JPS59132430A - Information reproducing device - Google Patents
Information reproducing deviceInfo
- Publication number
- JPS59132430A JPS59132430A JP23270883A JP23270883A JPS59132430A JP S59132430 A JPS59132430 A JP S59132430A JP 23270883 A JP23270883 A JP 23270883A JP 23270883 A JP23270883 A JP 23270883A JP S59132430 A JPS59132430 A JP S59132430A
- Authority
- JP
- Japan
- Prior art keywords
- signal
- pit
- pulse
- spot
- outputs
- 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
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
- G11B7/004—Recording, reproducing or erasing methods; Read, write or erase circuits therefor
- G11B7/005—Reproducing
Landscapes
- Optical Recording Or Reproduction (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は、情報再生装置、特にディスタ上に記録された
ディジタル情報信号波形のピーク値を検出する装置に関
する。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to an information reproducing device, and particularly to a device for detecting the peak value of a digital information signal waveform recorded on a disk.
従来の磁気ディスク、磁気テープに比較して桁違いの記
憶容量のある光ディスクは現在、大容量のディジタル情
報メモリーとして期待されている。Optical disks, which have a storage capacity that is orders of magnitude higher than conventional magnetic disks and magnetic tapes, are currently expected to be used as large-capacity digital information memories.
このとき、ディジタル情報を光ディスクに記録する記録
のパターンはピットLL Q II、 II I II
に対応して楕円形状の穴(以下ピットと称する)のある
なしの形で記録される。At this time, the recording pattern for recording digital information on the optical disc is pit LL Q II, II I II
It is recorded with or without elliptical holes (hereinafter referred to as pits) corresponding to .
通常、磁気ティス′り等において、記録されプ社ディジ
タル情報を読み出す場合には、II OgH、II I
Hの連続的なパターンが続いている波形の中から、+
10 Hg 、 ri 1 ggに対応する波形のピー
ク値を検出し、再生クロックとのタイミング関係から”
o”。Normally, when reading digital information recorded in a magnetic tape etc., II OgH, II I
From a waveform with a continuous pattern of H, +
Detect the peak value of the waveform corresponding to 10 Hg, ri 1 gg, and from the timing relationship with the reproduced clock.
o”.
” l ”のパターンを判定している。このときにピー
ク値を検出するための方法としては、微分回路を使う、
遅延線と差動増幅器との組み合せを用いる、フィルター
の周波数特性に工夫をするという種々の方法か考えられ
る。The pattern of "l" is being determined. At this time, the method to detect the peak value is to use a differentiation circuit.
Various methods can be considered, such as using a combination of a delay line and a differential amplifier, or modifying the frequency characteristics of the filter.
本発明はピーク検出の方法として、従来の磁気ディスク
に用いられた方法とは別に、光ディスクの原理的な動作
を利用したピーク検出を提案する。As a peak detection method, the present invention proposes a peak detection method that utilizes the principle operation of an optical disk, which is different from the method used for conventional magnetic disks.
第1図(A、)〜(C)は本発明の原理説明図である。 FIGS. 1A to 1C are explanatory diagrams of the principle of the present invention.
図において6は公知の方法で作成された位相型(凹凸の
変化として情報が記録されている)のピットの断面図で
ある。第2図(A)〜(C)は上記ピット6とレーザー
スポット7の位置関係によって、反射光の強度分布パタ
ーンが光検出器面トで変化する様子を表られしている。In the figure, reference numeral 6 is a cross-sectional view of a phase-type pit (information is recorded as a change in unevenness) created by a known method. FIGS. 2A to 2C show how the intensity distribution pattern of the reflected light changes on the surface of the photodetector depending on the positional relationship between the pit 6 and the laser spot 7.
第1図(A)ではスポット7はピット6の左端にある。In FIG. 1(A), spot 7 is at the left end of pit 6.
