JPS6310337A - Optical information recording and erasing device - Google Patents
Optical information recording and erasing deviceInfo
- Publication number
- JPS6310337A JPS6310337A JP61155308A JP15530886A JPS6310337A JP S6310337 A JPS6310337 A JP S6310337A JP 61155308 A JP61155308 A JP 61155308A JP 15530886 A JP15530886 A JP 15530886A JP S6310337 A JPS6310337 A JP S6310337A
- Authority
- JP
- Japan
- Prior art keywords
- erasing
- recording
- erasing light
- track
- light
- 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
Links
- 230000003287 optical effect Effects 0.000 title claims description 20
- 238000001816 cooling Methods 0.000 claims abstract description 10
- 239000000463 material Substances 0.000 claims description 12
- 238000010438 heat treatment Methods 0.000 claims description 6
- 239000000126 substance Substances 0.000 claims 1
- 238000002425 crystallisation Methods 0.000 abstract description 5
- 230000008025 crystallization Effects 0.000 abstract description 5
- 230000003685 thermal hair damage Effects 0.000 abstract description 4
- 238000010586 diagram Methods 0.000 description 11
- 238000002844 melting Methods 0.000 description 8
- 230000008018 melting Effects 0.000 description 8
- 239000010408 film Substances 0.000 description 4
- 238000010583 slow cooling Methods 0.000 description 4
- 239000000155 melt Substances 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 229910052787 antimony Inorganic materials 0.000 description 2
- WATWJIUSRGPENY-UHFFFAOYSA-N antimony atom Chemical compound [Sb] WATWJIUSRGPENY-UHFFFAOYSA-N 0.000 description 2
- 150000001786 chalcogen compounds Chemical class 0.000 description 2
- 239000013078 crystal Substances 0.000 description 2
- 229910052732 germanium Inorganic materials 0.000 description 2
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 2
- 230000001678 irradiating effect Effects 0.000 description 2
- 229910052714 tellurium Inorganic materials 0.000 description 2
- PORWMNRCUJJQNO-UHFFFAOYSA-N tellurium atom Chemical compound [Te] PORWMNRCUJJQNO-UHFFFAOYSA-N 0.000 description 2
- 239000010409 thin film Substances 0.000 description 2
- 238000002441 X-ray diffraction Methods 0.000 description 1
- NIXOWILDQLNWCW-UHFFFAOYSA-N acrylic acid group Chemical group C(C=C)(=O)O NIXOWILDQLNWCW-UHFFFAOYSA-N 0.000 description 1
- 238000000137 annealing Methods 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000001747 exhibiting effect Effects 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 150000002736 metal compounds Chemical class 0.000 description 1
- 229910044991 metal oxide Inorganic materials 0.000 description 1
- 150000004706 metal oxides Chemical class 0.000 description 1
- 230000001590 oxidative effect Effects 0.000 description 1
- 239000002952 polymeric resin Substances 0.000 description 1
- 238000002310 reflectometry Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 229920003002 synthetic resin Polymers 0.000 description 1
- 235000012976 tarts Nutrition 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
- 238000002834 transmittance Methods 0.000 description 1
- 238000004017 vitrification Methods 0.000 description 1
Landscapes
- Optical Recording Or Reproduction (AREA)
- Optical Head (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、レーザ光線の照射によって、その光学的性質
を可逆的に変化する感光性記録材料を用いた光ディスク
の情報記録部を消去する装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an apparatus for erasing the information recording portion of an optical disc using a photosensitive recording material whose optical properties are reversibly changed by irradiation with a laser beam. It is.
2 ペー、′
従来の技術
情報の訂正、書き換え可能々光ディスクとして、アクリ
ル等の高分子樹脂のディスク基板の上に、感光性材料を
薄膜の形で形成し、この光ディスクの上にレーザ照射す
ることにより加熱し、急冷と徐冷により、光学的特性す
なわち、反射率や透過率を変化させて記録、消去を行う
ものが一般に用いられている。2. Correction of conventional technical information: As a rewritable optical disc, a photosensitive material is formed in the form of a thin film on a disc substrate made of polymeric resin such as acrylic, and this optical disc is irradiated with a laser. Generally used are devices in which recording and erasing are performed by heating the recording medium and changing its optical properties, that is, reflectance and transmittance, by rapid cooling and slow cooling.
