JPS5871193A - Optical information recording medium - Google Patents

Optical information recording medium

Info

Publication number
JPS5871193A
JPS5871193A JP56169884A JP16988481A JPS5871193A JP S5871193 A JPS5871193 A JP S5871193A JP 56169884 A JP56169884 A JP 56169884A JP 16988481 A JP16988481 A JP 16988481A JP S5871193 A JPS5871193 A JP S5871193A
Authority
JP
Japan
Prior art keywords
film
recording
optical information
recording film
melting point
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.)
Granted
Application number
JP56169884A
Other languages
Japanese (ja)
Other versions
JPS6025278B2 (en
Inventor
Masao Mashita
真下 正夫
Noburo Yasuda
安田 修朗
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 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)

Abstract

PURPOSE:To enhance sensitivity and prolong useful life, by a method wherein light reflectance at a part along a recording track is enhanced as compared to that at other part, in a optical information recording medium film consisting of a metal having a specified melting point, C and H. CONSTITUTION:A recording film 12 consisting of a metal having a melting point of 25-600 deg.C, such as Te, In, Sn or an alloy thereof, and a compound containing C and H, such as methane, is formed on a substrate 11 such as an acrylic resin plate in a thickness of about 200Angstrom -1mum. When the metal having the low melting point is Te, sputtering is conducted in a gaseous mixture of methane and argon by using Te as a target. The amounts of C and H contained in the film are controlled by the mixing ratio of the gases and the high-frequency power impressed. The light reflectance is increased when an energy beam 13 is irradiated at a given energy value, while a recess is produced and the reflectance is lowered when the beam 13 is irradiated at a further higher energy value. Accordingly, reproduction and recording can be performed easily.

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読取り可能な光学
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四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 on which recorded information can be read optically, and in particular, a recording film in which holes or four parts are formed 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.

光学的情報記録媒体として、従来、警手−5===tC
券寸寸今≠基板/土に形成された記録膜l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ピット
ノ列を形成するようにしたものがある。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tとしてテル
ル(Te)を使用することが知られている。Te膜は非
常に低いエネルギーで所望の孔(ピット)を形成でき、
この種の用途においては高感度材料として極めて有望で
ある。ここで感度とは、単位面積当シの記録部(この場
合はピット)形成に要するエネルギー(mJ/crn)
で定義される。
As an optical information recording medium, conventionally, Kente-5===tC
There is one in which an energy beam is irradiated onto a recording film l formed on a substrate/soil to form a pit-no row corresponding to the information to be recorded. In such optical information recording media, it has been known to use tellurium (Te) as the recording film t. Te film can form desired holes (pits) with very low energy,
It is extremely promising as a highly sensitive material in this type of application. Sensitivity here refers to the energy (mJ/crn) required to form a recording section (pit in this case) per unit area.
Defined by

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。記録膜とし
て使用する場合、膜厚は700X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、ピット形成に要するエネルギ
ーが大きくなり、感度の劣化を来たす。
However, when Te is left in the atmosphere, it is oxidized by oxygen and moisture and quickly becomes transparent. When used as a recording film, the film thickness is extremely thin, about 700×, so the deterioration in sensitivity due to increased transparency caused by oxidation of the film is significant. That is, when the film is oxidized, the melting and evaporation temperatures increase, and absorption of energy such as light decreases due to transparency, so the energy required to form pits increases, resulting in deterioration of sensitivity.

例えば温度70℃、相対湿度85%の雰囲気に放置した
場合、約5時間で感度が約20%低下し、約15時間で
約50%低下してしまう。
For example, when left in an atmosphere with a temperature of 70° C. and a relative humidity of 85%, the sensitivity decreases by about 20% in about 5 hours, and by about 50% in about 15 hours.

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。
For this reason, various measures have been taken to prevent oxidation of the Te film.

その一つである安定無機物質でTe膜をコーティングす
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。
One of these methods, a method of coating a 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 advantageous in that they do not impair sensitivity to a small extent, but they allow oxygen and water to permeate through them relatively easily.
It is not very useful in preventing oxidation of the membrane.

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シ、そのため1
.5〜2μmピッチで記録トラックを形成させる必要が
ある。その場合記録。
In addition, high-density and large-capacity recording is now required for such optical information recording media, and therefore
.. It is necessary to form recording tracks at a pitch of 5 to 2 μm. In that case record.

再生時のトラッキングを容易とするだめ、ガラス板に写
真蝕刻法により溝を設けたものを原盤としてアクリル板
にトラッキング用溝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。
In order to facilitate tracking during playback, a method was used in which a glass plate with grooves formed by photolithography was used as the master, and the tracking grooves were transferred to an acrylic plate.
There were problems with the accuracy and cost of the tracking groove.

