JPS6252368B2 - - Google Patents
Info
- Publication number
- JPS6252368B2 JPS6252368B2 JP55055830A JP5583080A JPS6252368B2 JP S6252368 B2 JPS6252368 B2 JP S6252368B2 JP 55055830 A JP55055830 A JP 55055830A JP 5583080 A JP5583080 A JP 5583080A JP S6252368 B2 JPS6252368 B2 JP S6252368B2
- Authority
- JP
- Japan
- Prior art keywords
- film
- writing
- melting point
- temperature
- low
- 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
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/252—Record 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
- G11B7/257—Record 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 layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers
- G11B7/2572—Record 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 layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of organic materials
-
- 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
- G11B2007/2431—Metals or metalloids group 13 elements (B, Al, Ga, In)
-
- 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)
-
- 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
- G11B2007/24314—Metals or metalloids group 15 elements (e.g. Sb, Bi)
-
- 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
- G11B2007/24318—Non-metallic elements
- G11B2007/2432—Oxygen
-
- 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
- G11B7/252—Record 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
- G11B7/253—Record 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
- G11B7/2531—Record 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 glass
Landscapes
- Optical Record Carriers And Manufacture Thereof (AREA)
- Thermal Transfer Or Thermal Recording In General (AREA)
Description
【発明の詳細な説明】
本発明は、光記憶の分野における記憶媒体に関
するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a storage medium in the field of optical storage.
従来、光記憶媒体としては、各種の材料が提案
されているが、その中で基板上に付着せしめた金
属膜にレーザー光等によつて情報の書き込みを行
なう方法が注目されている。この種の記憶方式
は、レーザー光等の加工用ビームの熱的エネルギ
ーによつて膜にピツト(穴または凹部)を形成す
ることによつて行なうものである。 Conventionally, various materials have been proposed as optical storage media, but among these, a method of writing information on a metal film adhered to a substrate using laser light or the like is attracting attention. This type of storage method is performed by forming pits (holes or recesses) in the film using the thermal energy of a processing beam such as a laser beam.
光記憶システム全体を小形化するためには、小
形レーザーの使用が望ましく、書き込みエネルギ
ーの小さな記憶媒体が必要とされる。光記憶のピ
ツト形成に要する書き込みエネルギーは、光の吸
収率、表面の反射率、比熱、熱伝導率、書き込み
しきい温度などの種々のパラメータにより決定さ
れる。これらの中で特に書き込みしきい温度は重
要である。金属膜除去によるピツト形成の場合、
書き込みしきい温度が金属の沸点であるか融点で
あるか明確ではなく、従来低融点金属の利用が書
き込みエネルギー低減化に有効であると考えられ
ていた。このため、低融点金属で良質の膜の得ら
れるBi(融点271℃)膜を中心に検討されてき
た。また、さらに融点の低いIn(融点157℃)は
蒸着膜が島状構造となるため、単体膜では使用で
きず、SiO2などとの同時蒸着膜(サーメツト)
が使用されていた。しかし、BiあるいはInなどの
低融点金属を用いても書き込みエネルギーを大き
く低下させることはできなかつた。 In order to miniaturize the entire optical storage system, the use of small lasers is desirable and a storage medium with low writing energy is required. The writing energy required to form pits in optical storage is determined by various parameters such as light absorption, surface reflectance, specific heat, thermal conductivity, and writing threshold temperature. Among these, the writing threshold temperature is particularly important. In the case of pit formation by metal film removal,
It is not clear whether the writing threshold temperature is the boiling point or melting point of the metal, and conventionally it was thought that the use of low melting point metals was effective in reducing the writing energy. For this reason, studies have focused on Bi (melting point: 271°C) films, which are low melting point metals and provide high quality films. Furthermore, In, which has an even lower melting point (melting point 157°C), has an island-like structure in its evaporated film, so it cannot be used as a single film, and it can be used as a co-evaporated film (cermet) with SiO 2 etc.
was used. However, even if low melting point metals such as Bi or In were used, it was not possible to significantly reduce the writing energy.
