JPS589229A - Optical recording medium - Google Patents

Optical recording medium

Info

Publication number
JPS589229A
JPS589229A JP56105458A JP10545881A JPS589229A JP S589229 A JPS589229 A JP S589229A JP 56105458 A JP56105458 A JP 56105458A JP 10545881 A JP10545881 A JP 10545881A JP S589229 A JPS589229 A JP S589229A
Authority
JP
Japan
Prior art keywords
optical recording
recording medium
film
thermal conductivity
films
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
Application number
JP56105458A
Other languages
Japanese (ja)
Inventor
Noburo Yasuda
安田 修朗
Masao Mashita
真下 正夫
Tomoyuki Ishibashi
石橋 友行
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura 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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP56105458A priority Critical patent/JPS589229A/en
Publication of JPS589229A publication Critical patent/JPS589229A/en
Pending 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
    • 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
    • G11B7/2533Record 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 resins
    • 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
    • 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
    • G11B2007/24328Carbon

Landscapes

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

Abstract

PURPOSE:To obtain a high-sensitivity, long-life optical recording body which uses a low-output semiconductor laser while preventing the deformation of a resin plate and the oxidation of a recording film, by providing thin recording films, each consisting essentially of Te and C, on both sides of the organic resin plate which has low thermal conductivity. CONSTITUTION:On both surfaces of an organic resin substrate 3 with low thermal conductivity such as an acrylic resin plate having <=1X10<-3>cal/sec thermal conductivity, optical recording films 4 which consist essentially of Te and C while containing H and O are formed by sputtering Te in gaseous CH4, etc., obtaining an optical recording disk. Because both the surfaces of the resin plate 3 are covered with the films 4, neither curvature nor strain due to humidity and temperature is caused. Further, the films 4 never become transparent owing to oxidation and a high-sensitivity, long-life recording medium for optical recording and reading which uses a low-output semiconductor laser is obtained.

Description

【発明の詳細な説明】 本発明はヒート篭−ドによる光記録媒体に係)*g、高
書度記鎌記憶目的セし、集束したレーず一光を媒体属罵
照射しその熱によ)媒体膜を変質又は蒸発させて、馬の
反射率又は透過率、を変化させる光記録媒体に関す、す
る。4.、 。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical recording medium using a heat cage. ) Relating to an optical recording medium in which the reflectance or transmittance of the medium is changed by altering or evaporating the medium film. 4. , .

従来、tの種の代表的な、例はG、CJeuw@y @
亀alの論文、”All optical disk 
replac@s !5mg tape魯”(1111
8PIiiCTRUM、p襲、!・b、111?l)、
)に示されてい為如く、ディ、スフ、の一、体が主であ
)、ディスクの基板は熱伝導の低吟材質、を使用し媒、
体膜は低融点、低沸点、低熱伝導率の、金属層を使用、
する01lL在の技@’cは、基板にアクリル樹層を嚢
属、馬に鞠sOoム厚のテルル(’To)薄馬を連儒、
い実用4t−を前の段階に来−ている0、、。
Traditionally, typical examples of t species are G, CJeuw@y@
Kame al's paper, “All optical disk
reprac@s! 5mg Tape Lu” (1111
8PIiiiCTRUM, p attack!・b, 111? l),
) As shown in Figure 2, the disk substrate is made of a material with low thermal conductivity.
The body membrane uses a metal layer with low melting point, low boiling point, and low thermal conductivity.
The current technique of 01L is to use an acrylic tree layer on the substrate, a thick tellurium ('To) and a thin horse on the base.
0, which is coming to the previous stage of practical 4t.

第1511はヒのような従来の光−、、、g、媒体、や
、断面図で−る0すなわち、蝉明基板(峠の片、I!、
−反射率の内歯い(又畔遥遥率、の、小さい、)媒体、
属−をW!威し。
The 1511th is a conventional light beam such as H, G, medium, and a cross-sectional view of the Cicada substrate (pass piece, I!,
- A medium with a low internal reflectivity (also a small external reflectance),
Genus-W! Intimidation.

1Jllaφ11111!KLぼった書龜込み用レー、
ず一光を基板(1)儒スは媒体膜(2)側から一体属(
1)−照、射、し、媒体膜(2)を変質、*形、蒸発1
せて情報を、記i!11!せ、。
1Jllaφ11111! KL holder for calligraphy,
The light is connected to the substrate (1) and the light is integrated from the medium film (2) side (
1) - Irradiation, irradiation, alteration of medium film (2), *form, evaporation 1
Let me know the information! 11! height,.

