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JPH0456366B2 - - Google Patents
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JPH0456366B2 - - Google Patents

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Publication number
JPH0456366B2
JPH0456366B2 JP20906583A JP20906583A JPH0456366B2 JP H0456366 B2 JPH0456366 B2 JP H0456366B2 JP 20906583 A JP20906583 A JP 20906583A JP 20906583 A JP20906583 A JP 20906583A JP H0456366 B2 JPH0456366 B2 JP H0456366B2
Authority
JP
Japan
Prior art keywords
circuit
waveform
comparator
output
pulse
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
JP20906583A
Other languages
Japanese (ja)
Other versions
JPS60101703A (en
Inventor
Motoi Aoi
Nobumasa Nishama
Makoto Saito
Yasuhide Oochi
Takashi Tamura
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP20906583A priority Critical patent/JPS60101703A/en
Publication of JPS60101703A publication Critical patent/JPS60101703A/en
Publication of JPH0456366B2 publication Critical patent/JPH0456366B2/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
    • G11B20/10046Improvement or modification of read or write signals filtering or equalising, e.g. setting the tap weights of an FIR filter
    • G11B20/10203Improvement or modification of read or write signals filtering or equalising, e.g. setting the tap weights of an FIR filter baseline correction

Landscapes

  • Engineering & Computer Science (AREA)
  • Signal Processing (AREA)
  • Digital Magnetic Recording (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔発明の利用分野〕 本発明は磁気デイスク装置、磁気テープ装置等
デイジタル磁気記憶装置に好適な磁化反転に対応
するパルス再生回路に関する。 〔発明の背景〕 デイジタル磁気記憶装置では、第1図のように
磁化反転1の有無として情報を記憶する。この磁
化反転1は磁気ヘツドで磁化反転に対応するピー
クを有す波形2として再生される。再生波形のピ
ーク検出には、再生波形を微分し、ピーク位置を
微分波形3の零クロス点に変換し、再生波形2の
ピークに対応する読出しパルス4を得る方法が、
従来広く用いられている。例えば、電子通信学会
磁気記録研究会資料、MR−71−6参照。しかし
この方法では、微分回路により高い周波数での雑
音成分が強調されるため、帯域の選択によつては
S/Nの低下をまねく欠点がある。 この欠点を補う手法として、第2図に示す様に
微分の代りに積分を用い、積分波形5の中心レベ
ルでスライスし読出しパルス6を得る手法があ
る。例えば、電子通信学会磁気記録研究会資料
MR−77−46、IEEE Trans.on Mag,Vol
MAG−17、No.6,pp.3352−3354,No
VEMBER,1981等参照。この積分方式では、
S/Nが微分方式に比べ良いという利点を有する
が、積分回路を有するため、回路の直流ドリフト
等により、読出し誤りを生じ易い欠点を有する。 〔発明の目的〕 本発明の目的は、回路の直流ドリフトの影響を
除き、安定な積分方式を用いた磁化反転パルス再
生方式を提供することにある。 〔発明の概要〕 本発明では、積分波形の中心スライスレベルを
読出しパルスのピーク位置のずれを減少させるよ
うに、“1”,“0”の弁別に用いるPLL(Phase
Locked Loop)の位相比較器の出力を用いて補
正し、回路のドリフト等の影響を除くものであ
る。 〔発明の実施例〕 以下、本発明の実施例を第3図により説明す
る。磁気ヘツド7で読み出された信号は、再生増
幅器8で増幅され、磁化反転パルス再生回路31
においてパルス化される。読出しパルス6は、
PLL回路30に入力され、PLL回路30で読出
しパルス6に同期した弁別窓19を発生する。読
出しパルス6は弁別窓19とともに、弁別回路1
2に入力され、弁別回路の出力である弁別データ
28、クロツク29とともに上位機種へ転送され
る。 ここで、再生増幅器8はリニア増幅器であつて
も良いが、広く知られているパルススリミング回
路、波形等化回路等、再生波形をシヤープにする
波形処理回路の機能を有しても良い。PLL回路
30はデイジタル磁気記録装置の弁別のため広く
用いられているもので、弁別窓19と、読出しパ
ルス6との位相差を検出する位相比較器16、位
相比較器の位相検出出力から長い期間での平均的
位相ずれに相当する出力を得るための低域波器
17、及び入力の直流レベルに比較して発振周波
数の変化する電圧制御発振器18から成る。 本発明の主要部分である磁化反転パルス再生回
路31の構成、動作を第3図、第5図を用いて述
べる。再生増幅器8の出力は積分回路9を経て、
コンパレータ10で波形整形された後、パルス化
回路11でパルス化6される。ここで積分波形5
に回路のドリフト等による中心レベルのずれが生
じた場合に、ずれの影響を除く目的でコンパレー
タ10のスライスレベル32に補正を加える。補
正のための情報は、PLL回路30内の位相比較
器16の出力である周波数上昇信号24及び周波
数降下信号25を、積分波形5のスロープの方向
を識別するゲート信号22,23と比較すること
によりスライスレベル比較回路15で得られるス
ライスレベル上昇信号20及びレベル降下信号2
1を、低域波器13を通すことにより得る。 第4図はスライスレベル比較回路15および積
分波形スロープ識別回路14の実施例を示したも
のである。この図および第3図、第5図を用い、
スライスレベル補正動作を説明する。スロープ識
別回路14は前述のように積分波形50の“零”
クロス点でのスロープの向きを検出するための回
路であり、2つのコンパレータ141,142か
ら成る。入力はいずれも再生波形2であり、各々
は正、負のスライスレベル26,27が与えられ
る。積分波形5のスロープが正の場合は、再生波
形2の十側のパルスをスライスレベル26でスラ
イスし零クロス点の傾斜が正であることを示すゲ
ート信号22がコンパレータ141から発生
し、スロープが負の場合は同様にゲート信号2
3がコンパレータ142から発生する。 積分波形5にドリフト等がなく正しく零クロス
点で読出しパルス6が再生できた場合(第5図の
左側2ビツトの場合)には、読出しパルス6は弁
別窓19の中央に位置するので位相比較器16の
出力24,25はない。そのためレベル補正は行
なわれない。次に第5図の中央2ビツトに示した
様に、積分波形5が下側にシフトした場合を考え
る。この場合、左右の読出しパルスとも本来の零
クロス点より各々後および前にシフトする。その
ため位相比較器16の出力として、左、右の読出
しパルスに対応して、弁別窓の中央と読出しパル
スの位相差に等しい周波数降下信号25および周
波数上昇信号24を得る。逆に積分波形5が上側
