JPH0259526B2 - - Google Patents

Info

Publication number
JPH0259526B2
JPH0259526B2 JP59076256A JP7625684A JPH0259526B2 JP H0259526 B2 JPH0259526 B2 JP H0259526B2 JP 59076256 A JP59076256 A JP 59076256A JP 7625684 A JP7625684 A JP 7625684A JP H0259526 B2 JPH0259526 B2 JP H0259526B2
Authority
JP
Japan
Prior art keywords
recording medium
information recording
optical information
disk
thin film
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
JP59076256A
Other languages
Japanese (ja)
Other versions
JPS60219645A (en
Inventor
Teruo Kobayashi
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.)
Nippon Columbia Co Ltd
Original Assignee
Nippon Columbia 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 Columbia Co Ltd filed Critical Nippon Columbia Co Ltd
Priority to JP59076256A priority Critical patent/JPS60219645A/en
Publication of JPS60219645A publication Critical patent/JPS60219645A/en
Publication of JPH0259526B2 publication Critical patent/JPH0259526B2/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
    • 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
    • G11B7/26Apparatus or processes specially adapted for the manufacture of record carriers

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Thermal Transfer Or Thermal Recording In General (AREA)
  • Non-Silver Salt Photosensitive Materials And Non-Silver Salt Photography (AREA)
  • Optical Record Carriers And Manufacture Thereof (AREA)
  • Manufacturing Optical Record Carriers (AREA)

Description

【発明の詳細な説明】 本発明は光ビームを用いて情報が記録される光
情報記録媒体に関し、特に円盤状記録媒体であつ
て内周から外周にかけて徐々に記録感度を高くし
た光情報記録媒体に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical information recording medium in which information is recorded using a light beam, and in particular to an optical information recording medium that is a disk-shaped recording medium and has recording sensitivity gradually increased from the inner circumference to the outer circumference. It is related to.

光情報記録媒体としてはTe合金薄膜や色素薄
膜を用いた穿孔型記録媒体と非晶質−結晶質転移
や磁区反転を利用した濃淡型記録媒体が知られて
いるが、いずれの媒体も情報を記録するに要する
光エネルギーは媒体上のいかなる位置においても
一定である。光情報記録媒体が円盤状であり、こ
の媒体を角速度一定で回転させ情報を記録再生す
る場合、外周における線速度は内周における線速
度よりも大であるため情報を記録するに必要な光
エネルギーは外周になるに従つて大きくなる。一
般には記録エネルギーを内周から外周へ徐々に大
きくして均一な記録を行わねばならず、情報記録
位置に応じて光エネルギーを変化させる必要があ
つた。
As optical information recording media, there are perforated recording media that use Te alloy thin films or dye thin films, and density type recording media that utilize amorphous-crystalline transition or magnetic domain reversal, but both media are difficult to store information. The light energy required to record is constant at any location on the medium. When an optical information recording medium is disk-shaped and information is recorded and reproduced by rotating the medium at a constant angular velocity, the linear velocity at the outer circumference is higher than that at the inner circumference, so the optical energy required to record the information is becomes larger toward the outer periphery. Generally, it is necessary to gradually increase the recording energy from the inner circumference to the outer circumference to perform uniform recording, and it is necessary to change the optical energy depending on the information recording position.

本発明はこの様な欠点を改良する為になされた
もので、角速度一定で回転する円盤状光情報記録
媒体に情報を記録する時、従来の様に情報記録位
置に応じて光エネルギーを変化させなくても均一
な記録ができる光情報記録媒体を提供することを
目的とするものである。
The present invention has been made to improve these drawbacks, and when recording information on a disc-shaped optical information recording medium that rotates at a constant angular velocity, it is not possible to change the optical energy according to the information recording position as in the conventional method. The object of the present invention is to provide an optical information recording medium on which uniform recording can be performed even without the use of an optical information recording medium.

