JPH0466045B2 - - Google Patents

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Publication number
JPH0466045B2
JPH0466045B2 JP18211783A JP18211783A JPH0466045B2 JP H0466045 B2 JPH0466045 B2 JP H0466045B2 JP 18211783 A JP18211783 A JP 18211783A JP 18211783 A JP18211783 A JP 18211783A JP H0466045 B2 JPH0466045 B2 JP H0466045B2
Authority
JP
Japan
Prior art keywords
frequency
signal
recording
equalization
reproduced
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
JP18211783A
Other languages
Japanese (ja)
Other versions
JPS6074161A (en
Inventor
Misao Kato
Taiji Shimeki
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 JP18211783A priority Critical patent/JPS6074161A/en
Publication of JPS6074161A publication Critical patent/JPS6074161A/en
Publication of JPH0466045B2 publication Critical patent/JPH0466045B2/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
    • G11B20/10009Improvement or modification of read or write signals

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、磁気テープ、磁気デイスクなどの記
録媒体に、高密度にデイジタル信号を記録、再生
する装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to an apparatus for recording and reproducing digital signals at high density on a recording medium such as a magnetic tape or a magnetic disk.

従来例の構成とその問題点 従来から、磁気テープや磁気デイスクなどの記
録媒体にデイジタル信号を記録する装置がある。
これらの装置では、記録時には、デイジタル信号
を適当なデイジタル変調(たとえばFM:
requency odulation,MFM:odifided
requency odulation)を施し、デイジタル信
号の反転位置と前記磁気記録媒体の磁化反転位置
が一致するように記録素子を介して磁気記録媒体
に記録する。また再生時には、再生素子を介し
て、記録された信号を再生し、磁化反転位置をも
とのデイジタル信号の反転位置に対応するように
変換し、元のデイジタル信号を復調する。
2. Description of the Related Art Configurations of Conventional Examples and Their Problems Conventionally, there have been devices for recording digital signals on recording media such as magnetic tapes and magnetic disks.
In these devices, when recording, the digital signal is subjected to appropriate digital modulation (for example, FM :
requency Modulation , MFM: Modified F
Recording is performed on the magnetic recording medium via a recording element such that the inversion position of the digital signal coincides with the magnetization inversion position of the magnetic recording medium. Furthermore, during reproduction, the recorded signal is reproduced through the reproduction element, the magnetization reversal position is converted to correspond to the reversal position of the original digital signal, and the original digital signal is demodulated.

この記録、再生の過程において、一般には記録
素子、記録媒体、再生素子のもつ特性によつて、
周波数特性劣化が発生し、再生信号は高周波成分
が減衰した周波数特性を有する。この周波数特性
の劣化によつてもたらされる結果として、各磁化
反転に対応する波形の干渉が発生し、これによつ
て磁化反転位置がずれる(一般に磁気再生過程は
微分過程なので磁化反転位置は再生信号のピーク
位置に相当し、そのピーク位置がずれるのでピー
クシフトと呼ばれる)ことがある。このピークシ
フトが発生すると、再生信号から正しくデイジタ
ル信号を復調できなくなる。特に高密度にデイジ
タル信号を記録する場合には、必然的にデイジタ
ル信号のもつ周波数特性は高周波領域に特性がよ
くのびた、すなわち高周波成分を多くもつたもの
となる。
In this recording and reproducing process, generally depending on the characteristics of the recording element, recording medium, and reproducing element,
Frequency characteristic deterioration occurs, and the reproduced signal has frequency characteristics in which high frequency components are attenuated. As a result of this deterioration of frequency characteristics, interference occurs between the waveforms corresponding to each magnetization reversal, which causes the magnetization reversal position to shift (generally, since the magnetic regeneration process is a differential process, the magnetization reversal position is determined by the reproduction signal). (This corresponds to the peak position of When this peak shift occurs, it becomes impossible to correctly demodulate the digital signal from the reproduced signal. In particular, when digital signals are recorded at high density, the frequency characteristics of the digital signals necessarily extend well into the high frequency region, that is, have many high frequency components.

従つて、高記録密度になればなるほど、記録、
再生素子や媒体の周波数特性劣化によるピークシ
フトが大きくなり、正しくデイジタル信号を復調
できなくなる。
Therefore, the higher the recording density, the more
The peak shift due to the deterioration of the frequency characteristics of the reproduction element or medium increases, making it impossible to correctly demodulate the digital signal.

