JPH03181021A - Optical disk and its recording and reproducing method - Google Patents
Optical disk and its recording and reproducing methodInfo
- Publication number
- JPH03181021A JPH03181021A JP2231709A JP23170990A JPH03181021A JP H03181021 A JPH03181021 A JP H03181021A JP 2231709 A JP2231709 A JP 2231709A JP 23170990 A JP23170990 A JP 23170990A JP H03181021 A JPH03181021 A JP H03181021A
- Authority
- JP
- Japan
- Prior art keywords
- laser
- laser beam
- light
- groove
- optical disk
- 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 32
- 238000000034 method Methods 0.000 title claims description 14
- 239000010409 thin film Substances 0.000 description 2
- 239000002131 composite material Substances 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- 229910052714 tellurium Inorganic materials 0.000 description 1
- PORWMNRCUJJQNO-UHFFFAOYSA-N tellurium atom Chemical compound [Te] PORWMNRCUJJQNO-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Optical Recording Or Reproduction (AREA)
- Optical Record Carriers And Manufacture Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明(友 高品質情報を高密度に記録または再生可能
な光ディスクおよびその記録再生方法に関するものであ
も
従来の技術
レーザーをディスク上に絞り、画像信号を再生する「光
学式ビデオディスク」が市販されていも直径30cmの
ディスクに1.67μmのトラックピッチでFM変調さ
れたテレビジョン信号を記録しておき、毎分1800回
転させて再生時間は片面30分であも
また 光ディスク表面に記録材料薄膜(例えばテルル低
酸化物薄膜T e Ox、 x < 2 )を設けて
、ビデオテープと同様に信号を記録再生する方法が開発
され 「録再ビデオディスク」としての発展が期待され
ていも
最近でζよ 光ディスクにディジタルビデオ等の高品質
信号を実時間で記録再生することも望まれており、本発
明者達は以前にその一つの方法を特願昭57−1471
33において提供していもその概要を以下に述べも
光ディスク表面に 第5図の様なV字形の溝を形成し
その溝の全斜面を信号記録面とす&V字溝の山と山との
間隔を、例えば 現在市販されているビデオディスクの
トラックのトラックピッチに等しくしておく。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application This invention relates to an optical disc capable of recording or reproducing high-quality information at high density and a method for recording and reproducing the same. Even though "optical video discs" for reproducing signals are commercially available, FM-modulated television signals are recorded on discs with a diameter of 30 cm at a track pitch of 1.67 μm, rotated at 1800 revolutions per minute, and the playback time is limited to one side. In just 30 minutes, a method was developed for recording and reproducing signals in the same way as video tapes by providing a thin film of recording material (e.g. tellurium low oxide thin film T e Ox, x < 2) on the surface of an optical disc. It is also desired to record and play back high-quality signals such as digital video on optical discs in real time, and the inventors of the present invention previously filed a patent application for one method. Showa 57-1471
33, the outline of which is given below, forms a V-shaped groove on the surface of an optical disk as shown in Figure 5.
The entire slope of the groove is used as a signal recording surface, and the interval between the crests of the V-shaped groove is made equal to, for example, the track pitch of the tracks of video discs currently on the market.
