JPS6318263B2 - - Google Patents

Info

Publication number
JPS6318263B2
JPS6318263B2 JP11919180A JP11919180A JPS6318263B2 JP S6318263 B2 JPS6318263 B2 JP S6318263B2 JP 11919180 A JP11919180 A JP 11919180A JP 11919180 A JP11919180 A JP 11919180A JP S6318263 B2 JPS6318263 B2 JP S6318263B2
Authority
JP
Japan
Prior art keywords
pulse width
recording
pulse
digital signal
mfm
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
Application number
JP11919180A
Other languages
Japanese (ja)
Other versions
JPS5744233A (en
Inventor
Masatoshi Shinho
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP11919180A priority Critical patent/JPS5744233A/en
Publication of JPS5744233A publication Critical patent/JPS5744233A/en
Publication of JPS6318263B2 publication Critical patent/JPS6318263B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B20/00Signal processing not specific to the method of recording or reproducing; Circuits therefor
    • G11B20/10Digital recording or reproducing
    • G11B20/14Digital recording or reproducing using self-clocking codes
    • G11B20/1403Digital recording or reproducing using self-clocking codes characterised by the use of two levels
    • G11B20/1423Code representation depending on subsequent bits, e.g. delay modulation, double density code, Miller code

Landscapes

  • Engineering & Computer Science (AREA)
  • Signal Processing (AREA)
  • Signal Processing For Digital Recording And Reproducing (AREA)
  • Optical Recording Or Reproduction (AREA)

Description

【発明の詳細な説明】 本発明はアナログ信号をデイジタル化し、この
デイジタル信号を記録再生するMFM(Modified
Frequency Modulation)変調方式のデイジタル
信号記録再生装置に関し、波形ひずみによる信号
劣化を防止することができるデイジタル信号記録
再生装置を提供するものである。
[Detailed Description of the Invention] The present invention provides an MFM (Modified
The present invention relates to a digital signal recording and reproducing apparatus using a frequency modulation method, and provides a digital signal recording and reproducing apparatus that can prevent signal deterioration due to waveform distortion.

アナログ信号をデイジタル化し記録する方式は
その記録媒体の種類、あるいは手段等により数多
く提案されている。
Many methods for digitizing and recording analog signals have been proposed depending on the type of recording medium or means used.

アナログ信号をデイジタル化し記録再生する方
式の最大の特長のひとつは、記録再生る過程での
信号劣化のないことである。しかし、何の手段を
施さず、単に記録する場合、実際には記録媒体や
手段の不完全さから、信号の劣化が頻繁に発生す
る。この信号の劣化としては多くの要因がある
が、例えば、記録媒体の不均一性、傷、ゴミ等に
よる信号欠落、必要周波数帯域内での雑音、記録
媒体、手段に関連する周波数帯域の制限、位相特
性の非直線性による波形ひずみ、レーザビーム記
録しきい値、盤面入射ピークパワー、焦点ぼけ
量、波長とピツト径の制御不完全による波形ひず
み等がある。これら要因に対しては、それぞれの
対策が必要であり、一般的には、これら対策が施
されてはじめて、デイジタル記録の利点が生かさ
れるのである。
One of the greatest features of the method of recording and reproducing digital signals from analog signals is that there is no signal deterioration during the recording and reproducing process. However, when simply recording without applying any means, signal deterioration often occurs due to imperfections in the recording medium and means. There are many factors that cause this signal deterioration, such as non-uniformity of the recording medium, signal loss due to scratches, dust, etc., noise within the required frequency band, frequency band limitations related to the recording medium and means, There are waveform distortions due to nonlinearity of phase characteristics, laser beam recording threshold, peak power incident on the disc surface, amount of defocus, and waveform distortions due to incomplete control of wavelength and pit diameter. Each of these factors requires countermeasures, and in general, the advantages of digital recording can only be utilized if these countermeasures are taken.