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、しかもトラッキング用パターン
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。
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
もしくは四部として記録するものであって、記録膜を低
融点金属またはその合金とCおよびH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ドラッギ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25〜600℃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 、 In 、 Sn 、 Zn 、 Pb 、 
Bi。
The optical information recording medium according to the present invention records information as holes or four parts by irradiating a recording film on a substrate with an energy beam, and the recording film is made of a low melting point metal or an alloy thereof. It is characterized in that it is formed of a film containing C and H, and that a dragging pattern with a higher light reflectance than the surrounding area is formed in advance along the recording track on this recording film, thereby achieving high sensitivity and long length. In addition to having the advantages of 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° C. is used from the viewpoint of film forming technology and recording characteristics. Examples of such low melting metals include Cd, In, 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。
There are Te etc. These metals may be used alone, but
Alloys thereof can also be used.

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[7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射す
ると孔まだは凹部ができて、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。
That is, the present invention takes advantage of the fact that a high light reflectance can be obtained by irradiating the recording film with a relatively low-energy energy beam [7] Forming a tracking pattern,
Furthermore, when an energy beam of higher energy is irradiated, a concave portion is formed in the hole, and conversely, the light reflectance decreases, which is used to record information.

以下、図面を参照しながら本発明の実施、例を5− 詳細に説明する。Hereinafter, embodiments and examples of the present invention will be explained in 5-5 with reference to the drawings. Explain in detail.

第1図は本発明の一実施例を示す断面図である。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II上にCおよびH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、200X〜1μm
程度が適当である。
FIG. 1 is a sectional view showing one embodiment of the present invention. 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 H is formed on this substrate II. The thickness of this recording film 12 needs to be thick enough to obtain sufficient light reflectance and thin enough not to impair sensitivity, and is 200X to 1 μm.
The degree is appropriate.

例えば低融点金属としてTe膜を選んだ場合、記録膜1
2はTeをターケ゛ットとしてCおよびHを含むガス、
例えばメタン(CH4)とアルゴン(Ar)との混合ガ
ス中でスパッタリングすることによシ得られる。ここで
Te膜中のC,Hの含有量はCH4とAr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CH
4/Ar=16− の混合比で約0.3 W/cmの高周波(13,56M
Hz)電力をTeターダットと基板1ノとの間に印加す
ると、Teに対して原子数比で02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Te1
−xCx (H)と書き表わすことができ、膜が化学的
に最も安定するHの含有量はXによって決まる。ここで
は膜中に水素ガス(H2)が発生するほど多量に含有さ
せない限り、■含有量は任意に選ぶことができる。さら
に膜厚はスノRツタリング時間に比例するので、自由に
制御できる。
For example, if a Te film is selected as the low melting point metal, the recording film 1
2 is a gas containing C and H using Te as a target;
For example, it can be obtained by sputtering in a mixed gas of methane (CH4) and argon (Ar). Here, the content of C and H in the Te film can be freely controlled by the mixing ratio of CH4 and Ar and the applied high frequency power.
A high frequency of about 0.3 W/cm (13,56 M
When power (Hz) is applied between the Te conductor and the substrate 1, a film containing C in an atomic ratio of 02 to Te can be formed. In this case, the compositional formula of the film is Te1
It can be expressed as -xCx (H), and the H content at which the film is most chemically stable is determined by X. Here, (2) the content can be arbitrarily selected as long as it is not contained in such a large amount that hydrogen gas (H2) is generated in the film. Furthermore, since the film thickness is proportional to the snow R sagging time, it can be freely controlled.

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700Xの膜厚で反射率が50チと最大と
なシ、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は非晶値であシ、多結晶Te膜に比べて
記録状態の孔または凹部周辺ニップ部が滑らかとなシ、
情報再生時のノイズレベルを低くおさえることができる
The optical constants of the recording film 12 are determined by the film composition, and in the above example, a film thickness of about 700× had a maximum reflectance of 50×, and the recording characteristics were the best. Furthermore, the recording film 12 produced under these conditions has an amorphous value, and the nip area around the holes or recesses in the recording state is smoother than that of a polycrystalline Te film.
The noise level during information reproduction can be kept low.

本発明者は、上述したCおよびH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、お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を照射したと
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だ。第
2図は上記実施例によるCおよびH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1μm
、波長830 nmのレーザービームを4 m/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。
The inventor has proposed that the recording film 12 made of a low melting point metal such as the Te film containing C and H or an alloy film thereof is the first
As shown in the figure, when irradiated with an energy beam 13 such as a laser beam with energy above a certain value, the light reflectance increases, and when an even larger energy beam above a certain value is irradiated, depressions and even holes are formed. The main finding is that the light reflectance decreases to below the initial value. FIG. 2 shows a recording film 12 made of a Te film containing C and H according to the above embodiment with a spot diameter of 1 μm on the surface of the recording film 12.
, shows changes in the light reflectance of the recording film 12 with respect to beam energy when irradiated with a laser beam having a wavelength of 830 nm while scanning at a speed of 4 m/s.

すなわち、1.5〜35mWのレーザービームを4 m
/aで記録膜12上を走査することによシ、光反射率が
50チ(初期値)から80チ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ッキン
グ用ノぐターン2ノを形成することができる。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
3 5 mW以上のレーザービームを同じ速度でトラッ
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、トラッキング用ノ4
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置合せ、すなわちトラッキン
グを行うことにより、記録トラックピッチが1.5〜2
μmといった高密度の記録を容易に達成するコトカでき
る。壕だトラッキング用ノ♀ターン21は再生時のトラ
ッキングにも利用できることは勿論である。
That is, a laser beam of 1.5-35 mW is
By scanning the recording film 12 with /a, the light reflectance increases from 50 inches (initial value) to 80 inches, and as a result, tracking marks are formed along the recording track as shown in FIG. It is possible to form a second turn. Furthermore, by scanning a laser beam of 35 mW or more that is modulated (on, off) according to the information to be recorded along the tracking pattern 21 at the same speed,
It becomes possible to form holes or recesses 22 according to information. When recording this information, please use the tracking number 4.
While detecting reflected light or transmitted light from turn 21,
By aligning the recording laser beam, that is, tracking, the recording track pitch can be adjusted to 1.5 to 2.
It is possible to easily achieve high-density recording on the order of μm. Needless to say, the tracking No. 21 can also be used for tracking during playback.

第4図は温度70℃、相対湿度85チの雰囲気中で時間
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。この
図における感度の劣化6、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9− クリル基板上に形成された場合を示す。
Figure 4 shows the state of deterioration of sensitivity over time in an atmosphere with a temperature of 70°C and a relative humidity of 85°C, that is, the life characteristics.
FIG. 3 is a diagram showing a comparison between a case A of a conventional recording film made of a single Te and a case B of a recording film according to the present invention. In this figure, the deterioration in sensitivity 6 is expressed as a change with respect to 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.

この図かられかるように、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。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Hを含有するT8薄膜からなる記録膜の場合は、B
で示すように1,000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。
As can be seen from this figure, in the case of a recording film made of only Te, the sensitivity deteriorates over time as shown by A. This is because local transparent areas (spots) occur over time, and after about 170 hours, the sensitivity deteriorates over the entire recording film. On the other hand, in the case of the recording film made of a T8 thin film containing C and H according to the embodiment of the present invention, B
As shown in , even after 1,000 hours, no stains like those seen on recording films made of pure Te were observed, and the sensitivity remained almost constant, indicating that a long service life was achieved. .

第5図(、)は温度70℃、相対湿度85俤の条件下で
20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1,000時間放置された本発明の実
施例によるCおよびHを含有するTe膜からなる記録膜
の表面状態を示す。
Figure 5 (,) is an optical micrograph showing the surface condition of a conventional recording film made of pure Te on an acrylic substrate after 20 hours at a temperature of 70°C and a relative humidity of 85 m.
b) shows the surface condition of a recording film made of a Te film containing C and H according to an example of the present invention that was left for 1,000 hours under the same conditions.

倍率は(a) 、 (b)共に50倍である。The magnification is 50 times in both (a) and (b).

また本発明による記録膜の感度、すなわち単一10= 位面積当りの孔または四部の形成に要するエネルギー(
mJ/crn)は従来のTe膜膜体体記録膜の感度と同
等かまたはわずかに上1わる程度の値を示すことか確認
された。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
度という特長も兼ね備えている。
Also, the sensitivity of the recording film according to the present invention, that is, the energy required to form a hole or four parts per single 10=potential area (
It was confirmed that the sensitivity (mJ/crn) was equivalent to or slightly higher than the sensitivity of the conventional Te film body recording film. 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 advantage of high sensitivity.

なお、記録膜中のCの含有量はTeに対して原子数比で
005未満では上述した効果が認められず、またpo、
sを越えると感度の低下が見られた。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d1、金属元
素の総量に対し原子数比で0.05〜08の範囲にする
ことが望ましい。
Note that if the content of C in the recording film is less than 005 in atomic ratio to Te, the above-mentioned effect will not be observed;
A decrease in sensitivity was observed when the temperature exceeded s. This point also applies when a low melting point metal other than Te or an alloy thereof is used for the recording film. Therefore, it is desirable that the content d1 of C in the recording film is in the range of 0.05 to 0.08 in terms of atomic ratio to the total amount of metal elements.

