JPH0119450B2 - - Google Patents
Info
- Publication number
- JPH0119450B2 JPH0119450B2 JP60020274A JP2027485A JPH0119450B2 JP H0119450 B2 JPH0119450 B2 JP H0119450B2 JP 60020274 A JP60020274 A JP 60020274A JP 2027485 A JP2027485 A JP 2027485A JP H0119450 B2 JPH0119450 B2 JP H0119450B2
- Authority
- JP
- Japan
- Prior art keywords
- tin
- copper alloy
- copper
- thin film
- atomic
- 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
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/26—Apparatus or processes specially adapted for the manufacture of record carriers
- G11B7/266—Sputtering or spin-coating layers
-
- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C13/00—Alloys based on tin
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/242—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
- G11B7/243—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/242—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
- G11B7/243—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
- G11B2007/24302—Metals or metalloids
- G11B2007/24308—Metals or metalloids transition metal elements of group 11 (Cu, Ag, Au)
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/242—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
- G11B7/243—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
- G11B2007/24302—Metals or metalloids
- G11B2007/24312—Metals or metalloids group 14 elements (e.g. Si, Ge, Sn)
Landscapes
- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Inorganic Chemistry (AREA)
- Materials Engineering (AREA)
- Mechanical Engineering (AREA)
- Metallurgy (AREA)
- Organic Chemistry (AREA)
- Manufacturing & Machinery (AREA)
- Optical Record Carriers And Manufacture Thereof (AREA)
- Thermal Transfer Or Thermal Recording In General (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は、記録媒体用錫−銅合金に関する。[Detailed description of the invention] (Industrial application field) The present invention relates to a tin-copper alloy for recording media.
(従来の技術)
近年になつて、高速ランダムアクセスの可能な
高密度大容量の情報記録媒体円盤についての研究
開発が盛んに行なわれるようになつたが、レーザ
光スポツトの照射による情報の記録再生が可能
で、かつ、レーザ光または/及び必要に応じて適
当な補助手段をも用いて記録された情報を消去
し、新しい情報に書換えうるような機能も備えて
いる如き新規な記録媒体についての探索も行なわ
れている。(Prior Art) In recent years, research and development has been actively conducted on high-density, large-capacity information recording media disks that can be accessed at high speed and randomly. new recording media that are capable of erasing recorded information and rewriting it with new information using laser light and/or appropriate auxiliary means as necessary. Explorations are also underway.
ところで、レーザ光を用いて情報の記録、再生
が行なわれるようにされている記録媒体につい
て、レーザ光ビームのスポツトによる加熱作用に
より、記録媒体にどのような物理的な変化を生じ
させて情報の記録を行なうようにしているのかに
着目して、現在までに提案されている多くの記録
媒体を分類すると、ピツト形成型、泡あるいは凹
凸形成型、光磁気型、相変化型(熱エネルギによ
り光の透過率、反射率、吸収率等に変化が生じる
熱変態型)等の各種型式の記録媒体に大別でき
る。 By the way, regarding a recording medium on which information is recorded and reproduced using a laser beam, what kind of physical change is caused in the recording medium by the heating effect of the spot of the laser beam? The many recording media that have been proposed to date can be categorized based on how they perform recording: pit-forming type, bubble or unevenness-forming type, magneto-optical type, and phase-change type (which uses thermal energy to generate light). It can be broadly classified into various types of recording media, such as thermal transformation type (thermal transformation type) in which changes occur in transmittance, reflectance, absorption rate, etc.
そして、前記した各種型式の記録媒体の内で相
変化型に属する記録媒体は、既記録情報の消去の
可能性もあるという点で注目されていて、現在ま
でにこの種の記録媒体としては、カルコゲナイド
系の物質(ゲルマニウム、テルル、アンチモン、
シリコン、砒素、ビスマス、インジユウム、ガリ
ユウム、タリウム、セレン、硫黄)の色々な組合
わせからなる組成物の薄膜や、低級酸化物(例え
ば、TeとTeO2の混合組成物等)の薄膜を用いた
記録媒体が提案されている。 Of the various types of recording media mentioned above, phase-change recording media have attracted attention because of the possibility of erasing previously recorded information, and to date, as this type of recording media, Chalcogenide substances (germanium, tellurium, antimony,
We used thin films of compositions consisting of various combinations of silicon, arsenic, bismuth, indium, gallium, thallium, selenium, sulfur) and thin films of lower oxides (for example, mixed compositions of Te and TeO 2 ). A recording medium is proposed.
