JP2600659B2 - Apparatus for detecting secondary distortion of recording signal and optical recording apparatus - Google Patents
Apparatus for detecting secondary distortion of recording signal and optical recording apparatusInfo
- Publication number
- JP2600659B2 JP2600659B2 JP62007734A JP773487A JP2600659B2 JP 2600659 B2 JP2600659 B2 JP 2600659B2 JP 62007734 A JP62007734 A JP 62007734A JP 773487 A JP773487 A JP 773487A JP 2600659 B2 JP2600659 B2 JP 2600659B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- amplitude
- recording
- duty ratio
- reading
- 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.)
- Expired - Lifetime
Links
- 230000003287 optical effect Effects 0.000 title description 24
- 238000001514 detection method Methods 0.000 claims description 58
- 230000001678 irradiating effect Effects 0.000 claims description 3
- 238000001228 spectrum Methods 0.000 description 16
- 238000010586 diagram Methods 0.000 description 12
- 230000007423 decrease Effects 0.000 description 7
- 239000003990 capacitor Substances 0.000 description 4
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- 230000003595 spectral effect Effects 0.000 description 3
- 239000000284 extract Substances 0.000 description 2
- 238000009499 grossing Methods 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 230000003321 amplification Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 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
-
- 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
- G11B7/0045—Recording
-
- 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
- G11B7/007—Arrangement of the information on the record carrier, e.g. form of tracks, actual track shape, e.g. wobbled, or cross-section, e.g. v-shaped; Sequential information structures, e.g. sectoring or header formats within a track
-
- 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
- G11B7/007—Arrangement of the information on the record carrier, e.g. form of tracks, actual track shape, e.g. wobbled, or cross-section, e.g. v-shaped; Sequential information structures, e.g. sectoring or header formats within a track
- G11B7/013—Arrangement of the information on the record carrier, e.g. form of tracks, actual track shape, e.g. wobbled, or cross-section, e.g. v-shaped; Sequential information structures, e.g. sectoring or header formats within a track for discrete information, i.e. where each information unit is stored in a distinct discrete location, e.g. digital information formats within a data block or sector
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Head (AREA)
- Measuring Magnetic Variables (AREA)
- Optical Recording Or Reproduction (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は、光ディスクや光磁気ディスク等の記録媒体
に記録された情報に含まれる二次歪の有無を検出する光
学式記録情報の二次歪検出装置に関する。DETAILED DESCRIPTION OF THE INVENTION (Industrial application field) The present invention relates to a method for detecting the presence or absence of secondary distortion contained in information recorded on a recording medium such as an optical disk or a magneto-optical disk. The present invention relates to a distortion detection device.
(従来技術) 従来、記録情報に基づくレーザービームの照射等で光
ディスクに機械的な凹凸形状でなる記録ピットの形で情
報を記録する場合、或いは光磁気ディスクに上下方向に
向いた磁化方向による記録ビットの形で情報を記録する
場合、適正なレーザーの駆動パワーを得るためにデュー
ティ比が50%の2値信号を記録せしめ、媒体に記録され
た記録情報のデューティ比が50%となるように即ち二次
歪を含まないようにレーザーパワーを校正し、校正した
レーザーパワーにより記録している。(Prior Art) Conventionally, when information is recorded in the form of recording pits having mechanical irregularities on an optical disk by irradiating a laser beam based on the recorded information, or recording on a magneto-optical disk in a magnetization direction oriented vertically. When recording information in the form of bits, a binary signal having a duty ratio of 50% is recorded in order to obtain an appropriate laser drive power, and the duty ratio of the recorded information recorded on the medium is set to 50%. That is, the laser power is calibrated so as not to include the secondary distortion, and recording is performed using the calibrated laser power.
ところで、光ディスクに記録された情報に含まれる二
次歪の測定には、通常、スペクトルアナライザーが用い
られる。即ち、光ディスクの記録情報を読取ヘッドによ
り光学的に読取って電気信号に変換し、読取ヘッドから
得られた情報再生信号をスペクトラムアナイザーで解析
するようになる。Incidentally, a spectrum analyzer is usually used for measuring the secondary distortion included in the information recorded on the optical disc. That is, information recorded on an optical disk is optically read by a read head and converted into an electric signal, and an information reproduction signal obtained from the read head is analyzed by a spectrum analyzer.
このスペクトラムアナライザーにより記録情報の回析
を行なった場合、第8図(a)に示す(Ta/T)で与えら
れるデューティ比が50%となる理想的な記録信号による
記録状態にあっては、記録情報のスペクトルアナライザ
ーによる測定結果は第9図(a)に示すように、記録周
波数(基本周波数)fsに対し3fs,5fs,・・・というよう
に奇数次のみのスペクトル成分が得られる。When recording information is analyzed by this spectrum analyzer, in a recording state by an ideal recording signal in which the duty ratio given by (Ta / T) shown in FIG. 8A is 50%, As shown in FIG. 9 (a), the measurement result of the recorded information by the spectrum analyzer shows that only the odd-order spectral components such as 3fs, 5fs,... Are obtained with respect to the recording frequency (fundamental frequency) fs.
