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JPS62281133A - Optical disk - Google Patents

Optical disk

Info

Publication number
JPS62281133A
JPS62281133A JP61123757A JP12375786A JPS62281133A JP S62281133 A JPS62281133 A JP S62281133A JP 61123757 A JP61123757 A JP 61123757A JP 12375786 A JP12375786 A JP 12375786A JP S62281133 A JPS62281133 A JP S62281133A
Authority
JP
Japan
Prior art keywords
information
layer
recording
recording layer
recorded
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
JP61123757A
Other languages
Japanese (ja)
Other versions
JPH0572018B2 (en
Inventor
Ryutaro Tanaka
田中 龍太郎
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
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 filed Critical Toshiba Corp
Priority to JP61123757A priority Critical patent/JPS62281133A/en
Publication of JPS62281133A publication Critical patent/JPS62281133A/en
Publication of JPH0572018B2 publication Critical patent/JPH0572018B2/ja
Granted legal-status Critical Current

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  • Thermal Transfer Or Thermal Recording In General (AREA)
  • Optical Record Carriers And Manufacture Thereof (AREA)

Abstract

PURPOSE:To easily make the erasure of a bit of information impossible by providing a substrate layer formed with a material forming a bubble at a heating part by heating due to at least the radiation of a light beam, and a recording layer which is laminated on the substrate, and on which the recording and the erasure of the bit of information can be performed repeatedly. CONSTITUTION:A substrate layer 2 consisting of the material which is laminated on a substrate 1, and forms the bubble at the heating part by the heating due to at least the radiation of the light beam, and a recording layer 3 which is laminated on the substrate layer 2, and on which the recording and the erasure of the bit of information can be performed repeatedly, are provided. In case of making impossible the erasure of the bit of recorded information recorded on the recording layer 3, by projecting the light beam on the recording layer 3, by projecting the light beam on the substrate layer 2 part corresponding to the recording part of the recording layer 3, and heating the part, a bubble 7 is formed at the substrate layer of the heated part, and the bubble remains as it is after being cooled. The reproduction of the bit of information can be easily performed according to a difference between the formed part, and unformed part of the bubble 7. In this way, it is possible to make the erasure of the bit of information impossible.

Description

【発明の詳細な説明】 3、発明の詳細な説明 [発明の目的] (産業上の利用分野) 本発明は、光学的に情報の記録を(テう光ディスクに関
づるものである。
[Detailed Description of the Invention] 3. Detailed Description of the Invention [Object of the Invention] (Field of Industrial Application) The present invention relates to an optical disc on which information is optically recorded.

(従来の技術) 光ディスクは、高密度、大容昂の記録媒体として注目さ
れ、画像情報のファイルや電子計算機の外部メモリ等と
して広く普及している。
(Prior Art) Optical disks have attracted attention as high-density, large-capacity recording media, and are widely used as image information files, external memories for electronic computers, and the like.

この光ディスクには、再生専用タイプとユーザが書き込
める追記型(DRAW: DirectRead  A
 fter  W rijc)と呼ばれるタイプと(肖
去可能タイプとがあり、近年、情報を操り返して記録、
消去できる消去可能タイプがその利便性ゆえに広く普及
しつつある。
This optical disc has a read-only type and a write-once type (DRAW: Direct Read A).
There are two types: one type called ``retrieval'' and the other type, which can be used to record information by manipulating information.
Erasable types are becoming more popular due to their convenience.

消去可能タイプの光ディスクとしては、記録・消去方法
により、光磁気型、相変化型等が知られている。光磁気
型は例えば、非晶質希土類−遷移金立合金薄膜の垂直磁
化方向を記録部と未記録部とで変えて、情報の記録をし
、これらの部分の反射光のカー回転角の差を検出して情
報の再生をしている。
As erasable type optical discs, magneto-optical types, phase change types, etc. are known depending on the recording/erasing method. For example, the magneto-optical type records information by changing the perpendicular magnetization direction of an amorphous rare earth-transition metal alloy thin film between recorded and unrecorded areas, and calculates the difference in the Kerr rotation angle of reflected light from these areas. Detecting and reproducing information.