(発明が解決しようとする問題点)
ところが、カルコゲナイト系の物質の色々な組
合わせからなる組成物の薄膜や、低級酸化物(例
えば、TeとTeO2の混合組成物等)の薄膜を用い
て構成されている既提案の記録媒体では、レーザ
光強度(記録媒体に相変化を起こさせることがで
きる強度範囲内のレーザ光強度であつて、記録媒
体にその強度のレーザ光が照射された部分からの
再生信号中における2次高調波歪が極小になされ
る如きレーザ光強度)が一定となされる如き記録
媒体の薄膜を構成している物質の組成範囲が狭い
ので、所定の特性の記録媒体の大量生産を簡単に
行なうことができないという点が問題になつた。(Problems to be Solved by the Invention) However, thin films of compositions made of various combinations of chalcogenite-based substances or thin films of lower oxides (for example, mixed compositions of Te and TeO2, etc.) cannot be used. In the previously proposed recording medium, the laser light intensity (laser light intensity within the intensity range that can cause a phase change in the recording medium, and the portion where the recording medium is irradiated with laser light of that intensity) Since the composition range of the material constituting the thin film of the recording medium is narrow such that the second harmonic distortion in the reproduced signal from the recording medium is minimized and the laser beam intensity is constant, The problem was that it could not be easily mass-produced.
(問題点を解決するための手段)
本発明は、錫が40原子%乃至60原子%であつて
残部が銅である記録媒体用錫−銅合金を提供する
ものである。(Means for Solving the Problems) The present invention provides a tin-copper alloy for recording media, containing 40 atomic % to 60 atomic % of tin and the balance being copper.
(実施例)
錫と銅とからなる合金は、古くから青銅(唐金
と俗称されている合金)として知られており、普
通の青銅は錫4〜12重量%を含む銅−錫合金、す
なわち、銅−錫合金におけるαまたはα+γ固溶
体であり、古来、青銅貨、銅像などの美術品、機
械の部分品に用いられる砲金、鐘銅、工業用材料
用青銅、その他一般的な用途に応じて、それぞれ
組成を異にしているものが作られているが、上記
のような各種の用途に用いられている青銅は、そ
れらのものにおける何れのものでも錫が10重量%
程度、銅が90重量%程度の組成となされている銅
−錫合金である。(Example) An alloy consisting of tin and copper has long been known as bronze (commonly known as karakin), and ordinary bronze is a copper-tin alloy containing 4 to 12% by weight of tin, i.e. , an α or α+γ solid solution in a copper-tin alloy, and has been used since ancient times to produce works of art such as bronze coins and statues, gunmetal used in machine parts, bell copper, bronze for industrial materials, and other general uses. Bronze is made with different compositions, but all of the bronzes used for the various purposes mentioned above contain 10% tin by weight.
It is a copper-tin alloy with a composition of about 90% copper by weight.
ところで、錫の原子量は118.69であり、また、
銅の原子量は63.546であるから、前記したように
錫が10重量%程度、錫が90重量%適度の組成を持
つている銅−錫合金は、それの組成を原子%に換
算すると、銅が94原子%程度、錫が6原子%程度
の銅−錫合金として表わされるが、銅−錫合金に
おいて、錫の含有率を増加させて合金を作ろうと
すると偏析が生じて脆くなる等の欠点があるため
に、古来から広く実用されている青銅では、それ
の組成が前記のように錫が10重量%程度、銅が90
重量%程度となされているともいえる。 By the way, the atomic weight of tin is 118.69, and
Since the atomic weight of copper is 63.546, as mentioned above, a copper-tin alloy with a moderate composition of about 10% tin and 90% by weight can be converted into an atomic% of copper. It is expressed as a copper-tin alloy containing about 94 at.% tin and about 6 at.% tin, but if you try to make an alloy by increasing the tin content, there are drawbacks such as segregation and brittleness. Therefore, the composition of bronze, which has been widely used since ancient times, is approximately 10% by weight of tin and 90% by weight of copper.
It can be said that it is about % by weight.