本発明は先の要因中の最後者に関連する波形ひ
ずみを防ぐことができるデイジタル信号記録再生
装置を提供するものであり、あらかじめ記録時に
特定符号パターンを検出し、記録再生した時に理
想的な所望の再生波形が得られる様に補正するも
のであり、各種のデイジタル変調方式の中の
MFM(Modified Frequency Modulation)方式
に適用されるものである。以下、図とともに詳細
に説明する。
The present invention provides a digital signal recording and reproducing device that can prevent waveform distortion related to the last of the above factors, and detects a specific code pattern in advance during recording, and detects the ideal desired code pattern when recording and reproducing. It corrects so that a reproduced waveform of
This is applied to the MFM (Modified Frequency Modulation) method. A detailed explanation will be given below with reference to the drawings.

第1図はMFMの変調回路例で、第2図はその
タイミングチヤートである。第1図において、1
はNRZ表現された変調回路入力で、2,3はク
ロツク、4,5は遅延型フリツプフロツプ(D―
FF)、6,7はNANDゲート、8,9はORゲー
ト、10はMFM変調出力である。第2図の
MFMデータからも明らかな様にMFMは入力の
NRZデータのいかなる符号パターンの組合せに
対しても、NRZの“1”あるいは“0”の周期
をTとすると、そのパルス幅が2T、1.5T、T以
外はとり得ない特徴を有するものである。
Figure 1 is an example of an MFM modulation circuit, and Figure 2 is its timing chart. In Figure 1, 1
is the modulation circuit input expressed in NRZ, 2 and 3 are clocks, and 4 and 5 are delay type flip-flops (D-
FF), 6 and 7 are NAND gates, 8 and 9 are OR gates, and 10 is an MFM modulation output. Figure 2
As is clear from the MFM data, MFM is
For any combination of code patterns of NRZ data, if the cycle of NRZ "1" or "0" is T, the pulse width has a characteristic that it cannot be anything other than 2T, 1.5T, or T. .

第3図a〜hは本発明の基本原理を示す図であ
り、先のMFMデータをレーザビームを使つて記
録媒体に記録再生した場合を示す。31は記録す
べきMFMデータ、32は記録用のレーザビーム
径、33はレーザビームの記録しきい値以上のエ
ネルギー部、3は記録しきい値以上のレーザエネ
ルギーによつて実際に記録媒体に記録されたピツ
ト、t1はしきい値エネルギーと記録ピツトとの時
間ずれ、35は記録されたピツトを読み出すため
の再生レーザビーム径、36は実際に読み出され
たピツト再生波形、37はパルサ(コンパレー
タ)のしきい値、38はピツト再生波形のパルス
整形出力であり、このパルス整形出力は、先の記
録すべきMFMデータに比較してパルス幅が広く
なつている。MFM方式は、その性質上、T、
1.5T、2Tの3種類のパルス幅しかとり得ないの
で、それぞれの識別余裕は±0.5Tであり、これ
を越えると、Tが1.5Tと判定されたり、2Tが
1.5Tと判定されたりして信号劣化の原因となる。
したがつて、先の38の拡大されたパルスは極力
規定されたパルス幅となる様に補正する必要があ
る。そこで、ひとつの方法として39の如く記録
時にあらかじめ“1”あるいは“ON”のパルス
幅を細めに縮小補正して記録すれば、再生時には
40の如く理想的なパルス波形が得られることは
容易に理解される。しかし、39の如く、パルス
幅を縮小するとレーザビームの記録エネルギーが
低下するのでピツト径がさらに縮小する結果とな
り好ましくないので、あらかじめ、記録時にパル
ス幅を縮小しても記録エネルギーが低下しない
様、41の如くパルス幅ごとにパルス振幅を変化
させるものである。
FIGS. 3a to 3h are diagrams showing the basic principle of the present invention, and show the case where the previous MFM data is recorded and reproduced on a recording medium using a laser beam. 31 is the MFM data to be recorded, 32 is the laser beam diameter for recording, 33 is the energy part of the laser beam that is above the recording threshold, and 3 is the actual recording on the recording medium by the laser energy that is above the recording threshold. t1 is the time difference between the threshold energy and the recorded pit, 35 is the reproduction laser beam diameter for reading out the recorded pit, 36 is the actually read pit reproduction waveform, and 37 is the pulser ( The threshold value 38 of the comparator is the pulse-shaped output of the pit reproduction waveform, and this pulse-shaped output has a wider pulse width than the previous MFM data to be recorded. Due to its nature, the MFM method has T,
Since only three types of pulse widths, 1.5T and 2T, are possible, the discrimination margin for each is ±0.5T, and if this is exceeded, T will be determined to be 1.5T, or 2T will be determined.
It may be determined to be 1.5T, causing signal deterioration.
Therefore, it is necessary to correct the above 38 expanded pulses so that they have a prescribed pulse width as much as possible. Therefore, one method is to reduce and correct the pulse width of "1" or "ON" in advance during recording as shown in 39, and then it is easy to obtain an ideal pulse waveform as shown in 40 during playback. be understood. However, as shown in No. 39, reducing the pulse width will reduce the recording energy of the laser beam, resulting in a further reduction in the pit diameter, which is undesirable. 41, the pulse amplitude is changed for each pulse width.