少なくとも2つのレーザー光源を用いて、第5図のAと
よ あるいはCとD等の互いに隣合う2斜面の各々の中
央に 第6図の様にレーザースポットl及び2を照射す
も それらのレーザーを互いに独立に駆動し 隣合う2
斜面に異なる信号を同時に記録すん
特開昭57−105828の方法を用いて、■溝の1つ
の斜面上の信号を再生する場合、隣の斜面からのクロス
トークは十分に小さくすることができも 異なる光源か
らのレーザーは互いに干渉しないので、■溝の隣合う2
斜面の信号は2つのレーザーで独立に再生できも その
2斜面を1組として、 1つの情報を2つの斜面に分け
て記録することで、ディジタルビデオ等の高品質な情報
を記録再生できる様になん
NTSC方式のカラーテレビ信号をコンポジット方式で
ディジタル化する場合を考えも サンプリング周波数を
10. 74MHzとし 8ビツトで量子化すれば86
M b i t / s e cとなも しかし 帰
線期間を除き、エラー補正を加丸 フィールド内の隣接
画素間の相関を利用して、予測符号化で40〜50%に
帯域圧縮できも 従って、NTSC方式のカラーテレビ
信号は35〜43Mb i t / s e cで表わ
せるようになん現技術で(よ ディスクを毎分1800
回転させて、半径が50cmの位置で約10MHzのア
ナログ信号を記録再生できて、この事(戴 MFM変調
方式を用いて約20Mbit/secのディジタル信号
が記録再生できる事を意味すもしかし これだけではデ
ィジタルビデオ信号は扱えな〜 そこ℃ 前述した様に
V溝の2斜面を1組にすれば約40 M b i t
/ s e cのディジタル信号が記録再生でき、NT
SC方式カラーテレビのディジタル信号を実時間で記録
再生できもまf、 V溝の山と山との間隔;上 市販
のビデオディスクのトラックピッチに等しいの玄 ディ
ジタルビデオを扱う場合でL 再生時間は短くならなL
Xo 従って、直径30cmのディスク六 等角速度
で両面1時肌 等線速度で両面2時間のディジタルビデ
オの記録再生ができも
発明が解決しようとする課題
この様に 特願昭57−147133に記載の発明によ
って、記録再生レートを大幅に増加することが可能な原
理が開示されt4
この原理を実際の機器に展開するにあたって:よ2つの
レーザースポットを各々隣合う2斜面に沿って正確にト
ラッキングを行なうことが必要であも
本発明(友 この点に鑑へ 2つのレーザースポットを
各々隣合う2斜面に沿って正確にトラッキングを行なう
ことの可能な光ディスクの記録再生方法と、この記録再
生方法と共に用いて有用な光ディスクを提供することを
目的とすも
課題を解決するための手段
311、第2の光源からの2つのレーザースポット1、
2に加えて、第3の光源からの第3のレーザースポット
3を光ディスク上に絞も レーザースポット!、2のデ
ィスク半径方向の中心間隔をV溝の谷と谷との間隔の半
分にし 且つレーザースポット3をディスク半径方向で
レーザースポット1と2の中間に配置すも そして、レ
ーザースポット3の反射光の遠視野像をV溝の谷または
山に対称になるようにトラッキングする方法を用いも
作用
レーザースポット1. 2のディスク半径方向の中心間
隔がV溝の谷と谷との間隔の半分であり、レーザースポ
ット3はディスク半径方向でレーザースポットlと2の
中間に配置しているの玄 レーザースポット3でV溝の
山または谷にトラッキングすれζL レーザースポット
1. 2はV溝の隣合う2つの斜面にトラッキングでき
る事になん実施例
第1図に 第1、第2の光源として波長λlのレーザー
ダイオード11112を、第3の光源として波長λ2の
レーザーダイオードlOを用いた実施例の構成をしめす
。ここでダイオード11.12は1つのチップ上に構成
されていも また例えば λ1=780nrrx λ
2=840nmであも
な耘 第1図(b)、 (c〉1よ それぞれ同図(a
)におけるX矢視@ Y矢視図であも記録再生用のレー
ザーダイオード11、12からの光(友 対物レンズ1
3−1で集めらレミラー41で反射り、、4分の1波長
板23を通り、偏光ビームスプリッタ24で反射されも
その眞4分の1波長板25を通り、対物レンズ14で
絞られて斜面C,Dの中央に照射されも
光学フィルタ22は波長λ1の光を通過させ、波長λ2
の光は反射させも また2枚の4分のl波長板21、2
3でレーザー光の偏光方向を90度回転させて、偏光ビ
ームスプリッタ24ではS波として反射されるように
各々の光学要素は構成されていも
トラッキング用のレーザーダイオードlOからの光(九
対物レンズ13−2で集められ 偏光ビームスプリッ
タ24をP波として通過り、4分の1波長板23を通り
、光学フィルタ22で反射され 再び4分の1波長板2
3を通り、偏光ビームスプリッタ24でS波として反射
されも 続いて、4分の1波長板25を通り、対物レン
ズ14で絞られて、■溝の山または谷に照射されもすな
わ板 記録時あるいは再生時に(上 第1〜第3の光源
からの光(友 微小な円形状に集束された状態で第2図
に示す位置関係で光ディスク15上に照射されkV溝の
容土のスポット3はレーザーダイオード10からの光力
t 斜面上のスポット1、2はそれぞれレーザーダイオ
ード11512からの光が絞られたものであも
本実施例における記録再生時の焦点制御及びトラッキン
グ制御等(友 光ディスク15からの反射光を検出して
以下の様に行なわれも
先ず、光ディスク15からの反射光Gi 波長λl及
び波長λ2の両方の光ともに対物レンズ14.4分の1
波長板25を通り、偏光ビームスプリッタ24をP波と
して透過し 凸レンズ31で集められてハーフミラ−3
8へと向かう。Using at least two laser light sources, laser spots 1 and 2 are irradiated at the center of each of two adjacent slopes, such as A and C in FIG. 5 or C and D, as shown in FIG. 6. are driven independently of each other, and the adjacent 2
Using the method of JP-A-57-105828, which simultaneously records different signals on the slopes, ■ When reproducing the signal on one slope of the groove, the crosstalk from the adjacent slope can be made sufficiently small. Lasers from different light sources do not interfere with each other, so two adjacent grooves
Although the signal on the slope can be reproduced independently by two lasers, the two slopes are combined into a set, and by recording one piece of information separately on the two slopes, it is possible to record and play back high-quality information such as digital video. Let's consider a case where an NTSC color television signal is digitized using a composite method.The sampling frequency is set to 10. If you set it to 74MHz and quantize it with 8 bits, it will be 86.