本発明は相変化型(熱エネルギにより光の透過
率、反射率、吸収率等に変化が生じる熱変態型)
の記録媒体に適する記録材料の探索に当り銅と錫
とからなる合金に着目し、その錫−銅合金におけ
る銅と錫との組成を変化させて、錫が40原子%乃
至60原子%であつて残部が銅であるような組成範
囲の錫−銅合金が、相変化型の記録媒体に適した
特性を備えていることを見出したことに基づい
て、本発明の記録媒体用錫−銅合金を完成させた
ものである。 The present invention is a phase change type (thermal transformation type in which light transmittance, reflectance, absorption rate, etc. change due to thermal energy)
In searching for a recording material suitable for recording media, we focused on an alloy consisting of copper and tin, and by changing the composition of copper and tin in the tin-copper alloy, we created a material with tin content of 40 atomic % to 60 atomic %. Based on the discovery that a tin-copper alloy with a composition range in which the balance is copper has characteristics suitable for a phase change type recording medium, the tin-copper alloy for recording media of the present invention has been developed. It has been completed.
次に、添付図面を参照しながら本発明の記録媒
体用錫−銅合金について詳細に説明する。 Next, the tin-copper alloy for recording media of the present invention will be described in detail with reference to the accompanying drawings.
第1図は、二元蒸着法を適用して本発明の記録
媒体用錫−銅合金、すなわち、錫が40原子%乃至
60原子%であつて残部が銅であるような記録媒体
用錫−銅合金による薄膜記録媒体を基板表面に付
着形成させるようにする成膜装置の概略構成を示
す斜視図であり、この第1図において、1は表面
に対して記録媒体用錫−銅合金が付着形成される
べき基板であり、前記の基板1としては、例えば
ガラス円板、あるいはアクリル樹脂の円板、その
他適当な材料による円板が用いられてよい。 FIG. 1 shows a tin-copper alloy for recording media of the present invention obtained by applying a binary vapor deposition method, that is, a tin-copper alloy containing 40 at.
1 is a perspective view showing a schematic configuration of a film forming apparatus for depositing and forming a thin film recording medium made of a tin-copper alloy for recording media on a substrate surface in which the tin-copper alloy contains 60 atomic percent and the remainder is copper; In the figure, 1 is a substrate on which a tin-copper alloy for recording media is to be adhered and formed, and the substrate 1 may be made of, for example, a glass disk, an acrylic resin disk, or any other suitable material. A disc may be used.
2は前記した基板1を高速に回転させる回転軸
であつて、この回転軸2は図示されていない回転
駆動装置(例えばモータ)によつて所定の回転数
で高速に回転される。 Reference numeral 2 denotes a rotating shaft for rotating the substrate 1 described above at high speed, and this rotating shaft 2 is rotated at a predetermined number of rotations at high speed by a rotation drive device (for example, a motor) not shown.
3,4は、それぞれ蒸発材料を収容するボート
であり、また、5,6は前記したボート3,4を
加熱する電熱線であり、前記したボート3と電熱
線5とは一方の蒸発源Aを構成し、また、前記し
たボート4と電熱線6とは他方の蒸発源Bを構成
しており、前記した一方の蒸発源Aでは、それの
ボート3中に収容されている錫を加熱蒸発させ、
また、前記した他方の蒸発源Bでは、それのボー
ト4中に収容されている銅を加熱蒸発させる。 Reference numerals 3 and 4 are boats that accommodate evaporation materials, and 5 and 6 are heating wires that heat the boats 3 and 4, and the boat 3 and the heating wire 5 are connected to one of the evaporation sources A. The boat 4 and the heating wire 6 constitute the other evaporation source B, and the one evaporation source A heats and evaporates the tin contained in the boat 3. let me,
The other evaporation source B described above heats and evaporates the copper contained in the boat 4 thereof.
7は、前記した基板1と2つの蒸発源A,Bと
の間に出入自在になされているシヤツタ板であ
る。そして前記した各構成部分の全体は図示され
ていない容器内に収納され、前記した容器内に形
成される真空雰囲気中で、基板1に対する次のよ
うな成膜動作が行なわれるようになされている。 Reference numeral 7 denotes a shutter plate that can be freely moved in and out between the substrate 1 and the two evaporation sources A and B. The entirety of each of the above-described components is housed in a container (not shown), and the following film-forming operation is performed on the substrate 1 in a vacuum atmosphere formed in the container. .
