.
A disk with m and 80 nm was prepared and the reproduced waveform was observed. FIG. 6 shows the result, and FIG.
0 nm, 70 nm in FIG. 6 (b), 80 nm in FIG. 6 (c)
Is the case. As shown in the same figure, as the film thickness of the Si reflective layer increases, the distortion of the reproduced waveform increases. It was confirmed from TEM observation that this distortion was due to recrystallization in the central portion of the recorded amorphous mark caused by a decrease in cooling rate.
【0013】実施例2 下部保護層の最適膜厚を調べるため、実施例1と同様の
構成で下部保護層の膜厚を150〜300nmの間で変
化させたディスクを作成し、オーバライト特性の測定を
行った。非晶質状態および結晶状態の吸収率の下部保護
層厚依存性を測定したところ、図7のようになった。図
7において、○は結晶状態の吸収率、□は非晶質状態の
吸収率を示す。180〜260nmの範囲で結晶状態の
吸収率が非晶質状態の吸収率より高くなった。各ディス
クを実施例1と同じ条件でオーバライトし、ジッタの下
部保護層厚依存性を測定した結果、図7の●印で示すよ
うに、結晶状態の吸収率が非晶質状態の吸収率より高い
範囲で低ジッタとなった。Example 2 In order to investigate the optimum film thickness of the lower protective layer, a disk having the same structure as in Example 1 in which the film thickness of the lower protective layer was changed between 150 and 300 nm was prepared, and the disc with the overwrite characteristics was prepared. The measurement was performed. When the dependency of the absorptance in the amorphous state and the crystalline state on the thickness of the lower protective layer was measured, it was as shown in FIG. In FIG. 7, ◯ indicates the absorption rate in the crystalline state, and □ indicates the absorption rate in the amorphous state. In the range of 180 to 260 nm, the absorptance in the crystalline state was higher than that in the amorphous state. Each disk was overwritten under the same conditions as in Example 1 and the dependence of the jitter on the thickness of the lower protective layer was measured. As a result, as shown by the ● mark in FIG. 7, the absorptance in the crystalline state is that in the amorphous state. Low jitter in the higher range.
【0014】[0014]
【発明の効果】以上説明したように、本発明によれば、
波長670〜695nm近傍の光ヘッドを用いたマーク
エッジ記録において、オーバライトジッタを低減するこ
とが可能となり高密度化を実現することができる。As described above, according to the present invention,
In mark edge recording using an optical head with a wavelength in the vicinity of 670 to 695 nm, it is possible to reduce overwrite jitter and achieve higher density.
【図1】本発明による光学情報記録媒体の一例の吸収率
および反射率の下部保護層厚依存性を示す図である。FIG. 1 is a diagram showing the dependency of absorptance and reflectance on the thickness of a lower protective layer of an example of the optical information recording medium according to the present invention.
【図2】本発明による光学情報記録媒体の基本構成図で
ある。FIG. 2 is a basic configuration diagram of an optical information recording medium according to the present invention.
【図3】本発明による光学情報記録媒体の一例の光学特
性図である。FIG. 3 is an optical characteristic diagram of an example of an optical information recording medium according to the present invention.
【図4】従来例による光学情報記録媒体の一例の光学特
性図である。FIG. 4 is an optical characteristic diagram of an example of a conventional optical information recording medium.
【図5】従来例による光学情報記録媒体の一例の光学特
性図である。FIG. 5 is an optical characteristic diagram of an example of a conventional optical information recording medium.
【図6】再生波形のSi反射層厚依存性を示す図であ
る。FIG. 6 is a diagram showing the dependence of a reproduced waveform on the thickness of a Si reflective layer.
【図7】結晶状態と非晶質状態での吸収率およびジッタ
の下部保護層厚依存性を示す図である。FIG. 7 is a diagram showing dependency of absorptance and jitter in a crystalline state and an amorphous state on a thickness of a lower protective layer.
1 基板 2 下部保護層 3 記録層 4 上部保護層 5 反射層 1 substrate 2 lower protective layer 3 recording layer 4 upper protective layer 5 reflective layer
Claims (2)
ディスクにおいて、基板上に下部保護層、記録層、上部
保護層およびSiよりなる反射層が順次形成された構造
を有し、前記下部保護層の膜厚が180〜260nm、
前記記録層の膜厚が10〜13nm、前記上部保護層の
膜厚が13〜25nm、前記反射層の膜厚が55〜65
nmであることを特徴とする光学情報記録媒体。1. A phase change optical disk for recording / erasing / reproducing information, which has a structure in which a lower protective layer, a recording layer, an upper protective layer and a reflective layer made of Si are sequentially formed on a substrate, The thickness of the protective layer is 180 to 260 nm,
The recording layer has a film thickness of 10 to 13 nm, the upper protective layer has a film thickness of 13 to 25 nm, and the reflective layer has a film thickness of 55 to 65.
An optical information recording medium characterized by having a thickness of nm.
5nmの光ヘッドを用いて、マークエッジ記録を利用
し、情報の記録・消去・再生を行うものである請求項1
記載の光学情報記録媒体。2. The phase change optical disk has a wavelength of 670 to 69.
2. Information recording / erasing / reproducing is performed by using mark edge recording using a 5 nm optical head.
The optical information recording medium described.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6230671A JPH0877596A (en) | 1994-08-31 | 1994-08-31 | Optical information recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6230671A JPH0877596A (en) | 1994-08-31 | 1994-08-31 | Optical information recording medium |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0877596A true JPH0877596A (en) | 1996-03-22 |
Family
ID=16911482
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6230671A Pending JPH0877596A (en) | 1994-08-31 | 1994-08-31 | Optical information recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0877596A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5862122A (en) * | 1996-05-27 | 1999-01-19 | Nec Corporation | Phase change optical disk and a method for recording and playbacking optical information on or from an optical disk |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01149238A (en) * | 1987-12-04 | 1989-06-12 | Matsushita Electric Ind Co Ltd | optical information recording medium |
| JPH04212735A (en) * | 1990-03-14 | 1992-08-04 | Matsushita Electric Ind Co Ltd | Optical disk and method for recording optical information |
| JPH05298748A (en) * | 1992-04-17 | 1993-11-12 | Matsushita Electric Ind Co Ltd | Optical information recording medium and designing method for structure thereof |
-
1994
- 1994-08-31 JP JP6230671A patent/JPH0877596A/en active Pending
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01149238A (en) * | 1987-12-04 | 1989-06-12 | Matsushita Electric Ind Co Ltd | optical information recording medium |
| JPH04212735A (en) * | 1990-03-14 | 1992-08-04 | Matsushita Electric Ind Co Ltd | Optical disk and method for recording optical information |
| JPH05298748A (en) * | 1992-04-17 | 1993-11-12 | Matsushita Electric Ind Co Ltd | Optical information recording medium and designing method for structure thereof |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5862122A (en) * | 1996-05-27 | 1999-01-19 | Nec Corporation | Phase change optical disk and a method for recording and playbacking optical information on or from an optical disk |
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