一方、第8図(b)に示すように、記録信号のデュー
ティ比が50%より小さかったり、逆に第2図(c)に示
すようにデューティ比が50%より大きかった場合には、
このような記録信号による記録情報は第9図(b)に示
すスペクトルアナライザーの測定結果が得られ、この場
合には、記録周波数fsに対し2fs,3fs,4fs・・・という
ように偶数次のスペクトル成分も生じ、この2fsとなる
二次のスペクトル成分を二次歪という。On the other hand, when the duty ratio of the recording signal is smaller than 50% as shown in FIG. 8B, or when the duty ratio is larger than 50% as shown in FIG.
The recording information based on such a recording signal is obtained by the measurement result of the spectrum analyzer shown in FIG. 9 (b). In this case, the recording frequency fs has an even order such as 2fs, 3fs, 4fs. Spectral components are also generated, and the secondary spectral component of 2 fs is called secondary distortion.
(発明が解決しようとする問題点) しかしながら、スペクトラムアナライザーを用いた従
来の二次歪検出方法にあっては、例えば二次歪が出ない
ように、即ち記録情報のデューティ比を50%に保つよう
に記録信号となるレーザーパワーを自動的にコントロー
ルすることが次の理由により困難であった。(Problems to be Solved by the Invention) However, in the conventional secondary distortion detection method using the spectrum analyzer, for example, the secondary distortion is not generated, that is, the duty ratio of the recording information is maintained at 50%. As described above, it is difficult to automatically control the laser power serving as a recording signal for the following reasons.
第1に、スペクトラムアナライザーの測定結果にあっ
ては、第8図(b)(c)に示したように、記録信号の
デューティ比が50%より小さくとも逆に大きくとも第9
図(b)に示したように二次歪を現わす二次のスペクト
ラム成分が現われ、極性を検出できない。従って、二次
歪を検出できても二次歪を生じないデューティ比50%に
対し記録信号のデューティ比がどちらにずれているかが
分らず、レザーパワーの増減についての判断ができなか
った。First, as shown in FIGS. 8 (b) and 8 (c), the measurement results of the spectrum analyzer indicate that the duty ratio of the recording signal is less than 50% or less than 50%.
As shown in FIG. 2B, a second-order spectrum component representing second-order distortion appears, and the polarity cannot be detected. Therefore, it is not clear which of the duty ratios of the recording signals is shifted with respect to the duty ratio of 50% which does not cause the secondary distortion even if the secondary distortion can be detected, and it is not possible to judge the increase or decrease of the laser power.
第2に、記録周波数が低い場合、即ち、記録ビットが
大きくなった場合、スペクトラムアナライザーによる二
次スペクトル成分の検出精度が落ちるという問題がある
ことから、記録周波数fsを高くする必要があった。Secondly, when the recording frequency is low, that is, when the number of recording bits is large, there is a problem that the detection accuracy of the secondary spectrum component by the spectrum analyzer is reduced. Therefore, it is necessary to increase the recording frequency fs.
しかし、記録周波数がある程度高くなると、読取光学
系のMTF周波数特性により二次スペクトル成分が検出で
きなくなる。即ち、MTFとは光学系が記録情報を検出す
る感度の周波数特性を示したもので、第10図に示す特性
となる。この第10図から明らかなように、記録周波数fs
を図示のようにある程度高くすると、二次スペクトル成
分を与える2fsにおいてはMTFが零となり、2fsの信号を
検出することができない。However, when the recording frequency is increased to some extent, secondary spectrum components cannot be detected due to the MTF frequency characteristics of the reading optical system. That is, the MTF indicates the frequency characteristic of the sensitivity at which the optical system detects recorded information, and has the characteristic shown in FIG. As is clear from FIG. 10, the recording frequency fs
Is somewhat higher as shown in the figure, the MTF becomes zero at 2 fs which gives a secondary spectrum component, and a 2 fs signal cannot be detected.
(問題点を解決するための手段) 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、光ディスク等の記録媒体の記録情報に含まれる
二次歪の有無を検出すると同時に極性即ち二次歪の原因
となった記録信号のデューティ比がデューティ比50%に
対しどちらの方向にずれているかも簡単に検出できるよ
うにした、記録信号の二次歪検出装置及び、二次歪の検
出により記録時にレーザパワーを適正に制御可能な光学
式記録装置を提供することを目的にする。(Means for Solving the Problems) The present invention has been made in view of such a conventional problem, and detects the presence or absence of secondary distortion included in information recorded on a recording medium such as an optical disk, and at the same time, detects polarity. That is, a recording signal secondary distortion detecting device and a secondary distortion detecting device that can easily detect in which direction the duty ratio of the recording signal causing the secondary distortion is deviated from the duty ratio of 50%. It is an object of the present invention to provide an optical recording apparatus capable of appropriately controlling the laser power at the time of recording by detection of the information.
