JPS6342035A - Recording method for information to optical information recording medium - Google Patents

Recording method for information to optical information recording medium

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Publication number
JPS6342035A
JPS6342035A JP61185194A JP18519486A JPS6342035A JP S6342035 A JPS6342035 A JP S6342035A JP 61185194 A JP61185194 A JP 61185194A JP 18519486 A JP18519486 A JP 18519486A JP S6342035 A JPS6342035 A JP S6342035A
Authority
JP
Japan
Prior art keywords
information
recording medium
optical information
laser light
information recording
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.)
Pending
Application number
JP61185194A
Other languages
Japanese (ja)
Inventor
Nobuhiko Sakai
酒井 順彦
Kenichi Saito
斉藤 憲一
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.)
Dai Nippon Printing Co Ltd
Original Assignee
Dai Nippon Printing Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Dai Nippon Printing Co Ltd filed Critical Dai Nippon Printing Co Ltd
Priority to JP61185194A priority Critical patent/JPS6342035A/en
Publication of JPS6342035A publication Critical patent/JPS6342035A/en
Pending legal-status Critical Current

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  • Optical Recording Or Reproduction (AREA)
  • Thermal Transfer Or Thermal Recording In General (AREA)

Abstract

PURPOSE:To easily form accurate information pits even on an optical information recording medium of low scanning speed by interruptedly projecting a laser light as a pulse light. CONSTITUTION:In case of formation of one information pit, the laser light is projected interruptedly, namely, as the pulse light when a spot S scans an extent (x). Consequently, the outline of the formed information pit is waved and is not linear, but trouble of reading is not especially caused. Thus, information pits are formed without reducing the laser light power even in case of a low scanning speed, and the flat area of a graph can be used as the control area similarly to write on a recording medium of high scanning speed, and the pit width is accurately controlled.

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は光情報記録媒体への情報記録方法、特にレーザ
光を用いて光t1報記録カードに記録を行うのに適した
情報記録方法に関する。
[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention is a method for recording information on an optical information recording medium, particularly suitable for recording on an optical t1 information recording card using a laser beam. related to information recording methods.

(従来の技術) 現在、光デイスク装置をはじめ、光学的に情報の記録再
生を行う装置が普及している。これらの装置では、情報
記録媒体に微小な情報ピットを形成することによって情
報の記録が行われる。この情報ピットは、一般にレーザ
光の走査によって形成される。
(Prior Art) Currently, devices that optically record and reproduce information, including optical disk devices, are in widespread use. In these devices, information is recorded by forming minute information pits on an information recording medium. This information pit is generally formed by scanning with laser light.

(発明が解決しようと16問題点) 近年、新しい光情報記録媒体として、光情報記録カード
が注目されている。ところがこのような光情報記録カー
ドに情報ピットを形成する場合、従来の光ディスク等に
用いた方法では、正確な情報ピットの形成が困難である
という問題が生じる。
(16 Problems to be Solved by the Invention) In recent years, optical information recording cards have been attracting attention as a new optical information recording medium. However, when forming information pits on such an optical information recording card, a problem arises in that it is difficult to form accurate information pits using the method used for conventional optical discs.

この問題は走査速度の相違に起因する。例えば光ディス
クの場合、直径2001の光ディスクを50 Orl)
IIIの回転速度で回転させてレーザ光を走査したとす
れば、最外周トラックの走査速度は約520cm/se
cとなる。これに対し、光情報記録カードでは、走査速
度はたかだか8〜101/sec程度であり、オーダが
2桁近く小さくなる。
This problem is due to differences in scanning speed. For example, in the case of an optical disc, an optical disc with a diameter of 2001 is 50 Orl)
If the laser beam is scanned by rotating at the rotation speed of III, the scanning speed of the outermost track is approximately 520 cm/sec.
c. On the other hand, in the case of an optical information recording card, the scanning speed is at most about 8 to 101/sec, which is about two orders of magnitude smaller.