上記特性を示す記録材料として、例えばカルコゲン化合
物あるいはテルルにゲルマニウム、アンチモン等を添加
物としだ金属化合物が用いられ、これらを使って記録は
反射率の低い一般にアモルファスといわれる状態とし、
消去は加熱徐冷により反射率の高い結晶状態とすること
で、光学情報を実時間で記録、消去することができる。As a recording material exhibiting the above characteristics, for example, a chalcogen compound or a metal compound made by adding germanium, antimony, etc. to tellurium is used, and by using these, recording is made into a state generally called amorphous with low reflectance.
For erasing, optical information can be recorded and erased in real time by heating and slowly cooling it to a crystalline state with high reflectance.
光源としては、高い絞シ性能を満たし、かつ小型で直接
変調が可能な半導体レーザが一般的である。As a light source, a semiconductor laser that satisfies high aperture performance, is small, and can be directly modulated is generally used.
アモルファス記録のためには、第4図の光b1で示すよ
うな、よく絞りこまれた例えば半値幅で1μm程度のパ
ワー密度の大きい円形のレーザ光3 ページ
で記録トラック1上を照射し、第6図(A)の温度変化
図に示すように、記録材料を溶融し、急冷させるととが
必要である。これに対し消去時には、結晶化のために徐
冷する必要があるのか、第4図の光b2のような比較的
光スポット長の長い、例えば半値幅にして20μm程度
の長円光を照射し、第6図(B)の温度変化図に示した
ように徐冷し結晶化させるのが従来一般的であった。For amorphous recording, the recording track 1 is irradiated with three pages of well-focused circular laser light with a high power density of about 1 μm in half-width, as shown by light b1 in FIG. As shown in the temperature change diagram of FIG. 6(A), it is necessary to melt the recording material and rapidly cool it. On the other hand, when erasing, perhaps slow cooling is necessary for crystallization, and elongated light with a relatively long light spot length, such as light b2 in Fig. 4, for example, about 20 μm in half width, is irradiated. Conventionally, it has been common practice to slowly cool and crystallize as shown in the temperature change diagram of FIG. 6(B).
このようにして、生じた結晶状態は、固体状態での結晶
核の生成により生じたものであり、未記録部の結晶とは
、わずかながら光学定数がずれ、記録信号のこんせきを
残し、消去率が悪くなるという不都合を生じてき九〇
この不都合をさけるために、第6図で示すように長円光
の消去ビームC2の前に、比較的パワー密度の高い円形
光(以後メルト光と称する)C1を照射し、記録トラン
ク1上の情報記録部2、未記録部3を一様に溶融し、後
の長円光(以降アニール光と称する)C2により徐冷し
て確実に消去する試みがある(特開昭60−23192
8号公報)。In this way, the crystalline state that is generated is caused by the generation of crystal nuclei in the solid state, and the optical constants differ slightly from those of the crystal in the unrecorded area, leaving behind the recording signal and erasing it. In order to avoid this problem, as shown in Fig. 6, a circular light beam with a relatively high power density (hereinafter referred to as melt light) is inserted before the oblong erase beam C2, as shown in Fig. 6. ) C1 to uniformly melt the information recording part 2 and unrecorded part 3 on the recording trunk 1, and then slowly cooling it with the elliptical light (hereinafter referred to as annealing light) C2 to ensure erasing. There is (Japanese Unexamined Patent Publication No. 60-23192
Publication No. 8).
第7図(5)は前記の消去に用いられる円形のメルト光
C1の記録トラックに直交する方向のレーザ強度分布を
示したものであり、第7図(B)は記録材料薄膜の温度
分布を示したものである。メルト光としては、前記トラ
ンク幅とほぼ同等の広がりをもった情報記録部を溶融さ
せるために、レーザパワーにして16〜20 mW 、
これと対応する半値幅として、2〜3μm必要であ
り、小さいパワー例えば10 mW程度だと、確実に記
録トラック幅を溶融できず、逆に半値幅を犬きくとり、
記録トラックの幅以上を溶融するためには、上記のよう
に大きなレーザパワーが必要となってしまう。同時に、
このような形状のレーザ光を用いた場合、記録材料膜中
の最高温度を示す、記録トラック中央部の温度を、溶融
温度(Tm)より、かなり高い温度まで上昇させ、ひい
ては光ディスクの熱的損傷を生じてしまうことがあった
。Figure 7 (5) shows the laser intensity distribution of the circular melt light C1 used for erasing in the direction perpendicular to the recording track, and Figure 7 (B) shows the temperature distribution of the recording material thin film. This is what is shown. The melting light has a laser power of 16 to 20 mW, in order to melt the information recording part with a width almost equal to the trunk width.