読皐出しは書自込み時のレーザー光の74以下薯度のレ
ーず一光を媒体膜#2)K照射し、反射率変化又は透過
率変化で情報を読みとる。通常、透明基板(1)は1−
2■厚のアクリル樹脂であ〉、媒体膜(2)は約5oo
Xの〒・薄膜であシ、配録は〒・薄膜の蒸発による約I
J1111φの大で行われ、全体は直1に3Daa糧の
ディスク形となっている。
For reading, the medium film #2) is irradiated with a laser beam of 74 or less intensities of the laser beam used during self-writing, and the information is read by changes in reflectance or transmittance. Usually, the transparent substrate (1) is 1-
Made of acrylic resin with a thickness of 2mm, the media film (2) is approximately 5mm thick.
X's 〒・Thin film is used, and the distribution is 〒・Approximately I due to evaporation of the thin film.
It is made with a diameter of J1111φ, and the whole is in the shape of a disk with a diameter of 3 Daa.

しかしながらこのような従来の光記憶媒体においては、
実用化にふみ切れない大きな難問がある。
However, in such conventional optical storage media,
There is a big problem that cannot be solved in practical application.

それは寿命に対し何ら保証できないという事であシ、特
にアクリル樹脂基板とT@薄膜とに対する耐候性、耐灘
潤性の関連である。
This means that no guarantee can be given regarding the lifespan, especially regarding the weather resistance and wetness resistance of the acrylic resin substrate and the T@ thin film.

周知の如く、アクリル樹脂は可視光、近赤外光に対し透
明であ)1表面平滑性、成m性、貴意性に優れ、ガラス
よ〉も熱伝導率が低いためヒートモード記録用基板とし
て紘理想的な素材である。
As is well known, acrylic resin is transparent to visible light and near-infrared light, has excellent surface smoothness, formability, and preciousness, and has lower thermal conductivity than glass, so it is used as a substrate for heat mode recording. Hiro is an ideal material.

然し乍ら、水を吸収し中すく、その吸水度合により、樹
脂が伸縮するという有機′材料の欠点が、アクリル樹脂
は特に大きいという問題がある0即ちアクリル板の両面
を同一温湿度にさらせば、両面の伸縮度は同一とな)、
板のソリ、歪等社発生しないが、その板の片面に屓、例
えば水を吸収、透過させな一金属膜が形成されていると
、その面bアクリル樹脂呟温度に鈍轡になるが、他の面
は開放されているため敏感で返に、伸纏祉片面でのみ起
〉、板のソリ、歪等が直ちに発生する。この板のソリ、
歪等はデ′イスタ直径が大きい程激しくなり、m傷直徽
の場合、乾燥した日と′、雨天の日とではソリ方向が麦
シ、板厚方向で1−以上も変形する。又その変形に伴う
応力歪みが転向に発生し光の偏光角を複雑にか見させて
し重う。この板の変S唸し−ず一フォーカスが自動的に
追随できる板面の平面度よ〉大自くなってしまい、フォ
ーカスが不可能とな〉ν乍が不可能となってし重うため
、ディスクとしての機能が果せなくなる。又、偏光歪4
畔、媒体膜を保−する目的で使われる基頼儒からを賀す
る方式kかいて、レーず一光の分散、フォーカス不jL
J出力時のノイズ等の原因と*)、均一なディスクを供
給で龜なくなる。 。
However, acrylic resin has the disadvantage that organic materials tend to absorb water and the resin expands and contracts depending on the degree of water absorption.In other words, if both sides of an acrylic board are exposed to the same temperature and humidity, both sides will expand and contract. The degree of expansion and contraction of is the same),
Warpage and distortion of the board do not occur, but if a metal film is formed on one side of the board, for example, which does not absorb or transmit water, the temperature of the acrylic resin on that surface will be slower. Since the other sides are open, they are sensitive and, on the other hand, tension occurs only on one side, and warping and distortion of the board immediately occur. This board sled,
Distortion etc. becomes more severe as the diameter of the deformer increases, and in the case of straight flaws, the warp direction is distorted and the plate is deformed by more than 1 in the thickness direction on dry and rainy days. Furthermore, stress and strain associated with the deformation occur in the deflection, making the polarization angle of the light look complicated. The problem with this plate is that the flatness of the plate surface, which allows focus to follow automatically, has become so large that it has become impossible to focus. , the disk will no longer be able to function as a disk. Also, polarization distortion 4
However, based on the method derived from Motoyori, which is used for the purpose of preserving the media film, a laser beam is dispersed and focused.
This causes noise etc. during J output *) and slows down the supply of uniform discs. .

従ってアクリル樹脂を高密度ディスク記録層基板として
使用する場合には基板として成蓋し*時点から厳重な温
一度管理下におかれ、膜の形成。
Therefore, when acrylic resin is used as a high-density disk recording layer substrate, it is placed under strict temperature control from the time it is applied as a substrate and the film is formed.

Dlscとしての組み立て、動作時、保管時等すべて同
一条件下になければならない。これは、日本の様な高温
多湿、低温乾燥の気候で10年以上の寿命を保証するこ
とは不可能に近い0この問題はガラス基板を使えば郷決
で亀るが、ガラス@杜アクリル樹脂の2倍以上の熱伝導
率をもってシシ、それだけ熱の拡散が早いえめ、記憶厳
体膜にヒートモードで記録させ為には2倍以上の熱が必
要となシそのためにレーず低出力を大−く゛せざ、11
誓得1にら。
It must be under the same conditions during assembly, operation, storage, etc. as a DLSC. It is almost impossible to guarantee a lifespan of more than 10 years in a climate like Japan, which has high temperatures and humidity, and low temperatures and dryness.This problem can be resolved by using a glass substrate, but glass@Mori acrylic resin Since the heat conductivity is more than twice that of the previous one, heat dissipates faster, so more than twice as much heat is required to record on the storage film in heat mode. -Kuseza, 11
1 chive.

そして高出力レーザーを使うと、装置が大−化し調整、
保守寿命等に間−がToI、又高価でもある。
And when a high-power laser is used, the equipment becomes larger and adjustments are required.
It takes a long time (ToI) in terms of maintenance life, etc., and is also expensive.

半導体レーザーが普及して来九現在、ディ□スタ周辺の
小蓋化、高僧−′化は向上してきてお)、−置全体も低
領扁にできるが、ll状の半導体レーず−には高出力を
ださせると、寿命が極端に短かくなってしまう欠点かあ
〉J低出力でしが使え1に%/mため、上述メクラス基
板ディスクのレーず源としては使用できず、どうしても
アクリル樹M*@ディスクを必要とする。
Now that semiconductor lasers have become widespread, the area around the disk has become smaller and more compact. If high output is produced, the service life will be extremely short. Because of the low output and 1%/m, it cannot be used as a laser source for the above-mentioned Meclas board disk, and the acrylic Tree M*@requires disk.

一方、媒体膜として使用する〒唸薄膜にも寿命に対し大
歯な欠点をもっている。それは温気があると簡単に酸化
されてし會い、′七の酸化膜紘透明な丸め、轟初金属色
を%っていたTLaIl1MK%日本の気候で杜半都で
透明な膜となってし重い、記働膜として用をなさなくな
っ□てし會う。我々の加速テスシの結果では70℃;8
1!11BH下で、4時間で透明化が進む。119て水
分を透過す為アタリkI[とTe薄膜との組み食わせは
、ヒートモードle鎌の研究設階で社優れた結果を出し
てV%九が、実用北進には到っていないのが現状である
On the other hand, the thin film used as the media film also has a major drawback in terms of service life. It is easily oxidized in the presence of warm air, and the oxide film of '7' has a transparent round shape and a metallic color.In Japan's climate, it becomes a transparent film. It is heavy and has no use as a recording membrane. According to our accelerated test result, 70℃; 8
Under 1!11BH, transparency progresses in 4 hours. The combination of Atari kI and Te thin film to transmit moisture through 119V%9 produced excellent results at the research facility of the heat mode le sickle, but it has not yet reached the point of practical use. This is the current situation.

本発@紘それらの欠点を診査した。アクリル樹脂基板を
使用し、・10年以上の寿命を保証で龜るに一ト幡−ド
用光記録媒体を提供することを目的とする。
The original @Hiro examined those shortcomings. The purpose of the present invention is to provide an optical recording medium for one-to-one cards that uses an acrylic resin substrate and has a guaranteed lifespan of 10 years or more.

すなわち本発明の光記―厳体は熱伝導率の低い有機樹脂
!!板の両面に、テ5esp(T・)と炭素(C)とを
主成分とする記憶謀体膜を形成し丸ものであ如これによ
って、例えばアクリル樹脂からなる基板のソリ、・歪部
の変形を防止し、かつ記憶媒体朧の酸化を防止すること
かで龜、低出力の半導体レーザを用いた高感度、長寿命
の光記録・読取〉用記鎌媒体の実用化を可能とすゐこと
かで−る。
In other words, the light of the present invention is strictly an organic resin with low thermal conductivity! ! A memory film mainly composed of Te5esp (T) and carbon (C) is formed on both sides of the board, and by this, for example, warping of the board made of acrylic resin, distortion, etc. can be prevented. By preventing deformation and oxidation of the storage medium, it is possible to put into practical use a high-sensitivity, long-life optical recording/reading medium using a low-output semiconductor laser. That's it.

以下図面を参照して本発明の詳細な説明する。The present invention will be described in detail below with reference to the drawings.

第2Iiは本発明の記録媒体の−s麹例を示す断面図で
ある。
2Ii is a sectional view showing an example of -s koji of the recording medium of the present invention.

透明アクリル樹脂基1[(3)の両IIにテにル(テ・
)と炭素(C)とを主成分とした記偉薄膜(4)を形成
し、情報の記録、読み出しは反射率変化を別層して行な
われ、両面の薄膜を媒体膜として使用することを特長と
している。即ち、前述の如く、第1図の構造ではアクリ
ル基板に片面からの水の**UCよる変形が発生するが
、本発−の構造では、アクリル基板の両面が同一材質の
膜でおおわれているため変形線発生しない。但し、その
膜質に厳しい条件が要求され、tず第1に耐候性特に耐
湿潤性に優れている事でTI3)、第2 KTe薄膜と
同1度の反射率をもち、かつ同1度のレーザーパフ−で
情報を書き込め1事である。この両者を満尼する薄膜を
探究した結果、我々はT・とCとを主成分とした薄膜が
これらの条件をsuiする仁とを見つけ出しえ。この薄
膜はメタン(cH4)ガス中でのT・のスパツタリング
による、いわゆる反応性スバ、Jlリングで形成する。
Transparent acrylic resin group 1 [(3)
) and carbon (C) as the main components, recording and reading of information is performed using separate layers with different reflectances, and the thin films on both sides can be used as media films. It is a feature. That is, as mentioned above, in the structure shown in Fig. 1, the acrylic substrate is deformed by water **UC from one side, but in the structure of this invention, both sides of the acrylic substrate are covered with a film of the same material. Therefore, deformation lines will not occur. However, strict conditions are required for the film quality, and the first thing is that it has excellent weather resistance, especially moisture resistance, and the second is that it has a reflectance of 1 degree, which is the same as that of the KTe thin film, and has a reflectance of 1 degree. All you have to do is write information with a laser puff. As a result of searching for a thin film that satisfies both of these conditions, we found that a thin film containing T and C as main components satisfies these conditions. This thin film is formed by sputtering T· in methane (cH4) gas, so-called reactive sputtering, Jl ring.

膜質は一晶質であ〉、膜はTe、C。The film quality is monocrystalline, and the film is made of Te and C.

H,Oとからl)立ってお〕、主成分はTIとCとでh
る・又、 TIに比べ基カシ色に1&るが、半導体シー
ず−の波長域である800m近辺では嫌ぼ同一の反射率
をもっている。
h), the main components are TI and C
Also, although it has a base color of 1/2 compared to TI, it has almost the same reflectance in the vicinity of 800 m, which is the wavelength range of semiconductor seeds.

この薄膜は耐湿潤性が極めて嵐好である0例えば、加速
テストとしてTo’o、tssiiiの雰囲気を遥ぶと
、T・馬では4時間で酸化されてしまい実用に供電なく
なるが、上記?@−〇llは30日以上えっても何ら変
化を示さず単純計算でもテ・膜の1110倍の耐II性
があることがわか′つた。テ・馬の耐1lII性を半年
とすると、とのTI−C薄膜は110年もの耐amをも
つヒとになる。この結果から上述の第1の条件を十分K
11足すると判御できる。次に嬉3の条件で−4書き込
み感度も、ディスクの廖−mにしで評備しえ結果!@膜
並みの感度が得られることがわかった・ ヒート峰−ド記鍮故、感度はシーず−の照射パ9−と照
射時間の積で表わされるが、−例をあげれば、膜面上で
−Kk為亭導体レーシーを200m5照射すれば、T・
膜、T・−C膜共に予定通〉所望の穴が形成され、情報
を配−で龜s O,smWで十分ない比をもつ読み出し
出力が得られる。
This thin film has extremely good moisture resistance. For example, when exposed to the atmosphere of To'o and Tssiii as an accelerated test, it oxidizes in 4 hours in To'o and Tssiii, making it no longer practical to supply electricity. @-〇ll showed no change even after 30 days or more, and simple calculations showed that it had 1110 times the II resistance of the TE film. If the 1lII resistance of Te-uma is assumed to be half a year, the TI-C thin film of TE-MA has an AM resistance of 110 years. From this result, the first condition mentioned above is satisfied by K
You can figure it out by adding 11. Next, under the conditions of 3, the -4 write sensitivity was also evaluated at the disc's length! It was found that a sensitivity comparable to that of a film can be obtained. Due to the heat peak, the sensitivity is expressed as the product of the irradiation time of the sheet and the irradiation time. So, if you irradiate 200m5 of Kk Tamitei conductor Lacey, T.
Desired holes are formed in both the membrane and the T/-C membrane as planned, and a readout output with a sufficient ratio can be obtained by distributing the information.

テe−C膜がヒの橡な優れ九特性をもつ理由社、メタン
ガス中のスパツタリングでメナル基が@性化してラジカ
ルとな)、チーイオンと屓応してあたかも有機金属のよ
゛うなネツトワークを作)上けて膜となるためと推定さ
れる。この丸め、蒙化過寝が従来の金属とは1に9九〈
異な9え、もしろ酸化など有〉得ない構造となってい為
ので、耐候性に優れ、かクメチル基は照射光に対し何ら
作用しないので、テ・馬並みの感度をもつ仁とが幽鬼る
ものと考えられる。lLsて、従来のディメタ構造はサ
ンドウィッチ蓋が主体であるが、本発明のディスク構造
は第3図に示す如く一枚板の単純な構造とすることがで
きる・こζで、第3図にシーで(3)祉基板、(4)は
媒体膜、(5)はディスクの中心穴である。
The reason why the Tee-C film has such outstanding properties is that when sputtering in methane gas, the menal group changes to @ and becomes a radical), and reacts with Chi ions to create a network that looks like an organic metal. This is presumed to be due to the formation of a film. This rounding and oversizing is 1 to 99 times smaller than that of conventional metals.
On the other hand, since it has a structure in which oxidation is impossible, it has excellent weather resistance, and the methyl group does not have any effect on irradiated light, so it is said that it has a sensitivity similar to that of Teuma. considered to be a thing. lLs, the conventional Demeta structure is mainly composed of a sandwich lid, but the disc structure of the present invention can be made into a simple structure of a single plate as shown in Fig. 3. (3) is the substrate, (4) is the medium film, and (5) is the center hole of the disk.

本図かられかる如く本発明のディスタは貴意工IIK向
いた最も単純な構造となっている。
As can be seen from this figure, the distal device of the present invention has the simplest structure suitable for use in industrial engineering IIK.

以上説明しえ如く、アクリル樹脂基板の両WにTI−C
IQ鎌媒゛体膜を形成することによ〉、ヒート毫−ド記
借用媒体の長寿命化に成功し九〇しかもディスク構造に
した鳩舎、最も単純な構造となるえめ貴意に向自安儒に
供給で自る。叉、中導体シーず−を使える丸め、装置金
体も小量化でき、信m性も大巾に向上し光記鍮装置を実
用化するヒとが可能となった。
As explained above, TI-C is applied to both Ws of the acrylic resin board.
By forming a body film on the IQ sickle medium, we succeeded in extending the lifespan of the heat disk storage medium.90 Moreover, the pigeonhole was made into a disk structure, and it became the simplest structure, making it suitable for self-sustainability. self-sufficient supply. In addition, it was possible to use rounded conductor sheaths, reduce the size of the metal body of the device, greatly improve reliability, and make it possible to put optical recording devices into practical use.

&&、ディスクの取)扱い上、指紋、ゴミ等がWiK′
)自生す−ので、その保膿のえめに謀体属上に保■膜勢
を形成させてもよい。
&&, due to handling of the disc, fingerprints, dust, etc.
) Since it grows naturally, a membrane may be formed on the genus in order to preserve its suppurative function.

又、実施例で拡基板としてアクリル樹脂をあげ。In addition, acrylic resin was used as the expansion substrate in the examples.

て説明し九が、熱伝導率がI X 1G−”cat/s
・C以下の他の有機物基板、例えば塩ビ、酢ビ、ポリス
チレン等の基板で4h現象は岡であゐ、更にテe−C膜
の形成法としてメタンガス中の反応性スパッタ法をあげ
九が、他のガス、例えばエタン、プロパン、エチレン、
ア、−にチレン等のガスを用いる仁と亀て自、また他の
方法、例えば、グツズ啼重舎岬を用いることもで自る。
9, the thermal conductivity is I x 1G-"cat/s
- The 4-hour phenomenon is possible with other organic substrates of C or lower, such as vinyl chloride, vinyl acetate, polystyrene, etc. Furthermore, reactive sputtering in methane gas is cited as a method for forming the e-C film. other gases such as ethane, propane, ethylene,
A. It is also possible to use a gas such as tyrene or other methods, such as using a gas such as tyrene.

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

第1図は従来の光記鍮謀体の一画図、第j!図は本発明
の一実施例を示す一画図、第sIiは本発明の光記録媒
体をディスタ形状に構成し丸機会の断面図であ°る。 (3)・・・アクリル基板、 (4)・・・Te−C記鍮媒体属。 (5)・・・ディスク中心式。 第1図 1s 2 図 第8図
Figure 1 is a diagram of a conventional Koki Brass plot, No. J! The figure is a one-stroke diagram showing one embodiment of the present invention, and sIi is a cross-sectional view of a round frame in which the optical recording medium of the present invention is configured in a disk shape. (3)...Acrylic substrate, (4)...Te-C recording medium. (5)... Disk center type. Figure 1 1s 2 Figure 8

Claims (1)

【特許請求の範囲】 (五)低熱伝導率を有する有機樹脂基板と、この基板の
両−に形成されたテルル及び炭素を主成分とする記憶薄
膜とを偏見1.前記記像媒体膜にエネルギービームを照
射して一記、記憶媒体属を変質、変形もしくは蒸発させ
て情報をl!鍮するようにし九ことを特徴と、する光l
!鍮媒体@、。 (2)有機樹脂基板は、IXIF”C麿1/@@@以下
の熱伝導率を有するヒとを特徴とする特許請求の範鴎第
1項記載の光記録媒体。、・ 、   。 (3)有機樹゛・11!!板は、アクリ・ル、樹脂基板
であるしとt特徴とする特許請求の範囲第1項記載の光
記録媒体。 (4)記憶薄属祉テルル、炭素、水素、−素を含むもの
であることを41111とする特許請求の範−111項
記載の光記録媒体0     。
[Claims] (5) Prejudice between an organic resin substrate having low thermal conductivity and a memory thin film mainly composed of tellurium and carbon formed on both sides of this substrate.1. The recording medium film is irradiated with an energy beam to alter, deform, or evaporate the storage medium to transfer information. Features nine features, such as brass, and a light
! Brass medium @,. (2) The optical recording medium according to claim 1, wherein the organic resin substrate is a metal having a thermal conductivity of less than or equal to 1/@@@. ) The optical recording medium according to claim 1, characterized in that the organic tree 11!! board is an acrylic or resin substrate. (4) Memory thin metals such as tellurium, carbon, and hydrogen 41111. Optical recording medium 0 according to claim 111, wherein the optical recording medium 0 contains a -element.
JP56105458A 1981-07-08 1981-07-08 Optical recording medium Pending JPS589229A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56105458A JPS589229A (en) 1981-07-08 1981-07-08 Optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56105458A JPS589229A (en) 1981-07-08 1981-07-08 Optical recording medium

Publications (1)

Publication Number Publication Date
JPS589229A true JPS589229A (en) 1983-01-19

Family

ID=14408133

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56105458A Pending JPS589229A (en) 1981-07-08 1981-07-08 Optical recording medium

Country Status (1)

Country Link
JP (1) JPS589229A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59160841A (en) * 1983-03-04 1984-09-11 Toshiba Corp Optical recording medium film

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5627395A (en) * 1979-08-14 1981-03-17 Nippon Telegr & Teleph Corp <Ntt> Recording medium and preparation thereof
JPS5662192A (en) * 1979-10-29 1981-05-27 Nippon Telegr & Teleph Corp <Ntt> Medium for optical recording use and preparation thereof

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5627395A (en) * 1979-08-14 1981-03-17 Nippon Telegr & Teleph Corp <Ntt> Recording medium and preparation thereof
JPS5662192A (en) * 1979-10-29 1981-05-27 Nippon Telegr & Teleph Corp <Ntt> Medium for optical recording use and preparation thereof

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59160841A (en) * 1983-03-04 1984-09-11 Toshiba Corp Optical recording medium film
JPH0441056B2 (en) * 1983-03-04 1992-07-07 Tokyo Shibaura Electric Co

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