JPS6025278B2 - optical information recording medium - Google Patents

optical information recording medium

Info

Publication number
JPS6025278B2
JPS6025278B2 JP56169884A JP16988481A JPS6025278B2 JP S6025278 B2 JPS6025278 B2 JP S6025278B2 JP 56169884 A JP56169884 A JP 56169884A JP 16988481 A JP16988481 A JP 16988481A JP S6025278 B2 JPS6025278 B2 JP S6025278B2
Authority
JP
Japan
Prior art keywords
film
recording
recording film
recording medium
optical information
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
Application number
JP56169884A
Other languages
Japanese (ja)
Other versions
JPS5871193A (en
Inventor
正夫 真下
修朗 安田
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
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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP56169884A priority Critical patent/JPS6025278B2/en
Publication of JPS5871193A publication Critical patent/JPS5871193A/en
Publication of JPS6025278B2 publication Critical patent/JPS6025278B2/en
Expired 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
    • G11B7/242Record 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
    • G11B2007/2431Metals or metalloids group 13 elements (B, Al, Ga, In)
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/242Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
    • G11B7/243Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
    • G11B2007/24302Metals or metalloids
    • G11B2007/24312Metals or metalloids group 14 elements (e.g. Si, Ge, Sn)
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/242Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
    • G11B7/243Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
    • G11B2007/24302Metals or metalloids
    • G11B2007/24316Metals 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
    • 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

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】 本発明は、記録された情報を光学的に議取り可能な光学
的情報記録媒体に係り、特に光熱等のエネルギービーム
の照射により記録膜に孔または凹部が形成されることに
よって情報を記録するようにした光学的情報記録媒体に
関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical information recording medium in which recorded information can be optically exchanged, and in particular, holes or recesses are formed in a recording film by irradiation with an energy beam such as light or heat. The present invention relates to an optical information recording medium on which information is recorded by.

光学的情報記録媒体として、従来、基板上に形成された
記録膜にエネルギービームを照射し、記録されるべき情
報に対応したビット列を形成するようにしたものがある
2. Description of the Related Art Conventionally, there is an optical information recording medium in which a recording film formed on a substrate is irradiated with an energy beam to form a bit string corresponding to information to be recorded.

このような光学的情報記録媒体において、従来より記録
膜としてテルルTeを使用することが知られている。T
e膜は非常に低いエネルギーで所望の孔(ビット)を形
成でき、この蟹の用途においては高感度材料として極め
て有望である。ここで感豚とは、単位面積当りの記録部
(この場合はビット)形成に要するエネルギー(mJ/
の)で定義される。しかしながらTeは大気中に放置さ
れた場合、酸素や水分により酸化され、透明になる度合
が速い。
In such optical information recording media, it has been known to use tellurium Te as a recording film. T
The e-membrane can form desired holes (bits) with very low energy, making it extremely promising as a highly sensitive material in this crab application. Here, incubation refers to the energy (mJ/
) defined in ). However, when Te is left in the atmosphere, it is oxidized by oxygen and moisture and quickly becomes transparent.

記録膜として使用する場合、膜厚は700A程度と極め
て薄いため、膜の酸化で生じた透明度の増加に起因する
感度の劣化は著しい。すなわち、膜が酸化されると、融
解、蒸発温度が上昇するとともに、透明化により光等の
エネルギーの吸収が少なくなるため、ビット形成に要す
るエネルギーが大きくなり、感度の劣化を釆たす。例え
ば温度7ぴ○、相対湿度85%の雰囲気に放燈した場合
、約5時間で感渡が約20%低下し、約15時間で約5
0%低下してしまう。
When used as a recording film, the film thickness is extremely thin, about 700 Å, so the sensitivity deteriorates significantly due to increased transparency caused by oxidation of the film. That is, when the film is oxidized, the melting and evaporation temperatures rise, and absorption of energy such as light decreases due to transparency, which increases the energy required to form bits, resulting in deterioration of sensitivity. For example, if you light up an atmosphere with a temperature of 7 pm and a relative humidity of 85%, the sensitivity will drop by about 20% in about 5 hours, and about 50% in about 15 hours.
It will decrease by 0%.