このように走査速度が遅くなると、情報ピット幅の制御
が非常に困難になるということが、実験的に確認されて
いる。この実験結果を第3図および第4図に示す。第3
図は走査速度の速い光ディスクに情報ピットを形成する
場合のレーザ光パワーと形成されるピット幅との関係を
示すグラフ、第4図は走査速度の遅い光情報記録カード
に情報ピットを形成する場合の同じグラフであり、いず
れちテルルを用いた合金薄膜から成る媒体に、波長80
0〜830Mのレーザを照射した場合の特性グラフであ
る。媒体となる材質によつ【多少の相違はあるものの、
現在一般に用いられている光学的記録媒体では、はぼ同
じ特性が得られる。グラフに示されているように、レー
ザ光パワーが所定のしきい値WT□を越えるとピット形
成が行われ、パワーの増加とともに形成されるピット幅
も大きくなる。ただ、第3図の場合に比べ第4図の場合
は走査速度が近いため(前述のように2桁程度のオーダ
だけ異なる)、同じレーザ光パワーを与えると後者の方
がピット幅は大きくなる。
It has been experimentally confirmed that when the scanning speed decreases in this way, it becomes extremely difficult to control the information pit width. The results of this experiment are shown in FIGS. 3 and 4. Third
The figure is a graph showing the relationship between laser light power and pit width when forming information pits on an optical disk with a fast scanning speed, and Figure 4 shows the relationship between forming information pits on an optical information recording card with a slow scanning speed. These are the same graphs of
It is a characteristic graph when 0-830M laser is irradiated. Depending on the material of the medium [although there are some differences,
Almost the same characteristics can be obtained with optical recording media commonly used today. As shown in the graph, pits are formed when the laser beam power exceeds a predetermined threshold value WT□, and as the power increases, the width of the formed pits also increases. However, since the scanning speed in Figure 4 is similar to that in Figure 3 (as mentioned above, the difference is only about two orders of magnitude), the pit width will be larger in the latter when the same laser light power is applied. .

さて、実際に形成される情報ピットは第2図に示すよう
に走査方向XにtllJQいピットとなる。ここでピッ
トixはレーザ光の走査期間によって制御できるが、ピ
ット幅yはレーザ光パワーによって制御しなければなら
ない。通常このピット幅yは、1〜1.5μm程度に制
御される。ここで第3図のグラフを参照すると、ピット
幅を1〜1.5μmとするには、レーザ光パワーをa−
bの間に制御すればよい。ところが第4図のグラフでは
、同じくピット幅を1〜1.5μmとするには、レーザ
光パワーをc−dの間に制御しなくてはならない。即ち
、光情報記録カードの場合は、レーザ光パワーの調整範
囲が狭くなり、正確なピット幅の制御が困難となるので
ある。切言すれば、第3図ではグラフのフラットな領域
をit、+1111範囲として用いることができるのに
対し、第4図ではグラフの立上りの領域を制御範囲とし
て用いねばならないのである。従って光情報記録カード
に正確な幅を持ったピットの形成を行う場合には、レー
ザ光の安定性および記録媒体感度の均一性の条件がより
厳しく要求されることになる。
Now, the information pits actually formed are tllJQ pits in the scanning direction X, as shown in FIG. Here, the pit ix can be controlled by the scanning period of the laser beam, but the pit width y must be controlled by the laser beam power. Usually, this pit width y is controlled to about 1 to 1.5 μm. Referring to the graph in Figure 3, in order to make the pit width 1 to 1.5 μm, the laser light power should be adjusted to a-
It is sufficient if the control is performed during the period b. However, in the graph of FIG. 4, in order to similarly set the pit width to 1 to 1.5 μm, the laser light power must be controlled between c and d. That is, in the case of an optical information recording card, the adjustment range of the laser light power becomes narrow, making it difficult to accurately control the pit width. To put it bluntly, in FIG. 3, the flat region of the graph can be used as the it, +1111 range, whereas in FIG. 4, the rising region of the graph must be used as the control range. Therefore, when forming pits with accurate widths on optical information recording cards, more stringent conditions are required for the stability of the laser beam and the uniformity of the sensitivity of the recording medium.

そこで本発明は、走査速tηの遅い光情報記録媒体に対
しても正確な情報ピットの形成を容易に行うことができ
る情報記録方法を提供りることを目的とする。
Therefore, an object of the present invention is to provide an information recording method that can easily form accurate information pits even on an optical information recording medium with a slow scanning speed tη.

〔発明の構成〕[Structure of the invention]

(問題点を解決するための手段) 本発明は、レーザ光を所定方向に走査し、光情報記録媒
体上に細長い情報ピットを形成する光情報記録媒体への
情報記録方法において、レーザ光をパルス光として断続
的に照射するようにし、走査速度の遅い光情報記録媒体
に対しでも正確な情報ピットの形成を容易に行うことが
できるようにしたものである。
(Means for Solving the Problems) The present invention provides a method for recording information on an optical information recording medium in which a laser beam is scanned in a predetermined direction to form elongated information pits on the optical information recording medium. By irradiating light intermittently, it is possible to easily form accurate information pits even on optical information recording media with slow scanning speeds.