上記実施例では、記録膜をCH4とArとの混合ガス中
で反応性スパッタリングを行なうことによυ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Hを含むre膜からなる記録膜を形成することも可
能である。また、T(](CH3)2 (ツメチルテル
ル)やTe(C2Hs)2(ジエチルテルル)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。
In the above embodiment, the recording film was formed by reactive sputtering in a mixed gas of CH4 and Ar, but a re film containing C and H was formed on the substrate by using CH4 and Te vapor in the form of plasma. It is also possible to form a recording film consisting of: A similar recording film can also be formed by vapor phase growth or plasma vapor phase growth using T(](CH3)2 (trimethyltellurium) or Te(C2Hs)2 (diethyltellurium). Te as a method.

C,H原子の一部捷たけ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。
Some or all of the C and H atoms may be ionized and deposited on the substrate in the form of a beam.

低融金属としてはZn (融点−319℃)。The low-melting metal is Zn (melting point -319°C).

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     する。
Cd (320℃) etc. also have CH4 and Ar in exactly the same way as Te.
A recording film having properties equivalent to those described above can be obtained by sputtering in a mixed gas of

まだBi2Te3 (585℃)、In5b(535℃
)等の合金も低融点として知られ、上記同様ス・(ツタ
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。
Still Bi2Te3 (585℃), In5b (535℃
) is also known to have a low melting point, and similarly to the above, it is possible to form a record of the above properties by the tsuttering method. Sputtering of Bi (271°C) is impossible, but the above properties can be achieved by reactive vapor deposition. A recording film having the following properties can be formed.

また上記CH4ガスは、C2H4(エチレン)ガスやC
2H2(アセチレン)ガスで置き換えることも可能であ
る。
In addition, the CH4 gas mentioned above may be C2H4 (ethylene) gas or C2H4 gas.
It is also possible to replace it with 2H2 (acetylene) gas.

このように本発明による光学的情報8[シ録媒体は長寿
命かつ高感度であるとともに、溝をトラッキング用パタ
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。
In this way, the optical information recording medium according to the present invention has a long life and high sensitivity, and requires a transfer process using a master disc with grooves, unlike the conventional one in which grooves are used as a tracking pattern. This has the advantage that a tracking pattern can be easily formed to a good degree without any problems.

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

第1図は本発明の一実施例を説明するだめの断面図、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d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、27・・・トラッキング用パターン、13
− 22・・・孔または四部。 14− 第3図 第4図 膵造り早開(h) 第5図 (a) (b)
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.
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. DESCRIPTION OF SYMBOLS 11... Substrate, 12... Recording film, 13... Energy beam, 27... Tracking pattern, 13
-22...hole or four parts. 14- Figure 3 Figure 4 Early opening of the pancreas (h) Figure 5 (a) (b)

Claims (3)

【特許請求の範囲】[Claims] (1)基板と、この基板上に被着されエネルギービーム
の照射によシ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って、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
グ用ノ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。
(1) In an optical information recording medium consisting of a substrate and a recording film that is deposited on the substrate and records information by forming holes or recesses by irradiation with an energy beam, the recording film has a It is characterized by containing a metal or its alloy having a melting point of ~600°C, C and H, and having a tracking notarne formed along the recording track with a higher light reflectance than the surrounding area. Optical information recording medium.
(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。
(2) The optical information recording 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. Medium.
(3)  記録膜の厚さは200X〜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。
(3) The optical information recording medium according to claim 1 or 2, wherein the thickness of the recording film is 200X 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 true JPS5871193A (en) 1983-04-27
JPS6025278B2 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 (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4450020A (en) * 1982-07-01 1984-05-22 Santrade Ltd. Method of manufacturing cladding tubes of a zirconium-based alloy for fuel rods for nuclear reactors
JPS59160841A (en) * 1983-03-04 1984-09-11 Toshiba Corp Optical recording medium film
JPS63221090A (en) * 1987-03-10 1988-09-14 Toray Ind Inc Optical recording medium

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63284922A (en) * 1987-05-15 1988-11-22 Fujitsu Ltd Pulse generating circuit
KR102408990B1 (en) 2018-02-23 2022-06-14 가부시키가이샤 사무코 Quartz Glass Crucible

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4450020A (en) * 1982-07-01 1984-05-22 Santrade Ltd. Method of manufacturing cladding tubes of a zirconium-based alloy for fuel rods for nuclear reactors
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
JPS63221090A (en) * 1987-03-10 1988-09-14 Toray Ind Inc Optical recording medium

Also Published As

Publication number Publication date
JPS6025278B2 (en) 1985-06-17

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