にシフトした場合(第5図の右側2ビツトの場
合)には、左右の読出しビツトに対応し各々周波
数上昇信号24および周波数降下信号25を得
る。 以上のようにして得られた位相比較器16の出
力から第5図中央2ビツトに対してはレベル降下
信号21を、右側2ビツトに対してレベル上昇信
号20を得るには、表1に示す関係を満す論理回
路を構成すればよい。
[Field of Application of the Invention] The present invention relates to a pulse reproduction circuit corresponding to magnetization reversal suitable for digital magnetic storage devices such as magnetic disk devices and magnetic tape devices. [Background of the Invention] In a digital magnetic storage device, information is stored as the presence or absence of magnetization reversal 1 as shown in FIG. This magnetization reversal 1 is reproduced by a magnetic head as a waveform 2 having a peak corresponding to the magnetization reversal. To detect the peak of the reproduced waveform, there is a method of differentiating the reproduced waveform, converting the peak position to the zero cross point of the differential waveform 3, and obtaining the read pulse 4 corresponding to the peak of the reproduced waveform 2.
Conventionally widely used. For example, see IEICE Magnetic Recording Study Group Materials, MR-71-6. However, this method has the drawback that noise components at high frequencies are emphasized by the differentiating circuit, resulting in a reduction in S/N depending on the selection of the band. As a method to compensate for this drawback, as shown in FIG. 2, there is a method of using integration instead of differentiation and slicing at the center level of the integral waveform 5 to obtain the readout pulse 6. For example, materials from the Magnetic Recording Study Group of the Institute of Electronics and Communication Engineers
MR−77−46, IEEE Trans.on Mag, Vol.
MAG-17, No.6, pp.3352-3354, No.
See VEMBER, 1981, etc. In this integration method,
Although it has the advantage that the S/N ratio is better than the differential method, it has the disadvantage that reading errors are likely to occur due to DC drift of the circuit because it includes an integrating circuit. [Object of the Invention] An object of the present invention is to provide a magnetization reversal pulse regeneration method using a stable integration method, eliminating the influence of DC drift of the circuit. [Summary of the invention] In the present invention, a PLL (Phase
This method uses the output of the phase comparator (Locked Loop) to remove the effects of circuit drift, etc. [Embodiments of the Invention] Hereinafter, embodiments of the present invention will be described with reference to FIG. The signal read out by the magnetic head 7 is amplified by a regenerative amplifier 8 and sent to a magnetization reversal pulse reproducing circuit 31.
pulsed at The read pulse 6 is
The signal is input to the PLL circuit 30, which generates a discrimination window 19 synchronized with the read pulse 6. The readout pulse 6 is sent to the discrimination circuit 1 along with the discrimination window 19.
2, and is transferred to the host model together with the discrimination data 28 and clock 29 which are the outputs of the discrimination circuit. Here, the regenerative amplifier 8 may be a linear amplifier, but may also have the function of a waveform processing circuit that sharpens the regenerated waveform, such as a widely known pulse slimming circuit or waveform equalization circuit. The PLL circuit 30 is widely used for discrimination in digital magnetic recording devices, and includes a discrimination window 19, a phase comparator 16 that detects the phase difference with the read pulse 6, and a long period from the phase detection output of the phase comparator. It consists of a low frequency generator 17 for obtaining an output corresponding to the average phase shift at , and a voltage controlled oscillator 18 whose oscillation frequency changes compared to the input DC level. The configuration and operation of the magnetization reversal pulse regeneration circuit 31, which is the main part of the present invention, will be described with reference to FIGS. 3 and 5. The output of the regenerative amplifier 8 passes through the integrating circuit 9,