すなわち、基板1を回転軸2に固着し、また、
一方の蒸発源Aにおけるボート3中に蒸発材料と
される錫を収容し、また、前記した他方の蒸発源
Bにおけるボート4中に蒸発材料とされる銅を収
容してから、容器内の排気を行なつて容器内が必
要な真空度の真空雰囲気になるようにする。 That is, the substrate 1 is fixed to the rotating shaft 2, and
Tin, which is used as an evaporation material, is stored in the boat 3 of one evaporation source A, and copper, which is used as an evaporation material, is stored in the boat 4 of the other evaporation source B, and then the exhaust inside the container is to create a vacuum atmosphere with the required degree of vacuum inside the container.
次に、各蒸発源A,Bと基板1との間にシヤツ
タ板7を挿入し、また、基板1を所定の回転数で
高速回転させ、さらに各蒸発源A,Bにおける各
電熱線5,6に対して、それぞれ所定の加熱用電
圧を供給して、蒸発源Aのボート3内に収容され
ている錫と、蒸発源Bのボート4内に収容されて
いる銅とをそれぞれ溶融させる。 Next, a shutter plate 7 is inserted between each evaporation source A, B and the substrate 1, and the substrate 1 is rotated at a high speed at a predetermined number of rotations. A predetermined heating voltage is supplied to each of the evaporation sources 6 and 6 to melt the tin contained in the boat 3 of the evaporation source A and the copper contained in the boat 4 of the evaporation source B, respectively.
蒸発源Aのボート3内に収容されている錫の温
度と、蒸発源Bのボート4内に収容されている銅
の温度と、基板1の回転数とを制御して、基板1
の表面に対して所定の組成の錫−銅合金薄膜、す
なわち、錫が40原子%乃至60原子%で残部が銅で
あるような組成の錫−銅合金薄膜が形成されるよ
うにする。 By controlling the temperature of tin housed in the boat 3 of evaporation source A, the temperature of copper housed in the boat 4 of evaporation source B, and the rotation speed of the substrate 1,
A tin-copper alloy thin film having a predetermined composition, that is, a tin-copper alloy thin film having a composition of 40 atomic % to 60 atomic % tin and the remainder copper is formed on the surface of the wafer.
また、基板1の表面に対して蒸発物質による真
空蒸着を行なう時間長は、基板1の表面に錫が40
原子%乃至60原子%で残部が銅であるような組成
の錫−銅合金の薄膜が所定の厚さ、例えば500〜
1000オングストローム程度の厚さに付着形成され
るような時間値に設定されるのであり、それにし
たがつてシヤツタ板7に対する開閉制御が行なわ
れる。 Further, the time length for performing vacuum evaporation with the evaporation substance on the surface of the substrate 1 is such that tin is deposited on the surface of the substrate 1 at 40%.
A thin film of tin-copper alloy having a composition of atomic% to 60 atomic% and the balance being copper is deposited to a predetermined thickness, e.g.
The time value is set so that the film is deposited to a thickness of about 1000 angstroms, and the opening and closing of the shutter plate 7 is controlled accordingly.
前記したような二元蒸着法の適用により、基板
1の表面に錫が40原子%乃至60原子%で残部が銅
であるような組成の錫−銅合金が所定の厚さの薄
膜の記録層として付着形成された後に、基板1の
回転を停止するとともに、容器中に大気を導入
し、次いで、容器中から表面に記録層が形成され
た状態の基板1を取出す。 By applying the above-mentioned binary vapor deposition method, a thin recording layer of a predetermined thickness of a tin-copper alloy having a composition of 40 atomic % to 60 atomic % tin and the remainder copper is formed on the surface of the substrate 1. After the recording layer has been deposited, the rotation of the substrate 1 is stopped, air is introduced into the container, and then the substrate 1 with the recording layer formed on its surface is taken out from the container.
