JPH0229930A - Optimal recording power detection device and method for optical recording media - Google Patents

Optimal recording power detection device and method for optical recording media

Info

Publication number
JPH0229930A
JPH0229930A JP63178478A JP17847888A JPH0229930A JP H0229930 A JPH0229930 A JP H0229930A JP 63178478 A JP63178478 A JP 63178478A JP 17847888 A JP17847888 A JP 17847888A JP H0229930 A JPH0229930 A JP H0229930A
Authority
JP
Japan
Prior art keywords
recording
recording power
signal
output
amplitude
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
JP63178478A
Other languages
Japanese (ja)
Other versions
JP2769508B2 (en
Inventor
Shinichi Tanaka
慎一 田中
Kiyoshi Kimoto
木本 輝代志
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.)
Nikon Corp
Original Assignee
Nikon 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 Nikon Corp filed Critical Nikon Corp
Priority to JP63178478A priority Critical patent/JP2769508B2/en
Priority to US07/379,224 priority patent/US4979162A/en
Publication of JPH0229930A publication Critical patent/JPH0229930A/en
Application granted granted Critical
Publication of JP2769508B2 publication Critical patent/JP2769508B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Optical Head (AREA)
  • Optical Recording Or Reproduction (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、書替可能な光ディスク等の光学式記録媒体の
最適記録パワー検出装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an optimum recording power detection device for an optical recording medium such as a rewritable optical disc.

[従来の技術] 従来、この種の装置には特願昭62−7734号の装置
があり、そのブロック図を第2図に示す。
[Prior Art] Conventionally, this type of device includes the device disclosed in Japanese Patent Application No. 1987-7734, whose block diagram is shown in FIG.

第2図において、まず構成を説明すると、1は読取ヘッ
ドであり、記録媒体としての光ディスク1aにレーザー
ビーム等の照射で成る記録信号により書き込まれた記録
情報を光学的に読取って電気信号に変換し、情報再生信
号を出力する。
In FIG. 2, first, the configuration will be explained. Reference numeral 1 denotes a reading head, which optically reads recorded information written on an optical disk 1a as a recording medium by a recording signal formed by irradiation with a laser beam, etc., and converts it into an electrical signal. and outputs an information reproduction signal.

ここで、記録情報の二次子を検出するために光ディスク
1aに書き込まれる情報ビットとしては、2つの異なっ
た周波数を有する情報ビットをデユーティ比50%を予
定した同一の時間毎に交互に記録し、二次子を検出する
際にはこの2つの異なった周波数を有する情報ビットを
同−時間毎に交互に記録した部分を再生するようになる
Here, as the information bits written on the optical disc 1a in order to detect the secondary of the recorded information, information bits having two different frequencies are recorded alternately at the same time with a duty ratio of 50%. , when detecting a secondary child, a portion in which information bits having two different frequencies are recorded alternately at the same time is reproduced.

二次子を検出するために光ディスク1aに記録する情報
ビットを具体的に説明すると、例えば第3図(a)に示
す周波数の低い記録信号と、第3図(b)に示す周波数
の高い記録信号を記録する。
To specifically explain the information bits recorded on the optical disc 1a to detect secondary particles, for example, a low frequency recording signal shown in FIG. 3(a) and a high frequency recording signal shown in FIG. 3(b) Record the signal.

ここで第3図(b)に示す周波数の高い信号のビット長
をTとすると、第3図(a>に示す周波数の低い信号の
ビット長は2丁に設定される。勿論、ビット長2T、T
を持つ各記録信号のデユーティ比はそれぞれ50%とし
ているが、記録信号となるレーザーパワーのバラ付きに
より破線で示すようにデユーティ比の変動を生ずる。
Here, if the bit length of the high frequency signal shown in FIG. 3(b) is T, the bit length of the low frequency signal shown in FIG. 3(a) is set to 2.Of course, the bit length is 2T. , T
The duty ratio of each recording signal is set to 50%, but due to variations in the laser power used as the recording signal, the duty ratio varies as shown by the broken line.

今、ビット長2T、Tを有する2つの記録信号に同じビ
ット長の変動Δ丁が生じたとすると、ビット長Tの周波
数の高い信号に比べ、ビット長が2丁となる周波数の低
い信号のデユーティ比はあまり変化しない。従って、周
波数の低いビット長2丁の記録信号のデユーティ比は信
丹歪が多少生じても略デユーティ比50%に維持され、
後の説明で明らかにする二次子の検出において、周波数
の低いビット長2Tの記録信号を基準信号として用いる
Now, if two recording signals with bit lengths 2T and T have the same bit length fluctuation Δt, the duty of the low frequency signal with bit length 2 is higher than that of the high frequency signal with bit length T. The ratio does not change much. Therefore, the duty ratio of the recording signal of two bit lengths with low frequency is maintained at approximately 50% even if some Shintan distortion occurs.
In secondary child detection, which will be explained later, a recording signal with a low frequency and a bit length of 2T is used as a reference signal.

再び、第2図を参照するに、読取ヘッド1で読取られた
二次歪検出のための情報再生信号は、コンデンサC1に
よる交流結合をもってアンプ2に入力され、アンプ2で
交流増幅された後、同じく交流結合用のコンデンサC2
を介して包絡線検波回路3a、3bのそれぞれに入力さ
れる。
Referring again to FIG. 2, the information reproduction signal for second-order distortion detection read by the reading head 1 is input to the amplifier 2 with AC coupling by the capacitor C1, and after being AC amplified by the amplifier 2, Also capacitor C2 for AC coupling
The signal is inputted to each of the envelope detection circuits 3a and 3b via.

