JPS58220211A - Digital modulating method - Google Patents

Digital modulating method

Info

Publication number
JPS58220211A
JPS58220211A JP10425482A JP10425482A JPS58220211A JP S58220211 A JPS58220211 A JP S58220211A JP 10425482 A JP10425482 A JP 10425482A JP 10425482 A JP10425482 A JP 10425482A JP S58220211 A JPS58220211 A JP S58220211A
Authority
JP
Japan
Prior art keywords
bit
bits
codeword
modulation method
digital modulation
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP10425482A
Other languages
Japanese (ja)
Inventor
Masatoshi Shinpo
正利 新保
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 JP10425482A priority Critical patent/JPS58220211A/en
Publication of JPS58220211A publication Critical patent/JPS58220211A/en
Pending 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
    • G11B20/1426Code representation depending on subsequent bits, e.g. delay modulation, double density code, Miller code conversion to or from block codes or representations thereof

Landscapes

  • Engineering & Computer Science (AREA)
  • Signal Processing (AREA)
  • Signal Processing For Digital Recording And Reproducing (AREA)
  • Dc Digital Transmission (AREA)

Abstract

PURPOSE:To realize self-clocking, by dividing data bits to every 4 bits to convert these bits into code words of 9 bits to 16 combinations of data bits and then applying NRZI modulation to the series of code words. CONSTITUTION:The data bits are divided to every 4 bits and then converted into code words P1-P9 of 9 bits to 16 combinations of these bits. Then NRZI modulation is applied to the code word series, and at least >=2 bits 0 are included between the bit 1 and 1 of the code word series. At the same time, the number of bits 0 is reduced down to <=9 at most. Thus the minimum magnetization inverting interval is set as Tmin=1.33T compared with the conventional interval T along with the maximum magnetization inverting interval Tmax=4.44 and a product of 0.59T<2> of Tmin and the detecting window width. This process increases the linear bit density and realizes the self-clocking.

Description

【発明の詳細な説明】 本発明はディジタル変調方法、特にデータビット4ビツ
ト符号語9ビットに変換する4−9変換方法にもとづく
ディジタル変調方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a digital modulation method, and more particularly to a digital modulation method based on a 4-9 conversion method for converting 4 data bits into 9 bit code words.

一般にディジタル磁気記録は、多量の情報を経済的に記
録でき、それを長期的にかつ安定に保存できるなどの特
徴をもっている。そのための情報値go変調方式として
はRZ (Return to Zero)。
In general, digital magnetic recording has the characteristics of being able to economically record a large amount of information and to store it stably for a long period of time. The information value go modulation method for this purpose is RZ (Return to Zero).

RB (Raturn to Bias)、NRZ(N
on Return t。
RB (Rturn to Bias), NRZ (N
On Return.

Zero) 、 N RZ I (Non−Retur
n to Zero I) 。
Zero), N RZ I (Non-Retur)
n to Zero I).

F M (Frequency Modulation
)、 P R(phaseICncoding)、 M
FM(Modified FrequencyModu
lation)、M2FM (Modified MF
M)など各種提案されている。一方、最近ではこれら以
外の新しい変調方式も各種提案されている。例えば41
5MNRZI (Modified Non−Retu
rn to Zer。
F M (Frequency Modulation
), P R (phaseICncoding), M
FM (Modified Frequency Mod
ration), M2FM (Modified MF
Various proposals have been made, including M). On the other hand, recently, various new modulation methods other than these have been proposed. For example 41
5MNRZI (Modified Non-Retu
rn to Zer.

I)、 3PM(3Position Modulat
ion) 、 Z M(Zero Modulatio
n)などである。さらに最近では高密度化が進み上記以
外の新しい変調方式も考えられているが、ディジタル磁
気記録においては検出窓幅TW、最小磁化反転間隔Tw
in、あるいは線ビット密度の最高磁化反転密度に対す
る比DR(Devsity Ratio)の大きな変調
方式が望ましいとされている。又、高密度化の容易さを
最小磁化反転間隔Twinと検出窓幅Twとの積で表わ
すことが多い。
I), 3PM (3Position Modulat)
ion), Z M (Zero Modulation)
n) etc. Furthermore, recently, with increasing density, new modulation methods other than those mentioned above are being considered, but in digital magnetic recording, detection window width TW, minimum magnetization reversal interval Tw
It is said that a modulation method with a large ratio DR (Devsity Ratio) of in or linear bit density to the maximum magnetization reversal density is desirable. Furthermore, the ease of increasing the density is often expressed as the product of the minimum magnetization reversal interval Twin and the detection window width Tw.