本発明は、上記の欠点を除去するため、媒体膜
のピツト形成機構を追求し、ピツト形成の最初の
トリガーとして働らく層を積極的に導入し、書き
込みエネルギーを低下させたので以下説明する。 In order to eliminate the above-mentioned drawbacks, the present invention pursues the mechanism of pit formation in the medium film, actively introduces a layer that acts as an initial trigger for pit formation, and lowers the writing energy, which will be described below.
ピツト形成機構の検討では、最初に媒体膜の融
点に注目した。書き込みが金属の融点で起きると
すると、媒体をヒータなどで加熱すると、昇温と
ともに書き込みエネルギーが低下し、融点直下で
は、書き込みエネルギーは極めて小さくなるはず
である。実験を行なつた結果を第1図、第2図に
示す。第1図は、In―SiO2サーメツト膜
(SiO250体積パーセント、膜厚1000Å)を126℃
まで昇温してレーザー書き込み(Arレーザーを
使用)を行ないしきい値を調べたもので室温での
値で規格化してある。第2図は、Bi膜(膜厚700
Å)を180℃まで昇温して書き込みしきい値を調
べたものである。第2図中、白丸はピツト形成、
黒丸は酸化である。両者ともに書き込みしきい値
は室温における結果と変わりない。但し、Bi薄膜
は酸化されやすく、レーザー照射部で酸化が起こ
り変色する。第1図、第2図より、Bi,Inなどの
低融点金属を用いてもレーザー書き込みは融点で
は為されずかなり高温であることが明らかであ
り、沸点(Inは〜2000℃,Biは〜1500℃)まで昇
温されている可能性がある。すなわち、書き込み
時には、第3図のような温度分布になつていて高
温部は溶融状態にあると考えられ、ピツトの形成
は、沸点に達した中心部が蒸発して微小な穴を作
り、その後は液体の表面張力により微小な穴が拡
大され、融点以上に加熱された部分がピツトとな
る。このように、従来の単層の金属膜にピツトを
形成するには、金属膜の一部を沸点まで昇温する
エネルギーを要したわけである。本発明は、低沸
点物質が共存しているならば、それが気化するこ
とでトリガーとなり、比較的低温でピツト形成で
きるという考えに基づくものである。 In examining the pit formation mechanism, we first focused on the melting point of the media film. Assuming that writing occurs at the melting point of the metal, when the medium is heated with a heater or the like, the writing energy decreases as the temperature rises, and just below the melting point, the writing energy should become extremely small. The results of the experiment are shown in FIGS. 1 and 2. Figure 1 shows an In-SiO 2 cermet film (SiO 2 50 volume percent, film thickness 1000 Å) heated at 126°C.
The threshold value was investigated by laser writing (using an A r laser) at a temperature raised to 100°C, and is normalized to the value at room temperature. Figure 2 shows the Bi film (thickness 700 mm).
Å) was heated to 180°C and the write threshold was investigated. In Figure 2, white circles indicate pit formation.
Black circles are oxidation. In both cases, the write threshold is the same as the result at room temperature. However, the Bi thin film is easily oxidized, and oxidation occurs in the laser irradiated area, resulting in discoloration. From Figures 1 and 2, it is clear that even if low melting point metals such as Bi and In are used, laser writing is not done at the melting point, and the temperature is quite high, and the boiling point (In is ~2000℃, Bi is ~ The temperature may have been raised to 1500℃. In other words, at the time of writing, the temperature distribution is as shown in Figure 3, and the high-temperature part is considered to be in a molten state, and the formation of pits occurs when the center reaches the boiling point and evaporates, creating a minute hole. The tiny holes are enlarged by the surface tension of the liquid, and the part heated above the melting point becomes a pit. In this way, forming pits in a conventional single-layer metal film requires energy to raise the temperature of a portion of the metal film to its boiling point. The present invention is based on the idea that if a low boiling point substance coexists, its vaporization will act as a trigger, allowing pit formation at a relatively low temperature.