また、相変化型は記9:層を結晶から非結晶質へ相転移
させて記録を行い、記録がされた非結晶部分かと記録が
されていない結晶部分との反射率の違いを読み取って再
生している。
In addition, the phase change type is described in 9. Recording is performed by changing the phase of the layer from crystal to amorphous, and the difference in reflectance between the recorded amorphous part and the unrecorded crystal part is read and reproduced. are doing.

ところで、上述のような消去可能な光ディスクを使用す
る際に、記録情報の秘密性、安全性等を考慮して登録さ
れたコード番号の者のみが情報の再生を可能とするため
に、光デイスク使用者個有のコードを登録したり、また
、ディスク内部のアドレス情報等のように、消去される
と困る情報もある。
By the way, when using an erasable optical disc such as the one mentioned above, the optical disc is There is also information that would be problematic if erased, such as the registration of a code unique to the user and address information inside the disc.

従来より、消去可能な光ディスクに記録された情報を消
去不能にする試みとして、強力なレーザビームを照射し
て、記録層の記録部に穴を形成する方法等もある。しか
しながら、一般に光ディスクは記録層の酸化、劣化等を
防止するために上下両面からSiC等から成る保護層が
設けられており、穴の形成は困難である。また、穴を形
成するためにレーデビームの出力を高めることは、一般
の半導体レーザの出力30〜501RWを越えてしまう
といった問題点があった。
Conventionally, as an attempt to make information recorded on an erasable optical disk non-erasable, there has been a method of irradiating a powerful laser beam to form a hole in the recording portion of the recording layer. However, in general, optical discs are provided with protective layers made of SiC or the like on both upper and lower surfaces in order to prevent oxidation, deterioration, etc. of the recording layer, making it difficult to form holes. Further, there is a problem in that increasing the output of the Radhe beam to form the hole exceeds the output of a general semiconductor laser, which is 30 to 501 RW.

(発明が解決しようとする問題点) 上述のように、従来の消去可能タイプの光ディスクにあ
っては、記録情報の消去を不可能にする機能を合せ持つ
のが困難であった。
(Problems to be Solved by the Invention) As described above, it is difficult for conventional erasable type optical discs to have a function that makes it impossible to erase recorded information.

本発明は上記事情に基づいたもので、その目的は、この
種の光ディスクにおいて、容易に情報の消去を不能にす
ることができる光ディスクを提供することにある。
The present invention is based on the above-mentioned circumstances, and its object is to provide an optical disc of this type in which information can be easily erased.

[発明の構成1 (問題点を解決するための手段) 上記問題点を解決するために本発明は、基体上に積層さ
れ、少なくとも光ビームの照射による加熱によって加熱
部分にバルブを形成する材料で形成された下地層と、 この下地層上に積層され、繰り返して情報の記録・消去
が可能な記録層とを有する。
[Structure 1 of the Invention (Means for Solving the Problems) In order to solve the above problems, the present invention provides a material that is laminated on a substrate and forms a bulb in the heated portion by heating by at least irradiation with a light beam. It has a formed base layer and a recording layer that is laminated on the base layer and allows information to be recorded and erased repeatedly.

(作用) 記録層が光磁気型の場合には、未記録部分に対する記録
部分の垂filti化方向を可逆的に逆方向、同一方向
にさせて情報の記録・消゛去がされる。
(Function) When the recording layer is of a magneto-optical type, information is recorded and erased by reversibly making the perpendicular filtration direction of the recorded portion to the opposite direction to the unrecorded portion and to the same direction.

また、記録層が相変化型の場合には、記録部分を非晶質
と結晶質との間で可逆的に相転移させて情報の記録・消
去がされる。
Further, when the recording layer is of a phase change type, information is recorded and erased by reversibly changing the phase of the recording portion between amorphous and crystalline states.

一方、記録層に記録された記録情報の消去を不能にする
場合、記録層の記録部分に対応する下地層部分に光ビー
ムを照射して加熱すると、この加熱部分の下地層にバブ
ルが形成される。このバブルは冷却後もそのままの形で
維持される。
On the other hand, in order to make it impossible to erase the recorded information recorded on the recording layer, if a light beam is irradiated and heated on the underlayer part corresponding to the recorded part of the recording layer, bubbles will be formed in the underlayer at this heated part. Ru. This bubble remains in its shape even after cooling.