この目的を達成するために、第1の発明は、2つの異
なった周波数により信号が記録された記録媒体より、該
信号をそれぞれ読取る読取手段と、前記読取手段の出力
のある基準レベルの上側の振幅と下側の振幅との差をそ
れぞれ検出する振幅差検出手段と、前記振幅差検出手段
の2つの出力の比較によって前記信号に含まれる二次歪
の有無及び極性を判定する判定手段とを備えた構成とし
た。In order to achieve this object, a first aspect of the present invention provides a reading unit for reading a signal from a recording medium on which the signal is recorded at two different frequencies, and a reading unit for reading the signal, the output being higher than a certain reference level. Amplitude difference detection means for detecting the difference between the amplitude and the lower amplitude, and determination means for determining the presence or absence and polarity of the secondary distortion included in the signal by comparing two outputs of the amplitude difference detection means. A configuration was provided.
前記振幅差検出手段は包絡線検波手段を含むことが好
ましい。Preferably, the amplitude difference detecting means includes an envelope detecting means.
また、前記振幅差検出手段は半波整流手段を含むこと
が好ましい。Preferably, the amplitude difference detecting means includes a half-wave rectifier.
また、前記振幅差検出手段は、前記読取手段の出力を
交流増幅した後で前記差を検出することが好ましい。Preferably, the amplitude difference detecting means detects the difference after AC-amplifying the output of the reading means.
第2の発明は、レーザビームを照射することにより、
記録媒体に所定の信号を書込み、また、書込まれた前記
所定の信号を読取って電気信号に変換する書込及び読取
手段と、前記書込及び読取手段からの出力に含まれる二
次歪の有無及び極性を判定する判定手段と、前記判定手
段により判定結果に基づいて、前記書込及び読取手段か
ら書き込み時に照射するレーザビームのパワーを制御す
るレーザパワー制御手段とを備えた構成とした。The second invention irradiates a laser beam,
Writing and reading means for writing a predetermined signal to a recording medium and reading the written predetermined signal and converting the read signal into an electric signal; and a second-order distortion included in an output from the writing and reading means. A determination means for determining presence / absence and polarity, and a laser power control means for controlling the power of a laser beam emitted from the writing and reading means at the time of writing based on the determination result by the determination means.
(作用) このような第1の発明の構成によれば、周波数の低い
情報再生信号と周波数の高い情報再生信号が記録情報の
光学的な読取で交互に得られ、読取光学系のMTF周波数
特性に依存して周波数の大小により低い周波数では再生
レベルが大きく、高い周波数では再生レベルが低くなる
再生信号を交互に生ずる。(Operation) According to the configuration of the first aspect, a low-frequency information reproduction signal and a high-frequency information reproduction signal are alternately obtained by optically reading recorded information, and the MTF frequency characteristic of the reading optical system is obtained. Depending on the frequency, the reproduction level is higher at a lower frequency and the reproduction level is lower at a higher frequency.
また、再生信号のデューティ比による変化を見ると、
同じ情報ビットの変動分、例えば周波数の大小に応じて
径の異なる情報ピットの同じ径の変化について、情報ピ
ットが大きい方(低い周波数)の再生信号のデューティ
比の変化は小さく、逆に情報ピットの小さい方(高い周
波数)の再生信号のデューティ比の変化は大きくなる。
そこで、デューティ比の変化が少ない周波数の低い情報
ビットから得られる再生信号を基準として、デューティ
比の変化が大きい周波数の高い情報ビットから得られた
再生信号の二次歪に起因した変動を検出する。Also, looking at the change due to the duty ratio of the playback signal,
With respect to the same information bit variation, for example, the same diameter change of information pits having different diameters according to the magnitude of the frequency, the change in the duty ratio of the reproduced signal of the larger information pit (lower frequency) is small, and conversely, The change in the duty ratio of the reproduction signal of the smaller (higher frequency) becomes larger.
Therefore, based on a reproduced signal obtained from a low-frequency information bit having a small change in duty ratio, a change due to secondary distortion of a reproduced signal obtained from a high-information bit having a large change in duty ratio is detected. .
更に、デューティ比50%からの変化に対し基準となる
低い周波数の情報再生信号のレベル変化はほとんどない
が、高い周波数の情報再生信号については、デューティ
比が小さくなると、直流成分が減少し、逆にデューティ
比が大きくなると直流成分が増加する。そのため低い周
波数の情報再生信号の振幅中心レベルを基準に見ると、
高い周波数の情報再生信号はデューティ比の減少で下側
にシフトし、デューティ比の増加で上側にシフトするレ
ベル変化を起こす。Further, although there is almost no change in the level of the low-frequency information reproduction signal serving as a reference with respect to the change from the duty ratio of 50%, the DC component of the high-frequency information reproduction signal decreases as the duty ratio decreases. As the duty ratio increases, the DC component increases. Therefore, looking at the amplitude center level of the low-frequency information reproduction signal,
The information reproduction signal of a high frequency shifts downward when the duty ratio decreases, and shifts upward when the duty ratio increases.