このため、Te膜の酸化防止のために種々の対策がとら
れている。その一つである安定無機物質でTe膜をコー
プィングする方法は、Te膜の酸化防止には有効である
が、感度を低下させてしまうことと高価であることのた
め、実用化されていない。一方、プラスチックコーティ
ングは熱伝導率が小さいことから感度を損なう度合が小
さく有利であるが、酸素や水を比較的容易に透過させる
ため、Te膜の酸化防止にはあまり役立たない。また、
このような光学的情報記録媒体には、高密度で大容量の
記録が要求されるようになっており、そのため1.5〜
2仏のピッチで記録トラックを形成させる必要がある。
For this reason, various measures have been taken to prevent oxidation of the Te film. One of these methods, a method of coating the Te film with a stable inorganic substance, is effective in preventing oxidation of the Te film, but it has not been put to practical use because it reduces sensitivity and is expensive. . On the other hand, plastic coatings have a low thermal conductivity and are therefore advantageous in that they do not impair sensitivity to a small extent, but they allow oxygen and water to permeate through them relatively easily, so they are not very useful in preventing oxidation of the Te film. Also,
Such optical information recording media are required to have high-density and large-capacity recording, and therefore
It is necessary to form recording tracks at a pitch of 2 degrees.

その場合記録、再生時のトラッキングを容易とするため
、ガラス仮に写真員虫刻法により溝を設けたものを豚盤
としてアクリル板にトラッキング用簿を転写する方法が
とられていたが、トラッキング用溝の精度とコスト面で
問題があった。本発明は上記問題を解決するためになさ
れたもので、高感度の長寿命であって、しかもトラツキ
ング用パターンを精度よく簡単に形成できる光学的情報
記録媒体を提供することを目的とする。
In this case, in order to facilitate tracking during recording and playback, a method was used in which a piece of glass with grooves formed using the photographer's engraving method was used as a pig board, and the tracking book was transferred onto an acrylic board. There were problems with groove accuracy and cost. The present invention has been made to solve the above problems, and an object of the present invention is to provide an optical information recording medium with high sensitivity and long life, and in which a tracking pattern can be easily formed with high accuracy.

本発明に係る光学的情報記録媒体は、特に基板上に被着
された記録膜にエネルギービームの照射により情報を孔
もし〈は凹部として記録するものであって、記録膜を低
葛史点金属またはその合金とCおよび日を含有する膜に
よって形成し、さらにこの記録膜に記録トラックに沿っ
て光反射率が周囲より高いトラッキング用パターンを予
め形成するようにしたことを特徴としており、これによ
って高感度、長寿命かつ低ノイズの長所を兼ね備えると
ともに、トラッキングを容易とし、さらに低コスト化を
図ったものである。ここで低融点金属としては、膜形成
技術および記録特性から25〜600qoの融点をもつ
金属が用いられる。このような低融的金属としては、例
えばCd,ln,Sn,Zn,Pb,Bi,Te等があ
る。これらの金属を単体で用いてもよいが、それらの合
金を用いることもできる。すなわち、本発明は上記記録
膜に比較的低エネルギーのエネルギービームを照射する
と高い光反射率が得られることを利用して、トラッキン
グ用パターンを形成し、さらにより高いエネルギーのエ
ネルギービームを照擬すると孔または凹部ができて、逆
に光反射率が低くなることを利用して情報の記録を行な
うものである。
The optical information recording medium according to the present invention records information in the form of holes or recesses by irradiating a recording film deposited on a substrate with an energy beam, and the recording film is formed of a metal with a low friction point. The recording film is formed by a film containing carbon or an alloy thereof, and a tracking pattern having a higher light reflectance than the surrounding area is formed along the recording track in advance. In addition to having the advantages of high sensitivity, long life, and low noise, it also facilitates tracking and is designed to reduce costs. Here, as the low melting point metal, a metal having a melting point of 25 to 600 qo is used due to film forming technology and recording characteristics. Examples of such low-melting metals include Cd, ln, Sn, Zn, Pb, Bi, and Te. These metals may be used alone, but alloys thereof may also be used. That is, the present invention utilizes the fact that a high light reflectance can be obtained when the recording film is irradiated with a relatively low-energy energy beam, and forms a tracking pattern, and further irradiates the recording film with a higher-energy energy beam. Information is recorded by utilizing the fact that holes or recesses are formed and the light reflectance is reduced.