情報の再生は、バブル形成部分と未形成部分との反射率
の違いにより容易に行うことができる。
Information can be easily reproduced due to the difference in reflectance between the bubble-formed portion and the non-bubble-formed portion.

(実施例) 以下、本発明に係る光ディスクの一実施例を説明する。(Example) An embodiment of the optical disc according to the present invention will be described below.

第1図は本発明に係る光ディスクの第1実施例(実施例
−1)の断面構成を示しており、この光′ディスクは、
基板1、下地層2、第1の保F4層4a、記録層3、第
2の保護層4bおよび反!31−5が順番に積層されて
円板状に形成されている。
FIG. 1 shows a cross-sectional configuration of a first embodiment (Example-1) of an optical disc according to the present invention, and this optical disc has the following features:
The substrate 1, the underlayer 2, the first F4 retaining layer 4a, the recording layer 3, the second protective layer 4b, and the anti! 31-5 are laminated in order to form a disk shape.

基板1は、アクリル、エポキシ、ポリカーボネート(P
C) 、ポリイミド、ポリアミド等の有機樹脂材料やガ
ラス、AQ203、ZrO2等で形成された透明基板で
ある。
The substrate 1 is made of acrylic, epoxy, polycarbonate (P
C) A transparent substrate made of an organic resin material such as polyimide or polyamide, glass, AQ203, ZrO2, or the like.

下地Fi2は、プラズマ重合膜であり、CI−14(メ
タン)、C21(a(エタン)、C3H8(プロパン)
、C2H4(エヂレン) 、S! 1−14  (モノ
シラン)等のガスを単独で、または混合して形成するか
、あるいはこれらの単独ガスまたは混合ガス中に02.
03 、NH3、CO2,802(CN)2等の親水性
官能基を形成するガスを混合して形成したものである。
The base Fi2 is a plasma polymerized film, and includes CI-14 (methane), C21 (a (ethane), C3H8 (propane))
, C2H4 (Ejiren), S! 02.1-14 (monosilane) or the like alone or in a mixture, or in these gases alone or in a mixture thereof.
It is formed by mixing gases that form hydrophilic functional groups such as 03, NH3, CO2, and 802 (CN)2.

これらの親水性官能基を形成するガスを混入するのは無
機材料で形成された保護層4aや記録層3との親和力を
増して剥離を防止するためである。
The reason for mixing the gas that forms these hydrophilic functional groups is to increase the affinity with the protective layer 4a and the recording layer 3 formed of inorganic materials and to prevent peeling.

vylの保護層4aおよび第2の保M層4bは、3i0
や5i02等の無機誘電体材料をスパッタ法または蒸着
法にて19さ5o〜5000Aで形成したちのである。
The protective layer 4a and the second M retention layer 4b of Vyl are 3i0
An inorganic dielectric material such as 5i02 or 5i02 is formed by sputtering or vapor deposition to a thickness of 19 x 50 to 5000 amps.

これら!!1i4a 、4bにより記録層3の酸化や光
ビーム照射時における記8層3の蒸発による穴の形成が
防止される。
these! ! 1i4a and 4b prevent the formation of holes due to oxidation of the recording layer 3 and evaporation of the layer 3 during light beam irradiation.

本実施例の記録層3は、基板1而に対して垂直の磁気異
方性を有する薄膜であり、Tbj”cCo、Gd Tb
 Fe 、Gd Fe Co等の非晶質希土類−遷移金
属等、種々の材料から選択される。その膜厚は数10A
〜数1000Aである。
The recording layer 3 of this example is a thin film having magnetic anisotropy perpendicular to the substrate 1, and includes Tbj"cCo, Gd Tb
It is selected from various materials such as amorphous rare earth-transition metals such as Fe, GdFeCo, etc. The film thickness is several tens of amps
~ several thousand A.

反射層5は、Cu、Δ髪、Au等の金属で厚さ1000
A程度で積層されている。この反射層3により基板3側
から照射されたレーザビームのうち、記録層3で反射さ
れずに通過した光をすべて基板1 ff1lに反射ざじ
ることができ、そのため、記録層3からの反射光と反射
層5からの反射光とが重量され、その多重干渉効果によ
り記録感度が大幅に向上する。
The reflective layer 5 is made of metal such as Cu, Δhair, Au, etc. and has a thickness of 1000 mm.
Laminated at about A. This reflective layer 3 allows all of the light that passes through the recording layer 3 without being reflected from the laser beam irradiated from the substrate 3 side to be reflected onto the substrate 1ff1l, so that the reflected light from the recording layer 3 and the reflected light from the reflective layer 5, and the multiple interference effect greatly improves the recording sensitivity.