そこで第1の発明にあっては、再生信号が振幅中心レ
ベルに対しデューティ比に依存してシフトできるように
交流結合した後に振幅中心レベルの上側と下側に分けて
個別に包絡線検波する。Therefore, according to the first aspect, the reproduced signal is AC-coupled so as to be shifted from the amplitude center level depending on the duty ratio, and then the envelope detection is separately performed on the upper side and the lower side of the amplitude center level.
この包絡線検波による上側検波信号と下側検波信号との
間には、デューティ比が50%であれば振幅成分が等し
く、デューティ比が小さくなれば上側検波信号の振幅成
分が下側検波信号の振幅成分より大きくなり、更にデュ
ーティ比が大きくなると、逆に上側が下側に対し振幅成
分が小さくなる関係を生ずる。If the duty ratio is 50%, the amplitude component is equal between the upper detection signal and the lower detection signal by this envelope detection, and if the duty ratio is smaller, the amplitude component of the upper detection signal is lower than that of the lower detection signal. When the duty ratio becomes larger than the amplitude component and the duty ratio further increases, a relationship occurs that the amplitude component becomes smaller on the upper side than on the lower side.
そのため各包絡線検波出力を帯域フィルタを通すこと
で振幅成分を抽出して正弦波とした後に振幅ピーク値を
検出し、この検出ピーク値の大小比較から二次歪の有
無、二次歪を生じたときのデューティ比50%に対する大
小関係を判断するようにしたものである。Therefore, the amplitude component is extracted by passing each envelope detection output through a band-pass filter to make a sine wave, and then the amplitude peak value is detected. From the magnitude comparison of the detected peak values, the presence or absence of secondary distortion and secondary distortion are generated. In this case, the magnitude relation with respect to the duty ratio of 50% is determined.
また、第2の発明によれば、判定手段によって信号の
二次歪の有無及び極性を検出し、その結果によってレー
ザパワーの制御を適正に行うことができる。Further, according to the second aspect, the presence / absence and polarity of the secondary distortion of the signal are detected by the determination means, and the laser power can be appropriately controlled based on the result.
(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。(Embodiment) FIG. 1 is a block diagram showing an embodiment of the present invention.
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。First, the configuration will be described. Reference numeral 1 denotes a read head, which optically reads recorded information written on an optical disk 1a as a recording medium by a recording signal formed by irradiating a laser beam or the like, converts the information into an electrical signal, Is output.
ここで、記録情報の二次歪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ューティ比50%を予定
した同一の時間毎に交互に記録し、二次歪を検出する際
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
一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 information bits to be written on the optical disk 1a in order to detect the secondary distortion of the recorded information, information bits having two different frequencies are recorded alternately at the same time with a duty ratio of 50%. When the secondary distortion is detected, a portion in which the information bits having the two different frequencies are alternately recorded at the same time is reproduced.
二次歪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2図(a)に示
す周波数の低い記録信号と、第2図(b)に示す周波数
の高い記録信号を記録する。ここで第2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2図
(a)に示す周波数の低い信号のビット長は2Tに設定さ
れる。勿論、ビット長2T,Tを持つ各記録信号のデューテ
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ューテ
ィ比の変動を生ずる。ここで、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ΔT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
2Tとなる周波数の低い信号のデュ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2Tの記録信号の
デューティ比は信号歪が多少生じても略デューティ比50
%に維持され、後の説明で明らかにする二次歪の検出に
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。The information bits to be recorded on the optical disk 1a for detecting the secondary distortion will be specifically described. For example, a low-frequency recording signal shown in FIG. 2A and a high-frequency recording signal shown in FIG. Record the signal. Here, assuming that the bit length of the high frequency signal shown in FIG. 2 (b) is T, the bit length of the low frequency signal shown in FIG. 2 (a) is set to 2T. Of course, the duty ratio of each recording signal having a bit length of 2T, T is set to 50%, but the duty ratio fluctuates as shown by a broken line due to variations in the laser power serving as the recording signal. Here, 2 having a bit length of 2T, T
Assuming that the same bit length variation ΔT occurs in one recording signal, the bit length is longer than that of a signal having a high frequency of bit length T.
The duty ratio of a signal having a low frequency of 2T does not change much. Therefore, the duty ratio of a recording signal having a low frequency and a bit length of 2T is approximately 50% even if some signal distortion occurs.
%, And a detection signal of a low frequency and a bit length of 2T is used as a reference signal in the detection of the second-order distortion which will be described later.
再び、第1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. 1, the information reproduction signal read by the read head 1 for secondary distortion detection is input to the amplifier 2 with AC coupling by the capacitor C1, and after the AC amplification by the amplifier 2, Similarly, it is input to each of the envelope detection circuits 3a and 3b via the AC coupling capacitor C2.
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 on 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。Outputs of the envelope detection circuits 3a and 3b are respectively supplied to band-pass filters 4a and 4b, and the band-pass filters 4a and 4b respectively extract amplitude components of the envelope detection outputs and simultaneously convert the amplitude components into sine wave signals.