この為本発明は、円盤状記録媒体の記録薄膜と
して本出願人が概に昭和59年4月16日付で「光情
報記録媒体」として提案したGe1-xSnxTe(0<x
≦0.7)合金を主成分とする薄膜を用いるもので、
その特徴は上記円盤状記録媒体の内周から外周に
かけて徐々に上記xの値を増加させたことにあ
る。
Therefore, the present invention utilizes Ge 1-x Sn x Te (0<x
≦0.7) It uses a thin film whose main component is an alloy.
The feature lies in that the value of x gradually increases from the inner circumference to the outer circumference of the disc-shaped recording medium.

以下、本発明を実施例にしたがつて詳細に説明
する。
Hereinafter, the present invention will be explained in detail based on examples.

第1図は本発明による光情報記録媒体を製造す
る装置の一例を示したものである。真空チヤンバ
ー11の中に回転する基板ホルダー12が設けら
れており、円盤状基板13は該基板ホルダー12
の下方に取り付けられる。該円盤状基板13の中
心軸直下で距離H1の位置に第1の蒸発源14が
置かれ、GeTeを蒸発させるのに使用する。蒸発
源14からのGeTe蒸発量は電源16の出力を変
化させて制御する。第2の蒸発源15は第1の蒸
発源14から水平に距離Lの位置に置かれSnTe
を蒸発させるのに使用する。蒸発源15からの
SnTe蒸発量は電源17の出力を変化させて制御
する。
FIG. 1 shows an example of an apparatus for manufacturing an optical information recording medium according to the present invention. A rotating substrate holder 12 is provided in the vacuum chamber 11, and a disk-shaped substrate 13 is mounted on the substrate holder 12.
It is installed below the . A first evaporation source 14 is placed at a distance H 1 directly below the central axis of the disk-shaped substrate 13 and is used to evaporate GeTe. The amount of GeTe evaporated from the evaporation source 14 is controlled by changing the output of the power source 16. The second evaporation source 15 is placed horizontally at a distance L from the first evaporation source 14 and is made of SnTe.
used to evaporate. from evaporation source 15
The amount of SnTe evaporated is controlled by changing the output of the power source 17.

以上の様な構成において、蒸発源14から蒸発
したGeTe粒子の基板13への飛来量は基板13
の中心部で大であり外周部へと徐々に小さくな
る。内周部と外周部におけるGeTe粒子飛来量の
比は距離H1を変えることにより所望の値に調整
することができ、H1を大とすると外周部の内周
部に対する飛来GeTe粒子比R1は1に近ずく。逆
にH1を小とするとR1は1から遠ざかる。同様に
蒸発源15から蒸発したSnTe粒子の基板13へ
の飛来量はL及びH2を変化させると外周部で大
きく内周部で小さくすることができる。そして
H1,H2,L及び電源16および17の出力を適
切な値を選ぶと、円盤状基板13には、膜厚は内
周部と外周部で等しいGe1-xSnxTe合金薄膜が得
られ、その組成は内周部から外周部にかけてxが
連続的に増加した合金薄膜が得られる。
In the above configuration, the amount of GeTe particles evaporated from the evaporation source 14 flying to the substrate 13 is
It is large at the center and gradually decreases towards the periphery. The ratio of the amount of flying GeTe particles at the inner and outer peripheries can be adjusted to a desired value by changing the distance H 1. If H 1 is increased, the ratio of the GeTe particles at the outer periphery to the inner periphery increases . approaches 1. Conversely, if H 1 is made small, R 1 moves away from 1. Similarly, the amount of SnTe particles evaporated from the evaporation source 15 arriving at the substrate 13 can be made larger at the outer periphery and smaller at the inner periphery by changing L and H 2 . and
By selecting appropriate values for H 1 , H 2 , L and the outputs of the power supplies 16 and 17, a Ge 1-x Sn x Te alloy thin film is formed on the disc-shaped substrate 13 with the same film thickness on the inner and outer peripheries. As a result, an alloy thin film having a composition in which x continuously increases from the inner circumference to the outer circumference is obtained.