以上の構成を有する光ディスクにおいて、情報の記録は
、第2図に示すように、まずあらかじめ一定方向に磁化
された記録層3に記録情報信号に応じて変調されたレー
ザビームを集光させて、照射ビット部6の温度を上昇さ
せ、次いで、この光ディスクの磁化方向と逆の外部磁界
1−1を加える。
In the optical disc having the above configuration, information is recorded by first focusing a laser beam modulated according to a recording information signal on the recording layer 3, which has been magnetized in a certain direction in advance, as shown in FIG. The temperature of the irradiation bit section 6 is raised, and then an external magnetic field 1-1 opposite to the magnetization direction of the optical disk is applied.

照射ビット部6の温度がキュリ一点以上になった時点で
記録層3の照射ビット部6の磁化方向が反転し、この反
転状態が常温でも維持されることによって記録がされる
When the temperature of the irradiated bit portion 6 reaches the Curie point or above, the magnetization direction of the irradiated bit portion 6 of the recording layer 3 is reversed, and this reversed state is maintained even at room temperature, thereby recording is performed.

記録情報の再生は、再生用レーザビームを基板1側から
照射し、記録層3からの反射光のうち、記録ビット部と
記録がされていない部分のカー回転角の差を検出して光
強度を測定することでなされる。
To reproduce recorded information, a reproduction laser beam is irradiated from the substrate 1 side, and the difference in the Kerr rotation angle between the recorded bit part and the unrecorded part of the light reflected from the recording layer 3 is detected to determine the light intensity. This is done by measuring the

また、記録情報の消去は、記録層3の最初の磁化方向く
記録がされていない部分の磁化方向)に磁界を加え、消
去すべき記録ビット部をキュリ一点以上に加熱してその
磁化方向を元に戻ぼばよい。
In order to erase the recorded information, a magnetic field is applied to the initial magnetization direction of the recording layer 3 (the magnetization direction of the unrecorded part), and the recorded bit part to be erased is heated to more than one Curie point to change the magnetization direction. Just go back.

一方、記録情報の消去を不能にするには、第3図に示す
ように、情報が記録された記録ビット部に、記録用レー
ザビームより高いパワーのレーザビームL2を照射し、
下地層2にバブル7を形成する。このバブル7が形成さ
れると、従来の再生専用タイプの光ディスクと同様の読
取装置を使用して精欧よく情報を読み取ることが可能と
なる。
On the other hand, in order to make it impossible to erase the recorded information, as shown in FIG.
Bubbles 7 are formed in the base layer 2. Once this bubble 7 is formed, it becomes possible to read the information efficiently using a reading device similar to that used for conventional read-only type optical discs.

第6図は本発明に係る光ディスクの他の実施例(実施例
−2)の断面構成を示しており、この光ディスクは、基
板1、下地層2、記録層3及び保護層4を順番に積層し
て円板上に形成されている。
FIG. 6 shows a cross-sectional configuration of another embodiment (Example 2) of the optical disc according to the present invention, and this optical disc consists of a substrate 1, an underlayer 2, a recording layer 3, and a protective layer 4 laminated in this order. It is formed on a disk.

上記基板1、下地層2及び保護層4は前記第1の実施例
と同一構成である。
The substrate 1, base layer 2, and protective layer 4 have the same structure as in the first embodiment.

上記記録層3は、例えばレーザビームの照射による加熱
によって結晶と非晶質との間で可逆的に相転移する金属
や半導体材料で形成されている。
The recording layer 3 is made of a metal or semiconductor material that undergoes a reversible phase transition between crystal and amorphous when heated, for example, by laser beam irradiation.

その材料としては、Te1TeGe、InSb等種々の
材料から選択される。
Its material is selected from various materials such as Te1TeGe and InSb.