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。Outputs of the band-pass filters 4a and 4b are supplied to amplitude detection circuits 5a and 5b, and detect amplitude peak values in amplitude components of the envelope detection signals that have passed through the band-pass filters 4a and 4b, respectively.
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歪の度合いを判断す
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h1、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h1,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 applied to a judgment logic 6 as judgment means for judging the degree of secondary distortion included in the information reproduction signal based on the magnitude of the detected peak value. Assuming that the amplitude peak value detected by the amplitude detection circuit 5a is h1 and the amplitude detection value detected by the amplitude detection circuit 5b is h2, the determination logic 6 performs the following determination processing based on the amplitude peak values h1 and h2. .
(a)h1=h2のとき; 情報再生信号のデューティ比は50%で且つ二次歪を含
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 the secondary distortion.
(b)h1>h2のとき; 情報再生信号のデューティ比が50%より小さく、且つ
二次歪有りと判断する。(B) When h1>h2; It is determined that the duty ratio of the information reproduction signal is smaller than 50% and that the secondary distortion is present.
(c)h1<h2のとき; 情報再生信号はデューティ比が50%より大きく且つ二
次歪有りと判断する。(C) When h1 <h2: It is determined that the information reproduction signal has a duty ratio larger than 50% and that there is a second-order distortion.
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h1,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
得られらときには記録信号のデューティ比が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bが得られたときには、記録信号の
デューティ比が小さいことからレーザーパワーを高めて
記録信号のデューティ比を最適出力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
信号のデューティ比が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 selects one of the outputs a, b, c corresponding to the judgment conditions (a) to (c) based on the detected peak values h1, h2 from the amplitude detection circuits 5a, 5b. For example, when the laser power of the recording signal is controlled based on the output of the judgment logic 6, when the optimum output a is obtained, the duty ratio of the recording signal is 50%. The value at that time is maintained. On the other hand, when the judgment output b is obtained, since the duty ratio of the recording signal is small, the laser power is increased to control the duty ratio of the recording signal to 50% at which the optimum output a can be obtained. Conversely, when the judgment output c is obtained, since the duty ratio of the recording signal is larger than 50%, the laser power is reduced so that the optimum output a is obtained.
次に、第1図の実施例の作用を説明する。 Next, the operation of the embodiment of FIG. 1 will be described.
まず、光ディスク1aには第2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の記録信号(高い
周波数)を一定間隔で交互に記録しており、例えば第3
図(a)に示すように、ビット長2Tの記録信号に続いて
ビット長Tの信号を交互に記録していたものとする。First, a recording signal having a bit length of 2T (low frequency) and a recording signal having a bit length T (high frequency) shown in FIG. 2 are alternately recorded at regular intervals on the optical disk 1a.
As shown in FIG. 3A, it is assumed that a signal having a bit length T is recorded alternately after a recording signal having a bit length 2T.
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
T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。As described above, when information bits composed of two different frequencies recorded on the optical disk 1a are reproduced by the read head 1 to obtain an information reproduction signal, the detection sensitivity of the reading optical system shown in FIG. Bit length 2 depending on characteristics
The reproduced signal level differs between the reproduced signal of T and the reproduced signal of bit length T.
即ち、ビット長2T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2Tの記録ビットからの情報再生信号
は第4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4図の信
号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。That is, since the recording frequency of the bit length 2T is low, the value of the MTF is large as is clear from the MTF frequency characteristic in FIG.
As a result, the reproduction level of the information reproduction signal from the recording bit having the bit length of 2T is increased as shown by the signal 7 in FIG.
On the other hand, since the frequency of the recording signal having the bit length T is high, the value of the MTF in FIG. 10 is small, and as shown in the signal 8 in FIG. As described above, the reproduction level becomes low, and the reproduction signal having the bit length T becomes a substantially sine wave because a signal having a frequency component more than twice the fundamental frequency cannot be detected from 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
3図(a)の実線9に示すように、デューティ比50%で
記録された情報ビットの情報再生信号は、第3図(b)
に示す信号波形となる。このデューティ比50%のときの
信号波形はビット長2T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。Therefore, as shown by the solid line 9 in FIG. 3A due to the MTF frequency characteristic of the reading optical system, the information reproduction signal of the information bit recorded at the duty ratio of 50% is shown in FIG.
The signal waveform shown in FIG. The signal waveform at the duty ratio of 50% is a reproduced signal waveform that is vertically symmetrical with respect to the center level 12 for both the bit length 2T and the bit length T.
次に、第3図(a)に点線で示すデューティ比が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3図(c)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ューティ比変動分に
よる影響をほとんど受けないことから中心レベル12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
てはデューティ比が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.
The information reproduction signal from the information bit recorded with the smaller recording signal 10 is as shown in FIG. 3 (c). That is,
Since the reproduced signal of bit length 2T is hardly affected by the duty ratio fluctuation, it has a symmetrical waveform above and below the center level 12, but the reproduced signal of bit length T has a duty ratio smaller than 50%. As a result, the waveform becomes a waveform in which the DC component decreases, the amplitude component above the center level 12 decreases, and the amplitude component below the center level 12 increases.