However, excluding the blanking period, error correction can be performed.Using the correlation between adjacent pixels in the field, it is possible to compress the bandwidth to 40-50% with predictive coding. With current technology, NTSC color television signals can be expressed at 35 to 43 Mbit/sec.
By rotating it, an analog signal of about 10 MHz can be recorded and played back at a position with a radius of 50 cm, and this means that a digital signal of about 20 Mbit/sec can be recorded and played back using the MFM modulation method. It cannot handle digital video signals.As mentioned above, if you put two slopes of the V-groove into one set, it will be about 40 Mbit.
/sec digital signals can be recorded and played back, and NT
It is possible to record and play back the digital signals of an SC color TV in real time.The distance between the peaks of the V-groove; It should be short L
Xo Therefore, it is possible to record and play back digital video for 2 hours on both sides at constant angular speed and 2 hours on both sides at constant angular speed using a disk with a diameter of 30 cm.The problem to be solved by the invention is thus: The invention discloses a principle that can significantly increase the recording and reproducing rate.In applying this principle to actual equipment: Accurately track two laser spots along two adjacent slopes. In view of this, we have proposed a recording and reproducing method for an optical disc that can accurately track two laser spots along two adjacent slopes, and a method that can be used together with this recording and reproducing method. Means for solving the problem 311, two laser spots 1 from a second light source,
In addition to 2, a third laser spot 3 from a third light source is also apertured onto the optical disc.Laser spot! , 2, the distance between the centers in the radial direction of the disk is set to half the distance between the valleys of the V-groove, and the laser spot 3 is placed between laser spots 1 and 2 in the radial direction of the disk.Then, the reflected light of laser spot 3 The active laser spot 1. can also be tracked using a method of tracking the far-field image of the V-groove so that it is symmetrical to the valley or peak of the V-groove. The distance between the centers in the radial direction of the disc 2 is half the distance between the valleys of the V grooves, and the laser spot 3 is placed between laser spots 1 and 2 in the radial direction of the disc. Tracking the peaks or valleys of the groove ζL Laser spot 1. 2 is able to track the two adjacent slopes of the V-groove. In the example shown in FIG. The configuration of the example used is shown. Here, even if the diodes 11 and 12 are constructed on one chip, for example, λ1=780nrrx λ
2 = 840nm Figure 1 (b), (c〉1) Figure 1 (a)
) in the X-arrow view @Y-arrow view shows the light from the laser diodes 11 and 12 for recording and reproducing (objective lens 1
3-1, is reflected by the mirror 41, passes through the quarter-wave plate 23, is reflected by the polarizing beam splitter 24, passes through the quarter-wave plate 25, and is focused by the objective lens 14. Even when the center of the slopes C and D is irradiated, the optical filter 22 passes the light of wavelength λ1 and transmits the light of wavelength λ2.
The light is reflected by the two quarter-wave plates 21 and 2.
Step 3 rotates the polarization direction of the laser beam by 90 degrees so that it is reflected as an S wave by the polarizing beam splitter 24.
Although each optical element is configured, the light from the laser diode lO for tracking (9) is collected by the objective lens 13-2, passes through the polarizing beam splitter 24 as a P wave, passes through the quarter-wave plate 23, and is transmitted to the optical It is reflected by the filter 22 and passes through the quarter wave plate 2 again.
