JPS5814333A - Recording method for optical disc - Google Patents
Recording method for optical discInfo
- Publication number
- JPS5814333A JPS5814333A JP56110874A JP11087481A JPS5814333A JP S5814333 A JPS5814333 A JP S5814333A JP 56110874 A JP56110874 A JP 56110874A JP 11087481 A JP11087481 A JP 11087481A JP S5814333 A JPS5814333 A JP S5814333A
- Authority
- JP
- Japan
- Prior art keywords
- recording
- dirt
- light
- laser
- optical disc
- 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
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 20
- 238000000034 method Methods 0.000 title claims description 9
- 239000004065 semiconductor Substances 0.000 abstract description 15
- 230000002238 attenuated effect Effects 0.000 abstract description 3
- 239000011347 resin Substances 0.000 description 10
- 229920005989 resin Polymers 0.000 description 10
- 238000010586 diagram Methods 0.000 description 8
- 230000007423 decrease Effects 0.000 description 6
- 239000000428 dust Substances 0.000 description 4
- 230000001681 protective effect Effects 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 1
- 238000011109 contamination Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 230000003313 weakening effect Effects 0.000 description 1
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
- G11B7/12—Heads, e.g. forming of the optical beam spot or modulation of the optical beam
- G11B7/125—Optical beam sources therefor, e.g. laser control circuitry specially adapted for optical storage devices; Modulators, e.g. means for controlling the size or intensity of optical spots or optical traces
- G11B7/126—Circuits, methods or arrangements for laser control or stabilisation
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Recording Or Reproduction (AREA)
- Optical Head (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は記録式の光ディスクにおいて、ディスク表面が
汚れていた場合、記録用レーザー光の強度が低下して記
録が不可能となるが、この表面の汚れ等を測定検出して
、常に一定の光量で安定に記録する方法を提供しようと
するものである。DETAILED DESCRIPTION OF THE INVENTION In a recordable optical disc, if the disc surface is dirty, the intensity of the recording laser beam decreases and recording becomes impossible. The objective is to provide a method for stably recording with a constant amount of light.
再生専用のビデオディスクに対し、映像信号等の記録も
できる光学式のディスクが開発されつつある。一般に、
光学式のビデオディスクは1μ程度の小さな信号を含む
面の上には、厚い樹脂の層が形成されていて信号面を保
護しており、若しこの保護樹脂層の表面にじんあい等が
付着しても、レーザー光はこの表面では焦点からづれて
おり、200〜500μm程度の光スポットになってい
るので、この程度より小さい異物の影響は少いように設
計されている。ところが、指紋等の大きな汚れで表面で
の光スポツト径程度の大きさになると、これがレーザー
光を吸収又は散乱させて強度を弱める。しかし、再生専
用のビデオディスクでは、光信号強度に多少の変動があ
っても、信号振巾が多少変るだけであり、通常、FM変
調方式又はPCM変調方式をとっているので大きな影響
は無い。In contrast to playback-only video discs, optical discs that can also record video signals and the like are being developed. in general,
Optical video discs have a thick resin layer formed on the surface that contains signals as small as 1μ to protect the signal surface, and if dust or the like adheres to the surface of this protective resin layer. However, the laser beam is out of focus on this surface, resulting in a light spot of about 200 to 500 μm, so the design is such that the influence of foreign matter smaller than this size is small. However, if a large stain such as a fingerprint is about the size of a light spot on the surface, this will absorb or scatter the laser beam, weakening its intensity. However, in a playback-only video disc, even if there is some variation in the optical signal intensity, the signal amplitude will only change slightly, and since the FM modulation method or PCM modulation method is normally used, it does not have a big effect.
しかし、記録式の光ディスクでは、この汚れによる光量
減少によって、記録膜面での光強度が減少し、記録作用
に支障を来すようになる。However, in a recordable optical disc, the light intensity decreases due to this dirt, and the light intensity at the recording film surface decreases, which impedes the recording operation.