The corresponding half-width is required to be 2 to 3 μm, and if the power is small, for example, about 10 mW, the recording track width cannot be reliably melted, and on the contrary, the half-width is too small.
In order to melt more than the width of the recording track, a large laser power is required as described above. at the same time,
When a laser beam with such a shape is used, the temperature at the center of the recording track, which indicates the highest temperature in the recording material film, is raised to a temperature considerably higher than the melting temperature (Tm), which may result in thermal damage to the optical disk. Occasionally, this may occur.
発明が解決しようとする問題点
本発明は、従来用いられてきた消去用メルト光5 ペー
ジ
による前記問題点、すなわち■ 必要レーザパワーが大
きくなること、■ 記録トラック部を必要以上に加熱し
、光ディスクの耐熱性を下げることを解決し、小パワー
が確実に記録トラックを溶融し、消し残りのない、熱的
損傷の小さい消去装置を提供するものである。Problems to be Solved by the Invention The present invention solves the above-mentioned problems caused by conventionally used melt light for erasing, namely: (1) the required laser power becomes large; (2) the recording track portion is heated more than necessary, and the optical disk This solves the problem of lowering the heat resistance of the eraser, and provides an erasing device that reliably melts recording tracks with a small amount of power, leaves no erased residue, and causes little thermal damage.
問題点を解決するだめの手段
本発明は、前記問題点を解決するために、長手方向が記
録トラックとほぼ直交するように配置した長円形の第1
の消去光を、次いで長手方向が記録トラックと同一方向
に配置した長円形の第2の消去光を順次連続して記録ト
ラック上を照射し、情報記録部を消去するようにしたも
のである。Means for Solving the Problems In order to solve the above-mentioned problems, the present invention provides an elliptical first track arranged so that its longitudinal direction is substantially orthogonal to the recording track.
The information recording section is erased by successively irradiating the recording track with a second erasing light having an oval shape whose longitudinal direction is in the same direction as the recording track.
作 用
長手方向が記録トラックとほぼ直交するようにした長円
形の第1の消去光は、記録トラック幅をほぼ均一の強度
で照射し、かつ記録トラック方向には、レーザ強度が広
がらないため、より小さなパワーで、かつ記録膜温度の
過度の昇温を抑え、記録トラック部をほぼ均一に溶融温
度まで上げて6ベーソ
溶融し、第2の長円形の消去光のトラック方向に広がっ
たレーザ強度によシ、加熱された記録膜を徐冷すること
で、溶融、徐冷による確実な消去が実施できる。The elliptical first erasing light whose longitudinal direction is approximately perpendicular to the recording track illuminates the recording track width with approximately uniform intensity, and the laser intensity does not spread in the recording track direction. With smaller power and suppressing excessive temperature rise of the recording film, the recording track portion is almost uniformly raised to the melting temperature and melted by 6B, and the laser intensity spread in the track direction of the second oval erasing light. Alternatively, by slowly cooling the heated recording film, reliable erasure can be performed by melting and slow cooling.
実施例
以下、本発明の一実施例を図面を用いて詳細に説明する
。記録媒体としては、前述のように記録前後により光学
定数の変化するもの、すなわち加熱急冷により反射率の
低いアモルファス状態とし、加熱徐冷により反射率の高
い結晶状態を生む、例えばカルコゲン化合物、あるいは
、テルル、ゲルマニウム、アンチモン等を用いた金属酸
化物を用いる。これらの記録媒体の結晶−アモルファス
の相変態は、材料の組成によって微妙に異なるが、本発
明の方法とは直接関係なく、本発明を左右するものでは
ない。又、記録状態をアモルファス、消去状態を結晶と
定めているが、逆も当然のことながら、可能であり、本
発明では、便宜上、記録状態をアモルファス、消去状態
を結晶とする。EXAMPLE Hereinafter, an example of the present invention will be described in detail with reference to the drawings. The recording medium may be one whose optical constants change before and after recording, as described above, such as a chalcogen compound, which is made into an amorphous state with low reflectivity by heating and rapidly cooling, and which produces a crystalline state with high reflectance by heating and slowly cooling, or Metal oxides using tellurium, germanium, antimony, etc. are used. The crystal-amorphous phase transformation of these recording media differs slightly depending on the composition of the material, but is not directly related to the method of the present invention and does not affect the present invention. Furthermore, although the recorded state is defined as amorphous and the erased state as crystalline, the reverse is of course possible, and in the present invention, for convenience, the recorded state is defined as amorphous and the erased state as crystalline.