(作 用) 従来、光ディスク等に対しての情報ピットの書込みは、
レーザ光を連続照射しながら走査を行っていた。しかし
ながら、光情報記録カード等の走査速度の遅い記録媒体
については、同じ方法を適用するとレーザ光パワーを低
下させねばならない。
(Function) Conventionally, writing information pits on optical discs, etc.
Scanning was performed while continuously irradiating laser light. However, if the same method is applied to a recording medium with a slow scanning speed, such as an optical information recording card, the laser light power must be reduced.

mlち、所定の波長、所定のスポット径のレーザ光を用
いて書込みを行う場合に、レーザ光パワーをP、レーザ
のスポット径をω、レーザ照射時間をtとすれば、記録
媒体が受けた単位面積あたりのエネルギff1Eは、近
似的に式(1)で表わせる。
ml, when writing is performed using a laser beam of a predetermined wavelength and a predetermined spot diameter, if the laser beam power is P, the laser spot diameter is ω, and the laser irradiation time is t, then the recording medium receives Energy per unit area ff1E can be approximately expressed by equation (1).

E初P−t/ω     ・・・・・・・・・・・・・
・・・・・・・・・・・(1)ここで記録媒体の走査速
度を■とJるとt−ω/V  ・・・・・・・・・・・
・・・・・・・・・・・・・・・・・・・(2)と表わ
せることが知られでいるので、この関係を式(1)に代
入すれば、 E絢P/Vω  ・・・・・・・・・・・・・・・・・
・・・・・・・・・・(3)が得られる。即ち、走査速
度■が遅くなれば、同じレーザ光パワーPを用いて記録
しても、記録媒体が受ける単位面積あたりのエネルギm
Eは大きくなる。従って、エネルギーBEを適正値に保
つためにはPを低下せねばならないのである。
E first P-t/ω ・・・・・・・・・・・・・・・
・・・・・・・・・・・・(1) Here, if the scanning speed of the recording medium is ■ and J, then t-ω/V ・・・・・・・・・・・・
It is known that it can be expressed as (2), so by substituting this relationship into equation (1), we get E絢P/Vω・・・・・・・・・・・・・・・・・・
......(3) is obtained. In other words, if the scanning speed () becomes slower, even if the same laser light power P is used for recording, the energy per unit area received by the recording medium will be
E becomes larger. Therefore, in order to keep the energy BE at an appropriate value, P must be lowered.

このようにレーザ光パワーPを低下させると、レーザ光
パワーとピット幅との関係を示すグラフ上の変動の激し
い立上りのf!i域を制御21I領域としなければなら
ないことは前述のとおりである。
When the laser light power P is reduced in this way, the f! As mentioned above, the i area must be the control 21I area.

本発明による方法では、レーザ光をパルス光として継続
的に照射しながら走査を行うようにしたため、走査速度
が遅くなってもレーザ光パワーを低下させずに情報ピッ
トの形成を行うことができ、走査速度の速い記録媒体に
書込みを行う場合と同様、グラフのフラットな領域を制
御領域とし一〇用いることができ、ピッ1−幅の正確な
制御が可能となる。
In the method according to the present invention, since scanning is performed while continuously irradiating laser light as pulsed light, information pits can be formed without reducing the laser light power even if the scanning speed becomes slow. As in the case of writing on a recording medium with a high scanning speed, the flat area of the graph can be used as a control area, making it possible to accurately control the pitch width.

(実施例) 以下本発明を図示する実施例にL!づいて脱刷づ“る。(Example) Examples illustrating the present invention will be described below. It will then be deprinted.

従来の方法で1つの情報ピットを形成する場合は、第2
図に示すようにスポットSをXの距離だけ走査する際、
レーザ光を連続照射させることになる。これに対し本発
明に係る方法では、第1図に示すようにスポットSをX
の距離だけ走査する際、レーザ光を断続照射、即ち、パ
ルス光として照射させることになる。従って本発明に係
る方法では、形成された情報ピットの輪郭線は波状とな
り、直線にはならないが、読取り上特に問題は生じない
When forming one information pit using the conventional method, the second
As shown in the figure, when scanning the spot S by a distance of X,
Laser light is continuously irradiated. On the other hand, in the method according to the present invention, the spot S is
When scanning a distance of , the laser beam is irradiated intermittently, that is, as pulsed light. Therefore, in the method according to the present invention, although the contour line of the formed information pit is wavy and not a straight line, no particular problem arises in reading it.