上記構成において、情報の記録は、例えば記録情報で変
調されたレーザビームを記録層に照射して急速加熱、急
速冷即することより、レーザビーム照射部分の記8層が
例えば結晶から非晶質へと相転移することでなされる。
In the above configuration, information is recorded by, for example, irradiating the recording layer with a laser beam modulated by the recorded information and quickly heating and cooling the recording layer, so that the 8th layer in the laser beam irradiated area changes from crystal to amorphous, for example. This is done by undergoing a phase transition to .

また、記録の消去は、記録がされた非晶質部分に消去用
のレーザビームを照射して加熱した後、徐冷することに
より、再び結晶へ戻すことでなされる。さらに、情報の
再生は再生用のレーザビームを照射して、情報が記録さ
れた非晶質部分と記録されていない結晶部分との反射率
の違いを読み取ることで成される。
Further, erasing of a record is performed by irradiating the recorded amorphous portion with an erasing laser beam to heat it, and then slowly cooling it to transform it back into a crystal. Furthermore, information is reproduced by irradiating a reproduction laser beam and reading the difference in reflectance between the amorphous portion where information is recorded and the crystalline portion where information is not recorded.

一方、記録された情報の消去を不能にするには、前記実
施例と同様に、シー11−ビームの出力、パルス幅を高
くして記録ビット部に照)1して下地層2にバブル7を
形成すればよい。これにより、記録の消去が不能になり
、長期間安定して記録状態が維持できる。また、情報の
再生が容易となる。
On the other hand, in order to make it impossible to erase the recorded information, as in the previous embodiment, the output and pulse width of the sea beam 11 are increased to illuminate the recorded bit area) and the bubble 7 is applied to the underlayer 2. All you have to do is form. This makes it impossible to erase the recording, and the recorded state can be stably maintained for a long period of time. Furthermore, information can be easily reproduced.

以下、具体的な実施例についてM(明する。Hereinafter, specific examples will be explained.

(実施例−1) PC64脂製のJJ板1を使用し、回転台(図示せず)
に取付け、反応容器を真空に排気したi(、CO2を分
圧比で196含有する3iH4ガスを導入し、基板1に
所定の高周波電力を役人して3iH4ガスによるプラズ
マ重合膜(下地層2)を積層した。その膜厚は1000
0Δで形成した。
(Example-1) A JJ board 1 made of PC64 resin was used, and a rotating table (not shown) was used.
The reaction vessel was evacuated, 3iH4 gas containing 196% CO2 was introduced, and a predetermined high frequency power was applied to the substrate 1 to form a plasma polymerized film (base layer 2) using the 3iH4 gas. Laminated.The film thickness is 1000
It was formed at 0Δ.

次いで、スパッタ法にてSioから成る第1の保護層4
aを膜厚500人で積層した。
Next, a first protective layer 4 made of Sio is formed by sputtering.
A was laminated with a film thickness of 500 layers.

また、第1の保M F!A 4 a上にTb Fe C
oから成る光磁化膜を膜厚500人で形成し、記録層3
を形成した。
Also, the first protection midfielder! A 4 Tb Fe C on a
A photomagnetic film consisting of
was formed.

次いで、この記録層3上にSiOから成る第2の保護層
4bを膜1g500 Aで積層し、さらに、この保護層
4b上にΔ女から成る反射層5を膜厚1000Aで積層
して第1図に示した光ディスクを作成した。
Next, on this recording layer 3, a second protective layer 4b made of SiO is laminated with a film thickness of 1 g and 500 Å, and on this protective layer 4b, a reflective layer 5 made of ΔF is laminated with a thickness of 1000 Å. The optical disc shown in the figure was created.

上)ホしたようにして形成された光ディスクに出力(I
llW)及びパルス幅を変えたレーザービームを照射し
てその特性を調べた。なJ3、この場合、外部印加磁界
は2000e一定とした。
Top) Output (I
llW) and a laser beam with different pulse widths were irradiated to investigate its characteristics. In this case, the externally applied magnetic field was constant at 2000e.

その結果、第4図に示すように、領域へでは、記録層3
に同ら変化は生じず、情報の記録ができなかった。
As a result, as shown in FIG.
No change occurred, and no information could be recorded.