以下、図面を参照しながら本発明の実施例を詳細に説明
する。
Embodiments of the present invention will be described in detail below with reference to the drawings.

第1図は本発明の一実施例を示す断面図である。FIG. 1 is a sectional view showing an embodiment of the present invention.

図において、11は基板で本実施例では合成樹脂の1つ
であるアクリル板を用いるものとする。しかし他の合成
樹脂板またはガラス板であってもよく、情報の記録およ
び読み取り方法によって適宜選択することが可能である
。そしてこの基板11上にCおよび日を含む低融点金属
膜からなる記録膜12が形成される。この記録膜12の
膜厚は十分な光反射率が得られる程度に厚く、かつ感度
を損なわない程度に薄いことが必要であり、200A〜
lAm程度が適当である。例えば低融点金属としてTe
膜を選んだ場合、記録膜12はTeを夕−ゲットとして
Cおよび日を含むガス、例えばメタン(CH4)とアル
ゴン(〜)との混合ガス中でスパッタリングすることに
より得られる。
In the figure, reference numeral 11 denotes a substrate, and in this embodiment, an acrylic plate, which is one of synthetic resins, is used. However, other synthetic resin plates or glass plates may also be used, and can be appropriately selected depending on the information recording and reading method. Then, a recording film 12 made of a low melting point metal film containing C and hydrogen is formed on this substrate 11. The thickness of this recording film 12 must be thick enough to obtain sufficient light reflectance and thin enough not to impair sensitivity.
Approximately 1Am is appropriate. For example, Te as a low melting point metal.
When a film is selected, the recording film 12 is obtained by sputtering Te as a target in a gas containing C and hydrogen, for example, a mixed gas of methane (CH4) and argon (~).