第4図は光スポツトと記録ピツトとの関係図で
ある。スポツト直径2WOのレーザビームが記録媒
体に当たると、記録しきい値パワーPthを超えた
部分が溶解し、幅2WPのピツトができる。
FIG. 4 is a diagram showing the relationship between the light spot and the recording pit. When a laser beam with a spot diameter of 2W O hits a recording medium, the portion exceeding the recording threshold power Pth is melted, forming a pit with a width of 2W P.

2WPはPth、盤面入射ピークパワーP、焦点ぼ
け量Z、波長入により次式で与えられる。
2W P is given by the following equation using Pth, the peak power P incident on the disc surface, the amount of defocus Z, and the wavelength input.

W2 P=WO 2/2{1+(λ/π z/WO 22}ln {P/Pth/1+(λ/π z/WO 22} ピツト径WPは入射パワーとしきい値の比P/
Pthによつて変化することがわかる。デイスク表
面に焦点が合つているときは(Z=0) WP=WO/2lnP/Pth P/Pthが3となる強度のレーザ光を当てると
光スポツト径の約0.7倍の幅ピツトを得ることが
できる。すなわち、条件を選べば光スポツト径よ
り小さいピツトが記録可能である。
W 2 P = W O 2 /2 {1+(λ/π z/W O 2 ) 2 }ln {P/Pth/1+(λ/π z/W O 2 ) 2 } The pit diameter W P is the incident power. Threshold ratio P/
It can be seen that it changes depending on Pth. When the focus is on the disk surface (Z = 0) W P = W O /2lnP/Pth If you apply a laser beam with an intensity that makes P/Pth 3, you will get a pit with a width approximately 0.7 times the diameter of the beam spot. be able to. That is, if conditions are selected, it is possible to record pits smaller than the optical spot diameter.

第5図はWOをパラメータにしてP/Pthによる
WPの変化を求めたものであるが、グラフの傾き
が大きいところではP/Pthに対する依存度が大
となるため安定な記録が困難となる。また、第6
図はパルス入力とそれに対応した記録ピツトをモ
デル化したものであり、時間遅れt1を無視したも
のである。
Figure 5 shows P/Pth using W O as a parameter.
W P changes are determined, but where the slope of the graph is large, the dependence on P/Pth becomes large, making stable recording difficult. Also, the 6th
The figure is a model of the pulse input and the corresponding recording pit, ignoring the time delay t1 .

第7図は本発明の一実施例のブロツクを示して
いる。71は第1図に示されるMFM変調回路、
72はパルスの立ち上がりエツジで動作する単安
定マルチバイブレータ、74はパルスの立ち下が
りエツジで動作する単安定マルチバイブレータ、
75,76はD―FF、77は4ビツトバイナリ
カウンタ、78,79はD―FF、80は4ビツ
トのデイジタルマグニチユードコンパレータであ
り、このデイジタルマグニチユードコンパレータ
80はA0〜A3端子入力とプリセツト用B0〜B3
子のそれぞれの符号が全て一致したときのみA=
B端子より一致パルスが出力されるものである。
81〜83,92はANDゲート、84はインバ
ータ、93はORゲート、85はエクスクルーシ
ヴORゲート、86,87はペリフエラルANDド
ライバである。88〜90はそれぞれパルス幅
T、1.5T、2Tの検出回路であり、89,90は
88と基本的に同じ構成であるがデイジタルマグ
ニチユードコンパレータのプリセツト値が異なる
ものである。
FIG. 7 shows a block diagram of one embodiment of the present invention. 71 is the MFM modulation circuit shown in FIG.
72 is a monostable multivibrator that operates on the rising edge of the pulse; 74 is a monostable multivibrator that operates on the falling edge of the pulse;
75 and 76 are D-FF, 77 is a 4-bit binary counter, 78 and 79 are D-FF, and 80 is a 4-bit digital magnitude comparator, and this digital magnitude comparator 80 has terminals A0 to A3 . A = only when the input and preset B 0 to B 3 terminals have the same sign.
A matching pulse is output from the B terminal.
81 to 83 and 92 are AND gates, 84 is an inverter, 93 is an OR gate, 85 is an exclusive OR gate, and 86 and 87 are peripheral AND drivers. 88 to 90 are detection circuits for pulse widths T, 1.5T, and 2T, respectively, and 89 and 90 have basically the same configuration as 88, but have different preset values of the digital magnitude comparators.