また、C領域では、記録層3の磁化が反転し情報の記録
ができ、また、レーザ出力及びパルス幅を変えた消去用
のレーザビームを照射することで記録の消去がでさた。
Furthermore, in the C region, the magnetization of the recording layer 3 was reversed and information could be recorded, and the recording could be erased by irradiation with an erasing laser beam with varying laser output and pulse width.

このC領域では、下地層2にはバブルは発生していなか
った。
In this region C, no bubbles were generated in the base layer 2.

さらに、C領域では記録層3の磁化が反転し情報の記録
ができるとともに、下地層2にバブルが形成され、この
バブルは冷却後もそのままの状態で帷)コされていた。
Furthermore, in the C region, the magnetization of the recording layer 3 is reversed and information can be recorded, and bubbles are formed in the underlayer 2, and these bubbles remain as they are even after cooling.

そして、領11i!Bにおける再生特性として、反射率
30%、カー回転角0.6dec+ 、C/N比50d
 B (1、25MHz ) 、!=にメT優しu、l
Lf!7ることができた。
And territory 11i! The reproduction characteristics of B are: reflectance 30%, Kerr rotation angle 0.6 dec+, C/N ratio 50 d.
B (1,25MHz),! = nimeT kind u, l
Lf! I was able to do 7 things.

一方、下地層(Sit−I4+C○2プラズマ重合膜)
2が形成されたナンプルと、下地層2が形成されていな
いサンプルの双方を、湿度65 ’C、相対湿度90%
RH下で環境試験を行い、反射率変化(R/Ro)を調
べた。
On the other hand, the base layer (Sit-I4+C○2 plasma polymerized film)
Both the sample on which No. 2 was formed and the sample on which no base layer 2 was formed were heated at a humidity of 65'C and a relative humidity of 90%.
An environmental test was conducted under RH to examine the change in reflectance (R/Ro).

その結果、第5図に示すように、図中実線で示ずように
下地層2を有する勺ンブルは、15日経過後でも記録層
3に外見上何ら変化は見られなかった。 一方、下地g
J2が無いナンブルでは、PC樹脂基板1と下地層2と
の間に剥離が生じ、反射率が低下し、−15日経過後で
は、初期の反射率ROの約40%に低下していることが
判明した。
As a result, as shown in FIG. 5, no change in the appearance of the recording layer 3 was observed even after 15 days had elapsed in the recording layer 2 having the underlayer 2 as shown by the solid line in the figure. On the other hand, the base G
With the number without J2, peeling occurs between the PC resin substrate 1 and the base layer 2, and the reflectance decreases, and after -15 days, the reflectance has decreased to about 40% of the initial reflectance RO. found.

(実施例−2) PC樹脂製の基板1上にCH4ガスによるプラズマ重合
膜を3000△の厚さに積層して下地層2を形成した。
(Example 2) A base layer 2 was formed by laminating a plasma polymerized film using CH4 gas to a thickness of 3000Δ on a substrate 1 made of PC resin.

次いで、下地層2上に2元同時スパッタ法により、1n
ターゲツトとsbツタ−ットに投入する高周波電力を調
整してIn5oSb5oから成る記録層3を500△の
厚さで形成した。
Next, a 1n layer was deposited on the base layer 2 by dual simultaneous sputtering
The recording layer 3 made of In5oSb5o was formed with a thickness of 500Δ by adjusting the high frequency power applied to the target and the sb target.

次いで、記録層3上にスパッタ法でSiOから成る保護
層4を500Aの厚さで積層して、第4図に示した光デ
ィスクを得た。
Next, a protective layer 4 made of SiO was laminated to a thickness of 500 Å on the recording layer 3 by sputtering to obtain the optical disc shown in FIG. 4.

このようにして形成された光ディスクにレーザビームを
照射し、シー11出力、パルス幅を変化させてその特性
を調べた。
The optical disc thus formed was irradiated with a laser beam, and its characteristics were investigated by varying the output of the optical disc 11 and the pulse width.

その結束、第7図に示すように、へ領域では、照射後の
冷W速度が比較的遅く、InSbが結晶化して、その反
射率が低下していることが判明した。
As shown in FIG. 7, it was found that the cold W velocity after irradiation was relatively slow in the region, and InSb was crystallized, resulting in a decrease in the reflectance.