ここでTe膜中のC,日の含有量はCH4と〜との混合
比および印加高周波電力により自由に制御でき、例えば
CH4/Ar=1の浪合比で約0.3W/係の高周波(
13.58MHZ)電力をTeターゲットと基板1 1
との間に印加すると、Teに対して原子数比で0.2の
Cを含有した膜を形成することができる。この場合、膜
の組成式はTe,−丈x(H)と書き表わすことができ
、膜が化学的に最も安定する日の含有量はxによって決
まる。ここでは膜中に水素ガス(日2)が発生するほど
多量に含有させない限り、H含有量は任意に選ぶことが
できる。さらに膜厚はスパッタリング時間に比例するの
で、自由に制御できる。記録膜12の光学定数は膜組成
によって決まり、上記の実施例では約700Aの膜厚で
反射率が50%と最大となり、記録特性が最良となった
。また、この条件で作成した記録膜12は非晶値であり
、多結晶Te膜に比べて記録状態の孔または凹部周辺エ
ッヂ部が滑らかとなり、情報再生時の/イズレベルを低
くおさえることができる。本発明者は、上述したCおよ
び日を含有するTe膜の低融点金属あるいはその合金膜
からなる記録膜12は第1図に示すように、ある一定値
以上のエネルギーを有するレーザービーム等のエネルギ
ービーム13を照擬したとき光反射率が上昇し、更に大
きな一定値以上のエネルギービームを照射すると凹部さ
らには孔が形成されて光反射率が逆に初期値以下まで下
がることを見い出した。
Here, the content of C in the Te film can be freely controlled by the mixing ratio of CH4 and ~ and the applied high-frequency power.
13.58MHZ) power Te target and substrate 1 1
When the voltage is applied between 1 and 2, it is possible to form a film containing C in an atomic ratio of 0.2 to Te. In this case, the compositional formula of the film can be written as Te, - length x (H), and the content on the day when the film is chemically most stable is determined by x. Here, the H content can be arbitrarily selected as long as it is not contained in such a large amount that hydrogen gas (2) is generated in the film. Furthermore, since the film thickness is proportional to the sputtering time, it can be freely controlled. The optical constants of the recording film 12 are determined by the film composition, and in the above example, the reflectance reached a maximum of 50% at a film thickness of about 700 Å, and the recording characteristics were the best. Furthermore, the recording film 12 produced under these conditions has an amorphous value, and the edges around the holes or recesses in the recorded state are smoother than that of a polycrystalline Te film, and the noise level during information reproduction can be kept low. The present inventor has proposed that the recording film 12 made of a low-melting point metal such as the Te film containing C and hydrogen or an alloy film thereof can be used as an energy source such as a laser beam or the like having an energy of a certain value or more, as shown in FIG. It has been found that when the beam 13 is irradiated, the light reflectance increases, and when a larger energy beam of a certain value or more is irradiated, depressions and even holes are formed, and the light reflectance decreases to below the initial value.

第2図は上記実施例によるCおよび日を含有するTe膜
からなる記録膜12に記録膜12面でのスポット径1山
肌、波長83仇血のレーザービームを4m/sの速度で
走査しながら照射した場合のビームエネルギーに対する
記録膜12の光反射率の変化を示す。すなわち、1.5
〜38hWのレーザービームを4m/sで記録膜12上
を走査することにより、光反射率が50%(初期値)か
ら80%へと上昇することによって、第3図に示すよう
に記録トラックに沿ってトラツキング用パターン21を
形成することができる。
FIG. 2 shows a recording film 12 made of a Te film containing C and oxide according to the above embodiment while scanning a laser beam with a spot diameter of 1 mountain and a wavelength of 83 m/s on the surface of the recording film 12 at a speed of 4 m/s. It shows the change in light reflectance of the recording film 12 with respect to beam energy when irradiated. That is, 1.5
By scanning the recording film 12 with a ~38 hW laser beam at 4 m/s, the light reflectance increases from 50% (initial value) to 80%, and as a result, the recording track is formed as shown in FIG. A tracking pattern 21 can be formed along the line.

そしてさらに記録すべき情報に応じて変調(オン・オフ
)された38hW以上のレーザービームを同じ速度でト
ラツキング用パターン21に沿って走査することによっ
て、情報に応じた孔または凹部22を形成することが可
能となる。この情報の記録に際しては、トラッキング用
パターン21からの反射光または透過光を検出しながら
、記録用レーザービームの位直合せ、すなわちトラツキ
ングを行うことにより、記録トラックピッチが1.5〜
2ムmといった高密度の記録を容易に達成することがで
きる。またトラッキング用パターン21は再生時のトラ
ツキングにも利用できることは勿論である。第4図は温
度7ぴ0、相対湿度85%の雰囲気中で時間経過に対す
る感度の劣化の状態、すなわち寿命特性を、従来のTe
単体からなる記録膜の場合Aと本発明による記録膜の場
合Bとについて比較して示す図である。
Further, by scanning a laser beam of 38 hW or more modulated (on/off) according to the information to be recorded along the tracking pattern 21 at the same speed, a hole or a recess 22 according to the information is formed. becomes possible. When recording this information, the recording laser beam is aligned while detecting reflected light or transmitted light from the tracking pattern 21, that is, tracking is performed, so that the recording track pitch is 1.5 to 1.5.
High-density recording of 2 mm can be easily achieved. It goes without saying that the tracking pattern 21 can also be used for tracking during playback. Figure 4 shows the state of deterioration of sensitivity over time, that is, the life characteristics of conventional Te
FIG. 3 is a diagram showing a comparison between a case A of a recording film made of a single substance and a case B of a recording film according to the present invention.