第5図は、光情報記録カードに本発明に係るパルス光と
してレーザ光を照射して情報ピットを形成する場合のレ
ーザ光パワーと形成されるピット幅との関係を示すグラ
フである。このグラフは第3図および第4図に用いた書
込み系と同様の書込み系を用い、デユーティ比70%の
レーザ光を照射して書込みを行った結果得られた実測値
である。
FIG. 5 is a graph showing the relationship between the laser light power and the width of the pits formed when information pits are formed by irradiating the optical information recording card with laser light as pulsed light according to the present invention. This graph is an actual value obtained as a result of writing using a writing system similar to that used in FIGS. 3 and 4 and irradiating a laser beam with a duty ratio of 70%.

ピット幅を1〜1.5μmとするには、レーザ光パワー
をe−fの間に制御すればよいことがわかる。制御領i
ii!(e−f)としてグラフのフラットな領域を用い
ることがぐきるため、第4図に示す従来の方法(制@領
域C〜d)に比べ制御領域がかなり広くなる。従ってレ
ーザ光の不安定性、記録媒体感度の不均一性が生じた書
込み系においても正確なピット幅をもった情報ピットの
形成が可能である。
It can be seen that in order to set the pit width to 1 to 1.5 μm, the laser light power may be controlled between e and f. control area i
ii! Since it is possible to use a flat region of the graph as (e-f), the control region becomes considerably wider than the conventional method (control@regions C to d) shown in FIG. Therefore, it is possible to form information pits with accurate pit widths even in a writing system where instability of the laser beam and non-uniformity of the sensitivity of the recording medium occur.

なおパルス光のデユーティ比(断続供給されるパルス光
1周期に対して光照射の行われている111間の占める
割合)は、情報ピットが1つの連続した閉領域を形成し
つる程度に選ばなければならない。即ち、第1図に示す
ように、デユーティ比を小さくすると1つのスポットS
1とこれに隣接するスポットS2との距離が離れるよう
になるため、両スポットが完全に分離してしまう程デ1
−ティ比を下げた場合、もは費1つの情報ピットの形成
を行うことができなくなってしまうのである。従ってデ
ユーティ比はある程度以上下げることはできない。形成
される情報ピットの輪郭線をなめらかにするためには、
デユーティ比はできるだけ大きくとるのが望ましい。と
ころがデユーティ比をあまり高くすると本発明の効果が
低減してくることになる(極端な場合、デユーティ比を
100%とすれば連続光となり、従来方法と変らなくな
る)。一般にはデユーティ比50〜80%にとるのが最
も好ましい。
The duty ratio of the pulsed light (the ratio of 111 periods of light irradiation to one cycle of pulsed light that is intermittently supplied) must be selected to such an extent that the information pits form one continuous closed region. Must be. That is, as shown in FIG. 1, when the duty ratio is decreased, one spot S
1 and the adjacent spot S2 become farther apart, so that the distance between the spots S2 and S2 increases to the point where the two spots are completely separated.
- If the tee ratio is lowered, it will no longer be possible to form one information pit. Therefore, the duty ratio cannot be lowered beyond a certain level. In order to smooth the outline of the information pit that is formed,
It is desirable that the duty ratio be as large as possible. However, if the duty ratio is made too high, the effect of the present invention will be reduced (in an extreme case, if the duty ratio is set to 100%, continuous light will be produced, no different from the conventional method). Generally, it is most preferable to set the duty ratio to 50 to 80%.

なお本発明に係る方法を実fJ@するにあたっては、半
導体レーザを書込み用光源どするのが好ましい。
In carrying out the method according to the present invention, it is preferable to use a semiconductor laser as a writing light source.

半導体レーザの場合、パルス駆動を容易に行うことがで
き、また連続駆動に比べて寿命が延びるというメリット
も得られる。
In the case of a semiconductor laser, pulse driving can be easily performed, and it also has the advantage of having a longer life than continuous driving.

(発明の効果) 以上のとおり本発明によれば、パルス光を用いて情報ピ
ットの形成を行うようにしたため、走査速度の遅い記録
媒体に対しても広いピッ1−幅制御領域を確保でき、正
1AIなピット幅制御を行うことができる。
(Effects of the Invention) As described above, according to the present invention, since information pits are formed using pulsed light, a wide pitch width control area can be secured even for a recording medium with a slow scanning speed. Positive 1AI pit width control can be performed.