また、C領域では、記録層の冷却速度が比較的速く、I
nSbが非結晶化して、反射率が上界していることが判
明した。
In addition, in the C region, the cooling rate of the recording layer is relatively fast, and the I
It was found that nSb was amorphous and the reflectance was upper bound.

さらに、CI域では、CH4プラズマ重合膜(下地層)
がガス化してバブル7が形成されていることが判明した
Furthermore, in the CI region, CH4 plasma polymerized film (base layer)
It was found that bubble 7 was formed by gasification.

従って、本実施例の光ディスクにおいて、消去可能な情
報は、C領域で記録、AvA賊で消去すればよく、消去
を不能にするためにはC領域のレーザビームを照射寸れ
ばよいことが判明した。なお、C領域では記録層3に何
ら変化を生じなかった。
Therefore, in the optical disc of this example, it is clear that erasable information can be recorded in the C area and erased using AvA, and in order to make erasure impossible, it is sufficient to irradiate the C area with a laser beam. did. Note that no change occurred in the recording layer 3 in area C.

次に、この光ディスクの記録・消去を繰り返した特性を
記録用及び消去用のレーデビームの各出力、パルス幅を
それぞれ10m W、 50nscc及び3111’v
V、1μSQCで調べた。
Next, the characteristics of this optical disk after repeated recording and erasing are determined by measuring the outputs and pulse widths of the radar beams for recording and erasing at 10 mW, 50 nscc, and 3111'v, respectively.
V, examined by 1μSQC.

その結果、第8図に示すように、最初の5〜10回当り
で反射率の上昇はみられるが、その後は一定し、104
回の繰り返し後でも変化せず反射率が安定していること
が判明した。
As a result, as shown in Figure 8, an increase in reflectance was observed for the first 5 to 10 times, but after that it remained constant and 104
It was found that the reflectance remained stable even after repeated use.

[発明の効果] 以上説明したように、本発明の光ディスクによれば、基
体上に光ビームの照射加熱によりバブルを形成する下地
層を積層する構成としたので、容易に情報を消去不能に
することができる。そのため、光ディスクの応用範囲が
広がりその利便性が向上する。
[Effects of the Invention] As explained above, according to the optical disc of the present invention, since the base layer is laminated on the substrate to form bubbles by irradiation and heating with a light beam, information cannot be easily erased. be able to. Therefore, the range of applications of the optical disc is expanded and its convenience is improved.

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

第1図は本発明に係る光ディスクの一実施例の構成を示
す断面図、第2図は第1図の光ディスクの情報記録原理
を説明する図、第3図は第1図の光ディスクのバブル形
成状態を示す断面図、第4図は第1図実施例の光ディス
クの照射パルス幅−出力特性を示す図、第5図は第1図
実施例の環境試験の結果を示す図、第6図は本発明に係
る光ディスクの池の実施例の構成を示す断面図、第7図
は第6図実施例の光ディスクの照射パルス幅−出力特性
を示す図、第8図は第6図実施例の記録、消去繰り返し
特性を示す図である。 1・・・基板 2・・・下地層 3・・・記録層 4.4a、41)・・・保護層 5・・・反0−J層 7・・・バブル
FIG. 1 is a sectional view showing the configuration of an embodiment of the optical disc according to the present invention, FIG. 2 is a diagram explaining the information recording principle of the optical disc of FIG. 1, and FIG. 3 is a bubble formation of the optical disc of FIG. 1. 4 is a diagram showing the irradiation pulse width-output characteristics of the optical disk of the embodiment in FIG. 1, FIG. 5 is a diagram showing the results of the environmental test of the embodiment in FIG. 1, and FIG. 7 is a cross-sectional view showing the structure of an embodiment of the optical disc according to the present invention, FIG. 7 is a diagram showing the irradiation pulse width-output characteristics of the optical disc of the embodiment of FIG. 6, and FIG. 8 is a record of the embodiment of FIG. 6. , is a diagram showing erase repetition characteristics. 1... Substrate 2... Base layer 3... Recording layer 4.4a, 41)... Protective layer 5... Anti-0-J layer 7... Bubble

Claims (3)