このときの光検出器16」二での分布17(a)は左右
でアンバランスになる(第2図(A)に示す。)。また
第1図(B)のようにピット中心にスポット7が来ると
そのときの分布パターン17(b)は左右対称になり(
第2図(B)に示す。)、一方、第1図(C)のように
ピットの右側にスポット7が来るとそのときの分布パタ
ーン17(C)は17(a)と逆の方向にアンバランス
になる(第2図(C)に示す。)。以上の動作原理を用
いて、ピーク検出を実現するのが本発明の原理である。At this time, the distribution 17(a) on the photodetector 16'2 becomes unbalanced on the left and right (as shown in FIG. 2(A)). Furthermore, when the spot 7 comes to the center of the pit as shown in FIG. 1(B), the distribution pattern 17(b) at that time becomes symmetrical (
It is shown in FIG. 2(B). ), On the other hand, if spot 7 comes to the right side of the pit as shown in Fig. 1(C), the distribution pattern 17(C) at that time becomes unbalanced in the opposite direction to 17(a) (Fig. 2( (C). The principle of the present invention is to realize peak detection using the above operating principle.
以下、実施例を用いて、本発明の詳細な説明する。第3
図は光検出器の信号とり出し部分を説明する図である。Hereinafter, the present invention will be explained in detail using Examples. Third
The figure is a diagram illustrating a signal extraction portion of a photodetector.
第3図の光検出器の設置位置と第1図の光検出器と反射
パターンの関係は同じである。光検出器16(a)と1
6(d)の出力を加算器20で加算して分布パターンの
片側の強度に比例した信号30を得る。光検出器16(
b)と16 (c )の出力を加算器21で加算して分
布パターンのもう一方の強度に比例した信号30を得る
。光検出器16(d)と16(c)の出力を加算器21
で加算して分布パターンのもう一方の強度に比例した信
号31を得る。また4つの光検出器22によって加算す
ることによって反射光量全体の変化を示す信号33を得
る。The installation position of the photodetector in FIG. 3 is the same as the relationship between the photodetector and the reflection pattern in FIG. 1. Photodetector 16(a) and 1
The outputs of 6(d) are added by an adder 20 to obtain a signal 30 proportional to the intensity on one side of the distribution pattern. Photodetector 16 (
The outputs of b) and 16(c) are added by an adder 21 to obtain a signal 30 proportional to the intensity of the other distribution pattern. The outputs of the photodetectors 16(d) and 16(c) are added to the adder 21.
A signal 31 proportional to the intensity of the other distribution pattern is obtained. Further, by adding the signals by the four photodetectors 22, a signal 33 indicating a change in the total amount of reflected light is obtained.
第4図に前述の信号がピッ1−6の上をスポット40が
通過した(第4図(a)に示す)ときの変化を示す。第
4図(b)、(C)はそれぞれ加算器20゜21の出力
信号、すなわち回折光の強度を表わす、30.31の振
る舞′いである。第4図(d)は信号30.31の差を
とった信号32、すなわち回折光のアンバランスを示す
もの、の振舞いを示す。FIG. 4 shows how the aforementioned signal changes when spot 40 passes over pins 1-6 (as shown in FIG. 4(a)). FIGS. 4(b) and 4(c) show the output signals of the adders 20 and 21, that is, the behavior of 30.31 representing the intensity of the diffracted light, respectively. FIG. 4(d) shows the behavior of the signal 32 obtained by taking the difference between the signals 30 and 31, which indicates an unbalance of the diffracted light.
この波形において、第1図との対応関係からピットの中
心に光スポットがあるとき零となる。第4図(e)は反
射光量の全体の変化をとらえたもので、ピットに光スポ
ットが照射している間はレベルが下る。In this waveform, from the correspondence with FIG. 1, it becomes zero when the light spot is located at the center of the pit. FIG. 4(e) shows the overall change in the amount of reflected light, and the level decreases while the light spot is irradiating the pit.