最初、熱処理等で反射率の高い結晶状態とじた7ベー・
未記録の光ディスクに、ビームを絞ったパワー密度の大
きい円形光を照射して情報を記録する。First, information is recorded by irradiating a narrowed beam of circular light with high power density onto a 7B unrecorded optical disk that has been rendered into a highly reflective crystalline state through heat treatment.
例えば、1000 rpmで回転している光ディスクの
場合、光強度にして、10 mW前後、半値幅にして1
μm弱の円形光をディスク半径10crnのトランクに
照射すると、記録材料膜はよく絞られた光のために急速
に加熱せられ、かつ約100nSeCと短かい時間で、
レーザ光が通過するために急冷となり、はぼ記録トラッ
ク幅(一般に約7000A程度)と同等の幅がアモルフ
ァス化されて情報記録部(ビット)が作成される。For example, in the case of an optical disc rotating at 1000 rpm, the light intensity is around 10 mW, and the half width is 1
When circular light of a little less than μm is irradiated onto the trunk of a disk with a radius of 10 crn, the recording material film is rapidly heated due to the well-focused light, and in a short time of about 100 nSeC.
As the laser beam passes through it, it is rapidly cooled, and a width equivalent to the width of the recording track (generally about 7000 A) becomes amorphous, thereby creating an information recording section (bit).
第1図は本発明による消去光の光デイスク上の配置、お
よび形状を示したもので、長手方向が記録トラック1に
対して直交するように配置した長円形の第1の消去光a
1 と、長手方向が記録トラック1と同一線上に配置し
た第2の消去光a2 より成る。第2図(8)は前記2
つの消去光a 1 、 a 2を同一トラック上に照射
し、ディスクを回転した時のトラック上の一点の光強度
変化であり、申)はこの時の記録材料膜の温度変化の様
子を示しだものである。照射部の温度は、第1の消去光
a1 により急上昇し、融解点Tmに到達、メルトした
後、冷却されて凝固するが、第2の消去光a2により、
徐々に冷却され、結晶化温度Ta よりも高い温度で十
分長い時間保持され、結晶化される。FIG. 1 shows the arrangement and shape of the erasing light on the optical disk according to the present invention.
1 and a second erasing light a2 whose longitudinal direction is arranged on the same line as the recording track 1. Figure 2 (8) shows the above 2
This is the change in light intensity at one point on the track when two erasing beams a1 and a2 are irradiated onto the same track and the disk is rotated. It is something. The temperature of the irradiated part rises rapidly due to the first erasing light a1, reaches the melting point Tm, melts, and then cools and solidifies; however, due to the second erasing light a2,
It is gradually cooled and held at a temperature higher than the crystallization temperature Ta for a sufficiently long time to be crystallized.
記録トランクをX線回折で観測した所、第1の消去光a
1 により加熱冷却された時は記録状態と同じくトラッ
クの中心近傍はアモルファス状態となっているが、次い
で通過する第2の消去光によってガラス化温度Tq に
到達する前に冷却が押えられて、結晶化温度以上に長く
保たれるため、前記のアモルファス部分は結晶状態とな
り、消去が完了する。記録トラック上の情報記録部(ア
モルファス状態)、情報未記録部(結晶状態)の両者と
も、第1の消去光によって溶融され、液体状態となるた
め、十分に拡散し、両者の組成上の変化等、伺らの区別
も生じない。When the recording trunk was observed by X-ray diffraction, the first erasure light a
1, when the track is heated and cooled, the area near the center of the track is in an amorphous state, similar to the recording state, but the cooling is suppressed by the second erasing light that passes through the track, and the crystallization occurs before it reaches the vitrification temperature Tq. Since the amorphous portion is kept at a temperature higher than the oxidizing temperature for a long time, the amorphous portion becomes a crystalline state, and erasing is completed. Both the information recording area (amorphous state) and the non-information recording area (crystalline state) on the recording track are melted by the first erasing light and become a liquid state, so they are sufficiently diffused and a change in composition occurs between them. etc., there is no distinction between the two.
