JPH0530390B2 - - Google Patents

Info

Publication number
JPH0530390B2
JPH0530390B2 JP61122686A JP12268686A JPH0530390B2 JP H0530390 B2 JPH0530390 B2 JP H0530390B2 JP 61122686 A JP61122686 A JP 61122686A JP 12268686 A JP12268686 A JP 12268686A JP H0530390 B2 JPH0530390 B2 JP H0530390B2
Authority
JP
Japan
Prior art keywords
recording
layer
recording medium
optical recording
tellurium
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP61122686A
Other languages
Japanese (ja)
Other versions
JPS62278094A (en
Inventor
Masaki Ito
Akio Morimoto
Katsuji Nakagawa
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.)
NEC Corp
Original Assignee
Nippon Electric 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP61122686A priority Critical patent/JPS62278094A/en
Priority to US07/043,626 priority patent/US4839208A/en
Priority to EP87106262A priority patent/EP0243958B1/en
Priority to DE8787106262T priority patent/DE3781926T2/en
Publication of JPS62278094A publication Critical patent/JPS62278094A/en
Publication of JPH0530390B2 publication Critical patent/JPH0530390B2/ja
Granted legal-status Critical Current

Links

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
    • G11B7/252—Record 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
    • G11B7/257—Record 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 layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the 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
    • G11B7/243—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 inorganic materials only, e.g. ablative 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
    • G11B7/243—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 inorganic materials only, e.g. ablative layers
    • G11B2007/24302—Metals or metalloids
    • G11B2007/24316—Metals or metalloids group 16 elements (i.e. chalcogenides, Se, Te)
    • 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
    • G11B7/243—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 inorganic materials only, e.g. ablative layers
    • G11B2007/24318—Non-metallic elements
    • G11B2007/24322—Nitrogen
    • 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
    • G11B7/252—Record 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
    • G11B7/257—Record 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 layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers
    • G11B2007/25705—Record 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 layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of inorganic materials
    • G11B2007/25715—Record 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 layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of inorganic materials containing oxygen
    • 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
    • G11B7/00451—Recording involving ablation of the recording layer

Landscapes

  • Chemical & Material Sciences (AREA)
  • Inorganic Chemistry (AREA)
  • Thermal Transfer Or Thermal Recording In General (AREA)
  • Optical Record Carriers And Manufacture Thereof (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は半導体レーザ光によつて情報を記録再
生することのできる光記録媒体に関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an optical recording medium on which information can be recorded and reproduced using semiconductor laser light.

(従来の技術) レーザ光によつて情報を媒体に記録し、かつ再
生する光デイスクメモリは、記録密度が高いこと
から大容量記録装置として優れた特徴を有してい
る。この光記録媒体材料としては、Te等のカル
コゲン元素、又はこれらの化合物が使用されてい
る(特公昭47−26897)。とくにテルルセレン系合
金はよく使用されている(特公昭54−41902、特
公昭57−7919、特公昭57−56058)。
(Prior Art) Optical disk memories, which record and reproduce information on a medium using laser light, have excellent characteristics as large-capacity recording devices because of their high recording density. As materials for this optical recording medium, chalcogen elements such as Te or compounds thereof are used (Japanese Patent Publication No. 47-26897). In particular, tellurium selenium alloys are often used (Japanese Patent Publication No. 54-41902, Japanese Patent Publication No. 57-7919, Japanese Patent Publication No. 57-56058).

近年、記録装置を小型化するため、レーザ光源
としては半導体レーザが使用されてきている。半
導体レーザは発振波長が8000Å前後であるが、テ
ルルセレン系合金はこの波長帯にも比較的よく通
合し、適度な反射率と適度な吸収率が得られる
(フイジカ・ステイタス・ソリダイ(phys・
stat・sol・7、189、1964))。
In recent years, in order to downsize recording devices, semiconductor lasers have been used as laser light sources. Semiconductor lasers have an oscillation wavelength of around 8000 Å, but tellurium selenium alloys are relatively compatible with this wavelength band and can provide moderate reflectance and moderate absorption (physica status solidi).
stat・sol・7, 189, 1964)).