本発明はこのような要望に鑑みなされたものであり、最
小磁化反転間隔Tm1nが12/9T(=1.33T)
とMFMのTより大きく、磁化反転間隔Tm1nと検出
窓幅’rwとの積も4B/81 T”(Q59T2)と
MFMの0.5 T2  より大きい変調方式を提供す
るものである。
The present invention was made in view of these demands, and the minimum magnetization reversal interval Tm1n is 12/9T (=1.33T).
This provides a modulation method in which the product of magnetization reversal interval Tm1n and detection window width 'rw is 4B/81 T'' (Q59T2), which is larger than 0.5 T2 of MFM.

以下、本発明について実施例の図面と共に詳細に説明す
る。
Hereinafter, the present invention will be described in detail with reference to drawings of embodiments.

MF、M方式はビット“1”を反転ありに対応させ、ビ
ット“0″を反転なしに対応させる。さらにFMと同じ
ようにビットとビットの境界でも反6ベー二゛ 転させるが、ただし、ビット“0”とピッド0″の境界
だけで反転させる。この変調方式は最小磁化反転間隔T
winがTとFMのo、s Tより大きく、検出窓幅T
wも0,5TとFM並みで、しかも、セルフクロッキン
グが容易であるなどの特徴をもっている。
In the MF and M methods, bit "1" corresponds to inversion, and bit "0" corresponds to no inversion. Furthermore, like FM, the inverse 6-v inversion is performed at the boundaries between bits, but only at the boundaries between bit "0" and pit 0". This modulation method uses the minimum magnetization reversal interval T
win is larger than T and FM o,s T, detection window width T
The w is also 0.5T, which is comparable to FM, and it also has features such as easy self-clocking.

これに対し、第1図は本発明の4−9変換FNM(Fo
ur to N1ne Modulation)の変換
テーブルである。本方式u4ビットのデータを9ビツト
の符号語に変換して、その符号語の系列をNRZIで変
調するものである。符号語は、第2図aに示すようにビ
ット“1″と次のビット“1″との間に少なくとも2つ
以上のビット“O”が入り、多くとも9ケ以下となるよ
うに制限が加えられているのが特徴であるが、時系列的
に古い符号語の8ビツト目P8が“1゛′で、さら欲こ
れに続く符号語の1ビツト目P1が″“1′′であるよ
うな符号語の系列が生じた場合は本方式の条件が破られ
てしまうので、この場合は、古い符号語の8ビツト目P
8 とこれに続く符号語の1ピント目Plとをピッ6ベ
ージ ト“0”に反転し、古い符号語の9ビツト目P9をビッ
ト“1′°に反転する特別の規則を設けており、最小磁
化反転間隔Twin :133T 、最大磁化反転間隔
Tmax ’; 4.44T 、検出窓幅TW=0.4
4Tの特徴をもっている。従って、MFM方式と最小磁
化反転間隔Twinを同じにすれば線ピント密度を16
33倍にすることができる。
On the other hand, FIG. 1 shows the 4-9 conversion FNM (Fo
ur to N1ne Modulation) conversion table. This method converts 4-bit data into a 9-bit code word, and modulates the code word sequence with NRZI. The code word is limited so that at least two or more bits "O" are inserted between a bit "1" and the next bit "1", and there are no more than nine bits, as shown in Figure 2a. The characteristic is that the 8th bit P8 of the chronologically older code word is "1", and the 1st bit P1 of the code word that follows it is "1". If such a sequence of code words occurs, the conditions of this method are violated, so in this case, the 8th bit P of the old code word
8 and the 1st pin point Pl of the following code word are inverted to 6 bits "0", and the 9th bit P9 of the old code word is inverted to bit "1'°". Magnetization reversal interval Twin: 133T, maximum magnetization reversal interval Tmax'; 4.44T, detection window width TW=0.4
It has the characteristics of 4T. Therefore, if the MFM method and the minimum magnetization reversal interval Twin are the same, the line focus density can be increased to 16
It can be multiplied by 33 times.