一実施例を第4図に示すが、安定性が良く、蒸
着の容易な材料である有機色素のフタロシアニン
1をガラス基板2上に蒸着し、In―SiO2サーメツ
ト膜3を積層した。このような光記憶媒体にレー
ザー光を照射すると、フタロシアニン1に沸とう
部4が生じてトリガーとなり、同時にIn―SiO2サ
ーメツト膜3に溶融部5が生じてピツトが形成さ
れる。また、他の一実施例としてガラス基板上に
フタロシアニン、Bi膜を積層した。低沸点のフタ
ロシアニンをトリガー層として積層した効果を第
5図に示す。第5図は媒体をヒーターで加熱し
て、レーザー書き込みしきい値を調べたものであ
る。第5図中、白丸がIn―SiO2,黒丸がBiであ
る。In―SiO2サーメツト膜、Bi膜とも媒体温度の
上昇とともに書き込みしきい値が低下しており、
外挿して書き込み温度を求めると〜400℃前後と
なり、フタロシアニンの沸点で書き込みが為され
ている事は明らかである。ここで、第5図におい
て〜150℃以上でBiに対する測定点が外挿線より
下がつているのは、第2図と同様にBiが酸化され
ていることを示している。書き込まれたピツトを
観察すると、書き込みエネルギーが大きすぎる場
合には、金属膜、フタロシアニン膜の両方同時に
穴が開いているが、書き込みエネルギーが適正な
場合にはフタロシアニン膜には観察できるような
ピツトは形成されず、金属膜のみに読み出しに十
分な大きさ(〜1μm径程度)のピツトが形成さ
れる。なお、室温におけるしきい値は、In―SiO2
サーメツト膜、Bi膜でほぼ同じ値であり、また、
トリガー層を積層しない場合に比較し〜65%に低
下している。書き込みに要する光エネルギーは、
ここまで述べてきた書き込み温度の他に、表面の
反射率、比熱、熱伝導率などで決まるが、これら
を総合したものがIn―SiO2サーメツト膜とBi膜で
ほぼ同じであることを示している。但し、Bi膜
は、きわめて酸化しやすく、100℃以下でも簡単
に劣化してしまうため、実用に供するのは困難で
ある。単元素の金属膜では、他に適当な融点を有
するものはないが、さらに書き込みエネルギーを
低下させるために、ピツトを形成する金属膜とし
て、Bi,Pb,Snを主成分とする一群の低融点合
金を用いることができる。Bi単体は酸化されやす
いが、Pb,Sn等と合金化したものは酸化されに
くくなる。 An example is shown in FIG. 4, in which an organic dye phthalocyanine 1, which is a material with good stability and easy vapor deposition, was vapor-deposited on a glass substrate 2, and an In--SiO 2 cermet film 3 was laminated thereon. When such an optical storage medium is irradiated with a laser beam, a boiling part 4 is generated in the phthalocyanine 1, which acts as a trigger, and at the same time, a melting part 5 is generated in the In--SiO 2 cermet film 3, forming a pit. In addition, as another example, phthalocyanine and Bi films were laminated on a glass substrate. Figure 5 shows the effect of laminating a low-boiling point phthalocyanine as a trigger layer. In FIG. 5, the laser writing threshold was investigated by heating the medium with a heater. In Fig. 5, the white circles are In--SiO 2 and the black circles are Bi. For both the In-SiO 2 cermet film and the Bi film, the writing threshold value decreases as the medium temperature increases.
When the writing temperature is determined by extrapolation, it is around 400°C, and it is clear that writing is performed at the boiling point of phthalocyanine. Here, in FIG. 5, the measurement points for Bi at temperatures above 150° C. are lower than the extrapolated line, which indicates that Bi is oxidized as in FIG. 2. Observing the written pits, if the writing energy is too large, holes will be formed in both the metal film and the phthalocyanine film at the same time, but if the writing energy is appropriate, there will be no visible pits in the phthalocyanine film. However, pits with a size sufficient for readout (about 1 μm in diameter) are formed only in the metal film. Note that the threshold value at room temperature is In―SiO 2
The values are almost the same for the cermet film and the Bi film, and
This is ~65% lower than when no trigger layer is laminated. The light energy required for writing is
In addition to the writing temperature mentioned above, it is determined by the surface reflectance, specific heat, thermal conductivity, etc., and it has been shown that the total value of these is almost the same for the In-SiO 2 cermet film and the Bi film. There is. However, Bi films are extremely susceptible to oxidation and deteriorate easily even below 100°C, making it difficult to put them to practical use. There is no single-element metal film that has an appropriate melting point, but in order to further reduce the writing energy, we used a group of low-melting-point metal films containing Bi, Pb, and Sn as main components to further reduce the writing energy. Alloys can be used. Bi alone is easily oxidized, but alloyed with Pb, Sn, etc. is less likely to be oxidized.