基板1の表面に形成された記録層の表面に保護
層を形成することが必要な場合には、記録層の表
面に適当な合成樹脂の薄膜による保護層を被着さ
せる。前記した合成樹脂の薄膜による保護層の被
着は図示されていない蒸発源から適当な合成樹脂
材料を蒸発させることによつて行なわれるように
してもよい。基板1の表面に対して錫が40原子%
乃至60原子%で残部が銅であるような組成の錫−
銅合金を所定の厚さの薄膜の記録層として付着形
成させる手段としては、前記したような二元蒸着
法の適用の他に、スパツタリング法その他の適当
な成膜手段が採用されてもよいことは勿論である
が、基板1に対する成膜手段としてスパツタリン
グ法が採用された場合には、基板1の回転速度
と、銅のターゲツトに射突させるイオン(例えば
アルゴンイオン)のエネルギと、錫のターゲツト
に射突させるイオン(例えばアルゴンイオン)の
エネルギと、スパツタリングが行なわれるべき時
間長などを適当に設定することにより、基板1の
表面に錫が40原子%乃至60原子%で残部が銅であ
るような組成の錫−銅合金を所定の厚さの薄膜の
記録層として形成させることができる。また、ス
パツタリング法の適用による成膜に際しては、錫
と銅とのスパツタリングレートを考慮した組成の
錫−銅合金による1個のターゲツトを用いて成膜
が行なわれるようにしてもよい。 If it is necessary to form a protective layer on the surface of the recording layer formed on the surface of the substrate 1, a protective layer made of a thin film of a suitable synthetic resin is applied to the surface of the recording layer. The application of the protective layer with a thin film of synthetic resin as described above may also be carried out by evaporating a suitable synthetic resin material from an evaporation source (not shown). 40 atomic% of tin on the surface of substrate 1
Tin with a composition of 60 atomic percent to 60 atomic percent and the balance being copper.
In addition to the above-mentioned binary vapor deposition method, sputtering method or other suitable film forming method may be used as a means for depositing the copper alloy as a thin film recording layer of a predetermined thickness. Of course, if the sputtering method is adopted as a film forming method for the substrate 1, the rotational speed of the substrate 1, the energy of the ions (for example, argon ions) bombarded with the copper target, and the tin target By appropriately setting the energy of the ions (for example, argon ions) to be bombarded with the sputtering and the length of time during which sputtering should be performed, it is possible to form a surface of the substrate 1 that contains 40 to 60 atomic percent of tin and the remainder is copper. A tin-copper alloy having such a composition can be formed as a thin film recording layer of a predetermined thickness. Further, when forming a film by applying the sputtering method, the film may be formed using one target made of a tin-copper alloy whose composition takes into consideration the sputtering rate of tin and copper.
第2図は、ガラス製の基板の表面に、錫が53原
子%で残部が銅であるような組成の錫−銅合金を
500オングストロームの厚さの薄膜として被着さ
せたものにおける錫−銅合金薄膜を、45度の入射
角でHe−Neレーザ光(波長6328オングストロー
ム)を照射している状態で、前記した錫−銅合金
薄膜の温度を室温から200℃まで変化させた場合
における前記したような組成を有する錫−銅合金
の薄膜の光の反射率の変化の測定結果を示した図
である。この第2図から明らなように、錫が53原
子%で残部が銅であるような組成を有する錫−銅
合金の薄膜における光の反射率は、錫−銅合金の
薄膜の温度が120℃付近以上において顕著に変化
しており(光の透過率の変化も、錫−銅合金の薄
膜の温度が120℃付近以上において顕著に変化し
ているものとなる)また、前記の錫−銅合金の薄
膜の色調も、温度の変化に応じて変化することが
目視によつて明瞭に確認できた。 Figure 2 shows a tin-copper alloy with a composition of 53 atomic percent tin and the balance copper on the surface of a glass substrate.
A tin-copper alloy thin film deposited as a thin film with a thickness of 500 angstroms was irradiated with a He-Ne laser beam (wavelength: 6328 angstroms) at an incident angle of 45 degrees. FIG. 2 is a diagram showing the measurement results of changes in light reflectance of a tin-copper alloy thin film having the above-mentioned composition when the temperature of the alloy thin film is changed from room temperature to 200°C. As is clear from Figure 2, the reflectance of light in a thin film of a tin-copper alloy with a composition of 53 atomic percent tin and the remainder copper is as follows: (The change in light transmittance also changes significantly when the temperature of the tin-copper alloy thin film is around 120°C or higher.) It was clearly confirmed by visual observation that the color tone of the thin alloy film also changed in response to changes in temperature.