更に、第3図(a)に一点鎖線で示すように、記録信
号のデューティ比が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3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
てはデュ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の再生信号はデューティ比の増加で直流成分が
増加し、中心レベル12の上側の振幅が増加し逆に中心レ
ベルの下側の振幅が減少するようになる。Further, as shown by a dashed line in FIG. 3A, the information reproduction signal of the information bit recorded by the recording signal 11 in which the duty ratio of the recording signal is larger than 50% is shown in FIG.
It becomes as shown in. That is, the reproduced signal having a bit length of 2T has almost no fluctuation due to the increase in the duty ratio, and thus has a substantially symmetrical waveform above and below the center level 12, but the reproduced signal having the bit length T has a DC component due to an increase in the duty ratio. Increases, the amplitude above the center level 12 increases, and conversely, the amplitude below the center level decreases.
実際には第1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5
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との間にはサ
グ13が生じている。このサグが生じている間に検出しな
ければならない。従って、ビット長2Tの信号とビット長
Tの信号を記録する周期τはあまり大きくすることはで
きない。尚、本実施例では、ビット長2Tの信号とTの信
号を記録する時間は、双方向同一時間(それぞれτ/2ず
つ)であるが、これは最終的な検出信号が大きくとれる
からである。よって、必ずしも同一時間である必要はな
い。Actually, as shown in FIG. 1, since the AC coupling is performed by the capacitors C1 and C2, when the magnitude of the DC component of the reproduction signal of the bit length 2T and the magnitude of the DC component of the reproduction signal of the bit length T are different, the fifth
As shown in the figure, the center level 12a of the reproduced signal having a bit length of 2T
A sag 13 is generated between the reproduced signal having the bit length T and the center level 12b. It must be detected while this sag is occurring. Therefore, the period τ for recording the signal having the bit length 2T and the signal having the bit length T cannot be made too large. In the present embodiment, the time for recording the signal having the bit length 2T and the time for recording the T signal are the same time in both directions (each τ / 2), because the final detection signal can be large. . Therefore, it is not always necessary to be the same time.
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3図
(c)に示すようにデューティ比が50%より小さいとき
の情報再生信号を例にとって具体的に説明する。As described above, for detecting the secondary distortion of the information reproduction signal reproduced through the reading optical system of the reading head 1, the information reproduction signal when the duty ratio is smaller than 50% as shown in FIG. This will be described in detail using an example.
読取ヘッド1で再生されたデューティ比が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3
aは第6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6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 read head 1 when the duty ratio is smaller than 50% is AC-amplified by the amplifier 2 and then supplied to the envelope detection circuits 3a and 3b.
a produces a detection output of the upper envelope shown in FIG.
On the other hand, the envelope detection circuit 3b generates a detection output of the lower envelope shown in FIG. 6 (b).
この第6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. 6, a portion having a large amplitude represents a reproduced signal having a bit length of 2T, and a portion having a small amplitude component represents a reproduced signal having 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、帯域通過フィルタ4a,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9図(a)に示す上側包絡線検波信号は、第7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6図(b)に示す下側包絡線検波
信号は、第7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 detected by the envelope detection circuits 3a and 3b are input to the band-pass filters 4a and 4b. Here, the center frequency fc of the bandpass filters 4a and 4b
Is set to fc = 1 / τ, and the upper envelope detection signal shown in FIG. 9A passing through the bandpass filter 4a extracts the amplitude component shown in FIG. 6B. On the other hand, the lower envelope detection signal shown in FIG. 6B is a signal whose amplitude component is extracted and converted into a sine wave signal as shown in FIG. 7B. .
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7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歪の有無の検出及びデューティ比の
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. 7A and 7B obtained by passing through the band-pass filters 4a and 4b are converted to an amplitude detection circuit 5a. , 5b, the amplitude peak values h1, h2 are detected, and the determination logic 6 detects the presence or absence of secondary distortion and determines the duty ratio based on the magnitude relationship between the detected peak values h1, h2.
Judge the deviation from 50%.
即ち、第7図の場合にはh1>h2であることから、二次
歪を生じており、且つデューティ比が50%より小さいと
する判断出力bを生ずることになる。That is, in the case of FIG. 7, since h1> h2, a judgment output b is generated indicating that secondary distortion has occurred and the duty ratio is smaller than 50%.
勿論、第3図(d)に示すように、デューティ比が50
%より大きいときには振幅検出回路5a,5bから得られる
検出ピーク値h1,h2は、h1<h2となることから、判断ロ
ジック6は二次歪の発生を判断すると同時にデューティ
比が50%より大きいとなる判断出力cを生ずる。更に、
デューティ比が50%のときにはh1,=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.