この一実施例として、金属膜にBi―Pb―Sn―
Inの共晶合金(融点〜60℃)とSiO2の同時蒸着に
よるサーメツト膜を用いた。この場合にも、フタ
ロシアニンを積層すると、同様の効果が得られ書
き込みしきい値はフタロシアニンを積層したIn―
SiO2サーメツト膜に比べ〜50%に低下し、Biの
単層膜に比べると〜30%のきわめて小さな書き込
みしきい値となる。 As an example of this, Bi-Pb-Sn-
A cermet film made by co-evaporating an In eutectic alloy (melting point ~60°C) and SiO 2 was used. In this case as well, if phthalocyanine is laminated, a similar effect can be obtained, and the write threshold is
The write threshold is ~50% lower than that of a SiO 2 cermet film, and ~30% compared to a single layer Bi film.
上記実施例では、トリガー層としてフタロシア
ニンを用いたが、本発明のトリガー層はフタロシ
アニンのみに限定されるものではなく、他の低沸
点物質たとえばニトロセルロースなども含むもの
である。但し、発明の趣旨から明らかなように、
トリガー層の沸点は、ピツトを形成する金属膜の
融点より高い事が必要である。また、トリガー層
として、熱分解により揮発性物質を放出する物質
を用いる場合にも本発明は同様に適用できるもの
である。 In the above embodiments, phthalocyanine was used as the trigger layer, but the trigger layer of the present invention is not limited to only phthalocyanine, but may also include other low-boiling substances such as nitrocellulose. However, as is clear from the purpose of the invention,
The boiling point of the trigger layer needs to be higher than the melting point of the metal film forming the pits. Furthermore, the present invention is similarly applicable to the case where a substance that releases volatile substances through thermal decomposition is used as the trigger layer.
また、実施例ではガラス板上の媒体膜とトリガ
ー層の関係について述べたが、ガラス板に代つて
比較的低沸点あるいは、低温で分解しやすい基板
を用いるならば、基板に直接に媒体膜を付着する
方法もとれ、同様の効果が得られる。この場合に
は、基板のごく表面の蒸発を利用するもので、媒
体作製工程を簡略化することができる。このため
の基板としては、ポリメチルメタクリレート
(PMMA)が分解温度(350℃)で揮発性物質を
放出するので利用できる。但し、書き込みエネル
ギーが大き過ぎると基板自体も大きな損傷を受け
るので、ごく表面層のみが分解するような適正な
書き込みエネルギーを用いる必要がある。 In addition, although the relationship between the media film on the glass plate and the trigger layer was described in the example, if a substrate with a relatively low boiling point or that is easily decomposed at low temperatures is used instead of the glass plate, the media film can be directly applied to the substrate. The same effect can be obtained by other methods of adhesion. In this case, the evaporation of the very surface of the substrate is utilized, and the medium manufacturing process can be simplified. Polymethyl methacrylate (PMMA) can be used as a substrate for this purpose, as it releases volatile substances at its decomposition temperature (350°C). However, if the writing energy is too large, the substrate itself will be seriously damaged, so it is necessary to use an appropriate writing energy that will only decompose the very surface layer.
以上説明したように、金属膜除去による光記憶
において、金属膜をその沸点まで昇温する必要が
ないため、書き込みしきい値をきわめて小さくで
きる。また、低融点金属あるいは低融点合金を媒
体膜として使用する場合に、低融点である特徴を
有効に生かすことができる。 As explained above, in optical storage by removing a metal film, there is no need to raise the temperature of the metal film to its boiling point, so the write threshold can be made extremely small. Further, when a low melting point metal or a low melting point alloy is used as the medium film, the characteristic of a low melting point can be effectively utilized.