本発明は、このような問題を除去して記録光量を一定に
した、安定な記録を可能にする光記録方式を提供するも
のである。以下に本発明にかかる方法の詳細を説明する
。The present invention provides an optical recording method that eliminates such problems and makes stable recording possible by keeping the amount of recording light constant. The details of the method according to the present invention will be explained below.
第1図は、半導体レーザーによって記録再生するディス
クとその記録作用を説明する図である。FIG. 1 is a diagram illustrating a disk on which recording and reproduction is performed using a semiconductor laser and its recording operation.
図において、1は半導体レーザー光線、2はこれを収束
する対物レンズ、3は透明樹脂の板で厚さ約1m程度の
もの、4は記録膜であって、同心円状に形成された帯状
案内トラ、りの上に形成されている。5は保鰻用樹脂層
、6は透明樹脂板3の表に付着した汚れ、7はこの透明
樹脂板3の表面での光スポットを示している。半導体レ
ーザー光#1は対物レンズ2で収束されるが、ふつう記
録面では0.8μ程度の大きさにまで収束される。この
記録面の製作は無じん室で行われ、約0.3μ程度のし
ん埃まで管理され完全に被覆されるので、実用上この部
分での汚れは問題ない。透明樹脂板ズのNA及び透明樹
脂板の厚さによって異なるが200〜500μの直径で
ある。一般に言うほこりは100μ城下であるので、こ
のような小さなほこりはあっても大きな影響は与えない
。In the figure, 1 is a semiconductor laser beam, 2 is an objective lens that converges the beam, 3 is a transparent resin plate with a thickness of about 1 m, 4 is a recording film, and is a belt-shaped guide track formed in a concentric circle. It is formed on top of the Reference numeral 5 indicates a resin layer for preserving eel, 6 indicates dirt adhering to the surface of the transparent resin plate 3, and 7 indicates a light spot on the surface of the transparent resin plate 3. The semiconductor laser beam #1 is converged by the objective lens 2, and is generally converged to a size of about 0.8 μ on the recording surface. This recording surface is manufactured in a dust-free room, and dust particles of about 0.3 μm are controlled and completely covered, so contamination in this area is not a problem in practice. Although it varies depending on the NA of the transparent resin plates and the thickness of the transparent resin plate, the diameter is 200 to 500 μm. Generally speaking, dust is 100μ in size, so even if such small dust is present, it will not have a big impact.
問題は第1図の6のように、光スポ、ドアと同程度かそ
れ以上に大きな汚れがあった場合、レーザー光強度は弱
くなる。記録膜4に照射される光強度をIとし、汚れに
よって光が減衰する減衰係数をαとすると1汚れがない
場合の照射光強度!。The problem is, as shown in 6 in Figure 1, if there is dirt as big as or bigger than the light spot or door, the laser light intensity will be weaker. If the light intensity irradiated onto the recording film 4 is I, and the attenuation coefficient at which the light is attenuated due to dirt is α, then the irradiation light intensity when there is no dirt is 1! .
に対して
!=α■。 叫・・・・・・・・(1)が
成り立つ。このαを検出する方法があれば、っねにI=
I。となるようにレーザー出カを調整す、ればよいこと
がわかる。Against! =α■. Shouting... (1) holds true. If there is a way to detect this α, then I=