この図における感度の劣化は、記録に必要なエネルギー
ビームのエネルギーの逆数の初期値に対する変化として
表わされており、A,Bいずれも記録膜がアクリル基板
上に形成された場合を示す。この図からわかるように、
Te単体からなる記録膜の場合Aで示すように時間経過
とともに感度が劣化する。
The deterioration in sensitivity in this figure is expressed as a change from the initial value of the reciprocal of the energy of the energy beam necessary for recording, and both A and B show the case where the recording film is formed on an acrylic substrate. As you can see from this figure,
In the case of a recording film made of Te alone, as shown by A, the sensitivity deteriorates over time.

これは時間とともに局部的な透明領域(シミ)が生ずる
ためで、約170時間経過後には記録膜全面にわたって
感度が劣化する。これに対し、本発明の実施例によるC
および日を含有するTe薄膜からなる記録膜の場合は、
Bで示すように1.00俄時間経過後もTe単体からな
る記録膜に見られた様なシミは全く認められず、常にほ
ぼ一定の感度を保持しており、長寿命化を達成すること
がわかる。第5図aは温度70qo、相対湿度85%の
条件下で2q時間経過後のアクリル基板上の従来のTe
単体からなる記録膜の表面状態を示す光学顕微鏡写真で
、同図bは同条件下で1,00凪時間放置された本発明
の実施例によるCおよび日を含有するTe膜からなる記
録膜の表面状態を示す。
This is because local transparent areas (spots) occur over time, and after about 170 hours the sensitivity deteriorates over the entire recording film. In contrast, C
In the case of a recording film consisting of a Te thin film containing
As shown in B, even after 1.00 hours had elapsed, no stains like those seen on recording films made of pure Te were observed, and the sensitivity was always maintained at a nearly constant level, achieving a long service life. I understand. Figure 5a shows the conventional Te on an acrylic substrate after 2q hours at a temperature of 70qo and a relative humidity of 85%.
Figure b is an optical micrograph showing the surface condition of a recording film made of a single substance. Indicates surface condition.

倍率はa,b共に5ぴ音である。また本発明による記録
膜の感度、すなわち単位面積当りの孔または凹部の形成
に要するエネルギー(mJ/の)は従釆のTe膜単体の
記録膜の感度と同等かまたはわずかに上まわる程度の値
を示すことが確認された。
The magnification is 5 pm for both a and b. Furthermore, the sensitivity of the recording film according to the present invention, that is, the energy (mJ/) required to form holes or recesses per unit area, is equivalent to or slightly higher than the sensitivity of the secondary recording film made of a single Te film. It was confirmed that

すなわち本発明による光学的情報記録媒体は時間経過に
対する感度の劣化が少ないばかりでなく、高感頚蔓とい
う特長も兼ね備えている。なお、記録膜中のCの含有量
はTeに対して原子数比で0.05未満では上述した効
果が認められず、また0.8を越えると感度の低下が見
られた。
That is, the optical information recording medium according to the present invention not only exhibits little deterioration in sensitivity over time, but also has the feature of high sensitivity. Note that when the content of C in the recording film was less than 0.05 in atomic ratio to Te, the above-mentioned effect was not observed, and when it exceeded 0.8, a decrease in sensitivity was observed.