金属膜の光吸収は、可視光領域、近赤外領域の
波長において波長依存性が小さいため、使用する
レーザー波長に対してほとんど限定がない。さら
に、トリガー層に使用する物質については沸点の
みに注目すればよく、有機色素の単体膜の場合の
ように光吸収のピーク波長を使用するレーザー波
長に合致させる必要がない。 Since the light absorption of a metal film has little wavelength dependence in the visible light region and near-infrared region, there is almost no limitation on the laser wavelength used. Furthermore, with regard to the substance used in the trigger layer, it is only necessary to pay attention to the boiling point, and there is no need to match the peak wavelength of light absorption with the wavelength of the laser used, unlike in the case of a single film of organic dye.
以上のように、本発明の光記憶媒体は、多くの
利点を有するものである。 As described above, the optical storage medium of the present invention has many advantages.
第1図は、In―SiO2同時蒸着膜の書き込みしき
い値の媒体温度依存性の一例を示す特性図、第2
図は、Bi膜の書き込みしきい値の媒体温度依存性
の一例を示す特性図、第3図は、書き込み時の温
度分布の一例を示す特性図、第4図は、本発明の
一実施例の模式図、第5図は、本発明実施例の媒
体の書き込みしきい値の媒体温度依存性の一例を
示す特性図である。
1…フタロシアニン、2…基板、3…In―SiO2
サーメツト膜。
Figure 1 is a characteristic diagram showing an example of the medium temperature dependence of the writing threshold value of the In-SiO 2 co-deposited film.
The figure is a characteristic diagram showing an example of the medium temperature dependence of the writing threshold of a Bi film, FIG. 3 is a characteristic diagram showing an example of temperature distribution during writing, and FIG. 4 is an example of the present invention. FIG. 5 is a characteristic diagram showing an example of the dependence of the write threshold value on the medium temperature of the medium according to the embodiment of the present invention. 1...phthalocyanine, 2...substrate, 3...In-SiO 2
Cermet membrane.
Claims (1)
物質よりなる層と、この層の沸点若しくは分解温
度より低い融点を有しピツトが形成される金属膜
が積層して設けられる光記憶媒体において、ピツ
トが形成される金属膜がInとSiO2の混合物から
なるか、若しくは、Bi,Pb,Snを主成分とする
低融点合金とSiO2の混合物からなることを特徴
とする光記憶媒体。1. An optical storage medium in which a layer made of a low boiling point substance or a low decomposition temperature substance and a metal film having a melting point lower than the boiling point or decomposition temperature of this layer and in which pits are formed are laminated on a substrate, An optical storage medium characterized in that a metal film on which pits are formed is made of a mixture of In and SiO2, or a mixture of a low melting point alloy containing Bi, Pb, and Sn as main components and SiO2.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5583080A JPS56153543A (en) | 1980-04-26 | 1980-04-26 | Light storage medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5583080A JPS56153543A (en) | 1980-04-26 | 1980-04-26 | Light storage medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56153543A JPS56153543A (en) | 1981-11-27 |
| JPS6252368B2 true JPS6252368B2 (en) | 1987-11-05 |
Family
ID=13009880
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5583080A Granted JPS56153543A (en) | 1980-04-26 | 1980-04-26 | Light storage medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56153543A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58112790A (en) * | 1981-12-28 | 1983-07-05 | Ricoh Co Ltd | Optical information recording member |
| US4551828A (en) * | 1983-03-18 | 1985-11-05 | Minnesota Mining And Manufacturing Company | Quadrilayer optical draw medium |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| NL7809159A (en) * | 1977-09-29 | 1979-04-02 | Philips Nv | INFORMATION REGISTRATION ELEMENT WITH DYE CONTAINING AUXILIARY LAYER. |
-
1980
- 1980-04-26 JP JP5583080A patent/JPS56153543A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56153543A (en) | 1981-11-27 |
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