3 and is reflected as an S wave by the polarizing beam splitter 24.Then, it passes through the quarter wavelength plate 25, is focused by the objective lens 14, and is irradiated onto the peaks or valleys of the groove. At the time of playback or during playback, the light from the first to third light sources (above) is irradiated onto the optical disc 15 in the positional relationship shown in FIG. is the optical power t from the laser diode 10 Spots 1 and 2 on the slope are the light from the laser diode 11512, respectively. The process is carried out as follows by detecting the reflected light from the optical disc 15. First, the reflected light Gi from the optical disk 15. Both the light with the wavelength λl and the wavelength λ2 are detected by the objective lens 14.4.
It passes through the wavelength plate 25 and the polarizing beam splitter 24 as a P wave, and is collected by the convex lens 31 and sent to the half mirror 3.
Head to 8.
ハーフミラ−38は波長λ2の光だけを反射し波長λl
の光は透過させも
波長λ2の光が絞られる途中にミラー36が挿入されて
おり、絞り点に置かれた光検出器に、Lの出力に基づき
焦点制御が行なわれも
また 2分割光検出器S、 Tを用いて波長λ2の光
の遠視野像を対称に制御することで、レーザースポット
3の中心がV溝の谷または山に沿ってトラッキングされ
も
情報の再生(よ ハーフミラ−38を透過した波長λ1
の光を光検出器M、Nで受光させて行なう。The half mirror 38 reflects only the light of wavelength λ2 and reflects the light of wavelength λl.
Although the light of wavelength λ2 is transmitted, a mirror 36 is inserted in the middle where the light of wavelength λ2 is focused, and the focus control is performed on the photodetector placed at the aperture point based on the output of L. By controlling the far-field image of the light of wavelength λ2 symmetrically using the mirrors S and T, information can be reproduced even if the center of the laser spot 3 is tracked along the valley or peak of the V-groove. Transmitted wavelength λ1
The light is received by photodetectors M and N.
光検出器M、N上の様子G′!、、第3図で表わされも
スポット101、102ζよ 各々、レーザーダイオ
ード11及び12からの光であも 光検出器M1で斜面
Cの信号を、光検出器N2で斜面りの信号を再生すも
本実施例の光学系は 現在市販されている「光学式ビデ
オディスク」をも再生できも 「光学式ビデオディスク
」のディスク面の様子を第4図に示す。画像情報はビッ
ト40の列として記録されていも このビット列にトラ
ッキングするには公知の3ビ一ム方式が安定なことが知
られていも光検出部M1とN1の和の信号と、光検出器
M2、N2とわの信号とか転 各々、画像信号を取り出
し それらの包絡信号を比較してトラッキングすること
ができも 画像信号の再生に41 光検出器に、
L S、 Tの和の信号を用いもさて、■溝の隣合
う2つの斜面を1組として、ディジタルビデオが予め記
録された いわば再生専用ディジタルビデオディスクを
考えてみよう。Situation G' on photodetectors M and N! ,, As shown in Fig. 3, the light from the laser diodes 11 and 12 is also used for the spots 101 and 102ζ, respectively.The photodetector M1 reproduces the signal of the slope C, and the photodetector N2 reproduces the signal of the slope. The optical system of this embodiment can also play back "optical video discs" currently on the market. The appearance of the disc surface of the "optical video disc" is shown in FIG. Even though image information is recorded as a string of 40 bits, the known 3-beam system is known to be stable in order to track this bit string. It is possible to extract the image signals from M2 and N2 and track them by comparing their envelope signals.
Using the signal of the sum of L, S and T, let's consider a so-called playback-only digital video disk on which digital video is pre-recorded, using two adjacent slopes of the groove as one set.
斜面上の信号の形Fl上 反射率が変化した濃淡ビッ
トや穴状のビットがあん 本発明によれば 前述のよう
に 現在市販中の光学式ビデオディスクと互換性のあり
、かつ記録再生レートが大幅に向上したディジタルビデ
オディスクシステムを実現することができも
発明の効果
以上の様に 本発明によればV溝の隣合う2斜面を1組
の信号記録面として、記録再生レートを従来に比べて大
幅に向上でき、高品質の情報を実時間で記録 再生でき
もThe shape of the signal on the slope Fl is filled with shading bits and hole-shaped bits with varying reflectance.According to the present invention, as mentioned above, it is compatible with optical video discs currently on the market, and has a high recording and playback rate. According to the present invention, the two adjacent slopes of the V-groove are used as one set of signal recording surfaces, and the recording and reproducing rate is improved compared to the conventional one. This can greatly improve the ability to record and play back high-quality information in real time.