(発明が解決しようとする問題点) しかしながら、これらの媒体で信号品質が充分
に良好でかつ半導体レーザ記録に適するものはな
かつた。
(Problems to be Solved by the Invention) However, none of these media has sufficiently good signal quality and is suitable for semiconductor laser recording.

本発明の目的は、耐候性がよく、かつ信号品質
が充分に良好で記録パワー余裕度が大きい半導体
レーザ記録に適した光記録媒体を提供することに
ある。
An object of the present invention is to provide an optical recording medium suitable for semiconductor laser recording that has good weather resistance, sufficiently good signal quality, and a large recording power margin.

(問題を解決するための手段) 本発明の光記録媒体は情報を半導体レーザ光に
よつて記録しかつ読み取る光記録媒体であつて、
シリコン酸化物又はセリウム酸化物又はマグネシ
ウム酸化物又は錫酸化物の層と、テルルとセレン
と窒素を主成分とする層との少なくとも2層を有
していることを特徴とする。
(Means for solving the problem) The optical recording medium of the present invention is an optical recording medium in which information is recorded and read by semiconductor laser light, and includes:
It is characterized by having at least two layers: a layer of silicon oxide, cerium oxide, magnesium oxide, or tin oxide, and a layer containing tellurium, selenium, and nitrogen as main components.

(作用) 光記録媒体は従来は第2図のような構成になつ
ていた。即ち、基板1の上に記録層21が設けら
れている。記録用レーザ光は基板1を通して記録
層21に集光照射され、ピツト22が形成され
る。基板1としてはポリカーポネイト、ポリオレ
フイン、ポリメチルペンテル、アクリル、エポキ
シ樹脂等の合成樹脂が使用される。基板には、ピ
ツトが同心円状あるいはスパイラル状に一定間隔
で精度よく記録されるように案内溝が設けられて
いるレーザビーム径程度の幅の溝に光が入射する
と光は回折され、ビーム中心が溝からずれるにつ
れて回折光強度の空間分布が変化するので、これ
を検出してレーザビームを溝の中心に入射させる
ようにサーボ系が構成されている。溝の幅は通常
0.3〜1.3μmであり、溝の深さは使用するレーザ
波長の1/12から1/4の範囲に設定される。集光に
関しても同様にサーボ系が構成されている。情報
の読み出しは、記録のときより弱いパワーのレー
ザ光をピツト上を通過するように照射することに
より、ピツトの有無に起因する反射率の変化を検
出して行なう。
(Function) Conventionally, an optical recording medium has a structure as shown in FIG. That is, the recording layer 21 is provided on the substrate 1. The recording laser beam is focused and irradiated onto the recording layer 21 through the substrate 1, and pits 22 are formed. As the substrate 1, synthetic resins such as polycarbonate, polyolefin, polymethylpentyl, acrylic, and epoxy resins are used. The substrate is provided with guide grooves so that the pits are accurately recorded at regular intervals in a concentric or spiral pattern.When light enters a groove with a width about the diameter of a laser beam, the light is diffracted and the center of the beam is Since the spatial distribution of the diffracted light intensity changes as it deviates from the groove, a servo system is configured to detect this and direct the laser beam to the center of the groove. The width of the groove is usually
The depth of the groove is 0.3 to 1.3 μm, and the depth of the groove is set in the range of 1/12 to 1/4 of the wavelength of the laser used. A servo system is similarly configured for condensing light. Information is read by irradiating a laser beam with a weaker power than during recording so as to pass over the pits, and detecting changes in reflectance caused by the presence or absence of pits.