次に、合成樹脂製の基板(アクリル樹脂製の基
板)の表面に、錫が53原子%で残部が銅であるよ
うな組成の錫−銅合金を500オングストロームの
厚さの薄膜として被着させたものにおける錫−銅
合金の薄膜を、波長が8300オングストロームで径
が約1ミクロンのレーザ光のスポツトで照射して
錫−銅合金の薄膜に相変化を生じさせると、錫−
銅合金の薄膜には光の反射率、透過率の変化と、
室内光の下での目視によつても一目瞭然な色調の
変化とが生じた。 Next, on the surface of a synthetic resin substrate (acrylic resin substrate), a tin-copper alloy with a composition of 53 atomic percent tin and the balance copper is deposited as a thin film with a thickness of 500 angstroms. When a thin film of tin-copper alloy is irradiated with a laser beam spot with a wavelength of 8300 angstroms and a diameter of about 1 micron to cause a phase change in the thin film of tin-copper alloy, tin-
The copper alloy thin film has changes in light reflectance and transmittance,
Even when visually inspected under indoor light, an obvious change in color tone occurred.
そして、前記のようにして部分的に相変化を生
じさせた錫−銅合金の薄膜を走査電子顕微鏡によ
つて観察したところ、記録ドツトは全く認められ
なかつたが、このことは前記のようにレーザ光の
スポツトの照射によつて錫−銅合金の薄膜に生じ
た光の反射率、透過率の変化と、色調の変化は、
レーザ光の照射によつて錫−銅合金の薄膜の表面
に凹凸が生じることによつて起きたのではないこ
とを示している。 When the thin film of the tin-copper alloy, which had undergone a partial phase change as described above, was observed using a scanning electron microscope, no recorded dots were observed. Changes in light reflectance, transmittance, and color tone that occur in the tin-copper alloy thin film due to spot irradiation with laser light are as follows:
This shows that this is not caused by unevenness on the surface of the tin-copper alloy thin film caused by laser light irradiation.
しかし、錫−銅合金の薄膜における相変化によ
る記録ドツトは光学顕微鏡による観察によつては
色調の変化によつて明瞭に認められた。 However, recording dots due to phase change in the tin-copper alloy thin film were clearly recognized by a change in color tone when observed with an optical microscope.
次に、前記のようにしてレーザ光スポツトの照
射により相変化を生じさせた錫−銅合金の薄膜を
EPMA(Electron Probe Micro Analysis)によ
つて、それの記録部分と非記録部分とのそれぞれ
の部分における酸素量と窒素量とを測定したが、
両者間においての差は認められなかつた。このこ
とは前記のようにレーザ光のスポツトの照射によ
つて錫−銅合金の薄膜に生じた光の反射率、透過
率の変化と、色調の変化などは、レーザ光の照射
によつて錫−銅合金の薄膜に形成された記録部分
が、レーザ光の照射による加熱によつて非記録部
分とは異なる物質に変化したことによつて生じた
ものではないことを示している。 Next, a thin film of tin-copper alloy that had undergone a phase change by irradiation with a laser beam spot as described above was deposited.
The amount of oxygen and nitrogen in each of the recorded and non-recorded portions was measured using EPMA (Electron Probe Micro Analysis).
No difference was observed between the two. As mentioned above, changes in light reflectance, transmittance, and color tone that occur in a tin-copper alloy thin film due to spot irradiation with laser light are caused by tin irradiation with laser light. - This indicates that the recorded portion formed on the copper alloy thin film was not caused by being changed into a different material from the non-recorded portion due to heating by laser beam irradiation.
以上の実験結果から考えると、レーザ光のスポ
ツトの照射によつて錫−銅合金の薄膜に生じた光
の反射率、透過率の変化と、色調の変化は、レー
ザ光の照射によつて錫−銅合金の薄膜に与えられ
た熱エネルギにより、錫−銅合金の薄膜の構成物
質に原子配列の変化が生じ、それによつて錫−銅
合金の薄膜の光学的特性が記録部分と非記録部分
とにおいて変化しているものと推論される。 Considering the above experimental results, the changes in light reflectance and transmittance that occur in the tin-copper alloy thin film due to spot irradiation with laser light, as well as the changes in color tone, - Thermal energy applied to the copper alloy thin film causes a change in the atomic arrangement of the constituent materials of the tin-copper alloy thin film, thereby changing the optical properties of the tin-copper alloy thin film into recording and non-recording areas. It is inferred that there is a change in the
第3図は錫−銅合金中の錫の含有率(原子%)
の変化に対する錫−銅合金薄膜のレーザ光感度
(記録媒体に相変化を起こさせることができる強
度範囲内のレーザ光強度であつて、記録媒体にそ
の強度のレーザ光が照射された部分からの再生信
号中における2次高調波歪が極小になされる如き
レーザ光強度)の変化を示す図であるが、第3図
示の測定結果は、次の様な条件の下で得られたも
のである。 Figure 3 shows the tin content (atomic %) in the tin-copper alloy.