第1図は本発明を従来の光学式ビデオディスクの再生に
適用した時のレーザースポットの配置は第2図ζ上 本
発明のトラッキング方法の説明は第3図(上 再生光検
出器の配置は 第4図ζ戴 光学式ビデオディスクのデ
ィスク面の状態は 第5図ζよ v溝を設けた光ディス
クの構造を示す切り欠き斜視阻 第6図1よ 光ディス
ク上のレーザースポットの配置図であム
10.11,12・・・レーザーダイオード、 13−
1・・・対物レンX 15・・・光ディス久 21.
23、25・・・4分のl波長板 22・・・光学フィ
ル久A−F・・・斜五
M、
N・・・光検出毘Fig. 1 shows the arrangement of the laser spot when the present invention is applied to the reproduction of a conventional optical video disc. Fig. 2 shows the arrangement of the laser spot. The explanation of the tracking method of the invention is shown in Fig. 3 (top). Figure 4 ζ Dia The state of the disc surface of an optical video disc is shown in Figure 5 ζ Figure 6 is a perspective view of a notch showing the structure of an optical disc with a V-groove. Figure 6 is a diagram showing the arrangement of laser spots on an optical disc. 10.11,12...Laser diode, 13-
1... Objective lens X 15... Optical disc lens 21.
23, 25... Quarter wave plate 22... Optical filter A-F... Diagonal five M, N... Photo detection plate
Claims (2)
を形成し、第1、第2の2つのレーザー光を発振する光
源を備え、第1のレーザー光を前記V字形溝の第1斜面
に絞り、第2のレーザー光を第1斜面とは隣合う第2斜
面に絞り、前記第1及び第2のレーザー光の前記光ディ
スクからの反射光を分離して信号検出することで、光デ
ィスクに情報を記録、再生または消去する際に、前記隣
合う第1及び第2斜面に絞られた第1及び第2のレーザ
ー光の絞りスポット中心の中間に位置するV溝の山また
は谷に沿って、第3のレーザー光を絞って照射し、この
第3のレーザー光の光ディスクからの反射光を用いて、
焦点制御またはトラッキング制御を行なう事を特徴とす
る光ディスク記録再生方法。(1) A groove whose radial cross section is V-shaped is formed on the optical disk, and a light source that oscillates two laser beams, a first laser beam and a second laser beam, is provided, and the first laser beam is emitted into the first laser beam of the V-shaped groove. The second laser beam is focused on a slope, the second laser beam is focused on a second slope adjacent to the first slope, and the reflected lights of the first and second laser beams from the optical disk are separated and signal detected. When recording, reproducing or erasing information, the V-groove along the peak or valley located between the aperture spot centers of the first and second laser beams focused on the adjacent first and second slopes. Then, a third laser beam is focused and irradiated, and using the reflected light of this third laser beam from the optical disk,
An optical disc recording and reproducing method characterized by performing focus control or tracking control.
1組にして、情報を2つに分けて、その各々を前記隣合
う2斜面に記録した光ディスク。(2) A groove whose radial cross section is V-shaped is formed on the surface, two adjacent slopes of the V-shaped groove are made into a set, and information is divided into two parts, each of which is transmitted to the adjacent An optical disc recorded on two matching slopes.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2231709A JPH03181021A (en) | 1990-08-31 | 1990-08-31 | Optical disk and its recording and reproducing method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2231709A JPH03181021A (en) | 1990-08-31 | 1990-08-31 | Optical disk and its recording and reproducing method |
Related Parent Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP58175259A Division JPS6066332A (en) | 1983-09-21 | 1983-09-21 | Recording and reproducing method of optical disc and said optical disc |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH03181021A true JPH03181021A (en) | 1991-08-07 |
Family
ID=16927782
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2231709A Pending JPH03181021A (en) | 1990-08-31 | 1990-08-31 | Optical disk and its recording and reproducing method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH03181021A (en) |
-
1990
- 1990-08-31 JP JP2231709A patent/JPH03181021A/en active Pending
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