記録層21としては種々の材料を使用できる
が、耐候性を考慮するとテルルセレン系合金膜が
望ましい。しかしながら、テルルセレン合金層の
みでは信号品質が充分に良好ではなかつた。本発
明者らは記録層をテルルとセレンと窒素を主成分
とすることにより、信号品質が良好で半導体レー
ザ記録に適した媒体となることを見出し、すでに
提案している。本発明はこれをさらに改善したも
のであり、第1図に示すように基板1とテルルセ
レン窒素層3の間に金属酸化物層2を設けること
により、記録により形成されるピツトが大きく拡
がらないようになる。したがつて、ピツトをつめ
て記録できるので高密度記録が可能となる。又、
記録パワー変動に対する余裕度も大きくなるの
で、実用的な光記録媒体となる。さらに又、大き
なピツトが形成されないためトラツキングやフオ
ーカスサーボが不安定にならないので実用的な光
記録媒体となる。ピツトが大きく拡がらない理由
は明確ではないが、テルルセレン窒素層の有無に
よる表面エネルギーの差が金属酸化物層の形成に
より変化することによつていると考えられる。
Although various materials can be used for the recording layer 21, a tellurium selenium alloy film is preferable in consideration of weather resistance. However, the signal quality was not sufficiently good with only the tellurium selenium alloy layer. The inventors of the present invention have found that by making the recording layer mainly composed of tellurium, selenium, and nitrogen, a medium with good signal quality and suitable for semiconductor laser recording can be obtained, and has already proposed this method. The present invention further improves this, and by providing a metal oxide layer 2 between the substrate 1 and the tellurium selenium nitrogen layer 3 as shown in FIG. 1, the pits formed by recording do not spread significantly. It becomes like this. Therefore, since recording can be performed by filling the pits, high-density recording is possible. or,
Since the margin for fluctuations in recording power is also increased, the optical recording medium becomes a practical optical recording medium. Furthermore, since no large pits are formed, tracking and focus servo do not become unstable, making it a practical optical recording medium. The reason why the pits do not expand significantly is not clear, but it is thought to be due to the difference in surface energy depending on the presence or absence of the tellurium selenium nitrogen layer that changes due to the formation of the metal oxide layer.

(実施例) 以下、本発明の実施例について説明する。(Example) Examples of the present invention will be described below.

100℃で2時間アニール処理した内径15mm、外
径130mm、厚さ1.2mmのポリカーボネイト樹脂デイ
スク基板にSiO2を500Å厚形成し、ひきつづきこ
の上に、テルルセレン合金ターゲツトをアルゴン
と窒素の混合ガスでマグネトロンスパツタして、
テルルとセレンと窒息の比が原子パーセントで90
対4対6のテルルセレン窒素層を240Å厚形成し
た。この光デイスクを95℃の窒素雰囲気中で1時
間アニールしたのち、波長8300Åにおける基板入
射反射率を測定したところ34%であつた。波長
8300Åの半導体レーザ光を基板を通して入射して
記録層上で1.6μmφ程度に絞り、媒体線速度5.6
m/sec、記録周波数3.77MHz、記録パルス幅
70nsec、記録パワー7.0mWの条件で記録し、0.7
mWで再生した。バンド幅KHzのキヤリアーとノ
イズとの比(C/N)は52dBと良好であつた。
この光デイスクを70℃80%の高温高湿度の環境に
60分間保存した後、上記特性を調べたが変化はな
く、耐候性に優れた光記録媒体であることが確認
された。
SiO 2 was formed to a thickness of 500 Å on a polycarbonate resin disk substrate with an inner diameter of 15 mm, an outer diameter of 130 mm, and a thickness of 1.2 mm that had been annealed at 100°C for 2 hours.Subsequently, a tellurium selenium alloy target was placed on top of this using a magnetron with a mixed gas of argon and nitrogen. Splashing,
The ratio of tellurium to selenium to suffocation is 90 in atomic percent.
A tellurium selenium nitrogen layer having a ratio of 4 to 6 was formed to a thickness of 240 Å. After annealing this optical disk in a nitrogen atmosphere at 95° C. for 1 hour, the substrate incident reflectance at a wavelength of 8300 Å was measured and found to be 34%. wavelength
Semiconductor laser light of 8300 Å is incident through the substrate and focused to about 1.6 μmφ on the recording layer, and the linear velocity of the medium is 5.6.
m/sec, recording frequency 3.77MHz, recording pulse width
Recorded under the conditions of 70nsec and recording power 7.0mW, 0.7
Regeneration was performed at mW. The carrier-to-noise ratio (C/N) with a bandwidth of KHz was as good as 52 dB.
This optical disk is placed in a high temperature and high humidity environment of 70℃ and 80%.
After storage for 60 minutes, the above characteristics were examined, but there were no changes, confirming that the optical recording medium had excellent weather resistance.