When the duty ratio is larger than 50%, the detection peak values h1 and h2 obtained from the amplitude detection circuits 5a and 5b satisfy h1 <h2. Produces a decision output c. Furthermore,
When the duty ratio is 50%, h1 = h2. In this case, the optimum output a is generated.
尚、上記の実施例にあっては、光ディスクに記録した
ビット長2Tとビット長Tの情報ビットの情報再生信号を
例にとるものであった、周波数の異なる2つの記録ビッ
ト情報の差を大きくする程、二次歪の検出精度もよくな
ることから、第10図に示したMTF周波性特性の範囲内で
周波数の異なる記録信号のビット長の差を大きくするこ
とが望ましい。In the above embodiment, the information reproduction signal of the information bit of the bit length 2T and the information bit of the bit length T recorded on the optical disk is taken as an example. Therefore, it is desirable to increase the difference between the bit lengths of recording signals having different frequencies within the range of the MTF frequency characteristic shown in FIG.
また、上記の実施例は二次歪の検出に基づいて記録信
号となるレーザーパワーのコントロールを例にとるもの
であったが、本発明はこれに限定されず、単なる二次歪
の検出及びデューティ比の測定に使用してもよく、若し
くは二次歪あるいはデューティ比の検出出力に基づく適
宜の自動制御を行なうようにしてもよい。In the above embodiment, the control of the laser power serving as the recording signal based on the detection of the second-order distortion is taken as an example. However, the present invention is not limited to this. It may be used for measuring the ratio, or appropriate automatic control may be performed based on the detection output of the secondary distortion or duty ratio.
上記実施例によれば、包絡線検波回路(3a,3b)の出
力を帯域通過フィルタ(4a,4b)を介した後、振幅検出
回路(5a,5b)で振幅を検出し、双方の振幅の差を判断
ロジック6で判断するものを示したが、本発明はこれに
限られず、例えば半波整流回路の出力をコンデンサで平
滑して直流レベルを比較判定するよう構成することがで
きる。According to the above embodiment, after the outputs of the envelope detection circuits (3a, 3b) pass through the band-pass filters (4a, 4b), the amplitudes are detected by the amplitude detection circuits (5a, 5b). Although the difference is determined by the determination logic 6, the present invention is not limited to this. For example, the output of the half-wave rectifier circuit may be smoothed by a capacitor and the DC level may be compared and determined.
第11図は第1図における包絡線検波回路を半波整流回
路20と平滑回路21で構成する例で、第12図は上記回路の
各部における信号波形を示す図である。12は信号の振幅
中心レベル、31は半波整流回路20の出力波形、32は平滑
回路21の出力波形である。FIG. 11 shows an example in which the envelope detection circuit in FIG. 1 is composed of a half-wave rectifier circuit 20 and a smoothing circuit 21, and FIG. 12 is a diagram showing signal waveforms at various parts of the circuit. Reference numeral 12 denotes a signal amplitude center level, reference numeral 31 denotes an output waveform of the half-wave rectifier circuit 20, and reference numeral 32 denotes an output waveform of the smoothing circuit 21.
要するに本発明は再生情報信号の周波数による振幅の
差を振幅中心レベルの上側と下側とでそれぞれに検出
し、その大小関係を判定するよう構成する。本発明は回
転する円盤状媒体のみならず、例えば直線移動するカー
ド状媒体にも適用することができ、媒体の形状に限定さ
れない。In short, the present invention is configured to detect the difference between the amplitudes of the reproduction information signal depending on the frequency above and below the amplitude center level, and to determine the magnitude relationship. The present invention can be applied to not only a rotating disk-shaped medium but also, for example, a card-shaped medium which moves linearly, and is not limited to the shape of the medium.
(発明の効果) 以上説明してきたように本発明によれば、光ディスク
等に対する記録信号のデューティ比が50%から変化した
ことによる情報再生信号の直流成分の変化に基づいて二
次歪を簡単に検出することができ、且つ二次歪の検出と
同時にデューティ比が二次歪を生じない50%であるか、
デューティ比50%より大きいか小さいかを判断できるた
め、例えば従来のスペクトルアナライザーによる二次歪
検出では困難であった記録時のレーザーパワーの補正も
可能とすることができる。(Effects of the Invention) As described above, according to the present invention, the secondary distortion can be easily reduced based on the change in the DC component of the information reproduction signal due to the change in the duty ratio of the recording signal for the optical disk or the like from 50%. Whether the duty ratio can be detected and the secondary distortion is detected and the duty ratio is 50% at which no secondary distortion occurs,
Since it is possible to determine whether the duty ratio is larger or smaller than 50%, it is possible to correct the laser power at the time of recording, which has been difficult with, for example, the detection of secondary distortion by a conventional spectrum analyzer.