包絡線検波回路3aはアンプ2より得られた情報再生信
号を振幅中心レベルの上側で包絡線検波し、一方、包絡
線検波回路3bは振幅中心レベルの下側で包絡線検波を
行なう。
The envelope detection circuit 3a performs envelope detection of the information reproduction signal obtained from the amplifier 2 above the amplitude center level, while the envelope detection circuit 3b performs envelope detection below the amplitude center level.

包絡線検波回路3a、3bの出力はそれぞれ帯域通過フ
ィルタ4a、4bに与えられ、帯域通過フィルタ4a、
4bのそれぞれにおいて包絡線検波出力の振幅成分を抽
出すると同時に正弦波信号に変換する。
The outputs of the envelope detection circuits 3a and 3b are given to bandpass filters 4a and 4b, respectively.
4b, the amplitude component of the envelope detection output is extracted and simultaneously converted into a sine wave signal.

帯域通過フィルタ4a、4bの出力は振幅検出回路5a
、5bに与えられ、帯域通過フィルタ4a、4bを通過
した包絡線検波信号の振幅成分における振幅ピーク値を
それぞれ検出する。
The outputs of the bandpass filters 4a and 4b are sent to the amplitude detection circuit 5a.
, 5b, and detects the amplitude peak values of the amplitude components of the envelope detection signals that have passed through the bandpass filters 4a and 4b.

振幅検出回路5a、5bの出力は検出ピーク値の大小に
基づいて情報再生信号に含まれる二次子の度合いを判断
する判断手段としての判断ロジック6に与えられる。判
断ロジック6は振幅検出回路5aで検出された振幅ピー
ク値をhl、振幅検出回路5bで検出された振幅検出値
をh2とすると、この振幅ピーク値hl、h2に基づい
て次の判断処理を行なう。
The outputs of the amplitude detection circuits 5a and 5b are provided to a judgment logic 6 as a judgment means for judging the degree of quadratic included in the information reproduction signal based on the magnitude of the detected peak value. The judgment logic 6 performs the following judgment process based on the amplitude peak values hl and h2, assuming that the amplitude peak value detected by the amplitude detection circuit 5a is hl and the amplitude detection value detected by the amplitude detection circuit 5b is h2. .

(a)h1=h2のとき: 情報再生信号のデユーティ比は50%で且つ二次子を含
まないものと判断する。
(a) When h1=h2: It is determined that the duty ratio of the information reproduction signal is 50% and does not include a secondary child.

(b)hl>h2のとき; 情報再生信号のデユーティ比が50%より小さく、且つ
二次中有りと判断する。
(b) When hl>h2; It is determined that the duty ratio of the information reproduction signal is smaller than 50% and that secondary is present.

(c)hl<h2のとき; 情報再生信号はデユーティ比が50%より大きく且つ二
次中有りと判断する。
(c) When hl<h2; It is determined that the duty ratio of the information reproduction signal is greater than 50% and there is secondary content.

即ち、判断ロジック6は振幅検出回路5a、5bからの
検出ピーク値i1.h2に基づいて前記(a)〜(C)
の判断条件のもとに対応する出力a、b、cのいずれか
1つを出力し、例えば判断ロジック6の出力に基づいて
記録信号のレーザーパワーをコントロールする場合、最
適出力aが得られたときには記録信号のデユーティ比が
50%となっていることから、レーザーパワーをそのと
きの値に維持し、一方、判断出力すが得られたときには
、記録信号のデユーティ比が小さいことからレーザーパ
ワーを高めて記録信号のデユーデイ比を最適出力aが得
られる50%に°制御し、逆に判断出力Cが得られてい
るときには、記録信号のデユーティ比が50%より大き
いことから、レーザーパワーを下げて最適出力aが得ら
れるように制御するようになる。
That is, the judgment logic 6 uses the detected peak values i1. (a) to (C) above based on h2
For example, when outputting one of the corresponding outputs a, b, and c under the judgment conditions of , and controlling the laser power of the recording signal based on the output of the judgment logic 6, the optimum output a was obtained. Sometimes, the duty ratio of the recording signal is 50%, so the laser power is maintained at the value at that time, while when a judgment output is obtained, the duty ratio of the recording signal is small, so the laser power is kept at that value. By increasing the duty ratio of the recording signal, the duty ratio of the recording signal is controlled to 50% where the optimum output a is obtained, and conversely, when the judgment output C is obtained, the duty ratio of the recording signal is greater than 50%, so the laser power is lowered. control is performed so that the optimum output a is obtained.

次に、第2図の実施例の作用を説明する。Next, the operation of the embodiment shown in FIG. 2 will be explained.

まず、光ディスク1aには第3図に示したビット長2T
の記録信号(低い周波数)とビット長Tの記録信@(高
い周波数)を一定間隔で交互に記録しており、例えば第
4図(a)に示すように、ビット長2丁の記録信号に続
いてビット長Tの信号を2つ交互に記録していたものと
する。
First, the optical disc 1a has a bit length of 2T as shown in FIG.
A recording signal (low frequency) with a bit length T (low frequency) and a recording signal @ (high frequency) with a bit length T are alternately recorded at regular intervals. For example, as shown in Figure 4 (a), a recording signal with a bit length T Assume that two signals of bit length T are subsequently recorded alternately.

このように光ディスク1aに記録された2つの異なる周
波数で成る情報ビットを読取ヘッド1により再生して情
報再生信号を得ると、第10図に示した読取光学系の検
出感度、即ち記録周波数に対するMTF特性によりビッ
ト長2丁の再生信号とビット長Tの再生信号とでは再生
信号レベルが異なる。
When the information bits of two different frequencies recorded on the optical disk 1a are reproduced by the reading head 1 to obtain an information reproduction signal, the detection sensitivity of the reading optical system shown in FIG. 10, that is, the MTF with respect to the recording frequency Depending on the characteristics, the reproduced signal level of the reproduced signal with a bit length of 2 and the reproduced signal with the bit length T is different.