比較のためのSiO2層を設けない光デイスクに
比べて、45dB以上のC/Nが得られる記憶パワ
ー範囲はおそよ3倍大きくなり、記憶パワー変動
に対する余裕度の大きいことが確認された。又、
トラツキングやフオーカスのサーボも不安定にな
ることはなかつた。
Compared to a comparison optical disk without a SiO 2 layer, the storage power range in which a C/N of 45 dB or more can be obtained is approximately three times larger, confirming that there is a large margin against storage power fluctuations. or,
The tracking and focusing servos did not become unstable.

金属酸化物としては種々の酸化物を使用するこ
とができるが、その中ではCeO2、MgO、SiO、
SiO2、SnO2がとくに望ましい。膜の内部応力は
小さくするか又はやや圧縮応力となるように作製
することが、膜のクラツクを防止する点で望まし
い。金属酸化物層の膜厚は、5Åから2500Åの範
囲が望ましい。金属酸化物層の屈折率が基板の屈
折率もより小さい場合には膜中波長の1/4の厚さ
に設定することにより媒体反射率を極大にするこ
とができる。金属酸化物層の屈折率が基板の屈折
率よりも大きい場合には膜中波長の1/2の厚さに
設定することにより、媒体反射率が小さくなるこ
とを防ぐことができる。逆に、膜中波長の1/4或
いは3/4の厚さに設定すれば、媒体反射率は小さ
くなるが記録膜での吸収は最大となるので高感度
化することができる。
Various oxides can be used as the metal oxide, among which CeO 2 , MgO, SiO,
SiO 2 and SnO 2 are particularly desirable. In order to prevent cracks in the film, it is desirable to manufacture the film so that the internal stress is small or slightly compressive stress. The thickness of the metal oxide layer is preferably in the range of 5 Å to 2500 Å. When the refractive index of the metal oxide layer is smaller than that of the substrate, the medium reflectance can be maximized by setting the thickness to 1/4 of the wavelength in the film. When the refractive index of the metal oxide layer is larger than that of the substrate, the medium reflectance can be prevented from becoming small by setting the thickness to 1/2 of the wavelength in the film. On the other hand, if the thickness is set to 1/4 or 3/4 of the wavelength in the film, the medium reflectance will be small, but the absorption in the recording film will be maximized, so high sensitivity can be achieved.

テルルセレン窒素層の厚さは180Åから400Åの
範囲が記録再生特性の観点から望ましく、窒素の
含有量は原子パーセントで2パーセント以上10パ
ーセント以下が記録再生特性、耐候性の観点から
望ましく、セレンの含有量は原子パーセントで2
パーセント以上30パーセント以下、とくに10パー
セント以上30パーセント以下の範囲が耐候性の観
点で望ましい。
The thickness of the tellurium selenium nitrogen layer is preferably in the range of 180 Å to 400 Å from the viewpoint of recording/reproducing characteristics, and the nitrogen content is preferably 2% or more and 10% or less in atomic percent from the viewpoint of recording/reproducing characteristics and weather resistance. The amount is atomic percent 2
A range of 10% to 30%, particularly 10% to 30%, is desirable from the viewpoint of weather resistance.