【特許請求の範囲】[Claims] (1)基体上に積層され、少なくとも光ビームの照射に
よる加熱によつて加熱部分にバブルを形成する材料から
成る下地層と、 この下地層上に積層され、繰り返して情報の記録・消去
が可能な記録層とを有することを特徴とする光ディスク
(1) A base layer made of a material that is laminated on the substrate and forms bubbles in the heated area when heated by at least light beam irradiation; and a base layer that is laminated on this base layer and allows information to be repeatedly recorded and erased. An optical disc characterized by having a recording layer.
(2)前記下地層は、CH_4、C_2H_6、C_3
H_8、C_2H_8、C_2H_4、SiH_4の単
独ガスまたはそれらの混合ガスによるプラズマ重合膜で
あることを特徴とする特許請求の範囲第1項に記載の光
ディスク。
(2) The base layer is CH_4, C_2H_6, C_3
The optical disc according to claim 1, wherein the optical disc is a plasma polymerized film using a single gas of H_8, C_2H_8, C_2H_4, SiH_4 or a mixture thereof.
(3)前記下地層はCH_4、C_2H_6、C_3H
_8、C_2H_8、C_2H_4、SiH_4の単独
ガスまたはそれらの混合ガスにO_2、O_3、NH_
3、CO_2、SO_2(CN)_2等の親水性官能基
を形成するガスを混合したガスによるプラズマ重合膜で
あることを特徴とする特許請求の範囲第1項に記載の光
ディスク。
(3) The base layer is CH_4, C_2H_6, C_3H
_8, C_2H_8, C_2H_4, SiH_4 alone or a mixture thereof with O_2, O_3, NH_
3. The optical disc according to claim 1, which is a plasma polymerized film made of a gas mixed with a gas forming a hydrophilic functional group such as CO_2, SO_2(CN)_2, etc.
JP61123757A 1986-05-30 1986-05-30 Optical disk Granted JPS62281133A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61123757A JPS62281133A (en) 1986-05-30 1986-05-30 Optical disk

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61123757A JPS62281133A (en) 1986-05-30 1986-05-30 Optical disk

Publications (2)

Publication Number Publication Date
JPS62281133A true JPS62281133A (en) 1987-12-07
JPH0572018B2 JPH0572018B2 (en) 1993-10-08

Family

ID=14868545

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61123757A Granted JPS62281133A (en) 1986-05-30 1986-05-30 Optical disk

Country Status (1)

Country Link
JP (1) JPS62281133A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63200334A (en) * 1987-02-13 1988-08-18 Tdk Corp Optical recording medium
JPH02139732A (en) * 1988-08-26 1990-05-29 Taiyo Yuden Co Ltd Optical recording medium and its manufacture
JPH02168446A (en) * 1988-09-01 1990-06-28 Taiyo Yuden Co Ltd Optical information recording medium
FR2884032A1 (en) * 2005-03-29 2006-10-06 Commissariat Energie Atomique IRREVERSIBLE OPTICAL RECORDING MEDIUM BY FORMING BUBBLES HAVING LIMITED HEIGHT BY THE GENERANT GAS SOURCE

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63200334A (en) * 1987-02-13 1988-08-18 Tdk Corp Optical recording medium
JPH02139732A (en) * 1988-08-26 1990-05-29 Taiyo Yuden Co Ltd Optical recording medium and its manufacture
JPH02168446A (en) * 1988-09-01 1990-06-28 Taiyo Yuden Co Ltd Optical information recording medium
FR2884032A1 (en) * 2005-03-29 2006-10-06 Commissariat Energie Atomique IRREVERSIBLE OPTICAL RECORDING MEDIUM BY FORMING BUBBLES HAVING LIMITED HEIGHT BY THE GENERANT GAS SOURCE
WO2006103340A3 (en) * 2005-03-29 2007-05-03 Commissariat Energie Atomique Irreversible optical recording medium by formation of bubbles having a height limited by the gas source generating them
JP2008535133A (en) * 2005-03-29 2008-08-28 コミサリア、ア、レネルジ、アトミク Irreversible optical recording medium by formation of bubbles limited in height by a gas source generating bubbles
US7903536B2 (en) 2005-03-29 2011-03-08 Commissariat A L'energie Atomique Irreversible optical recording medium by formation of bubbles having a height limited by the gas source generating them
KR101178083B1 (en) 2005-03-29 2012-08-30 엠피오 인터내셔날 Irreversible optical recording medium by formation of bubbles having a height limited by the gas source generating them

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