即ち、ビット長2丁の記録周波数は低いことから第10
図のMTF周波数特性から明らかなようにMTFの値が
大きく、その結果、ビット長2丁の記録ビットからの情
報再生信号は第5図の信号7に示すように再生レベルが
高くなる。これに対しビット長Tの記録信号の周波数は
高いことから、第10図におけるMTFの値が小さくな
り、第5図の信@8に示すようにビット長2Tの再生信
号7に対し再生信号8のように再生レベルが低くなり、
更にビット長Tの再生信号については基本周波数の2倍
以上の周波数成分の信号が光学系から検出できないため
、略正弦波となる。
In other words, since the recording frequency for two bit lengths is low, the 10th
As is clear from the MTF frequency characteristics shown in the figure, the value of MTF is large, and as a result, the reproduction level of the information reproduction signal from the recording bits with a bit length of 2 becomes high as shown in signal 7 of FIG. On the other hand, since the frequency of the recording signal with bit length T is high, the value of MTF in FIG. 10 becomes small, and as shown in FIG. The playback level becomes lower as shown in
Furthermore, the reproduced signal with bit length T becomes a substantially sinusoidal wave because signals with frequency components that are twice the fundamental frequency or more cannot be detected by the optical system.

そこで、読取光学系におけるMTF周波数特性により第
4図(a)の実線9に示すように、デユーティ比50%
で記録された情報ビットの情報再生信号は、第4図(b
)に示す信号波形となる。
Therefore, due to the MTF frequency characteristics in the reading optical system, the duty ratio is 50%, as shown by the solid line 9 in Fig. 4(a).
The information reproduction signal of the information bits recorded in FIG.
) is the signal waveform shown.

このデユーティ比50%のときの信号波形はビット長2
丁及びビット長Tのいずれの信号についても、中心レベ
ル12に対し上下に対称な再生信号波形となる。
The signal waveform when the duty ratio is 50% is bit length 2.
For both signals with a bit length of 1 and a bit length of T, the reproduced signal waveforms are vertically symmetrical with respect to the center level 12.

次に、第4図(a)に点線で示すデユーティ比が50%
より小さい記録信号10で記録された情報ビットからの
情報再生信号は、第4図(C)に示すようになる。即ち
、ビット長2丁の再生信号についてはデユーティ比変動
分による影響をほとんど受けないことから中心レベル1
2の上下に対称な波形となるが、ビット長Tの再生信号
についてはデユーティ比が50%より小さくなることで
直流成分が減少し、中心レベル12の上側の振幅成分が
減少すると同時に下側の振幅成分が増加した波形となる
Next, the duty ratio shown by the dotted line in Fig. 4(a) is 50%.
The information reproduction signal from the information bits recorded with the smaller recording signal 10 is as shown in FIG. 4(C). In other words, since the reproduced signal with a bit length of 2 bits is hardly affected by the duty ratio fluctuation, the center level is 1.
2, the waveform is symmetrical above and below, but for the reproduced signal with bit length T, when the duty ratio becomes smaller than 50%, the DC component decreases, and the upper amplitude component of center level 12 decreases, while at the same time the lower amplitude component decreases. The resulting waveform has an increased amplitude component.

更に、第4図(a)に−点鎖線で示すように、記録信号
のデユーティ比が50%より大きくなった記録信号11
で記録された情報ビットの情報再生信号は、第4図(d
>に示すようになる。即ち、ビット長2Tの再生信号に
ついてはデユーティ比の増加による変動がほとんどない
ことから、中心レベル12の上下に略対称な波形となる
が、ビット長Tの再生信号はデユーティ比の増hoで直
流成分が増加し、中心レベル12の上側の振幅が増加し
逆に中心レベル12の下側の振幅が減少するようになる
Furthermore, as shown by the dashed line in FIG. 4(a), the recording signal 11 whose duty ratio is greater than 50%
The information reproduction signal of the information bits recorded in FIG.
> is shown. In other words, since the reproduced signal with a bit length of 2T has almost no fluctuation due to an increase in the duty ratio, it has a waveform that is approximately symmetrical above and below the center level 12, but the reproduced signal with a bit length T has a DC current as the duty ratio increases. As the component increases, the amplitude above the center level 12 increases and conversely the amplitude below the center level 12 decreases.

実際には第2図に示したように、コンデンサC1、C2
で交流結合しているため、ビット長2Tの再生信号とビ
ット長Tの再生信号の直流成分の大きさが異なるとき、
第6図に示すようにビット長2Tの再生信号の中心レベ
ル12aとビット長Tの再生信号の中心レベル12bと
の間にはリグ13が生じている。このリグが生じている
間に検出しなければならない。従って、ピッ1ル長2丁
の信号とビット長Tの信号を記録する周期ではあまり大
きくすることはできない。
Actually, as shown in Figure 2, capacitors C1 and C2
Since the AC coupling is performed at
As shown in FIG. 6, a rig 13 is generated between the center level 12a of the reproduced signal with bit length 2T and the center level 12b of the reproduced signal with bit length T. This rig must be detected while it is occurring. Therefore, the period for recording a signal with two pill lengths and a signal with a bit length T cannot be made very large.

このように読取ヘッド1の読取光学系を介して再生され
る情報再生信号の二次歪検出につき、例えば第4図(C
)に示すようにデユーティ比が50%より小さいとぎの
情報再生信号を例にとって具体的に説明する。
Regarding the second-order distortion detection of the information reproduction signal reproduced through the reading optical system of the reading head 1, for example, FIG.
), the information reproduction signal having a duty ratio smaller than 50% will be specifically explained.