従来、このようなピークシフトを抑制する手段
として、等化と呼ばれる方法がとられていた。代
表的な等化方法として余弦等化が知られている。
余弦等化の目的は、信号振幅の周波数特性の劣化
を第1図に示すような余弦特性で高周波成分を強
調し、周波数特性の劣化を補償することにある。
この余弦等化を実現する構成例を第2図に示し、
その動作を説明する。1は再生信号入力端子であ
り、再生素子からの再生信号が入力される。この
再生信号はさらに、第1の遅延回路2に入力され
るとともに、減衰器4−aで減衰されて加算回路
5に入力される。第1の遅延回路2では入力信号
をτ(>0)だけ時間遅延させ出力する。この出
力信号は第2の遅延回路3に入力され、τだけ遅
延されたあとさらに減衰器4−bで減衰され加算
回路5に入力される。加算回路5では、再生信号
入力端子1からの再生信号、第1、第2の遅延回
路2および3によつて2τだけ遅延された信号、第
1の遅延回路2の出力信号とを加算し、再生信号
出力端子6に出力する。
Conventionally, a method called equalization has been used as a means to suppress such peak shifts. Cosine equalization is known as a typical equalization method.
The purpose of cosine equalization is to compensate for the deterioration of the frequency characteristics of the signal amplitude by emphasizing high frequency components using cosine characteristics as shown in FIG.
An example of a configuration for realizing this cosine equalization is shown in Figure 2.
Let's explain its operation. Reference numeral 1 denotes a reproduction signal input terminal, into which a reproduction signal from a reproduction element is input. This reproduced signal is further input to the first delay circuit 2, attenuated by an attenuator 4-a, and input to the addition circuit 5. The first delay circuit 2 delays the input signal by τ (>0) and outputs the signal. This output signal is input to the second delay circuit 3, delayed by τ, further attenuated by an attenuator 4-b, and input to the adder circuit 5. The adder circuit 5 adds the reproduced signal from the reproduced signal input terminal 1, the signal delayed by 2τ by the first and second delay circuits 2 and 3, and the output signal of the first delay circuit 2, It is output to the playback signal output terminal 6.

今、再生信号入力端子1に(t−τ)で表現
される信号が入力されたとすると第1の遅延回路
2の出力信号は(t)となり、第2の遅延回路
3の出力信号は(t+τ)となり、減衰器4−
a、4−bでK/2(K>0)に減衰されるとする と、加算回路5の出力信号は(t)−K/2{(t −τ)+(t+τ)}となつて再生信号出力端子
6に出力される。この(t)−K/2{(t−τ) +(t+τ)}を周波数軸上の振幅特性で表現す
ると1−cos2πτとなり、第1図に示した周波数
特性を有する。従つてK,τを変えることによつ
て、周波数特性を変えることができる。
Now, if a signal expressed as (t-τ) is input to the reproduced signal input terminal 1, the output signal of the first delay circuit 2 will be (t), and the output signal of the second delay circuit 3 will be (t+τ). ), and the attenuator 4-
If it is attenuated to K/2 (K>0) in a and 4-b, the output signal of the adder circuit 5 is reproduced as (t)-K/2{(t-τ)+(t+τ)} The signal is output to the signal output terminal 6. If this (t)-K/2{(t-.tau.) + (t+.tau.)} is expressed in terms of amplitude characteristics on the frequency axis, it becomes 1-cos2.pi..tau., which has the frequency characteristics shown in FIG. Therefore, by changing K and τ, the frequency characteristics can be changed.

またステツプパルスを記録した場合の再生信号
は第3図のaのような形となり孤立再生信号と呼
ばれる。この孤立再生信号のピーク値の50%の振
幅を有するところの時間軸上の幅は半値幅
(W50)と呼ばれており、半値幅が狭いほど周波
数特性がよいことはよく知られている。そこで第
2図の余弦等化回路の定数K,τを適当な値を選
択すると、第3図aの孤立再生信号は同図bのよ
うに半値幅をW50′(<W50)とすることができ
周波数特性を改善することができる。一般に再生
過程において、重ね合せの定理が成立つことろで
は、あらゆるパターンの信号は孤立再生信号の重
ね合せで表現でき、前記のように半値幅を狭くす
ると周波数特性が改善され波形干渉によるピーク
シフトが抑圧される。
Further, when a step pulse is recorded, the reproduced signal has a form as shown in a of FIG. 3 and is called an isolated reproduced signal. The width on the time axis where the isolated reproduction signal has an amplitude of 50% of the peak value is called the half-width (W 50 ), and it is well known that the narrower the half-width, the better the frequency characteristics. . Therefore, by selecting appropriate values for the constants K and τ of the cosine equalization circuit in Fig. 2, the isolated reproduced signal in Fig. 3a has a half-width of W 50 '(<W 50 ) as shown in Fig. 3b. It can improve the frequency characteristics. In general, in the reproduction process, if the superposition theorem holds true, any signal pattern can be expressed by a superposition of isolated reproduced signals, and as mentioned above, narrowing the half-width improves the frequency characteristics and shifts the peak due to waveform interference. is suppressed.