この点は記録膜にTe以外の低融点金属あるいはその合
金を用いた場合も同様である。従って記録膜中のCの含
有量は、金属元素の総量に対し原子数比で0.05〜0
.8の範囲にすることが望ましい。上記実施例では、記
録膜をCH4とArとの混合ガス中で反応性スパッタI
Jングを行なうことにより形成したが、CH4とTeの
蒸気とをプラズマ状にして基板にCおよび日を含むTe
膜からなる記録膜を形成することも可能である。また、
Te(CH3)2(ジメチルテルル)やTe(C2日5
)2(ジェチルテルル)を用いた気相成長またはプラズ
マ気相成長によっても同様の記録膜を形成することが可
能である。さらに他の方法としてTe,C,日原子の一
部または全部をイオン化してビーム状として基板上に積
もらせるようにしてもよい。低融金属としてはZn(繭
&点=31ぴ○)、Cd(320℃)等もTeと全く同
様にCH4とArの混合ガス中でスパッタリングして、
上記特性と同等の特性を有する記録膜を得ることができ
る。またBi2Te3(斑?○)、lnSd(535q
o)等の合金も低融点として知られ、上記同様スパッタ
リング法により上記特性の記録を形成することができる
。Bi(271℃)はスパッタリングは不可能であるが
、反応性蒸着によって上記特性を有する記録膜を形成す
ることができる。また上記CH4ガスは、C2日4(エ
チレン)ガスやC2日2(アセチレン)ガスで置き換え
ることも可能である。このように本発明による光学的情
報記録媒体は長寿命かつ高感度であるとともに、溝をト
ラツキング用パターンとする従来のもののように溝を形
成した原盤を用いての転写工程等を要することなくトラ
ッキング用パターンを簡単に程度よく形成することがで
きるという利点を有する。
This point also applies when a low melting point metal other than Te or an alloy thereof is used for the recording film. Therefore, the content of C in the recording film is 0.05 to 0 in terms of atomic ratio to the total amount of metal elements.
.. A range of 8 is desirable. In the above embodiment, the recording film was formed by reactive sputtering I in a mixed gas of CH4 and Ar.
Although it was formed by conducting J-type process, the Te vapor containing C and Te was formed on the substrate by making CH4 and Te vapor into plasma.
It is also possible to form a recording film consisting of a film. Also,
Te(CH3)2 (dimethyltellurium) and Te(C2day5
) 2 (jetyl tellurium) or plasma vapor phase epitaxy can also form a similar recording film. Still another method is to ionize some or all of the Te, C, and Ni atoms and deposit them on the substrate in the form of a beam. Low-melting metals such as Zn (cocoon & point = 31 pi○) and Cd (320°C) are also sputtered in a mixed gas of CH4 and Ar in exactly the same way as Te.
A recording film having properties equivalent to those described above can be obtained. Also, Bi2Te3 (spotted?○), lnSd (535q
Alloys such as (o) and the like are also known to have low melting points, and similarly to the above, a record of the above characteristics can be formed by the sputtering method. Bi (271° C.) cannot be sputtered, but a recording film having the above characteristics can be formed by reactive vapor deposition. Furthermore, the CH4 gas can be replaced with C2day4 (ethylene) gas or C2day22 (acetylene) gas. As described above, the optical information recording medium according to the present invention has a long life and high sensitivity, and can be tracked without the need for a transfer process using a master disc with grooves, unlike conventional ones that use grooves as a tracking pattern. It has the advantage that a pattern for use can be easily formed with good quality.