After being waveform-shaped by a comparator 10, it is pulsed 6 by a pulsing circuit 11. Here, integral waveform 5
When a center level shift occurs due to circuit drift or the like, correction is applied to the slice level 32 of the comparator 10 in order to eliminate the influence of the shift. Information for correction is obtained by comparing the frequency rising signal 24 and frequency falling signal 25, which are the outputs of the phase comparator 16 in the PLL circuit 30, with gate signals 22 and 23 that identify the direction of the slope of the integral waveform 5. The slice level increase signal 20 and level decrease signal 2 obtained by the slice level comparison circuit 15 are
1 is obtained by passing it through a low frequency filter 13. FIG. 4 shows an embodiment of the slice level comparison circuit 15 and the integral waveform slope identification circuit 14. Using this figure and Figures 3 and 5,
The slice level correction operation will be explained. As mentioned above, the slope identification circuit 14 detects the "zero" of the integral waveform 50.
This is a circuit for detecting the direction of the slope at the cross point, and consists of two comparators 141 and 142. Both inputs are reproduced waveforms 2, and positive and negative slice levels 26 and 27 are applied to each input. When the slope of the integral waveform 5 is positive, the pulse on the ten side of the reproduced waveform 2 is sliced at the slice level 26, and a gate signal 22 is generated from the comparator 141 indicating that the slope of the zero crossing point is positive, and the slope is Similarly, if it is negative, gate signal 2
3 is generated from comparator 142. If there is no drift in the integral waveform 5 and the readout pulse 6 can be reproduced correctly at the zero cross point (in the case of 2 bits on the left side of FIG. 5), the readout pulse 6 is located at the center of the discrimination window 19, so phase comparison is possible. There are no outputs 24, 25 of the device 16. Therefore, no level correction is performed. Next, consider the case where the integral waveform 5 is shifted downward as shown in the center 2 bits of FIG. In this case, both the left and right read pulses are shifted behind and before the original zero-crossing point, respectively. Therefore, as the output of the phase comparator 16, a frequency drop signal 25 and a frequency rise signal 24 equal to the phase difference between the center of the discrimination window and the read pulse are obtained corresponding to the left and right read pulses. Conversely, when the integral waveform 5 shifts upward (in the case of 2 bits on the right side in FIG. 5), a frequency increase signal 24 and a frequency decrease signal 25 are obtained corresponding to the left and right read bits, respectively. Table 1 shows how to obtain the level drop signal 21 for the center 2 bits in FIG. 5 and the level increase signal 20 for the right 2 bits from the output of the phase comparator 16 obtained as described above. It is sufficient to construct a logic circuit that satisfies the relationship.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、積分回路のドリフト等の問題
が除去できるので、積分回路を用いた磁化反転パ
ルス再生回路が実現できる。
According to the present invention, since problems such as drift of the integrating circuit can be eliminated, a magnetization reversal pulse reproducing circuit using the integrating circuit can be realized.