第8図、第9図は第7図の回路のタイミングチ
ヤートである。1はNRZデータ、2はMFM変調
出力、17はパルス幅T検出出力、21はパルス
幅検出出力のうち“H”レベルのもの検出出力2
5はパルス幅Tのパルス幅補正後出力、26はパ
ルス幅Tのパルス幅及び振幅補正後出力、27は
パルス幅T、1.5T、2Tのそれぞれのパルス幅及
び振幅補正後の加算出力で、レーザ駆動回路入力
である。
8 and 9 are timing charts of the circuit shown in FIG. 7. 1 is NRZ data, 2 is MFM modulation output, 17 is pulse width T detection output, 21 is "H" level detection output 2 among pulse width detection outputs
5 is the output after pulse width correction of pulse width T, 26 is the output after pulse width and amplitude correction of pulse width T, 27 is the addition output after pulse width and amplitude correction of pulse width T, 1.5T, and 2T, This is the laser drive circuit input.

以上の如く、本発明によれば、アナログ信号を
デイジタル化し記録再生する場合のMFM変調出
力のそれぞれのパルス幅を記録時にあらかじめ検
出し縮小するとともにそれぞれのパルス幅に適応
してパルス振幅を変化させることにより、再生時
の理想的な所望のパルス幅を得ることができる利
点を有するものである。
As described above, according to the present invention, when an analog signal is digitized and recorded and reproduced, each pulse width of the MFM modulation output is detected and reduced in advance during recording, and the pulse amplitude is changed in accordance with each pulse width. This has the advantage that an ideal desired pulse width can be obtained during reproduction.

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

第1図はMFM変調回路のブロツク図、第2図
は同MFM変調回路のタイミングチヤート、第3
図a〜hは本発明の基本原理を示す図、第4図は
光スポツトと記録ピツトの関係を示す図、第5図
はレーザ入射パワーとピツト幅の関係を示す図、
第6図はパルス入力と記録ピツトモデル説明図、
第7図は本発明の一実施例におけるデイジタル信
号記録再生装置のブロツク図、第8図、第9図は
同装置のタイミングチヤートである。 4,5…遅延型フリツプフロツプ(D―FF)、
6,7…NANDゲート、8,9…ORゲート、7
1…MFM変調回路、72…単安定マルチバイブ
レータ、73,74…単安定マルチバイブレー
タ、75,76…D―FF、77…4ビツトバイ
ナリカウンタ、78,79…D―FF、80…デ
イジタルマグニチユードコンパレータ、81〜8
3…ANDゲート、84…インバータ、85…エ
クスクルーシブORゲート、86,87…ペリフ
エラルANDドライバ、88〜90…パルス幅検
出回路。
Figure 1 is a block diagram of the MFM modulation circuit, Figure 2 is a timing chart of the MFM modulation circuit, and Figure 3 is a block diagram of the MFM modulation circuit.
Figures a to h are diagrams showing the basic principle of the present invention, Figure 4 is a diagram showing the relationship between the optical spot and recording pit, and Figure 5 is a diagram showing the relationship between laser incident power and pit width.
Figure 6 is an explanatory diagram of pulse input and recording pit model.
FIG. 7 is a block diagram of a digital signal recording/reproducing device according to an embodiment of the present invention, and FIGS. 8 and 9 are timing charts of the same device. 4, 5...delayed flip-flop (D-FF),
6, 7...NAND gate, 8, 9...OR gate, 7
1... MFM modulation circuit, 72... Monostable multivibrator, 73, 74... Monostable multivibrator, 75, 76... D-FF, 77... 4-bit binary counter, 78, 79... D-FF, 80... Digital magnici Youdo comparator, 81-8
3...AND gate, 84...Inverter, 85...Exclusive OR gate, 86, 87...Peripheral AND driver, 88-90...Pulse width detection circuit.