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

第1図は本発明の一実施例を説明するための断面図、第
2図は同実施例における記録膜に照射されるレーザービ
ームのエネルギーと記録膜の光反射率との関係を示す図
、第3図は同実施例におけるトラッキング用パターンと
情報記録状態を示す平面図、第4図は本発明の記録媒体
と従来の記録媒体との寿命特性を比較して示す図、第5
図a,bは従来の記録媒体と本発明の記録媒体における
記録膜表面状態を示す顕微鏡写真である。 11・・・・・・基板、12・・・・・・記録膜、13
・・・・・・エネルギービーム、21……トラツキング
用パターン、22・・・・・・孔または凹部。 第1図 第2図 第3図 簾ム図 第5図
FIG. 1 is a cross-sectional view for explaining one embodiment of the present invention, and FIG. 2 is a diagram showing the relationship between the energy of the laser beam irradiated to the recording film and the light reflectance of the recording film in the same embodiment. FIG. 3 is a plan view showing the tracking pattern and information recording state in the same embodiment, FIG. 4 is a diagram comparing the life characteristics of the recording medium of the present invention and a conventional recording medium, and FIG.
Figures a and b are micrographs showing the surface state of the recording film in a conventional recording medium and a recording medium according to the present invention. 11... Substrate, 12... Recording film, 13
... Energy beam, 21 ... Tracking pattern, 22 ... Hole or recess. Figure 1 Figure 2 Figure 3 Blind screen Figure 5

Claims (1)

【特許請求の範囲】 1 基板と、この基板上に被着されエネルギービームの
照射により孔または凹部が形成されることによつて情報
を記録する記録膜とからなる光学的情報記録媒体におい
て、前記記録膜は25〜600℃の融点をもつ金属また
はその合金とCおよびHを含有するものであつて、記録
トラツクに沿つて光反射率が周囲より高いトラツキング
用パターンが形成されたものであることを特徴とする光
学的情報記録媒体。 2 記録膜中のCの含有量は金属元素の総量に対して原
子数比で0.05〜0.8であることを特徴とする特許
請求の範囲第1項記載の光学的情報記録媒体。 3 記録膜の厚さは200Å〜1μmであることを特徴
とする特許請求の範囲第1項または第2項記載の光学的
情報記録媒体。
[Scope of Claims] 1. An optical information recording medium comprising a substrate and a recording film which is deposited on the substrate and records information by forming holes or recesses by irradiation with an energy beam. The recording film shall contain a metal or its alloy with a melting point of 25 to 600°C, C and H, and shall have a tracking pattern formed along the recording track with a higher light reflectance than the surrounding area. An optical information recording medium characterized by: 2. The optical information recording medium according to claim 1, wherein the content of C in the recording film is in an atomic ratio of 0.05 to 0.8 with respect to the total amount of metal elements. 3. The optical information recording medium according to claim 1 or 2, wherein the recording film has a thickness of 200 Å to 1 μm.
JP56169884A 1981-10-23 1981-10-23 optical information recording medium Expired JPS6025278B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56169884A JPS6025278B2 (en) 1981-10-23 1981-10-23 optical information recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56169884A JPS6025278B2 (en) 1981-10-23 1981-10-23 optical information recording medium

Publications (2)

Publication Number Publication Date
JPS5871193A JPS5871193A (en) 1983-04-27
JPS6025278B2 true JPS6025278B2 (en) 1985-06-17

Family

ID=15894735

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56169884A Expired JPS6025278B2 (en) 1981-10-23 1981-10-23 optical information recording medium

Country Status (1)

Country Link
JP (1) JPS6025278B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0473889B2 (en) * 1987-05-15 1992-11-24
KR20200106528A (en) 2018-02-23 2020-09-14 가부시키가이샤 사무코 Quartz glass crucible

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
SE434679B (en) * 1982-07-01 1984-08-06 Asea Ab DEVICE FOR HERMETICALLY CLOSED LOAD CELLS FOR ELIMINATING THE IMPACT OF THE DIFFERENCE BETWEEN PRESSURE IN A SENSOR SPACE AND ATMOSPHERIC PRESSURE
JPS59160841A (en) * 1983-03-04 1984-09-11 Toshiba Corp Optical recording medium film
JP2570727B2 (en) * 1987-03-10 1997-01-16 東レ株式会社 Optical recording medium

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0473889B2 (en) * 1987-05-15 1992-11-24
KR20200106528A (en) 2018-02-23 2020-09-14 가부시키가이샤 사무코 Quartz glass crucible

Also Published As

Publication number Publication date
JPS5871193A (en) 1983-04-27

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