第3図はFNM方式と従来の変調方式との記録電流波形
を比較して示す図であり、同図(力はデータ、(イ)F
iNRZI方式による波形、(り)はFM方式による波
形、(場はMFM方式による波形、(オ)は3PM方式
による波形、(力)はFNM方式による波形である。な
お、図で、Tはビット周期を示している。
Figure 3 shows a comparison of recording current waveforms between the FNM method and the conventional modulation method.
The waveform by the iNRZI method, (ri) is the waveform by the FM method, (field is the waveform by the MFM method, (o) is the waveform by the 3PM method, and (force) is the waveform by the FNM method. In the figure, T is the bit. It shows the cycle.

現在、大容量磁気ディスク装置で最も一般に用いられて
いるMFM方式の場合は、磁化反転間隔はT、1,5T
、2Tの3種類であり、最小磁化反転間隔ハ1nはTで
ある。MFM方式以外の変調方式の場合はTwinとし
てNRZIが、T、FMが045Tである。一方、最大
磁化反転間隔Tmax7ペー已 はNRZIが■、FMがT 、MFMが2Tである。
In the case of the MFM method, which is currently most commonly used in large-capacity magnetic disk drives, the magnetization reversal interval is T, 1.5T.
, 2T, and the minimum magnetization reversal interval C1n is T. In the case of a modulation method other than the MFM method, NRZI is used as Twin, T and FM is 045T. On the other hand, the maximum magnetization reversal interval Tmax is 7 pages for NRZI, T for FM, and 2T for MFM.

又、sPM方式は最小磁化反転間隔Tlll1nが1.
6T、最大磁化反転間隔Tmaxが6Tである。したが
って、本FNM方式は最小磁化反転間隔Tm1nを1゜
33TとMFM方式のTより改善し、最大磁化反転間隔
Tmaxを4.44Tと3PM方式の6Tより改善した
ものとなっている。又、第4図は各種変調方式の比較を
示している。
In addition, in the sPM method, the minimum magnetization reversal interval Tllll1n is 1.
6T, and the maximum magnetization reversal interval Tmax is 6T. Therefore, in the present FNM method, the minimum magnetization reversal interval Tm1n is 1°33T, which is improved from T in the MFM method, and the maximum magnetization reversal interval Tmax is 4.44T, which is better than 6T in the 3PM method. Further, FIG. 4 shows a comparison of various modulation methods.

以上説明したように本発明によれば、最小磁化反転間隔
T winが1.33TとMFM方式のTより大きく、
最大磁化反転間隔Tmaxが4.44Tと3PM方式の
6Tより小さく、又、高密度化の容易さを表わす最小磁
化反転間隔Twinと検出窓幅Twとの積が0.59T
2  とMFM方式(7)0.6T2ヨ1)大きく、さ
らにセルフクロッキング可能な変調方式を提供すること
ができる。
As explained above, according to the present invention, the minimum magnetization reversal interval T win is 1.33T, which is larger than T in the MFM method.
The maximum magnetization reversal interval Tmax is 4.44T, which is smaller than 6T of the 3PM method, and the product of the minimum magnetization reversal interval Twin, which indicates the ease of high density, and the detection window width Tw is 0.59T.
2 and MFM method (7) 0.6T2 yo 1) It is possible to provide a modulation method that is large and also capable of self-clocking.

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

第1図は本発明のディジタル変調方法におけるFNMの
変換テーブル図、第2図iFNMにおける最大磁化反転
間隔の発生する場合及び特別規則適用例を説明するため
の図、第3図はFNMと従来変調方式の記録電流波形の
比較図、第4図は各種変調方式の比較図である。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 第2図 4T79 X 10 = 4.44T 4T/9に2 = 0.89T 妊
Figure 1 is an FNM conversion table diagram in the digital modulation method of the present invention. Figure 2 is a diagram for explaining the case where the maximum magnetization reversal interval occurs in iFNM and an example of application of special rules. Figure 3 is a diagram showing FNM and conventional modulation. FIG. 4 is a comparison diagram of recording current waveforms of various modulation methods. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 4T79 x 10 = 4.44T 2 to 4T/9 = 0.89T Pregnancy

Claims (3)