テルルセレン窒素層には、鉛、ヒ素、スズ、ゲ
ルマニウム、カドミウム、タリウム、リン、イン
ジウム、ガリウム、亜鉛、アルミニウム、銅、
銀、マグネシウム、タンタル、金、バラジウム、
コバルトの群から選ばれた少なくとも1種の元素
を添加すると、ピツトの形成を良好に整える場合
がある。ただし添加量は原子パーセントで20パー
セント未満が望ましい。
The tellurium selenium nitrogen layer contains lead, arsenic, tin, germanium, cadmium, thallium, phosphorus, indium, gallium, zinc, aluminum, copper,
silver, magnesium, tantalum, gold, palladium,
Addition of at least one element selected from the group of cobalt may improve the formation of pits. However, the amount added is preferably less than 20% in atomic percent.

成膜方法は、スパツタリング法の他に、蒸着
法、反応性蒸着法、イオンプレーテイング法、イ
オンビームデポジシヨン法等でもよい。
In addition to the sputtering method, the film forming method may be a vapor deposition method, a reactive vapor deposition method, an ion plating method, an ion beam deposition method, or the like.

(発明の効果) 上記実施例から明らかなように、本発明により
耐候性がよくかつ信号品質が充分に良好で記録パ
ワー余裕度が大きく半導体レーザ記録に適した光
記録媒体が得られる。
(Effects of the Invention) As is clear from the above embodiments, the present invention provides an optical recording medium that has good weather resistance, sufficiently good signal quality, a large recording power margin, and is suitable for semiconductor laser recording.

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

第1図は本発明の光記録媒体の一例を示す断面
概略図、第2図は従来の光記録媒体の断面概略図
である。 図において、1は基板、2は金属酸化物層、3
はテルルセレン窒素を主成分とする層、21は記
録層、22はピツトを表わす。
FIG. 1 is a schematic cross-sectional view showing an example of the optical recording medium of the present invention, and FIG. 2 is a schematic cross-sectional view of a conventional optical recording medium. In the figure, 1 is a substrate, 2 is a metal oxide layer, and 3 is a metal oxide layer.
21 represents a layer containing tellurium selenium nitrogen as a main component, 21 represents a recording layer, and 22 represents a pit.

Claims (1)

【特許請求の範囲】[Claims] 1 情報を半導体レーザ光によつて記録しかつ読
み取る光記録媒体において、シリコン酸化物又は
セリウム酸化物又はマグネシウム酸化物又は錫酸
化物の層と、テルルとセレンと窒素を主成分とす
る層との少なくとも2層を有していることを特徴
とする光記録媒体。
1. In an optical recording medium in which information is recorded and read by semiconductor laser light, a layer of silicon oxide, cerium oxide, magnesium oxide, or tin oxide and a layer mainly composed of tellurium, selenium, and nitrogen are used. An optical recording medium characterized by having at least two layers.
JP61122686A 1986-04-30 1986-05-27 Optical recording medium Granted JPS62278094A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP61122686A JPS62278094A (en) 1986-05-27 1986-05-27 Optical recording medium
US07/043,626 US4839208A (en) 1986-04-30 1987-04-28 Optical information recording medium
EP87106262A EP0243958B1 (en) 1986-04-30 1987-04-29 Optical information recording medium
DE8787106262T DE3781926T2 (en) 1986-04-30 1987-04-29 MEDIUM FOR OPTICAL INFORMATION RECORDING.

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61122686A JPS62278094A (en) 1986-05-27 1986-05-27 Optical recording medium

Publications (2)

Publication Number Publication Date
JPS62278094A JPS62278094A (en) 1987-12-02
JPH0530390B2 true JPH0530390B2 (en) 1993-05-07

Family

ID=14842112

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61122686A Granted JPS62278094A (en) 1986-04-30 1986-05-27 Optical recording medium

Country Status (1)

Country Link
JP (1) JPS62278094A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005018947A1 (en) * 2003-08-21 2005-03-03 Mitsubishi Kagaku Media Co., Ltd. Recording medium

Also Published As

Publication number Publication date
JPS62278094A (en) 1987-12-02

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