読取ヘッド1で再生されたデユーティ比が50%より小
さいときの情報再生信号はアンプ2で交流増幅された後
、包絡線検波回路3a、3bに与えられ、包絡線検波回
路3aは第7図(a>に示す上側包絡線の検波出力を生
じ、一方、包絡線検波回路3bは第7図(b)に示す下
側包絡線の検波出力を生ずる。
The information reproduction signal reproduced by the reading head 1 when the duty ratio is smaller than 50% is AC amplified by the amplifier 2 and then applied to the envelope detection circuits 3a and 3b. The envelope detection circuit 3b produces a detection output of the upper envelope shown in FIG. 7(b).

この第7図に示す上側及び下側の包絡線検波信号におい
て、振幅の大きい部分はビット長2Tの再生信号を表し
、振幅成分の小さい部分がビット長Tの再生信号を表す
In the upper and lower envelope detection signals shown in FIG. 7, a portion with a large amplitude component represents a reproduced signal with a bit length of 2T, and a portion with a small amplitude component represents a reproduced signal with a bit length of T.

包絡線検波回路3a、3bで包絡線検波された上側及び
下側の包絡線検波信号は帯域通過フィルタ4a、4bに
入力される。ここで、帯域通過フィ/L’la、4bの
中心周波数fcはfc=1/τに設定されており、帯域
フィルタ4aを通過した第7図(a)に示す上側包絡線
検波信号は、第8図(a)に示す振幅成分を抽出し且つ
正弦波に変換された信号となり、一方、第7図(b)に
示す下側包絡線検波信号は、第8図(b)に示すように
振幅成分を抽出し且つ正弦波信号に変換された信号とな
る。
The upper and lower envelope detection signals subjected to envelope detection by the envelope detection circuits 3a and 3b are input to band pass filters 4a and 4b. Here, the center frequency fc of the bandpass filter 4b is set to fc=1/τ, and the upper envelope detection signal shown in FIG. 7(a) that has passed through the bandpass filter 4a is The amplitude component shown in Fig. 8(a) is extracted and converted into a sine wave, and the lower envelope detection signal shown in Fig. 7(b) is the signal shown in Fig. 8(b). The amplitude component is extracted and the signal is converted into a sine wave signal.

この帯域通過フィルタ4a、4bを通過することで得ら
れた第8図(a)、(b)に示す上側包絡線検波出力の
振幅成分及び下側包絡線検波信号の振幅成分は振幅検出
回路5a、5bのそれぞれにおいて振幅ピーク値h1.
h2が検出され、判断ロジック6において検出ピーク値
h1.h2の大小関係に基づいて二次子の有無の検出及
びデユーティ比の50%からのずれを判断する。
The amplitude component of the upper envelope detection output and the amplitude component of the lower envelope detection signal shown in FIGS. 8(a) and 8(b) obtained by passing through the band pass filters 4a and 4b are obtained by the amplitude detection circuit 5a. , 5b, the amplitude peak value h1.
h2 is detected, and in the judgment logic 6, the detected peak value h1. Based on the magnitude relationship of h2, the presence or absence of a secondary child is detected and the deviation of the duty ratio from 50% is determined.

即ち、第8図の場合にはhl>h2であることから、二
次子を生じており、且つデユーティ比が50%より小さ
いとする判断出力すを生ずることになる。
That is, in the case of FIG. 8, since hl>h2, a determination is made that a secondary child is generated and the duty ratio is smaller than 50%.

勿論、第4図(d)に示すように、デユーティ比が50
%より大きいとぎには振幅検出回路J a t5bから
得られる検出ピーク値h1.h2は、hl<h2となる
ことから、判断ロジック6は二次子の発生を判断すると
同時にデユーティ比が50%より大きいとなる判断出力
Cを生ずる。更に、デユーティ比が50%のとぎにはh
l、=h2であり、このときは最適出力aを生ずるよう
になる。
Of course, as shown in FIG. 4(d), the duty ratio is 50.
%, the detected peak value h1. obtained from the amplitude detection circuit J a t5b. Since h2 is hl<h2, the decision logic 6 determines the occurrence of a secondary child and at the same time generates a decision output C in which the duty ratio is greater than 50%. Furthermore, when the duty ratio is 50%, h
l,=h2, and in this case, the optimum output a is produced.

[発明が解決しようとする課題] しかしながら、このような従来装置にあっては、二次子
のない最適な記録パワーを検出する場合、第8図に示し
た厳密にh1=h2となる記録パワーを検出することは
回路上不可能なため、実際には所定値α(αは正)に対
し hl−h2<α の範囲内となる記録パワーが適正であると判定する。
[Problems to be Solved by the Invention] However, in such a conventional device, when detecting the optimal recording power without secondary particles, the recording power that strictly satisfies h1=h2 as shown in FIG. Since it is impossible to detect it due to the circuit, it is actually determined that the recording power that falls within the range of hl-h2<α for a predetermined value α (α is positive) is appropriate.

このため二次歪検出に基づいて最適な記録パワーを検出
する際に、記録パワーの初期値が過大又は過少であった
場合、(l hl−h2 1 >が所定値α内に収まる
ように記録パワーを補正すると、常に適正と判定する境
界のところ hl−h2+=α で最適な記録パワーになったものと判定していまう。
Therefore, when detecting the optimum recording power based on second-order distortion detection, if the initial value of the recording power is too large or too small, the When the power is corrected, it is determined that the optimum recording power is reached at hl-h2+=α at the boundary where it is always determined to be appropriate.

そこで二次子の検出精度を上げるためには、所定値αを
小さくしなければならないが、所定値αを小さくすると
回路上、検出が困難になる問題があった。
Therefore, in order to improve the accuracy of secondary child detection, it is necessary to reduce the predetermined value α, but if the predetermined value α is reduced, there is a problem in that detection becomes difficult due to the circuit.