I. It turns out that all you have to do is adjust the laser output so that .
次に、とのαの検出方法を述べる。第2図は、記録式の
光ディスク及びこの光学系を説明する図である。図にお
いて8は半導体レーデ−の駆動口 1路、9は半導
体レーザー、10はこの半導体、レーザーよりの光を集
光する集光レンズ、11はハーフミラ−112は反射鏡
で、これの微小駆動によりてトラ、キングを行うもので
あり、13は対物レンズ、14は記録用ディスクである
。半導体レーザー9より発射された光は上述の光学系を
通ってディスク14に照射され、その一部は記録膜で反
射されて、同じ光学系を戻っていくが、途中ノ・−フミ
ラー11で直角に曲げられて、対物レンズ15を通じて
光検出器16で測定される。この光検出器16で受ける
光電流をiとすると0、半導体レーデ−9の光は、行き
と帰りにディスク表面の汚れを通過することになり、そ
の減衰を2回受けるととになる。汚れが無い場合、の光
電流をi。とするとi=α2i、 ・・・
・・・・・・・・・(2)の関係が成立ち、
αハΔフ〒 ・・・・・・・・・・・・(3)
が導かれる。即ち、αは光検出器での光電流の比の平方
根として求められる。汚れによる吸収量が小さくてαχ
1の場合には、近似的に
となる。Next, a method for detecting α will be described. FIG. 2 is a diagram illustrating a recordable optical disc and its optical system. In the figure, 8 is a drive port 1 path of a semiconductor radar, 9 is a semiconductor laser, 10 is a condensing lens for condensing the light from this semiconductor, 11 is a half mirror, and 112 is a reflecting mirror, which is minutely driven. 13 is an objective lens, and 14 is a recording disk. The light emitted from the semiconductor laser 9 passes through the above-mentioned optical system and is irradiated onto the disk 14. A portion of the light is reflected by the recording film and returns through the same optical system, but on the way it is turned at a right angle by the nof mirror 11. It is measured by a photodetector 16 through an objective lens 15. If the photocurrent received by the photodetector 16 is i, then 0, the light from the semiconductor radar 9 passes through dirt on the disk surface on its way out and on its way back, and is attenuated twice. When there is no dirt, the photocurrent of i. Then i=α2i,...
・・・・・・・・・The relationship in (2) is established, αhaΔf〒 ・・・・・・・・・・・・(3)
is guided. That is, α is determined as the square root of the ratio of photocurrents at the photodetector. The amount of absorption due to dirt is small and αχ
1, approximately.
上述のように求めた減少分だけ半導体レーザーの出力を
大きくする帰還回路を設けてやればよい。A feedback circuit may be provided to increase the output of the semiconductor laser by the decrease determined as described above.
つ回路設計を行う。Perform circuit design.
第3図は、記録膜面で反射された記録光の受光電流信号
の一例を示す。i4ルス記録の例でありこのノ4ルスの
高さがioである。ディスク表面に汚れがあれば、この
ピーク値が減少しiとなる。FIG. 3 shows an example of a received light current signal of the recording light reflected on the recording film surface. This is an example of i4rus recording, and the height of this no4rus is io. If there is dirt on the disk surface, this peak value decreases to i.
第4図は、半導体レーザーの駆動電流対出力光強度を示
す図である。これは半導体レーザ一種類に応じて異なる
ので、この特性を考慮に入れて補正回路の設計を行う必
要がある。FIG. 4 is a diagram showing drive current versus output light intensity of a semiconductor laser. Since this varies depending on the type of semiconductor laser, it is necessary to take this characteristic into consideration when designing the correction circuit.
以上のような一簡単な設計、す、なわち記Q用のレーザ
ーの反射光を用いることにより、汚れによるレーザー強
度の減少の補正を行うことが出来、汚れの影響を除いた
安定な記録をすることが可能となった。By using a simple design as described above, that is, using the reflected light of the Q laser, it is possible to compensate for the decrease in laser intensity due to dirt, and to achieve stable recording without the influence of dirt. It became possible to do so.
゛第1図は、記録再生するディスクとその記録作用を説
明するための図、
第2図は、記録式の光ディスク及びその光学系を示す図
、
第3図は、記録膜面で反射された記録光の受光電流信号
の一例を示す図、
第4図は、半導体レーザーの駆動電流対出力光強度を示
す図である。
1・・・半導体レーザー光線、2・・・対物レンズ、3
・・・透明樹脂板、4・・・記録膜、5・・・保護用樹
脂層、6・・・汚れ、7・・・光スポット、8・・・レ
ーザー駆動回路、9・・・半導体レーザー、10・・・
集光レンズ、11・・・ハーフミラ−112・・・反射
鏡、13・・・対物Cンズ、14・・・記録用ディスク
、16・・・光検出器。
4F! J$I −m @や
ミ
躯 や ε゛Figure 1 is a diagram for explaining a recording/reproducing disk and its recording function. Figure 2 is a diagram showing a recording type optical disk and its optical system. Figure 3 is a diagram showing the optical disc reflected on the recording film surface. FIG. 4 is a diagram showing an example of a received light current signal of recording light. FIG. 4 is a diagram showing driving current versus output light intensity of a semiconductor laser. 1... Semiconductor laser beam, 2... Objective lens, 3
... Transparent resin plate, 4... Recording film, 5... Protective resin layer, 6... Dirt, 7... Light spot, 8... Laser drive circuit, 9... Semiconductor laser , 10...