【特許請求の範囲】[Claims] (1)高密度記録するだめのディジタル変調方法であっ
て、データビットを4ビット単位に分割し、この4ビッ
ト単位のデータビットの16通りの組合せに対し、9ビ
ツトの符号語(F’l’P2P3P4 Ps P6 P
7 Ps P9 )としてそのデ゛−タ時間列群を ■  000010000 ■  000100000 ■  000010010 ■  01001001 0 ■  1001001 00 ■  1 00100010 ■  000100010 ■  001 0001 00 ■  010001 000 [相]  1 oOol ooO0 2ベージ 0001ooO01゜ @  oloooool。 @  100000010 ■ oloooo 100 [相] 100000100 @  100001000 とし、これらのデータ列を対応させ、その後NRZIで
変調することを特徴とするディジタル変調方法。
(1) A digital modulation method for high-density recording, in which data bits are divided into 4-bit units, and a 9-bit code word (F'l 'P2P3P4 Ps P6 P
7 Ps P9 ) and the data time sequence group as ■ 000010000 ■ 000100000 ■ 000010010 ■ 01001001 0 ■ 1001001 00 ■ 1 00100010 ■ 000100010 ■ 001 0001 00 ■ 01000 1 000 [Phase] 1 oOol ooO0 2 pages 0001ooO01゜@ olooooool . @ 100000010 ■ oloooo 100 [phase] 100000100 @ 100001000 A digital modulation method characterized by making these data strings correspond and then modulating with NRZI.
(2)符号語と符号語の連結部における符号語系列パタ
ーンの時系列的に古い符号語の8ビツト目P8と9ビツ
ト目P9及び時系列的に新しい符号語の1ビツト目P1
が101となる場合は前記9ビツト目P9をビット°“
1′′に反転し、前記8ビツト目P8と1ビツト目P1
をビット“O”に反転させることを特徴とする特許請求
の範囲第1項記載のディジタル変調方法。
(2) The 8th bit P8 and the 9th bit P9 of the chronologically older codeword and the 1st bit P1 of the chronologically newer codeword in the codeword series pattern at the codeword-to-codeword concatenation part
is 101, the 9th bit P9 is set to
1'', the 8th bit P8 and the 1st bit P1
2. The digital modulation method according to claim 1, wherein the digital modulation method is inverted to bit "O".
(3)符号語系列のビット“1′′とビットII 11
1との間にピッ)’IIoIIを少なくとも2個以上含
み、多くとも9個以下となるように構成したことを3ペ
ージ 特徴とする特許請求の範囲第1項又は第2項記載のディ
ジタル変調方法。
(3) Bit “1'' and bit II 11 of codeword sequence
The digital modulation method according to claim 1 or 2, characterized in that the third page is configured to include at least two or more, and at most nine or less, 'IIoII'. .
JP10425482A 1982-06-16 1982-06-16 Digital modulating method Pending JPS58220211A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10425482A JPS58220211A (en) 1982-06-16 1982-06-16 Digital modulating method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10425482A JPS58220211A (en) 1982-06-16 1982-06-16 Digital modulating method

Publications (1)

Publication Number Publication Date
JPS58220211A true JPS58220211A (en) 1983-12-21

Family

ID=14375789

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10425482A Pending JPS58220211A (en) 1982-06-16 1982-06-16 Digital modulating method

Country Status (1)

Country Link
JP (1) JPS58220211A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0618576A2 (en) * 1993-04-02 1994-10-05 Kabushiki Kaisha Toshiba Digital data modulation/demodulation system
US5666338A (en) * 1994-03-16 1997-09-09 Kabushiki Kaisha Toshiba Recording medium formatted for error correction and density recording and an apparatus for recording information thereon and/or recording information therefrom

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0618576A2 (en) * 1993-04-02 1994-10-05 Kabushiki Kaisha Toshiba Digital data modulation/demodulation system
EP0618576A3 (en) * 1993-04-02 1996-07-03 Toshiba Kk Digital data modulation/demodulation system.
US5666338A (en) * 1994-03-16 1997-09-09 Kabushiki Kaisha Toshiba Recording medium formatted for error correction and density recording and an apparatus for recording information thereon and/or recording information therefrom
US5848051A (en) * 1994-03-16 1998-12-08 Kabushiki Kaisha Toshibo Recording medium formatted for error correction and high density recording and an apparatus for recording information thereon and/or reproducing information therefrom
US5909417A (en) * 1994-03-16 1999-06-01 Kabushiki Kaisha Toshiba Recording medium formatted for error correction and high density recording and an apparatus for recording information thereon and/or reproducing information therefrom
US5956306A (en) * 1994-03-16 1999-09-21 Kabushiki Kaisha Toshiba Recording medium, signal recording apparatus thereof and signal reproducing apparatus thereof

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