また光学系統の分解能力の差によって第11図の■■の
ように、MTFの周波数特性が変わるため、低い周波数
f1の信号の振幅差と、高い周波数f2の信号の振幅差
が異なることになる。
Also, as shown in Figure 11, the frequency characteristics of the MTF change due to differences in the resolution ability of the optical system, so the amplitude difference between the low frequency f1 signal and the high frequency f2 signal will differ. .

例えば、MTF周波数特性が第11図の■のとき、第2
図に示した上側及び下側の包絡線検波回路3a、3bの
出力は第12図(a )のJ:うになり、一方、MTF
周波数特性が第11図の■のときは、上側及び下側の包
絡線検波回路3a 、 3bの出力は第12図(b )
のようになる。即ち、光学系のMTF周波数特性によっ
て振幅差りが変化する。
For example, when the MTF frequency characteristic is ■ in Figure 11, the second
The outputs of the upper and lower envelope detection circuits 3a and 3b shown in the figure are J in FIG. 12(a), while the MTF
When the frequency characteristics are shown in Figure 11 (■), the outputs of the upper and lower envelope detection circuits 3a and 3b are as shown in Figure 12 (b).
become that way. That is, the amplitude difference changes depending on the MTF frequency characteristics of the optical system.

このため二次子の検出精度を示す所定値αに対し振幅り
が小さくなると、 hl−h21−α のとき、上側包絡線検波出力の波形と下側包絡線検波出
力の波形との非対象性が大きくなり、二次子の検出精度
が悪くなる。
Therefore, when the amplitude decreases with respect to a predetermined value α that indicates the detection accuracy of the quadratic, when hl-h21-α, there is an asymmetry between the waveform of the upper envelope detection output and the waveform of the lower envelope detection output. becomes large, and the secondary child detection accuracy deteriorates.

従って、光学系の分解能の相違により二次子の検出精度
が変ってしまうという問題があった。
Therefore, there is a problem in that the detection accuracy of secondary particles changes due to the difference in resolution of the optical system.

本発明は、このような従来の問題点に鑑みてなされたも
ので、二次歪検出の回路精度を高めることなく且つヘッ
ドの光学的分解にばらつきがあっても常に二次子を最小
とする最適な記録パワーを検出することのできる光学式
記録媒体の最適記録パワー検出装置を提供することを目
的とする。
The present invention was made in view of these conventional problems, and it is possible to always minimize the secondary distortion even if there are variations in the optical decomposition of the head without increasing the circuit accuracy of secondary distortion detection. It is an object of the present invention to provide an optimal recording power detection device for an optical recording medium that can detect the optimal recording power.

[課題を解決するための手段] この目的を達成するため本発明にあっては、記録媒体に
2つの異なった周波数によるデユーティ比率50%を予
定した2値情報を交互に光学的に記録すると共に、該記
録情報を光学的に読取って電気信号tこ変換する記録読
取手段と:該記録読取手段の出力信号を交流増幅する交
流増幅手段と:該交流増幅手段の出力の振幅中心レベル
の上側と下側で記録周波数の相違に曇づいて生ずる振幅
差hl 、 h2のそれぞれを検出する2つの振幅差検
出手段と;該2つの振幅差検出手段の出力差(hl−h
2 )を所定の値+αと値−αと比較して前記記録情報
に含まれる二次歪みの有無及び極性を判定する判定手段
と:記録パワーを発光させるに必要な電流を発生するレ
ーザー駆動手段と:前記判定手段から前記2つの振幅差
検出手段の出力差(旧−h2 )が前記値+α及び値−
αと一致する判定出力が得られるように前記レーザ駆動
手段により記録パワーを変化させ、該十α及び−αに一
致する出力差が得られた時の各記録パワーの平均値とし
て最適記録パワーを検出して前記レーザー駆動手段に設
定する制御手段と:を設けるようにしたものである。
[Means for Solving the Problems] In order to achieve this object, the present invention optically records binary information with a scheduled duty ratio of 50% using two different frequencies on a recording medium alternately, and , recording reading means for optically reading the recorded information and converting it into an electric signal; AC amplifying means for AC amplifying the output signal of the recording reading means; and above the amplitude center level of the output of the AC amplifying means. two amplitude difference detection means for detecting each of the amplitude differences hl and h2 caused by the difference in recording frequency on the lower side; an output difference (hl-h) of the two amplitude difference detection means;
2) Judgment means that compares 2) with predetermined values +α and -α to determine the presence or absence and polarity of secondary distortion included in the recorded information; and: laser drive means that generates a current necessary to emit recording power. and: The output difference (old -h2) of the two amplitude difference detection means from the judgment means is the value +α and the value -
The recording power is changed by the laser driving means so as to obtain a judgment output that matches α, and the optimum recording power is determined as the average value of each recording power when an output difference that matches α and −α is obtained. and a control means for detecting and setting the laser driving means.

[作用] このような構成を備えた本発明の光学式記録媒体の最適
記録パワー検出装置にあっては、記録パワーを変化させ
たときの2つの振幅差検出回路の出力旧、h2の差につ
いて、 hl−h21<α となる範囲の境界(上限及び下限)となる各記録パワー
、即ち、出ツノ差(hl−h2 )が値+α及び値−α
に一致するときの各記録パワーを検出し、この+αと−
αを与える記録パワーの中心となる平均値の記録パワー
を最適記録パワーとして検出する。
[Function] In the optimum recording power detection device for an optical recording medium of the present invention having such a configuration, it is possible to determine the difference between the outputs of the two amplitude difference detection circuits h2 and h2 when the recording power is changed. , each recording power that is the boundary (upper limit and lower limit) of the range where hl-h21<α, that is, the output horn difference (hl-h2) is the value +α and the value -α.
Detect each recording power when it matches, and calculate the +α and −
The average recording power that is the center of the recording powers that give α is detected as the optimum recording power.