また、余弦等化をさらに拡張したトランスバー
サル型等化回路もあるが、これは、遅延回路を数
段タツプ付きの定遅延素子で構成し、各タツプ出
力に適当な定数をかけて、それらの出力を加算し
たものである。
There is also a transversal equalization circuit that further expands cosine equalization, but this consists of a delay circuit consisting of constant delay elements with several stages of taps, and each tap output is multiplied by an appropriate constant. It is the sum of the outputs.

以上、前記余弦等化回路もトランスバーサル型
等化回路もピークシフトを抑圧するために、ピー
クシフトを最小にできる最適な定数を求める必要
がある。
As described above, in order to suppress the peak shift in both the cosine equalization circuit and the transversal type equalization circuit, it is necessary to find an optimal constant that can minimize the peak shift.

ところが、より高密度にデイジタル信号を記録
再生する場合、磁化反転における波形干渉が大き
くなり、ピークシフトが増大し、前記のような余
弦等化回路ではピークシフトの抑圧ができない
か、ほとんど抑圧効果を得られない領域が存在す
る。たとえば、最小磁化反転間隔をTnioとすると
W50/Tnioが2を超えるような場合である。この
ような領域では、単に余弦等化の定数を変えて半
値幅W50を小さくできても、ピークシフトは抑圧
されるどころか逆に悪くなることさえある。
However, when recording and reproducing digital signals at higher density, waveform interference in magnetization reversal increases and peak shift increases, and the cosine equalization circuit described above either cannot suppress the peak shift or has almost no suppression effect. There are areas where this is not possible. For example, if the minimum magnetization reversal interval is T nio
This is a case where W 50 /T nio exceeds 2. In such a region, even if the half width W 50 can be reduced by simply changing the cosine equalization constant, the peak shift may not be suppressed, but may even worsen.

このように余弦等化回路では、高記録密度にな
ると、ピークシフトを抑圧できないことがある。
また、トランスバーサル型の等化回路では、必要
なタツプ数が増大し、最適な定数をさがし出すこ
とが難しくなる。
As described above, the cosine equalization circuit may not be able to suppress peak shifts when the recording density becomes high.
Furthermore, in a transversal type equalization circuit, the number of required taps increases, making it difficult to find optimal constants.

発明の目的 本発明は、磁気テープや磁気デイスクなどの磁
気記録媒体にデイジタル信号を記録、再生する際
に再生信号の周波数特性劣化を余弦等化では補償
することができない高記録密度の領域において、
周波数特性劣化を補償し、高密度にデイジタル信
号を記録し、再生する磁気記録再生装置を提供す
ることを目的とする。
Purpose of the Invention The present invention provides a method for recording and reproducing digital signals on magnetic recording media such as magnetic tapes and magnetic disks in high recording density areas where deterioration in frequency characteristics of reproduced signals cannot be compensated for by cosine equalization.
It is an object of the present invention to provide a magnetic recording and reproducing device that compensates for frequency characteristic deterioration and records and reproduces digital signals at high density.

発明の構成 本発明は、デイジタル信号を磁気記録媒体上に
記録再生し、再生時に、最高記録周波数の2分の
1の周波数の第3次高調波周波数のところまでは
周波数の増加にともない一定の率で出力を強調す
る増幅回路と、カツトオフ周波数が最高記録周波
数の2倍でかつカツトオフ周波数付近で一定のロ
ールオフ率のローパスフイルタとからなる等化手
段を有する磁気記録再生装置であり、ピークシフ
トの充分な抑圧効果が得られ、高密度にデイジタ
ル信号を記録再生できるものである。
Composition of the Invention The present invention records and reproduces digital signals on a magnetic recording medium, and during reproduction, the frequency remains constant as the frequency increases up to the third harmonic frequency of half the highest recording frequency. This is a magnetic recording and reproducing device that has equalization means consisting of an amplifier circuit that emphasizes the output by a peak shift rate, and a low-pass filter whose cutoff frequency is twice the highest recording frequency and whose rolloff rate is constant around the cutoff frequency. A sufficient suppression effect can be obtained, and digital signals can be recorded and reproduced at high density.

実施例の説明 実施例を説明するまえに本発明の考え方につい
て説明する。
DESCRIPTION OF EMBODIMENTS Before describing embodiments, the concept of the present invention will be explained.