Laser light sensitivity of a tin-copper alloy thin film to changes in laser light intensity (laser light intensity within the intensity range that can cause a phase change in the recording medium, from the part where the recording medium is irradiated with laser light of that intensity) The measurement results shown in Figure 3 were obtained under the following conditions. .
すなわち、合成樹脂製の円盤状の基板(アクリ
ル樹脂製の円盤状の基板)の表面に、錫の含有率
が30原子%〜75原子%の範囲で残部が銅であるよ
うな組成の錫−銅合金を500オングストロームの
厚さの薄膜として被着させてなる情報記録媒体円
盤を、それの中心を回転軸に固着して毎分900回
転させ、前記した情報記録円盤における中心から
50mmの径の位置を、周波数が500KHzの信号によ
つて強度変調されている波長が8300オングストロ
ームレーザ光の径が約1ミクロンのスポツトによ
つて照射し、錫−銅合金の薄膜に500KHzの信号
を相変化によつて記録するようにした場合のもの
であり、第3図示の測定結果を得るための実験
は、錫の含有率が30原子%〜75原子%の範囲で残
部が銅であるような組成の錫−銅合金を500オン
グストロームの厚さの薄膜として被着させてなる
情報記録媒体円盤として、30原子%〜75原子%の
範囲で錫の含有率を、それぞれ異にしている如き
多数の情報記録媒体円盤を用いて行なわれたもの
である。 That is, on the surface of a disk-shaped substrate made of synthetic resin (a disk-shaped substrate made of acrylic resin), a tin composition having a tin content in the range of 30 atomic % to 75 atomic % and the balance being copper is applied. An information recording medium disk on which a thin film of copper alloy is deposited with a thickness of 500 angstroms is fixed at its center to a rotating shaft and rotated at a speed of 900 per minute.
A spot with a diameter of 50 mm is irradiated with a spot of laser light with a wavelength of 8300 angstroms whose diameter is approximately 1 micron and whose intensity is modulated by a signal with a frequency of 500 KHz, and a 500 KHz signal is applied to the tin-copper alloy thin film. The experiment to obtain the measurement results shown in Figure 3 was conducted when the tin content was in the range of 30 atomic % to 75 atomic %, with the balance being copper. Information recording medium disks are made by depositing a tin-copper alloy with the following composition as a thin film with a thickness of 500 angstroms. This was done using a large number of information recording medium disks.
第3図に示されている錫−銅合金中の錫の含有
率(原子%)の変化に対する錫−銅合金薄膜のレ
ーザ光強度の変化特性を見ると、錫−銅合金薄膜
におけるレーザ光感度は、錫−銅合金中の錫の含
有率(原子%)が40原子%〜60原子%という広い
範囲にわたつて略々一定の状態に保たれていると
いうような特性を示していることが判かる。 Looking at the change characteristics of the laser light intensity of the tin-copper alloy thin film with respect to the change in tin content (atomic %) in the tin-copper alloy shown in Figure 3, the laser light sensitivity of the tin-copper alloy thin film is shows that the tin content (atomic %) in the tin-copper alloy remains approximately constant over a wide range of 40 atomic % to 60 atomic %. I understand.
このように、錫−銅合金では錫の含有率が40原
子%〜60原子%というように広い範囲で変動して
も、錫−銅合金薄膜のレーザ光感度が略々一定に
保たれる(錫が40原子%〜60原子%という広い組
成範囲にわたつて錫−銅合金薄膜のレーザ光感度
が略々一定に保たれる)から、記録媒体の製作時
における記録層の構成物質の組成のばらつきの許
容度が広く、したがつて、記録媒体の大量生産が
容易になる。 In this way, even if the tin content in a tin-copper alloy varies over a wide range of 40 to 60 at.%, the laser light sensitivity of the tin-copper alloy thin film remains approximately constant ( The laser light sensitivity of the tin-copper alloy thin film remains approximately constant over a wide composition range of 40 at% to 60 at% tin), so it is clear that the composition of the constituent materials of the recording layer during the production of the recording medium is The tolerance for variations is wide, thus facilitating mass production of recording media.