具体的には、記録パワーを変化させて hl−h2=−α となる記録パワーへ(上限)と、 hl−h2.=+α となる記録パワーB(下限)を検出し、(A+8)/2 となる平均記録パワーを最適記録パワーとして求める。Specifically, by changing the recording power hl-h2=-α To the recording power (upper limit), hl-h2. =+α Detect the recording power B (lower limit) that becomes (A+8)/2 Find the average recording power that gives the optimum recording power.

このような最適記録パワーの検出にあっては、所定値α
をより小さな値に厳密に設定する必要がないため、回路
上の負担が小さくなり、また光学系統のばらつきに影響
されずに、常に二次歪を最小とする最適な記録パワー、
即ち、 hl−h21丹O となる最適記録パワーを検出して設定することができる
In detecting such optimal recording power, a predetermined value α
Since there is no need to strictly set the value of
That is, it is possible to detect and set the optimum recording power that satisfies hl-h21tanO.

[実施例] 第1図は本発明の一実施例を示したブロック図である。[Example] FIG. 1 is a block diagram showing one embodiment of the present invention.

第1図において、1は読取記録ヘッドであり、記録媒体
としての光ディスク1aにレーザービーム等の照射で記
録信号により情報を書込み、また書込まれた記録情報を
光学的に読取って電気信号に変換して情報再生信号を出
力する。
In FIG. 1, numeral 1 denotes a reading/recording head, which writes information in the form of a recording signal by irradiating an optical disk 1a as a recording medium with a laser beam or the like, and optically reads the written recording information and converts it into an electrical signal. and outputs an information reproduction signal.

破線で囲んだ二次歪検出回路2oは、第2図に示した従
来装置と同じ回路構成を有する。
A secondary distortion detection circuit 2o surrounded by a broken line has the same circuit configuration as the conventional device shown in FIG.

二次歪検出回路20の出力、即ち判定ロジック6の出力
は、記録パワーが過大、適正及び過少の、3つの判定出
力となる。
The output of the second-order distortion detection circuit 20, that is, the output of the determination logic 6, becomes three determination outputs: excessive, appropriate, and insufficient recording power.

具体的には、振幅検出回路5a、5bの出力h1、[1
2と所定値αに基づき、 hl−h21<α の比較判定を行なって過大、適正及び過少の判定出力を
生ずる。
Specifically, the output h1, [1
2 and a predetermined value α, a comparison judgment of hl−h21<α is performed to generate judgment outputs of excessive, appropriate, and insufficient.

7はCPUであり、CPU7は二次歪検出回路20の判
定出力に基づいて、ある一定の割合で記録パワーの設定
値を変化させたり、波節するものであり、CPU7の制
御機能によって最適記録パワーの検出処理が行なわれる
7 is a CPU, and the CPU 7 changes or modulates the setting value of the recording power at a certain rate based on the judgment output of the secondary distortion detection circuit 20, and the control function of the CPU 7 determines the optimal recording. Power detection processing is performed.

8はD/Aコンバータであり、CPLI7がら送られて
きたレーザーの記録パワー設定値となるディジタル値を
アナログ電圧に変換する。9はレーザー駆動回路であり
、D/Δコンバータ8のアナログ電圧によるレーザーの
記録パワーの設定値に応じたレーザー駆動電流を発生す
る。
8 is a D/A converter, which converts the digital value sent from the CPLI 7, which is the laser recording power setting value, into an analog voltage. Reference numeral 9 denotes a laser drive circuit, which generates a laser drive current according to the set value of laser recording power based on the analog voltage of the D/Δ converter 8.

次に第1図の実施例の動作を説明する。Next, the operation of the embodiment shown in FIG. 1 will be explained.

まずCPLJ7は、そのとき設定されている任意の記録
パワーの初期値による二次歪検出回路20の判定出力を
読込む。
First, the CPLJ 7 reads the determination output of the secondary distortion detection circuit 20 based on the initial value of the arbitrary recording power set at that time.

このとき、二次歪検出回路20の判定出力が過少である
ことを示していた場合には、CPU7はある一定割合で
記録パワーの設定値を増加させ、ある割合を増加させる
毎に記録再生を繰り返し、二次歪検出回路20の判定出
力が適正となったならば、その時の記録パワーの設定値
Bを記憶保持する。
At this time, if the judgment output of the secondary distortion detection circuit 20 indicates that the output is too low, the CPU 7 increases the set value of the recording power at a certain rate, and performs recording/reproduction every time the set value of the recording power is increased by a certain rate. Repeatedly, when the judgment output of the secondary distortion detection circuit 20 becomes appropriate, the recording power setting value B at that time is stored and held.

即ち、記録パワーの初期値が過少とは、(hl−h2)
<十α の場合となる下限値より小さい場合であり、この状態で
記録パワーを段階的に増加させることにより適正出力と
なるのは、 (hl−h2)=+α となった時である。
In other words, when the initial value of recording power is too small, (hl-h2)
<10α, which is the case, is smaller than the lower limit value, and by increasing the recording power stepwise in this state, a proper output is achieved when (hl−h2)=+α.

この関係は、 (h2−hl)>−α (h2−hl)=−α と現わすこともできる。This relationship is (h2-hl)>-α (h2-hl)=-α It can also be expressed as

続いてCPU7は更に記録パワーの設定値を増加させ、
二次歪検出回路20の判定出力が過大となった時、その
直前の判定出力が適正となっていた時の記録パワーの設
定値Aを記憶保持する。
Next, the CPU 7 further increases the setting value of the recording power,
When the judgment output of the secondary distortion detection circuit 20 becomes excessive, the set value A of the recording power when the judgment output immediately before was appropriate is stored and held.