第3図(杓は、記録トラック1に直交する方向(トラッ
ク幅方向)の第1の消去光の光強度分布を示したもので
あり、第3図(6)は、第1の消去光9 ペー/゛
によって加熱された時の記録材料の最高到達温度を、同
じくトラック幅方向に対して示したものである。FIG. 3 (the ladle shows the light intensity distribution of the first erasing light in the direction perpendicular to the recording track 1 (track width direction), and FIG. 3 (6) shows the light intensity distribution of the first erasing light 9 The maximum temperature reached by the recording material when heated by the paper is also shown in the track width direction.
第2図、第3図に示した結果は、記録部材をTe6oG
e1゜5n16Au16とした光ディスクを回転し、線
速度を10 m/sec とし、第1の消去光のパワー
を10 mW 、半値幅を記録トラックと直交方向に3
μm、トラック方向に1μmとしただ円光を照射した時
、得られたものである。第3図(B)に示したように、
記録材料の最高到達温度がタルト温度に対して、比較的
される温度差にとどまっており、しかも溶融領域が、情
報記録部の幅、すなわちトラック幅よりも十分広く、確
実に溶融し、消し残りの原因となる溶融残りは生じてい
ない。The results shown in FIGS. 2 and 3 show that the recording member was Te6oG.
An optical disk made of e1゜5n16Au16 was rotated, the linear velocity was 10 m/sec, the power of the first erasing light was 10 mW, and the half-width was 3 in the direction orthogonal to the recording track.
μm, which was obtained when elliptical light with a diameter of 1 μm in the track direction was irradiated. As shown in Figure 3 (B),
The maximum temperature of the recording material remains at a relatively small temperature difference with respect to the tart temperature, and the melting area is sufficiently wider than the width of the information recording section, that is, the track width, so that it melts reliably and does not remain unerased. There was no melting residue that would cause this.
第1の消去光の記録トラック方向の半値幅はできるだけ
短い方が、光パワーは小さくてすむが、絞り込み限界に
近い半値幅1μmを短軸としただ円光に対して、長軸側
、すなわちトラックと直交方向の半値幅が、1.6〜4
μm、第1の消去光の光パワーにして7〜16rIMの
範囲で、記録トラック10”
幅を溶融し有効に前述の機能を発揮した。第2の消去光
としては、徐冷のために、長軸が記録トランク方向の長
円光であることが望ましい。詳しく説明すれば、第1の
消去光により生じたトラック幅のほぼ%〜1倍の幅のア
モルファス部を、結晶化温度に長時間保持して結晶化さ
せるだめに、短軸の半値幅1μm程度、長袖の半値幅1
0〜20μm、第1の消去光と第2の消去光との中心か
ら中心の間隔にして2〜16μm程度であれば、第2の
消去光のパワーが6〜10 mWの弱いパワーであって
も確実に結晶化できた。The shorter the half-width of the first erasing light in the recording track direction, the smaller the optical power will be. The half width in the direction perpendicular to the track is 1.6 to 4.
μm, and the optical power of the first erasing light was in the range of 7 to 16 rIM, melting the recording track 10" width and effectively exerting the above function. As the second erasing light, for slow cooling, It is desirable that the long axis is an elliptical beam in the direction of the recording trunk.To explain in detail, an amorphous portion having a width of approximately % to 1 times the track width generated by the first erasing beam is heated to a crystallization temperature for a long time. In order to hold and crystallize, the half-width of the short axis is about 1 μm, and the half-width of the long sleeve is 1 μm.
If the distance between the centers of the first erasing light and the second erasing light is about 2 to 16 μm, the power of the second erasing light is a weak power of 6 to 10 mW. was also successfully crystallized.