また、前記のように記録媒体の製作時における
記録層の構成物質の組成のばらつきの許容度が広
いことから、錫及び銅の溶融固化物による錫−銅
合金のターゲツトを使用した連続インラインスパ
ツタリングによる情報記録媒円盤の製作も容易に
行なわれ得るのである。 In addition, since there is a wide tolerance for variations in the composition of the constituent materials of the recording layer during the production of recording media as mentioned above, continuous in-line sputtering using a tin-copper alloy target made from a molten solidified product of tin and copper is also possible. It is also possible to easily manufacture an information recording medium disk using a ring.
(効果)
以上、詳細に説明したところから明らかなよう
に、本発明の錫が40原子%乃至60原子%であつて
残部が銅である記録媒体用錫−銅合金では、錫の
含有率が40原子%〜60原子%というように広い範
囲で変動しても、錫−銅合金薄膜のレーザ光感度
が略々一定に保たれる(錫が40原子%〜60原子%
という広い組成範囲にわたつて錫−銅合金薄膜の
レーザ光感度が略々一定に保たれる)ものであ
り、これは従来のカルコゲナイド系や低級酸化物
系の相変化型の記録媒体では到底得ることができ
なかつたものであり、本発明の記録媒体用錫−銅
合金を用いた記録媒体は、従来の相変化型の記録
媒体に比べて大量生産が容易であり、本発明によ
り既述した従来の欠点はすべて良好に解決され
る。(Effects) As is clear from the above detailed explanation, in the tin-copper alloy for recording media of the present invention in which tin is 40 atomic % to 60 atomic % and the balance is copper, the tin content is low. The laser light sensitivity of the tin-copper alloy thin film remains almost constant even when the concentration varies over a wide range of 40 to 60 atom%.
The laser light sensitivity of the tin-copper alloy thin film remains approximately constant over a wide composition range), which is something that cannot be achieved with conventional chalcogenide-based or lower oxide-based phase change recording media. However, the recording medium using the tin-copper alloy for recording media of the present invention is easier to mass produce than conventional phase change type recording media, and the present invention allows for All previous drawbacks are successfully resolved.
第1図は成膜装置の一例の概略構成を示す斜視
図、第2図は記録媒体用錫−銅合金薄膜の温度と
光の反射率との関係を示す図、第3図は錫−銅合
金薄膜の錫の含有率とレーザ光感度との関係を示
す図である。
1……基板、2……回転軸、3,4……ボー
ト、5,6……電熱線、7……シヤツタ板、A,
B……蒸発源。
Figure 1 is a perspective view showing a schematic configuration of an example of a film forming apparatus, Figure 2 is a diagram showing the relationship between temperature and light reflectance of a tin-copper alloy thin film for recording media, and Figure 3 is a diagram showing the relationship between the temperature and light reflectance of a tin-copper alloy thin film for recording media. FIG. 3 is a diagram showing the relationship between the tin content of the alloy thin film and the laser light sensitivity. 1... Board, 2... Rotating shaft, 3, 4... Boat, 5, 6... Heating wire, 7... Shutter plate, A,
B... Evaporation source.
Claims (1)
である記録媒体用錫−銅合金。1. A tin-copper alloy for recording media, containing 40 atomic % to 60 atomic % tin and the balance being copper.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60020274A JPS61179828A (en) | 1985-02-05 | 1985-02-05 | Tin-copper alloy for recording medium |
| US06/822,037 US4704326A (en) | 1985-02-05 | 1986-01-24 | Tin alloys for recording media |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60020274A JPS61179828A (en) | 1985-02-05 | 1985-02-05 | Tin-copper alloy for recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61179828A JPS61179828A (en) | 1986-08-12 |
| JPH0119450B2 true JPH0119450B2 (en) | 1989-04-11 |
Family
ID=12022593
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60020274A Granted JPS61179828A (en) | 1985-02-05 | 1985-02-05 | Tin-copper alloy for recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61179828A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6046339A (en) * | 1983-08-24 | 1985-03-13 | Hitachi Ltd | Information recording and regenerating apparatus |
-
1985
- 1985-02-05 JP JP60020274A patent/JPS61179828A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61179828A (en) | 1986-08-12 |
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