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3図は記録信号のデューティ比を50%、50
%より小、50%より大としたときの情報再生信号を示し
た信号波形図、第4図は読取光学系統の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5
図は直流成分の相違により生ずる再生信号のザグを示し
た信号波形図、第6図は第1図の包絡線検波信号の波形
説明図、第7図は第1図の帯域フィルタの出力を示した
信号波形図、第8図は記録信号のデューティ比の変化を
示した信号波形図、第9図は従来のスペクトルアナライ
ザーにより得られる基本周波数に対するスペクトル成分
を示したスペクトル分布図、第10図は読取光学系統のMT
F周波数特性を示したグラフ図、第11図は他の実施例を
示した回路ブロック図、第12図はその信号波形図であ
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(判断手段)FIG. 1 is a block diagram showing an embodiment of the present invention, FIG. 2 is an explanatory diagram of recording signals having two different frequencies to be subjected to secondary distortion detection, and FIG. , 50
FIG. 4 is a signal waveform diagram showing the information reproduction signal when it is smaller than 50% and larger than 50%. FIG. 4 is a signal waveform diagram showing a change in the level of the reproduction signal due to the MTF frequency characteristic of the reading optical system.
FIG. 6 is a signal waveform diagram showing a zag of a reproduced signal caused by a difference in a DC component. FIG. 6 is an explanatory diagram of a waveform of the envelope detection signal of FIG. 1, and FIG. 7 is an output of the bandpass filter of FIG. FIG. 8 is a signal waveform diagram showing a change in the duty ratio of a recording signal, FIG. 9 is a spectrum distribution diagram showing a spectrum component with respect to a fundamental frequency obtained by a conventional spectrum analyzer, and FIG. MT of reading optical system
FIG. 11 is a graph showing F frequency characteristics, FIG. 11 is a circuit block diagram showing another embodiment, and FIG. 12 is a signal waveform diagram thereof. 1: Read head 1a: Optical disk 2: Amplifier 3a, 3b: Envelope detection circuit 4a, 4b: Bandpass filter 5a, 5b: Amplitude detection circuit 6: Judgment logic (judgment means)
Claims (5)
れた記録媒体より、該信号をそれぞれ読取る読取手段
と; 前記読取手段の出力のある基準レベルの上側の振幅と下
側の振幅との差をそれぞれ検出する振幅差検出手段と; 前記振幅差検出手段の2つの出力の比較によって前記信
号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; を備えたことを特徴とする記録信号の二次歪検出装置。1. Reading means for reading a signal from a recording medium on which a signal is recorded at two different frequencies, and a difference between an upper amplitude and a lower amplitude of a reference level of an output of the reading means. And a determination means for determining the presence or absence and the polarity of the secondary distortion included in the signal by comparing two outputs of the amplitude difference detection means. Signal second-order distortion detector.
むことを特徴とする特許請求の範囲第1項記載の記録信
号の二次歪検出装置。2. The apparatus according to claim 1, wherein said amplitude difference detecting means includes an envelope detecting means.
ことを特徴とする特許請求の範囲第1項記載の記録信号
の二次歪検出装置。3. The apparatus according to claim 1, wherein said amplitude difference detection means includes a half-wave rectification means.
力を交流増幅した後で前記差を検出することを特徴とす
る特許請求の範囲第1項記載の記録信号の二次歪検出装
置。4. An apparatus according to claim 1, wherein said amplitude difference detecting means detects the difference after AC-amplifying an output of said reading means. .
媒体に所定の信号を書込み、また、書込まれた前記所定
の信号を読取って電気信号に変換する書込及び読取手段
と; 前記書込及び読取手段からの出力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; 前記判定手段による判定結果に基づいて、前記書込及び
読取手段から書き込み時に照射するレーザビームのパワ
ーを制御するレーザパワー制御手段と; を備えたことを特徴とする光学式記録装置。5. A writing and reading means for writing a predetermined signal on a recording medium by irradiating a laser beam, reading the written predetermined signal and converting it into an electric signal; Determining means for determining the presence or absence and polarity of the secondary distortion included in the output from the reading means; and controlling the power of the laser beam emitted at the time of writing from the writing and reading means based on the determination result by the determining means. And a laser power control means.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62007734A JP2600659B2 (en) | 1987-01-16 | 1987-01-16 | Apparatus for detecting secondary distortion of recording signal and optical recording apparatus |
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 |
---|---|---|---|
JP62007734A JP2600659B2 (en) | 1987-01-16 | 1987-01-16 | Apparatus for detecting secondary distortion of recording signal and optical recording apparatus |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS63177318A JPS63177318A (en) | 1988-07-21 |
JP2600659B2 true JP2600659B2 (en) | 1997-04-16 |
Family
ID=11673933
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62007734A Expired - Lifetime JP2600659B2 (en) | 1987-01-16 | 1987-01-16 | Apparatus for detecting secondary distortion of recording signal and optical recording apparatus |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2600659B2 (en) |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2724996B2 (en) * | 1983-12-20 | 1998-03-09 | パイオニア株式会社 | Relative position detection device |
JPS6116070A (en) * | 1984-07-02 | 1986-01-24 | Nippon Telegr & Teleph Corp <Ntt> | Detector for optical information |
-
1987
- 1987-01-16 JP JP62007734A patent/JP2600659B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPS63177318A (en) | 1988-07-21 |
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