即ち、二次歪検出回路20の判定出力が過大となるのは
、 (hl−h2)>−α と上限値を越えた時であり、その直前にあっては、hl
−h2〜−α となる関係が1qられており、この時の記録パワーの設
定値Aを記憶保持する。
That is, the determination output of the second-order distortion detection circuit 20 becomes excessive when (hl-h2)>-α exceeds the upper limit value, and just before that, hl
A relationship of -h2 to -α is set as 1q, and the set value A of the recording power at this time is stored and held.

このようにしてCPU7は、記録パワーが適正範囲の上
限となる設定値A及び下限となる設定値Bを検出する。
In this way, the CPU 7 detects the setting value A that is the upper limit of the recording power range and the setting value B that is the lower limit of the appropriate recording power range.

続いてCPU7は記録パワーが適正となる範囲の上限設
定1aAと下限設定値Bとの平均値を、(A+B)/2 として演痒し、この演算された平均値を最適記録パワー
を与える設定値としてレーザー駆動回路9に設定し、一
連の最適記録パワーの設定処理を終了する。
Next, the CPU 7 calculates the average value of the upper limit setting 1aA and the lower limit setting B in the range where the recording power is appropriate as (A+B)/2, and uses this calculated average value as the setting value that provides the optimum recording power. The optimum recording power is set in the laser drive circuit 9, and a series of optimum recording power setting processes are completed.

一方、記録パワーの初期値による二次歪検出回路20の
判定出力が過大であった場合には、逆にCPU7は記録
パワーの設定値をある割合で段階的に減少させることに
よって、同様に記録パワーの適正範囲を決める上限設定
値A及び下限設定値Bを検出して両者の平均値として最
適記録パワーの設定値を検出することができる。
On the other hand, if the judgment output of the secondary distortion detection circuit 20 based on the initial value of the recording power is excessive, the CPU 7 conversely decreases the set value of the recording power step by step at a certain rate to perform the same recording process. It is possible to detect the upper limit setting value A and the lower limit setting value B that determine the appropriate range of power, and to detect the optimum recording power setting value as the average value of both.

更に、記録パワーの初期値による二次歪検出回路20の
判定出力が適正であった場合には、適正状態から例えば
記録パワーの設定値をある割合で増加させて上限設定値
Aを検出し、その後に記録パワーの設定値を減少させて
下限設定値Bを検出すればよい。
Furthermore, if the judgment output of the secondary distortion detection circuit 20 based on the initial value of the recording power is appropriate, for example, the setting value of the recording power is increased at a certain rate from the appropriate state to detect the upper limit setting value A, Thereafter, the lower limit setting value B may be detected by decreasing the recording power setting value.

[発明の効果] 以上説明してきたように本発明によれば、二次歪検出の
ための回路上の精度を厳しくする必要がなく、またヘッ
ド光学系の分解能のばらつきに影響されず、常に二次歪
を最小とする最適な記録パワーを検出して設定すること
ができる。
[Effects of the Invention] As explained above, according to the present invention, there is no need to tighten the accuracy of the circuit for detecting second-order distortion, and it is not affected by variations in the resolution of the head optical system, and the second-order distortion is always It is possible to detect and set the optimum recording power that minimizes the order distortion.

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

第1図は本発明の一実施例を示したブロック図:第2図
は従来装置を示したブロック図:第3図し二次歪検出対
象とする2つの周波数の異なる記録信号の説明図; 第4図は記録信号のデユーティ比率を50%、50%よ
り小、50%より大とした時の再生信号を示した信号波
形図: 第5図は読取光学系のMTF周波数特性による再生信号
のレベル変化を示した信号波形図:第6図は直流成分の
相違により生ずる再生信号のザブを示した信号波形図: 第7図は第2図の包絡線検波信号の波形説明図;第8図
は第2図の帯域フィルタの出力を示した信号波形図: 第9図は記録信号のデユーティ比率の変化を示した信号
波形図: 第10図は読取光学系のMTF周波数特性を示したグラ
フ図: 第11図は読取光学系の分解能の違いによるMTF周波
数特性の相違を示したグラフ図:第12図は第11図の
MTF周波数特性の相違による上側及び下側包絡線検波
出力の波形シ1明図である。 1:読取ヘッド 1a:光ディスク 2:アンプ 3a 、 3b :包絡線検波回路 4a 、 4b :帯域通過フィルタ 5a 、 5b :振幅検出回路 6:判断ロジック 7:CPU 8 : D/Aコンバータ 9:レーザー駆動回路
FIG. 1 is a block diagram showing an embodiment of the present invention; FIG. 2 is a block diagram showing a conventional device; FIG. 3 is an explanatory diagram of recording signals with two different frequencies to be detected as secondary distortion; Figure 4 is a signal waveform diagram showing the reproduction signal when the duty ratio of the recording signal is 50%, less than 50%, and greater than 50%. Figure 5 shows the reproduction signal according to the MTF frequency characteristics of the reading optical system. Signal waveform diagram showing level changes: Figure 6 is a signal waveform diagram showing dips in the reproduced signal caused by differences in DC components; Figure 7 is an explanatory diagram of the waveform of the envelope detection signal in Figure 2; Figure 8 Figure 9 is a signal waveform diagram showing the output of the bandpass filter in Figure 2. Figure 9 is a signal waveform diagram showing changes in the duty ratio of the recording signal. Figure 10 is a graph diagram showing the MTF frequency characteristics of the reading optical system. : Figure 11 is a graph showing the difference in MTF frequency characteristics due to the difference in the resolution of the reading optical system; Figure 12 is a graph showing the waveforms of the upper and lower envelope detection outputs due to the difference in the MTF frequency characteristics in Figure 11. This is a clear diagram. 1: Reading head 1a: Optical disk 2: Amplifier 3a, 3b: Envelope detection circuit 4a, 4b: Band pass filter 5a, 5b: Amplitude detection circuit 6: Judgment logic 7: CPU 8: D/A converter 9: Laser drive circuit