ここで、本出願人が昭和59年4月16日付で「光
情報記録媒体」として提案した前記出願で用いら
れるGe1-xSnxTe合金薄膜は、第2図に示される
ごとくxの値が増加するにしたがつて曲線21の
様に転移点の温度が下降し、曲線22の様に情報
を記録するに必要な光エネルギーが減少する。従
つて上述の如き構造を有する円盤状光情報記録媒
体では内周部から外周部へと連続的に小さい光エ
ネルギーで情報を記録することができる。したが
つて上述の様にして得られた光情報記録媒体を一
定角速度で回転させて情報を記録する時、従来の
様に情報を記録する位置に応じて光エネルギーを
変化させなくても、該媒体上にどの位置にも均一
に情報を記録することが可能である。
Here, the Ge 1-x Sn x Te alloy thin film used in the aforementioned application, which was proposed by the present applicant as an "optical information recording medium" dated April 16, 1980, has a value of x as shown in FIG. As the temperature increases, the temperature at the transition point decreases as shown by curve 21, and the light energy required to record information decreases as shown by curve 22. Therefore, in the disc-shaped optical information recording medium having the above-described structure, information can be recorded continuously from the inner circumference to the outer circumference with small optical energy. Therefore, when recording information by rotating the optical information recording medium obtained as described above at a constant angular velocity, the optical information recording medium obtained as described above can be rotated at a constant angular velocity to record information without changing the optical energy depending on the position where information is recorded as in the past. It is possible to record information uniformly at any position on the medium.

なお通常xの値は0と0.7の間にするが、この
理由はx>0.7のとき第2図曲線21に示す様に
Ge1-xSnxTe合金薄膜の非晶質−結晶質転移点が
室温付近となり情報を記録する前に転移してしま
うことがあるからである。従つて、もつと高温の
還境で使用する場合はxの値の最大値をさらに低
下させる必要がある。円盤状記録媒体において情
報を記録する領域の内径をr1、外径をr2とすると
一般にr2/r1=2となるよう選択され、内外周に
おける媒体の回転時の線速比はr2/r1に比例し、
情報を記録するに必要なエネルギー比は√2 1
〜r2/r1の範囲の値になる。したがつて第2図に
より、記録光エネルギーの比が1.4〜2となるよ
うに、xの値を内周で小さく外周で大きくなるよ
う選択すればよい。例えば内周部でx=0.1のと
き外周部でx=0.4〜0.6とするのが適当である。
xの値は上記r2/r1=2のとき内周部でx=0〜
0.25、外周部でx=0.3〜0.7で選ぶことができる。
The value of x is usually between 0 and 0.7, but the reason for this is that when x > 0.7, as shown in curve 21 in Figure 2,
This is because the amorphous-crystalline transition point of the Ge 1-x Sn x Te alloy thin film is near room temperature, and the transition may occur before information is recorded. Therefore, when used in a high-temperature ambient environment, it is necessary to further reduce the maximum value of x. If the inner diameter of the area for recording information in a disc-shaped recording medium is r 1 and the outer diameter is r 2 , it is generally selected so that r 2 /r 1 = 2, and the linear velocity ratio during rotation of the medium at the inner and outer peripheries is r Proportional to 2 /r 1 ,
The energy ratio required to record information is √ 2 1
The value will be in the range ~r 2 /r 1 . Therefore, as shown in FIG. 2, the value of x may be selected to be small at the inner circumference and large at the outer circumference so that the ratio of recording light energy is 1.4 to 2. For example, when x=0.1 at the inner circumference, it is appropriate that x=0.4 to 0.6 at the outer circumference.
The value of x is from x=0 to the inner circumference when r 2 /r 1 = 2 above.
0.25, x can be selected from 0.3 to 0.7 at the outer periphery.

なお蒸発源14および蒸発源15は抵抗加熱式
蒸発源、電子ビーム加熱式蒸発源のいずれも用い
ることができる。又、記録薄膜作製法は本実施例
に示した真空蒸発法に限定することなくスパツタ
リング法によることもでき、この場合粒子の発生
源として第1図の蒸発源の位置にターゲツトを置
き換えるだけで良い。この場合、粒子発生源はタ
ーンテーブルの下方に限るものではなく、例えば
第1図の位置関係をさかさまにして、ターンテー
ブルの上方にしてもよく、又横倒し状態にしてタ
ーンテーブルの横にしてもよいことは勿論であ
る。
Note that the evaporation source 14 and the evaporation source 15 can be either a resistance heating type evaporation source or an electron beam heating type evaporation source. Furthermore, the recording thin film manufacturing method is not limited to the vacuum evaporation method shown in this example, but may also be a sputtering method, in which case it is sufficient to simply replace the target at the position of the evaporation source shown in Figure 1 as the source of particle generation. . In this case, the particle generation source is not limited to being below the turntable; for example, it may be placed above the turntable by turning the positional relationship shown in Figure 1 upside down, or it may be placed sideways to the side of the turntable. Of course, this is a good thing.