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

第1図は微分回路を用いた磁化反転パルス再生
方式を説明するための波形図、第2図は積分回路
を用いた磁化反転パルス再生方式を説明するため
の波形図、第3図、第4図は本発明の一実施例の
構成図、第5図はその各部の波形を示す図であ
る。 7……記録、再生用磁気ヘツド、8……再生増
幅器、30……Phase Locked Loop、16……
位相比較器、31……磁化反転パルス再生回路、
9……積分回路、10……コンパレータ、11…
…パルス化回路、14……積分波形スロープ識別
回路、15……スライスレベル比較器、13,1
7……低域波器、18……電圧制御発振器、1
2……弁別回路。
Fig. 1 is a waveform diagram for explaining the magnetization reversal pulse regeneration method using a differentiating circuit, Fig. 2 is a waveform diagram for explaining the magnetization reversal pulse regeneration method using an integrating circuit, Figs. The figure is a block diagram of one embodiment of the present invention, and FIG. 5 is a diagram showing waveforms of each part thereof. 7...Magnetic head for recording and reproduction, 8...Reproduction amplifier, 30...Phase Locked Loop, 16...
Phase comparator, 31...Magnetization reversal pulse regeneration circuit,
9...Integrator circuit, 10...Comparator, 11...
...Pulsing circuit, 14... Integral waveform slope identification circuit, 15... Slice level comparator, 13,1
7...Low frequency generator, 18...Voltage controlled oscillator, 1
2...discrimination circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 磁化反転信号を積分する積分回路と、該積分
回路の出力を基準レベルと比較するコンパレータ
と、該コンパレータの出力をパルス化するパルス
化回路と、該パルス化回路の出力に同期して発振
する発振器とを有し、該発振器の出力と該パルス
化回路の出力の位相差に応じて、上記コンパレー
タの基準レベルを補正することを特徴とする磁化
反転パルス再生方式。
1. An integrating circuit that integrates the magnetization reversal signal, a comparator that compares the output of the integrating circuit with a reference level, a pulsing circuit that pulsates the output of the comparator, and oscillates in synchronization with the output of the pulsing circuit. 1. A magnetization reversal pulse regeneration method comprising: an oscillator; the reference level of the comparator is corrected in accordance with the phase difference between the output of the oscillator and the output of the pulsing circuit.
JP20906583A 1983-11-09 1983-11-09 Magnetization reversal pulse regeneration method Granted JPS60101703A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20906583A JPS60101703A (en) 1983-11-09 1983-11-09 Magnetization reversal pulse regeneration method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20906583A JPS60101703A (en) 1983-11-09 1983-11-09 Magnetization reversal pulse regeneration method

Publications (2)

Publication Number Publication Date
JPS60101703A JPS60101703A (en) 1985-06-05
JPH0456366B2 true JPH0456366B2 (en) 1992-09-08

Family

ID=16566666

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20906583A Granted JPS60101703A (en) 1983-11-09 1983-11-09 Magnetization reversal pulse regeneration method

Country Status (1)

Country Link
JP (1) JPS60101703A (en)

Also Published As

Publication number Publication date
JPS60101703A (en) 1985-06-05

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