第5図は本発明のピーク位置検出の説明図である。信号
32を零点検出用のコンパレータ(回路及び素子は公知
のものでよい)40に通して零点でII OIIからs
r 1 uに立ち上る波形を作り、これを単安定マルチ
バイブレータ4】に入力させ前記の波形の立ち上りに応
じて短いパルス幅のパルスを出力する。信号33はコン
パレータ42を通してピットをスポットが通過する間だ
け” 1 ”を保つパルスを出す。ゲート回路43に零
クロスを示すパルス(41の出力)を入れ、42の出力
をゲート信号として” 1 ”の間だけ41の出力を通
するようにする。するとピットの真中にスポットが来た
ときにパルスを出す。このパルスが反射光景最大に減少
する点、また、反射光量のピークになる点、すなわち、
ピットの真中を正確に表わす。FIG. 5 is an explanatory diagram of peak position detection according to the present invention. The signal 32 is passed through a comparator 40 for zero point detection (circuits and elements may be of known type) and the signal 32 is passed from II OII to s at the zero point.
A waveform that rises at r 1 u is created, and this is input to a monostable multivibrator 4, which outputs a pulse with a short pulse width in response to the rise of the waveform. The signal 33 outputs a pulse that remains "1" only while the spot passes through the pit through the comparator 42. A pulse indicating a zero cross (output of 41) is input to the gate circuit 43, and the output of 42 is used as a gate signal to pass the output of 41 only during "1". Then, when the spot is in the middle of the pit, it emits a pulse. The point at which this pulse reduces the reflected light to its maximum, and also the point at which the amount of reflected light reaches its peak, i.e.
Accurately represents the center of the pit.
以上の如く、本発明によれば、簡単な回路を付加するだ
けで、ピットの真中を正確に検出できる。As described above, according to the present invention, the center of a pit can be accurately detected by simply adding a simple circuit.
本発明は、記録情報の周波数が高い場合に特に有効であ
る。The present invention is particularly effective when the frequency of recorded information is high.
第1図及び第2図は、本発明の詳細な説明するための図
、第3図は、本発明の一実施例の要部の構成を示す図、
第4図は、その動作説明図、第5図は、本発明の一実施
例の要部の他の構成を示す図である。
第 4 図
第 5 図FIG. 1 and FIG. 2 are diagrams for explaining the present invention in detail, and FIG. 3 is a diagram showing the configuration of main parts of an embodiment of the present invention.
FIG. 4 is an explanatory diagram of its operation, and FIG. 5 is a diagram showing another configuration of essential parts of an embodiment of the present invention. Figure 4 Figure 5
Claims (1)
生する情報再生装置において、上記記録媒体上からの反
射又は透過光を受光する光検出器を、少なくとも二つ以
上の受光部から構成し、各々の受光部からの信号の差を
とることによって、上記情報のピーク値を検出すること
を特徴とする情報再生装置。't. In an information reproducing device that optically reproduces information recorded on a recording medium, a photodetector that receives reflected or transmitted light from the recording medium is composed of at least two or more light receiving sections. , an information reproducing apparatus characterized in that the peak value of the information is detected by taking the difference between the signals from each light receiving section.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP23270883A JPS59132430A (en) | 1983-12-12 | 1983-12-12 | Information reproducing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP23270883A JPS59132430A (en) | 1983-12-12 | 1983-12-12 | Information reproducing device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59132430A true JPS59132430A (en) | 1984-07-30 |
JPS6321257B2 JPS6321257B2 (en) | 1988-05-06 |
Family
ID=16943531
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP23270883A Granted JPS59132430A (en) | 1983-12-12 | 1983-12-12 | Information reproducing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59132430A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS62187418U (en) * | 1986-05-16 | 1987-11-28 |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5164944A (en) * | 1974-10-07 | 1976-06-04 | Philips Nv |
-
1983
- 1983-12-12 JP JP23270883A patent/JPS59132430A/en active Granted
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5164944A (en) * | 1974-10-07 | 1976-06-04 | Philips Nv |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS62187418U (en) * | 1986-05-16 | 1987-11-28 |
Also Published As
Publication number | Publication date |
---|---|
JPS6321257B2 (en) | 1988-05-06 |
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