Claims (1)

【特許請求の範囲】 1 アナログ信号をデイジタル化し記録再生する
MFM変動方式のデイジタル信号記録再生装置に
おいて、記録時に変調前のデータの周期をTとし
たときのMFM変調出力のパルス幅T、1.5T、
2Tをそれぞれ個別に検出し、かつ該パルス幅を
持つパルスのうち“H”レベルのパルスのみを抽
出し、該それぞれのパルスの幅をあらかじめ定め
られた所定のパルス幅だけ縮小するとともにそれ
ぞれの振幅を縮小するパルス幅分に相当するだけ
増幅したのち加算することを特徴とするデイジタ
ル信号記録再生装置。 2 特許請求の範囲第1項記載のデイジタル信号
記録再生装置において、記録されたパルスを再生
したとき、そのパルス幅がそれぞれあらかじめ定
められたT、1.5T、2Tのパルス幅となる様にそ
れぞれのパルス幅及び振幅を補正することを特徴
とするデイジタル信号記録再生装置。
[Claims] 1. Digitizing and recording/reproducing analog signals
In a digital signal recording and reproducing device using the MFM variation method, the pulse width T of the MFM modulation output is 1.5T, where T is the period of data before modulation during recording.
2T individually, extract only the "H" level pulses from among the pulses with the corresponding pulse width, reduce the width of each pulse by a predetermined pulse width, and reduce the amplitude of each pulse. A digital signal recording/reproducing device characterized in that the digital signal is amplified by an amount corresponding to the pulse width to be reduced and then added. 2. In the digital signal recording and reproducing device according to claim 1, each pulse width is adjusted so that when the recorded pulse is reproduced, the pulse width becomes the predetermined pulse width of T, 1.5T, and 2T, respectively. A digital signal recording and reproducing device characterized by correcting pulse width and amplitude.
JP11919180A 1980-08-28 1980-08-28 Recorder and reproducer of digital signal Granted JPS5744233A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11919180A JPS5744233A (en) 1980-08-28 1980-08-28 Recorder and reproducer of digital signal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11919180A JPS5744233A (en) 1980-08-28 1980-08-28 Recorder and reproducer of digital signal

Publications (2)

Publication Number Publication Date
JPS5744233A JPS5744233A (en) 1982-03-12
JPS6318263B2 true JPS6318263B2 (en) 1988-04-18

Family

ID=14755163

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11919180A Granted JPS5744233A (en) 1980-08-28 1980-08-28 Recorder and reproducer of digital signal

Country Status (1)

Country Link
JP (1) JPS5744233A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20230140811A (en) * 2022-03-30 2023-10-10 아우토리브 디벨롭먼트 아베 Seat belt apparatus

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58212628A (en) * 1982-06-04 1983-12-10 Sony Corp Disc recording device
US4526429A (en) * 1983-07-26 1985-07-02 Augat Inc. Compliant pin for solderless termination to a printed wiring board
IT1206332B (en) * 1983-10-25 1989-04-14 Honeywell Inf Systems DIGITAL APPARATUS FOR RECOVERY SYSTEM OF BINARY INFORMATION RECORDED ON MAGNETIC MEDIA.
JPS6185156U (en) * 1984-11-09 1986-06-04
JPS6325867A (en) * 1986-07-18 1988-02-03 Canon Inc Information recording method
JP2603632B2 (en) * 1987-05-13 1997-04-23 シャープ株式会社 Optical information recording / reproducing device
JP2543362B2 (en) * 1987-04-28 1996-10-16 ヤマハ株式会社 Optical disk recorder
JP2617512B2 (en) * 1988-03-30 1997-06-04 アイワ株式会社 Optical disc playback device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20230140811A (en) * 2022-03-30 2023-10-10 아우토리브 디벨롭먼트 아베 Seat belt apparatus

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Publication number Publication date
JPS5744233A (en) 1982-03-12

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