第4図に磁気記録再生装置の孤立再生信号波形
の一例を示す。この孤立再生信号の半値幅W50
図より約220nsecである。今、最小磁化反転間隔
Tnioが86.2nsec、Tnaxが174.2nsecであるFM変調
されたデイジタル信号を記録再生した場合に、実
際にパターンを記録再生しなくても第4図の孤立
再生波形を重ね合せることにより、任意のパター
ンのピークシフトを見積ることができる。FM変
調方式の波形干渉によるピークシフトがもつとも
大きいパターンは、第5図に示すパターンとな
り、最大磁化反転間隔Tnaxの磁化反転がピーク
シフトによつて内側に狭くなる。そのピークシフ
トの状態を第6図に示す。この場合ピークシフト
量は変調前のデイジタル信号のビツト周囲をT0
とすると約0.17T0となつている。
FIG. 4 shows an example of an isolated reproduction signal waveform of a magnetic recording/reproduction device. The half width W 50 of this isolated reproduction signal is approximately 220 nsec from the figure. Now, the minimum magnetization reversal interval
When recording and reproducing an FM-modulated digital signal with T nio of 86.2 nsec and T nax of 174.2 nsec, it is possible to create an arbitrary The peak shift of the pattern can be estimated. A pattern with a large peak shift due to waveform interference in the FM modulation method is a pattern shown in FIG. 5, in which the magnetization reversal of the maximum magnetization reversal interval T nax narrows inward due to the peak shift. The state of the peak shift is shown in FIG. In this case, the peak shift amount is T 0 around the bit of the digital signal before modulation.
Then, it becomes approximately 0.17T 0 .

前記第4図の半値幅W50とTnioの比をとると
W50/Tnio≒2.55となつており、余弦等化では周
波数特性劣化を補償し、ピークシフトを抑圧する
よう改善することはできなかつた。そこで、第7
図に示すように磁気記録において孤立再生信号の
近似式として最もよく知られている(t)=
A/1+(2t/W502(ローレンツ波形と呼ばれるこ ともある。Aは最大振幅値)をTbの周期で振幅
が0になるような理想的な波形(ナイキスト波形
と呼ばれることもある) h(t)=sin(πt/Tb)/πt/Tb・cos(πβt/Tb
)/1−2βt/Tb2に等化す る等化伝達関数を求めた。それは次式のようにな
る。
Taking the ratio of the half width W 50 and T nio in Figure 4 above,
W 50 /T nio ≈2.55, and cosine equalization could not compensate for frequency characteristic deterioration and suppress peak shift. Therefore, the seventh
As shown in the figure, (t)=
A/1 + (2t/W 50 ) 2 (sometimes called the Lorentz waveform. A is the maximum amplitude value) is an ideal waveform (sometimes called the Nyquist waveform) in which the amplitude becomes 0 with a period of T b ) h(t)=sin(πt/T b )/πt/T b・cos(πβt/T b
)/1−2βt/T b ) An equalization transfer function that equalizes to 2 was obtained. It becomes as follows.

F()=2/W50πAl〓 F()=2/W 50 πAl〓

Claims (1)

【特許請求の範囲】[Claims] 1 デイジタル信号を磁気記録媒体上に記録再生
し、再生時に、最高記録周波数の2分の1の周波
数の第3次高調波周波数のところまでは周波数の
増加にともない一定の率で出力を強調する増幅回
路と、カツトオフ周波数が最高記録周波数の2倍
でかつカツトオフ周波数付近で一定のロールオフ
率のローパスフイルタとからなる等化手段を有す
ることを特徴とする磁気記録再生装置。
1 Record and reproduce digital signals on a magnetic recording medium, and during reproduction, emphasize the output at a constant rate as the frequency increases up to the third harmonic frequency, which is half the highest recording frequency. 1. A magnetic recording and reproducing apparatus comprising an equalizing means comprising an amplifier circuit and a low-pass filter having a cutoff frequency twice the highest recording frequency and a constant roll-off rate near the cutoff frequency.
JP18211783A 1983-09-29 1983-09-29 Magnetic recording and reproducing device Granted JPS6074161A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18211783A JPS6074161A (en) 1983-09-29 1983-09-29 Magnetic recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18211783A JPS6074161A (en) 1983-09-29 1983-09-29 Magnetic recording and reproducing device

Publications (2)

Publication Number Publication Date
JPS6074161A JPS6074161A (en) 1985-04-26
JPH0466045B2 true JPH0466045B2 (en) 1992-10-22

Family

ID=16112627

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18211783A Granted JPS6074161A (en) 1983-09-29 1983-09-29 Magnetic recording and reproducing device

Country Status (1)

Country Link
JP (1) JPS6074161A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH067403B2 (en) * 1985-06-17 1994-01-26 ティアツク株式会社 Digital magnetic reproducing circuit
JPH01122002A (en) * 1987-11-06 1989-05-15 Canon Electron Inc Signal reader

Also Published As

Publication number Publication date
JPS6074161A (en) 1985-04-26

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