発明の効果
以上示したように、本発明による消去方法は、第1の消
去光を記録トラックと直交する方向に幅広くとり、かつ
トラック方向に幅狭い長円光とすることにより、確実に
記録トラック幅を溶融し、連続して照射される第2の消
去光により徐冷して結晶化させるので、小パワーで、消
し残りがなく、しかも熱損失が少ない消去が達成できる
。Effects of the Invention As shown above, in the erasing method according to the present invention, the first erasing light is made wide in the direction orthogonal to the recording track, and narrow in the track direction, so that the erasing method reliably erases the recording track. Since the width is melted and then slowly cooled and crystallized by the second erasing light that is continuously irradiated, erasing can be achieved with low power, without leaving any unerased material, and with little heat loss.
11 ベーン
第1図は本発明の一実施例の消去光の形状、配置を示す
説明図、第2図は(ハ)は消去光による記録トランク上
の一点の光強度変化特性図、(ト)は同じく記録膜の温
度変化特性図、第3図(ハ)は第1の消去光の光強度分
布図、(ロ)は温度分布図、第4図は従来の記録光消去
光の形状図、第6図(5)は記録時、(B)は消去時の
温度変化特性図、第6図は別の従来例の消去光の形状、
配置の説明図、第7図(8)は従来例の第1消去光の光
強度分布図、(B)は温度分布図である。
1・・・・・・記録トラック、2・・・・・・情報記録
部、3・・・・・・情報未記録部。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図
第2図
時開
時開
第3図
午臣r
第4図
第5図
時間
時間
第6図11 Vane FIG. 1 is an explanatory diagram showing the shape and arrangement of the erasing light according to an embodiment of the present invention, and FIG. 3(c) is a light intensity distribution diagram of the first erasing light, (b) is a temperature distribution diagram, and FIG. 4 is a shape diagram of the conventional recording light erasing light. Fig. 6 (5) is a temperature change characteristic diagram during recording, (B) is a temperature change characteristic diagram during erasing, and Fig. 6 shows the shape of erasing light in another conventional example.
An explanatory diagram of the arrangement, FIG. 7(8) is a light intensity distribution diagram of the first erasing light of the conventional example, and FIG. 7(B) is a temperature distribution diagram. 1... Recording track, 2... Information recording section, 3... Information unrecorded section. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 Time Opening Time Opening 3 Figure 4 Figure 5 Time Time Figure 6
Claims (1)
とした光ディスクにおける光照射パワーを高めて加熱急
冷させて作成した情報記録部に長手方向が記録トラック
に対して直交するように配置した長円形の第1の光ビー
ムを照射し加熱することで情報記録部を溶融し、次いで
長手方向が記録トラックと同一方向に配置した長円形の
第2の光ビームを照射し、溶融された状態から徐冷する
ことにより消去することを特徴とする光学情報記録消去
装置。In an optical disk whose recording material is a substance whose optical properties change depending on the state of light irradiation, the information recording section is created by increasing the light irradiation power and heating and rapidly cooling the information recording section, which is an ellipse arranged so that the longitudinal direction is perpendicular to the recording track. The information recording section is irradiated with a first light beam and heated to melt the information recording section, and then a second elliptical light beam whose longitudinal direction is arranged in the same direction as the recording track is irradiated to gradually remove the information from the melted state. An optical information recording/erasing device characterized by erasing information by cooling it.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61155308A JPH0685234B2 (en) | 1986-07-02 | 1986-07-02 | Optical information recording / erasing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61155308A JPH0685234B2 (en) | 1986-07-02 | 1986-07-02 | Optical information recording / erasing device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6310337A true JPS6310337A (en) | 1988-01-16 |
JPH0685234B2 JPH0685234B2 (en) | 1994-10-26 |
Family
ID=15603057
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61155308A Expired - Lifetime JPH0685234B2 (en) | 1986-07-02 | 1986-07-02 | Optical information recording / erasing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0685234B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04271019A (en) * | 1991-02-26 | 1992-09-28 | Nec Corp | Initializing device for phase change type optical disk |
-
1986
- 1986-07-02 JP JP61155308A patent/JPH0685234B2/en not_active Expired - Lifetime
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04271019A (en) * | 1991-02-26 | 1992-09-28 | Nec Corp | Initializing device for phase change type optical disk |
Also Published As
Publication number | Publication date |
---|---|
JPH0685234B2 (en) | 1994-10-26 |
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