以上述べたように、本発明による円盤状光記録
媒体においては、内周から外周になるに従い連続
的に記録感度が高くなつているので、情報を記録
するに必要なエネルギーは外周になるにしたがつ
て小さくて良いので、媒体上のどの位置にも均一
に情報を記録することが可能である。
As described above, in the disc-shaped optical recording medium according to the present invention, the recording sensitivity increases continuously from the inner circumference to the outer circumference, so that the energy required to record information decreases from the outer circumference. Since it is small in size, it is possible to record information uniformly at any position on the medium.

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

第1図本発明の光情報記録媒体を製造する装置
の一例であり、第2図は本発明の光情報記録媒体
記録膜組成と記録光エネルギーの関係を示す図で
ある。 12……ターンテーブル、13……光情報記録
媒体、14,15……蒸発源。
FIG. 1 is an example of an apparatus for manufacturing the optical information recording medium of the present invention, and FIG. 2 is a diagram showing the relationship between the recording film composition of the optical information recording medium of the present invention and the recording light energy. 12... Turntable, 13... Optical information recording medium, 14, 15... Evaporation source.

Claims (1)

【特許請求の範囲】 1 基体と該基体上に形成された薄膜を有し、該
薄膜へ光ビームを照射し情報を記録する円盤状光
情報記録媒体において、上記薄膜をGe1-xSnxTe
(0<x≦0.7)なる組成の合金膜を主成分とする
薄膜とし、上記円盤状光情報記録媒体の内周から
外周に向けて、上記合金膜のxの値を徐々に増加
させたことを特徴とする光情報記録媒体。 2 デイスクを回転させるターンテーブルと、該
ターンテーブルの回転軸の延長線上で上記ターン
テーブルのデイスク装着面に対向する位置に
GeTe粒子の発生源を設け、上記延長線から外れ
て上記デイスク装着面に対向する位置にSnTe粒
子の発生源を設けた光情報記録媒体の製造装置。
[Scope of Claims] 1. A disk-shaped optical information recording medium that has a base and a thin film formed on the base and records information by irradiating the thin film with a light beam, the thin film being Ge 1-x Sn x Te
(0<x≦0.7), and the value of x of the alloy film is gradually increased from the inner circumference to the outer circumference of the disk-shaped optical information recording medium. An optical information recording medium characterized by: 2. A turntable that rotates a disk, and a position facing the disk mounting surface of the turntable on an extension of the rotation axis of the turntable.
An apparatus for producing an optical information recording medium, wherein a GeTe particle generation source is provided, and a SnTe particle generation source is provided at a position away from the extension line and facing the disk mounting surface.
JP59076256A 1984-04-16 1984-04-16 Optical information recording medium and its manufacture Granted JPS60219645A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59076256A JPS60219645A (en) 1984-04-16 1984-04-16 Optical information recording medium and its manufacture

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59076256A JPS60219645A (en) 1984-04-16 1984-04-16 Optical information recording medium and its manufacture

Publications (2)

Publication Number Publication Date
JPS60219645A JPS60219645A (en) 1985-11-02
JPH0259526B2 true JPH0259526B2 (en) 1990-12-12

Family

ID=13600121

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59076256A Granted JPS60219645A (en) 1984-04-16 1984-04-16 Optical information recording medium and its manufacture

Country Status (1)

Country Link
JP (1) JPS60219645A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61243966A (en) * 1985-04-22 1986-10-30 Matsushita Electric Ind Co Ltd Optical information carrier disk
JP2674837B2 (en) * 1989-07-19 1997-11-12 日本電気株式会社 Phase change optical disk

Also Published As

Publication number Publication date
JPS60219645A (en) 1985-11-02

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