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

第1図は本発明に係る記録方法の原理図、第2図は従来
の記録方法の原理図、第3図は光ディスクに従来方法で
書込みを行った場合の制ti領域を示すグラフ、第4図
は光情報記録カードに従来方法で書込みを行った場合の
制御領域を示すグラフ、第5図は光情報記録カードに本
発明に係る記録方法で書込みを行った場合のai制御領
域を示すグラフである。 S、Sl、S2・・・レーザ光のスポット、X・・・情
報ピット長、y・・・情報ピット幅、WTll・・・し
きい値。 出願人代理人  佐  藤  −雄 第1図 第2図
FIG. 1 is a diagram of the principle of the recording method according to the present invention, FIG. 2 is a diagram of the principle of the conventional recording method, FIG. 3 is a graph showing the restricted area when writing to an optical disc by the conventional method, The figure is a graph showing the control area when writing is performed on an optical information recording card using the conventional method, and FIG. 5 is a graph showing the ai control area when writing is performed on the optical information recording card using the recording method according to the present invention. It is. S, Sl, S2... Laser light spot, X... Information pit length, y... Information pit width, WTll... Threshold. Applicant's agent Mr. Sato Figure 1 Figure 2

Claims (1)

【特許請求の範囲】 1、レーザ光を所定方向に走査し、光情報記録媒体上に
前記所定方向に細長い情報ピットを形成する情報記録方
法において、前記レーザ光をパルス光として断続的に照
射することを特徴とする光情報記録媒体への情報記録方
法。 2、情報ピットが、1つの連続した閉領域を形成するよ
うに、前記パルス光のデューティ比を選択することを特
徴とする特許請求の範囲第1項記載の光情報記録媒体へ
の情報記録方法。 3、パルス光のデューティ比が50〜80%であること
を特徴とする特許請求の範囲第2項記載の光情報記録媒
体への情報記録方法。 4、光情報記録媒体が光情報記録カードであることを特
徴とする特許請求の範囲第1項乃至第3項のいずれかに
記載の光情報記録媒体への情報記録方法。 5、レーザ光の光源として半導体レーザを用いることを
特徴とする特許請求の範囲第1項乃至第4項のいずれか
に記載の光情報記録媒体への情報記録方法。
[Claims] 1. An information recording method in which laser light is scanned in a predetermined direction to form elongated information pits in the predetermined direction on an optical information recording medium, in which the laser light is intermittently irradiated as pulsed light. A method for recording information on an optical information recording medium, characterized in that: 2. A method for recording information on an optical information recording medium according to claim 1, characterized in that the duty ratio of the pulsed light is selected so that the information pits form one continuous closed area. . 3. The method for recording information on an optical information recording medium according to claim 2, wherein the duty ratio of the pulsed light is 50 to 80%. 4. The method for recording information on an optical information recording medium according to any one of claims 1 to 3, wherein the optical information recording medium is an optical information recording card. 5. A method for recording information on an optical information recording medium according to any one of claims 1 to 4, characterized in that a semiconductor laser is used as a light source of the laser beam.
JP61185194A 1986-08-08 1986-08-08 Recording method for information to optical information recording medium Pending JPS6342035A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61185194A JPS6342035A (en) 1986-08-08 1986-08-08 Recording method for information to optical information recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61185194A JPS6342035A (en) 1986-08-08 1986-08-08 Recording method for information to optical information recording medium

Publications (1)

Publication Number Publication Date
JPS6342035A true JPS6342035A (en) 1988-02-23

Family

ID=16166504

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61185194A Pending JPS6342035A (en) 1986-08-08 1986-08-08 Recording method for information to optical information recording medium

Country Status (1)

Country Link
JP (1) JPS6342035A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01286144A (en) * 1988-05-12 1989-11-17 Nec Corp Method and device for manufacturing optical master disk
US5511063A (en) * 1989-05-15 1996-04-23 Seiko Epson Corporation Optical data recording medium

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01286144A (en) * 1988-05-12 1989-11-17 Nec Corp Method and device for manufacturing optical master disk
US5511063A (en) * 1989-05-15 1996-04-23 Seiko Epson Corporation Optical data recording medium
US6185181B1 (en) 1989-05-15 2001-02-06 Seiko Epson Corporation Optical data recording medium having clock pits, servo pits, and auxiliary clock pits disposed thereon

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