Condensing lens, 11...Half mirror, 112...Reflecting mirror, 13...Objective lens, 14...Recording disk, 16...Photodetector. 4F! J$I −m @ya mi body ya ε
Claims (2)
生する光ディスクにおいて、記録膜面に照射された記録
用レーザー光を膜面により反射させ、これを光検出器で
受光してその変動を測定し、受光信号が弱くなったとき
はレーザー光出力を増大させるように制御を行い、膜面
での照射強度を常に一定に制御することを特徴とした光
ディスクの記録方法。(1) In optical discs that use laser light to record and reproduce video and other signals, the recording laser light that is irradiated onto the recording film surface is reflected by the film surface, and this is received by a photodetector to measure its fluctuations. , an optical disc recording method characterized by controlling the laser light output to be increased when the received light signal becomes weak, and controlling the irradiation intensity on the film surface to always be constant.
i。とじたとき、ioと受光信号強度iとの比の平方根
Jフ几に逆比例してレーデ−光出力を増大させることを
特徴とする特許請求の範囲第(1)項記載の光ディスク
の記録方法。(2) The received light signal intensity when there is no dirt on the disk surface is i. The method for recording an optical disc according to claim (1), characterized in that when the optical disc is closed, the radar light output is increased in inverse proportion to the square root J of the ratio between io and the received light signal intensity i. .
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56110874A JPS5814333A (en) | 1981-07-17 | 1981-07-17 | Recording method for optical disc |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56110874A JPS5814333A (en) | 1981-07-17 | 1981-07-17 | Recording method for optical disc |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5814333A true JPS5814333A (en) | 1983-01-27 |
Family
ID=14546886
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP56110874A Pending JPS5814333A (en) | 1981-07-17 | 1981-07-17 | Recording method for optical disc |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5814333A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5042022A (en) * | 1986-07-31 | 1991-08-20 | Sony Corporation | Optical disk recording/reproducing apparatus with synchronized data writing |
US5184343A (en) * | 1991-05-06 | 1993-02-02 | Johann Donald F | Compensation for dust on an optical disk by increasing laser writing power |
US7023777B2 (en) * | 2000-01-13 | 2006-04-04 | Matsushita Electric Industrial Co., Ltd. | Optical disk recording/reproduction apparatus with a detection means for detecting dirt on the optical disk |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS523405A (en) * | 1975-06-27 | 1977-01-11 | Canon Inc | Signal recording appliance |
JPS536516A (en) * | 1976-07-08 | 1978-01-21 | Matsushita Electric Ind Co Ltd | Optical recording and reproducing unit |
-
1981
- 1981-07-17 JP JP56110874A patent/JPS5814333A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS523405A (en) * | 1975-06-27 | 1977-01-11 | Canon Inc | Signal recording appliance |
JPS536516A (en) * | 1976-07-08 | 1978-01-21 | Matsushita Electric Ind Co Ltd | Optical recording and reproducing unit |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5042022A (en) * | 1986-07-31 | 1991-08-20 | Sony Corporation | Optical disk recording/reproducing apparatus with synchronized data writing |
US5184343A (en) * | 1991-05-06 | 1993-02-02 | Johann Donald F | Compensation for dust on an optical disk by increasing laser writing power |
US7023777B2 (en) * | 2000-01-13 | 2006-04-04 | Matsushita Electric Industrial Co., Ltd. | Optical disk recording/reproduction apparatus with a detection means for detecting dirt on the optical disk |
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