Claims (1)

【特許請求の範囲】[Claims] (1)記録媒体に、2つの異なつた周波数によるデュー
ティ比率50%を予定した2値情報を交互に光学的に記
録すると共に、該記録情報を光学的に読取つて電気信号
に変換する記録読取手段と;該記録読取手段の出力信号
を交流増幅する交流増幅手段と; 該交流増幅手段の出力の振幅中心レベルの上側と下側で
記録周波数に基づいて生ずる振幅差h1、h2のそれぞ
れを検出する2つの振幅差検出手段と;該2つの振幅差
検出手段の出力差(h1−h2)を所定の最大値+α及
び最小値−αと比較して前記記録情報に含まれる二次歪
の有無及び極性を判定する判定手段と; 記録パワーを発光させるに必要な電流を発生するレーザ
駆動手段と; 前記判定手段から前記2つの振幅差検出手段の出力差(
h1−h2)が最大値+α及び最小値−αとに一致する
判定出力が得られるように前記レーザ駆動手段により記
録パワーを変化させ、該最大値+α及び最小値−αに一
致する出力差が得られた時の各記録パワーの平均値とし
て最適記録パワーを検出して前記レーザ駆動手段に設定
する制御手段と; を備えたことを特徴とする光学式記録媒体の最適記録パ
ワー検出装置。
(1) A recording/reading means for optically recording alternately binary information with a scheduled duty ratio of 50% at two different frequencies on a recording medium, and optically reading the recorded information and converting it into an electrical signal. and; AC amplifying means for AC amplifying the output signal of the recording/reading means; and detecting amplitude differences h1 and h2 that occur based on the recording frequency above and below the amplitude center level of the output of the AC amplifying means. two amplitude difference detection means; the output difference (h1-h2) of the two amplitude difference detection means is compared with a predetermined maximum value +α and minimum value −α to determine the presence or absence of secondary distortion contained in the recorded information; a determination means for determining polarity; a laser drive means for generating a current necessary to emit recording power; and a determination means for detecting an output difference (
The recording power is changed by the laser driving means so that a judgment output in which h1-h2) matches the maximum value +α and the minimum value -α, and the output difference that matches the maximum value +α and the minimum value -α is An apparatus for detecting optimum recording power for an optical recording medium, comprising: a control means for detecting an optimum recording power as an average value of the respective recording powers obtained and setting the optimum recording power to the laser driving means;
JP63178478A 1987-01-16 1988-07-18 Apparatus and method for detecting optimum recording power of optical recording medium Expired - Fee Related JP2769508B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP63178478A JP2769508B2 (en) 1988-07-18 1988-07-18 Apparatus and method for detecting optimum recording power of optical recording medium
US07/379,224 US4979162A (en) 1987-01-16 1989-07-13 Apparatus for detecting the secondary distortion of optical type recorded information

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63178478A JP2769508B2 (en) 1988-07-18 1988-07-18 Apparatus and method for detecting optimum recording power of optical recording medium

Publications (2)

Publication Number Publication Date
JPH0229930A true JPH0229930A (en) 1990-01-31
JP2769508B2 JP2769508B2 (en) 1998-06-25

Family

ID=16049189

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63178478A Expired - Fee Related JP2769508B2 (en) 1987-01-16 1988-07-18 Apparatus and method for detecting optimum recording power of optical recording medium

Country Status (1)

Country Link
JP (1) JP2769508B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0636288A (en) * 1992-07-22 1994-02-10 Sanyo Electric Co Ltd Rf signal amplitude controller for optical reproducer
JP2008099501A (en) * 2006-10-16 2008-04-24 Hokuriku Electric Power Co Inc:The Transmission tower line marking device

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54173705U (en) * 1978-05-29 1979-12-07

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54173705U (en) * 1978-05-29 1979-12-07

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0636288A (en) * 1992-07-22 1994-02-10 Sanyo Electric Co Ltd Rf signal amplitude controller for optical reproducer
JP2008099501A (en) * 2006-10-16 2008-04-24 Hokuriku Electric Power Co Inc:The Transmission tower line marking device

Also Published As

Publication number Publication date
JP2769508B2 (en) 1998-06-25

Similar Documents

Publication Publication Date Title
JPH0365705B2 (en)
CA1275730C (en) Reading circuit in an optical disk apparatus
JP2810592B2 (en) Digital information reproducing device
JP3555981B2 (en) Quality signal extracting method, recording device and reading device
US5057946A (en) Magnetic disk drive apparatus
JP3107263B2 (en) Information playback device
JPH0229930A (en) Optimal recording power detection device and method for optical recording media
JPH07101511B2 (en) Information recording / reproducing device
JPS63304427A (en) Signal recording and reproducing system
JP2826327B2 (en) Optical recording / reproducing device
JP2600659B2 (en) Apparatus for detecting secondary distortion of recording signal and optical recording apparatus
JPS58199410A (en) Magnetic recording method for digital signals
JP2584821B2 (en) Optical disc playback device
JPS6145415A (en) Reading circuit of optical storage device
JPS6350978A (en) Optical disk demodulation circuit
JP3286025B2 (en) Digital signal detection circuit
JPS59113529A (en) Reading out circuit of storage device
JP2507019B2 (en) Recording and playback device
JPH0540978A (en) Optical information recording / reproducing device
JPH01165004A (en) Reproducing circuit of magnetic recording/reproducing device
JPH0689438A (en) Laser power adjusting circuit for optical disk device
JPH02128326A (en) Optical recording and reproducing device
Shimpuku et al. Variable length RLL codes for high-density optical recording
JPH0421251B2 (en)
JPH0413275A (en) Optical information recording and reproducing device

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees