JPS60169286A - Magnetic reproducing device - Google Patents

Magnetic reproducing device

Info

Publication number
JPS60169286A
JPS60169286A JP59022820A JP2282084A JPS60169286A JP S60169286 A JPS60169286 A JP S60169286A JP 59022820 A JP59022820 A JP 59022820A JP 2282084 A JP2282084 A JP 2282084A JP S60169286 A JPS60169286 A JP S60169286A
Authority
JP
Japan
Prior art keywords
frequency
signal
luminance signal
reproduced
magnetic reproducing
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
JP59022820A
Other languages
Japanese (ja)
Inventor
Kuniaki Miura
三浦 邦昭
Isao Fukushima
福島 勇夫
Makoto Shiomi
誠 塩見
Shinya Ichimura
市村 信也
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 JP59022820A priority Critical patent/JPS60169286A/en
Publication of JPS60169286A publication Critical patent/JPS60169286A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N5/00Details of television systems
    • H04N5/76Television signal recording
    • H04N5/91Television signal processing therefor
    • H04N5/93Regeneration of the television signal or of selected parts thereof
    • H04N5/95Time-base error compensation

Landscapes

  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Television Signal Processing For Recording (AREA)

Abstract

PURPOSE:To obtain a jitter correcting means leading to low cost and high performance by using an oscillated frequency of a VCO so as to modulate a high frequency portion of a reproduced luminance signal and providing nearly same jitter component as that of the reproduced luminance signal to the oscillated frequency of the VCO. CONSTITUTION:An FM luminance signal reproduced from a head 3 is amplified by a preamplifier 4 and the frequency is corrected by a peaking circuit 5. After the high frequency of an output of the peaking circuit 5 is converted at a high frequency converting circuit 11, one frequency is extracted by a BPF12 and demodulated by a demodulation circuit 6. On the other hand, a horizontal synchronizing signal (h) separated from the luminance signal by a synchronizing separator circuit 9 is compared for the phase with a reference signal hr at a phase comparator 15 and its output (v) is fed to the VCO17 via an LPF16. As a result, an output of the VCO17 has nearly the same jitter component as the reproduced luminance signal and the reproduced luminance signal is subject to high frequency conversion by a high frequency converting circuit 11 based on the signal, then the luminance signal suppressed with jitter component is obtained.

Description

【発明の詳細な説明】 〔利用分野〕 本発明は、周波数変動(以下、ジッタと略す)補正手段
を有する磁気再生装f(以下、VTRと呼ぶ)に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application] The present invention relates to a magnetic reproducing device f (hereinafter referred to as a VTR) having a frequency fluctuation (hereinafter abbreviated as jitter) correcting means.

〔背 景〕[Background]

第1図は家庭用VTR(たとえばVH8方式)の記録信
号スペクトラムを示したもので、FM変調された輝度信
号1と低域変換されたカラー信号2が周波数多重されて
いる様子を示す。
FIG. 1 shows a recording signal spectrum of a home VTR (for example, VH8 system), and shows how an FM-modulated luminance signal 1 and a low-frequency converted color signal 2 are frequency-multiplexed.

第2図は、従来のFM輝度信号再生回路を示したもので
ある。ヘッド3から再生されたFM輝度信号はプリアン
プ4により増幅され、ピーキング回路5により周波数特
性を補正された後、復調回路6により復調されLPF 
7を通って輝度信号りとなる。家庭用VTRの場合、信
号の記録再生は回転ドラム上に設置された磁気ヘッドに
より行なっているため、ドラムの回転むらなどによコレ
クタが生じ、再生画面を不安定なものとしている。
FIG. 2 shows a conventional FM luminance signal reproducing circuit. The FM luminance signal reproduced from the head 3 is amplified by a preamplifier 4, its frequency characteristics are corrected by a peaking circuit 5, and then demodulated by a demodulation circuit 6 and sent to an LPF.
7 and becomes the luminance signal. In the case of a home VTR, since signals are recorded and reproduced using a magnetic head installed on a rotating drum, collectors occur due to uneven rotation of the drum, making the reproduced screen unstable.

第3図は、上記の回路によって発生するジッタを補正す
る従来例を示す、この従来回路はLPF 7から出力さ
れたジッタを含んだ輝度信号りを、CCDなどの可変遅
延線8を用いてジッタ補正するものである。すなわち、
輝度信号りから同期分離回路9によりジッタを含む水平
同期信号りを分離し、これによりクロック発振器10の
クロック周波数を変化させる。可変遅延線8の遅延時間
はクロック周波数により一義的に決まり、クロック周波
数をジッタに応じて変化させることにより遅延時間を変
化させ、最終的にジッタのない輝度信号L を得る。
FIG. 3 shows a conventional example of correcting the jitter generated by the above circuit. This conventional circuit uses a variable delay line 8 such as a CCD to correct the jitter-containing luminance signal output from the LPF 7. This is a correction. That is,
A horizontal synchronization signal including jitter is separated from the luminance signal by a synchronization separation circuit 9, thereby changing the clock frequency of a clock oscillator 10. The delay time of the variable delay line 8 is uniquely determined by the clock frequency, and by changing the clock frequency according to jitter, the delay time is changed, and finally a jitter-free luminance signal L 2 is obtained.

omp 、ここに示したジッタ補正回路は次のような欠点を有し
ている。
omp, the jitter correction circuit shown here has the following drawbacks.

(1)広帯域なビデオ信号を通過させるだめの可変遅延
線が非常に高価である。
(1) A variable delay line for passing wideband video signals is very expensive.

(2)クロックのもれ込みによjl) S/N が劣化
する。
(2) S/N deteriorates due to clock leakage.

従来のジッタ補正回路は上記のような欠点を有している
ので、コストおよび性能的に家庭用VTRへの適用はむ
ずかしい。また〜の変換器、ンA変換器およびメモリを
用いたいわゆるディジタルタイムベースコレクタもコス
トが極めて高いなどの欠点がある。
Since the conventional jitter correction circuit has the above-mentioned drawbacks, it is difficult to apply it to home VTRs in terms of cost and performance. Furthermore, the so-called digital time base collector using the converter of 1-A, the N-A converter, and the memory also has drawbacks such as extremely high cost.

〔目 的〕〔the purpose〕

本発明の目的は、上記した従来の欠点をなくし、低コス
トかつ高機能化につながるジッタ補正手段を提供するに
ある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a jitter correction means which eliminates the above-mentioned conventional drawbacks and which leads to low cost and high functionality.

〔概 要〕〔overview〕

本発明の特徴は、再生輝度信号を高域変換する手段と、
復調信号から水平同期信号を分離する手段と、水平同期
信号と基準信号を伝相比較する手段と、位相比較出力か
ら制御電圧を取シ出すフィルタと、該制御電圧にょシ発
振周波数が変化する電圧制御型発振器(以下vcoと略
す)を設け、VCOの発振周波数を用いて再生輝度信号
を高域変換し、かつvCOの発振周波数が再生輝度信号
とほぼ同じジッタ 成分を持つように、フィードバック
制御をかけることにょシ、再生輝度信号のジッタを抑圧
するようにした点にある。
The present invention is characterized by a means for high-frequency conversion of a reproduced luminance signal;
means for separating the horizontal synchronization signal from the demodulated signal; means for comparing the horizontal synchronization signal and the reference signal; a filter for extracting a control voltage from the phase comparison output; and a voltage at which the oscillation frequency changes when the control voltage is applied. A controlled oscillator (hereinafter abbreviated as VCO) is provided, and the reproduced luminance signal is converted to a high frequency using the oscillation frequency of the VCO, and feedback control is performed so that the oscillation frequency of the VCO has approximately the same jitter component as the reproduced luminance signal. The key point is that jitter in the reproduced luminance signal is suppressed.

〔実施例〕〔Example〕

以下に本発BAを具体的実施例に基き、詳細に説明する
。第4図は本発明の第一の実施例を示す。
The BA of the present invention will be described in detail below based on specific examples. FIG. 4 shows a first embodiment of the invention.

この実施例が第3因の従来例と異なる点は、次の点であ
る。
This embodiment differs from the conventional example of the third factor in the following points.

(1)ピーキング回路5と復調器6の間に、高域変換回
路11およびBPF12が設けられている。
(1) A high frequency conversion circuit 11 and a BPF 12 are provided between the peaking circuit 5 and the demodulator 6.

(2)同期分離回路9によシ輝度信号から分離された水
平同期信号りは、基準信号発生器13からてい倍および
分局回路14を通って作られた基準信号hrと位相比較
器15において位相比較される。
(2) The horizontal synchronization signal separated from the luminance signal by the synchronization separation circuit 9 is outputted from the reference signal generator 13 through the multiplier and branching circuit 14, and the reference signal hr and the phase comparator 15. be compared.

(3)位相比較器15の出力はLPF16によシ帝域制
限された制御電圧Vとなって電圧制御発振器(以下、V
COと記す)17を制御し、VCO17の出力は高域変
換回路11に入力され、ピーキング回路5を通って来た
再生輝度信号をVCO17の発振周波数によシ高域変換
する。
(3) The output of the phase comparator 15 becomes the control voltage V which is limited by the LPF 16, and the voltage controlled oscillator (hereinafter referred to as V
The output of the VCO 17 is input to a high-frequency conversion circuit 11, and the reproduced luminance signal that has passed through the peaking circuit 5 is high-frequency converted according to the oscillation frequency of the VCO 17.

VCO17の制御電圧Vは次のように表わされる。The control voltage V of the VCO 17 is expressed as follows.

y =x v0±ΔV ここで、vμ基準電位、lv は、ジッタ成分に相当す
る誤差電圧でおる。
y=x v0±ΔV Here, vμ reference potential, lv, is an error voltage corresponding to a jitter component.

VCO17は、第5図に示すようにリニアなり−f変換
器であシ、例えばv=V。の時、出力信号の周波数f 
fi f = f、 v = Vo+:jv の時、f
=fo±Δfとなる。ここで、foは標準状態における
高域変換周波数である。
The VCO 17 is a linear -f converter as shown in FIG. 5, for example, v=V. When , the frequency f of the output signal
When fi f = f, v = Vo+:jv, f
=fo±Δf. Here, fo is the high frequency conversion frequency in the standard state.

今、再生輝度信号の中心周波数をfY で表わすと、高
域変換回路11の出力の周波数は、f−1:fYとなる
。BPF12はfl=f+fY あるいはf、= f 
−fY の一方の周波数を有する信号を取り出し、取υ
山された信号は復調回路6により復調される。ここで、
実際の再生輝度信号はジッタを含み、この場合、再生輝
度信号の中心周波数fYはfy =fy。+、jf と
表わすことができる。
Now, if the center frequency of the reproduced luminance signal is represented by fY, the frequency of the output of the high frequency conversion circuit 11 will be f-1:fY. BPF12 is fl=f+fY or f,=f
Take out the signal with one frequency of -fY and take the signal υ
The peaked signal is demodulated by a demodulation circuit 6. here,
The actual reproduced luminance signal includes jitter, and in this case, the center frequency fY of the reproduced luminance signal is fy = fy. +, jf.

本発明のねらいは、VCO17の出力信号の周波数を±
lf 変動させるようなフィードバックループを形成し
て、上記のジッタ±jfを改善することにある。
The aim of the present invention is to adjust the frequency of the output signal of VCO 17 to ±
The purpose of this invention is to improve the above jitter ±jf by forming a feedback loop that varies lf.

以下に、復調信号として、BPF12で選択された周波
数f1を使う場合と、f、を使う場合に分けて説明する
In the following, a case where the frequency f1 selected by the BPF 12 is used and a case where the frequency f is used as the demodulated signal will be explained separately.

(1)fX−f+tアを使り場合、 fY=fYO±jf とすると、BPF12の出力信号
の周波#j、f1は次のようになる。
(1) When using fX-f+ta, if fY=fYO±jf, the frequencies #j and f1 of the output signal of the BPF 12 are as follows.

f、= f + fy= f + fyo±jfしたが
って、VCO17の出力周波数fがf=fO+−、il
f となるように制御をかければ、BPF12の出力信号の
周波数11は次のようになシ、ノックを補正できる。
f, = f + fy = f + fyo ± jf Therefore, the output frequency f of VCO 17 is f = fO + -, il
If control is applied so that the frequency 11 of the output signal of the BPF 12 becomes f, the knock can be corrected as follows.

f、=f眸jf +f工。±jf=f0+ fア。f, = f eye j f + f work. ±jf=f0+fa.

これは、すなわち、再生輝度信号の周波数fYが外乱等
によシ増加課は減少ルた時、VCO17の発振周波数f
を減少収は増加片せるよりに制御をかけることを意味す
る。
This means that when the frequency fY of the reproduced luminance signal increases due to disturbance etc., the oscillation frequency f of the VCO 17 decreases.
A decrease in yield means more control than an increase in yield.

なお、上記の各式に訃ける符号は復号同順である。下記
の各式においても同様である。
Note that the codes that appear in each of the above equations are decoded in the same order. The same applies to each formula below.

(2) f、= f −fY を使う場合fY””fY
o±If とすると、BPF12の出力信号の周波数1
2は次のようになる。
(2) When using f, = f − fY, fY””fY
o±If, the frequency 1 of the output signal of BPF12
2 becomes as follows.

f、=f−fY xf−fY0手If したがって、VCO17の出力周波数fがf=fo±Δ
f となるように制御をかければ、BPF12の出力信号の
周波数f、は次のようになシ、ジッタを補正できる。
f, =f-fY xf-fY0 If Therefore, the output frequency f of the VCO 17 is f=fo±Δ
If control is applied so that the frequency f of the output signal of the BPF 12 becomes f, the jitter can be corrected as follows.

b−f、f If −fYo乎Δf!fo−f、。b-f, f If -fYo乎Δf! fo-f,.

これは、すなわち、再生輝度信号の周波数fYが、外乱
等によシ増加(又は減少)した時、vC017の発振周
波afを増加(又は減少)させるように制御をかけるこ
とを意味する。
This means that when the frequency fY of the reproduced luminance signal increases (or decreases) due to disturbance or the like, control is applied to increase (or decrease) the oscillation frequency af of vC017.

実際のジッタの改善効果はフィードバンクルーズのルー
プゲインで決まシ±j4 のジッタは±Δf/(ループ
ゲイン)となる。
The actual jitter improvement effect is determined by the loop gain of the feed bank cruise, and the jitter of the signal ±j4 is ±Δf/(loop gain).

第6図は本発明の第2の実施例を示す。この実施例が第
4図の第1の実施例と異なる点は、第4図のピーキング
回路5とBPF12の代りに、1つのピーキング回路1
8が、高域変換回路11と復調器60間に存在する点で
ある。
FIG. 6 shows a second embodiment of the invention. This embodiment differs from the first embodiment shown in FIG. 4 by using one peaking circuit 1 instead of the peaking circuit 5 and BPF 12 shown in FIG.
8 is a point existing between the high frequency conversion circuit 11 and the demodulator 60.

本実施例のピーキング回路18としては、弾性表面波フ
ィルタ(以下、SAWフィルタと略す)を用いることが
できる。SAWフィルタの特性の一例を第7図に示す。
As the peaking circuit 18 of this embodiment, a surface acoustic wave filter (hereinafter abbreviated as SAW filter) can be used. FIG. 7 shows an example of the characteristics of the SAW filter.

第7図はFM輝度信号を約10皿工高域変換した場合の
特性の一例である。
FIG. 7 shows an example of the characteristics when the FM luminance signal is converted into a high frequency range by about 10 degrees.

SAWフィルタの群遅延特性19は、第7図がら明らか
なように、はぼ平坦である。また、SAWフィルタは所
望のゲイン特性20を得ることができる。
As is clear from FIG. 7, the group delay characteristic 19 of the SAW filter is almost flat. Further, the SAW filter can obtain desired gain characteristics 20.

したがって、高域変換回路11から出力された信号は、
SAWフィルタによって歪みを受けず、かつ所望のピー
キングを受けることができる。また、該SAWフィルタ
がBPFの働きをしていることは、該ゲイン特性20か
ら明らかであろう。
Therefore, the signal output from the high frequency conversion circuit 11 is
It is possible to receive desired peaking without being subjected to distortion by the SAW filter. Furthermore, it is clear from the gain characteristic 20 that the SAW filter functions as a BPF.

なお、高域変換輝度信号をピーキングする場合、LCフ
ィルタではQが取れなくなるが、SAWフィルタでは任
怠のQを得ることができる。また、SAWフィルタは、
弾性表面波の波長でそのサイズがほぼ決定され、扱う周
波数が高い程、小形かつ低コストになる。
Note that when peaking a high-frequency converted luminance signal, an LC filter cannot obtain a high Q, but a SAW filter can obtain a satisfactory Q. In addition, the SAW filter is
Its size is almost determined by the wavelength of the surface acoustic wave, and the higher the frequency it handles, the smaller it will be and the cost will be lower.

以上のよりに、本実施例によれば、第4図で示した第1
実施例のBPF12をピーキング回路18で兼用できる
という利点がある。また、本実施例は、ピーキング回路
18としてSAWフィルタを用いると、SAWフィルタ
が上記のような特性および特徴を有するので、特に効果
的である。
From the above, according to this embodiment, the first
There is an advantage that the peaking circuit 18 can also be used as the BPF 12 of the embodiment. Furthermore, this embodiment is particularly effective when a SAW filter is used as the peaking circuit 18 because the SAW filter has the characteristics and characteristics described above.

なお、本実施例において、高域変換輝度信号として、f
+f式=f1)を使う場合に必要なSAWフィルタの特
性が第7図のようであったとすると、高域変換輝i(i
号として、t −tY< −rt)を使う場合には、該
SAWフィルタの特性は、第8図のようにほぼ14 M
Hzで第7図の特性を軸対称とした特性にする必要があ
る。
In this example, f
If the characteristics of the SAW filter required when using +f formula = f1) are as shown in Figure 7, then the high-frequency conversion brightness i (i
When using t −tY< −rt) as the signal, the characteristics of the SAW filter are approximately 14 M as shown in FIG.
It is necessary to make the characteristics shown in FIG. 7 axially symmetrical at Hz.

上記した本発明の各実施例においては、基準信号発生器
13と位相比較器15との間にてい倍および分周回路1
4を設けたが、この回路14は、基準信号発生器13が
水平周波数を発生する場合は不要である。また、基準信
号発生器130周波 d数によっては、てい倍あるいは
分周回路の一方だけでよい場合もあることは勿論である
。さらに、基準信号発生器13として、カラー系で用い
られる3、58■hの水晶発振器などを用いてもよい。
In each of the embodiments of the present invention described above, a multiplier and frequency divider circuit 1 is provided between the reference signal generator 13 and the phase comparator 15.
4 is provided, but this circuit 14 is not necessary when the reference signal generator 13 generates a horizontal frequency. Furthermore, it goes without saying that depending on the frequency d of the reference signal generator 130, only one of a multiplier or a frequency divider circuit may be required. Further, as the reference signal generator 13, a 3.58 h crystal oscillator used in color systems may be used.

〔効 果〕〔effect〕

以上述べたように本発明では、高域変換に用いられるv
COの発振周波数が再生FM輝度信号のジッタを補正す
るような周波数変動を持つようにフィードバックをかけ
ているので、ジッタを減少させることができ、再生画面
の安定化および画質の向上に極めて大きな効果がある。
As described above, in the present invention, v
Feedback is applied so that the oscillation frequency of the CO has a frequency fluctuation that corrects the jitter of the reproduced FM luminance signal, so jitter can be reduced, which is extremely effective in stabilizing the reproduced screen and improving image quality. There is.

また高域変換後にSAWフィルタによシビーキ/グをか
ける構成とすると、群趙延特性の劣化を招くことがなく
、再生波形の歪を減少させることができるなどの効果が
大きい。
Furthermore, if the configuration is such that severe keying is applied to the SAW filter after high-frequency conversion, there is no deterioration of the waveform characteristics, and the distortion of the reproduced waveform can be reduced, which is a great effect.

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

第1図は輝度信号およびカラー信号のスペクトラム、第
2図は従来のFM輝度信号再生回路のブロック図、第3
図はジッタ補正回路を含む従来のFM輝度信号再生回路
のブロック図、第4図は本発明の第一の実施例を示すブ
ロック図、第5図はVCoのマーf変換特性図、第6図
は本発明の第二の実施例を示すブロック図、第7図およ
び第8図USAWフィルタの特性の一例を示す特性図で
ある。 11・・・高域変換回路、12・・・BPF、13・・
・基準信号発生器、14・・・てい倍および分周回路、
15−・・位相比較器、16 ・LPF、 17−VC
o。 1B−・−ビー#:yf回路、19 ・5AWf)i’
F !延時性、20・・・SAWのゲイン特性 代理人弁理士 平 木 道 人 第 1 図 第 2 図 士if 第3図 第 4 図 第 5 図 第 6 図
Figure 1 is the spectrum of the luminance signal and color signal, Figure 2 is a block diagram of a conventional FM luminance signal reproducing circuit, and Figure 3 is the spectrum of the luminance signal and color signal.
Figure 4 is a block diagram of a conventional FM luminance signal reproducing circuit including a jitter correction circuit, Figure 4 is a block diagram showing the first embodiment of the present invention, Figure 5 is a VCo mar-f conversion characteristic diagram, Figure 6 FIG. 7 is a block diagram showing a second embodiment of the present invention, and FIGS. 7 and 8 are characteristic diagrams showing an example of characteristics of the USAW filter. 11...High frequency conversion circuit, 12...BPF, 13...
・Reference signal generator, 14... multiplier and frequency divider circuit,
15--Phase comparator, 16-LPF, 17-VC
o. 1B-・-B#:yf circuit, 19・5AWf)i'
F! Time delay, 20...Gain characteristics of SAW Attorney Michihito Hiraki 1st figure 2 if figure 3 figure 4 figure 5 figure 6

Claims (4)

【特許請求の範囲】[Claims] (1)FM変調された輝度信号を再生する磁気再生装置
において、再生信号の周波数特性補正手段と、再生信号
を高域変換する手段と、高域変換信号を復調する手段と
、復調信号から同期信号を分離する手段と、該同期信号
を基準信号と位相比較する手段と、位相比較出力から制
御電圧を取9出すフィルタと、該制御電圧によシ発振周
波数が変化する電圧制御型発振器とを少くとも具備し、
該電圧制御型発振器の発振周波数を用いて前記再生信号
を高域変換し、かつ該電圧制御型発振器の発振周波数が
前記再生信号とはソ同じジッタ成分をもつようにフィー
ドバック制御をかけるようにしたことを特徴とする磁気
再生装置。
(1) In a magnetic reproducing device that reproduces an FM-modulated luminance signal, a means for correcting the frequency characteristics of the reproduced signal, a means for high-frequency conversion of the reproduced signal, a means for demodulating the high-frequency conversion signal, and synchronization from the demodulated signal. A means for separating signals, a means for comparing the phase of the synchronizing signal with a reference signal, a filter for extracting a control voltage from the phase comparison output, and a voltage-controlled oscillator whose oscillation frequency changes depending on the control voltage. Equipped with at least
The oscillation frequency of the voltage controlled oscillator is used to convert the reproduced signal to a high frequency, and feedback control is applied so that the oscillation frequency of the voltage controlled oscillator has the same jitter component as the reproduced signal. A magnetic reproducing device characterized by:
(2)前記再生信号の周波数をfY1前記電圧制御屋発
振器の発振周波数をfとし、前記復調手段に(f+fY
)の高域変換信号を入力するとき、該再生信号の周波数
fY が外乱等により増加(又は減少)した場合に、前
記電圧制御型発振器の発振周波数が減少(又は増加)す
るよりに制御をかけるようにしたことを特徴とする特許 第1項記載の磁気再生装置。
(2) The frequency of the reproduced signal is fY1, the oscillation frequency of the voltage controller oscillator is f, and the demodulation means (f+fY
), when the frequency fY of the reproduced signal increases (or decreases) due to disturbance etc., control is applied to prevent the oscillation frequency of the voltage controlled oscillator from decreasing (or increasing). 1. A magnetic reproducing device according to Patent No. 1, characterized in that:
(3)前記再生信号の周波数をfY1前記電圧制御戴発
振器の発振周波数をfとし、前記復調手段に(f−fY
)の高城変換信号を入力するとき、該再生信号の周波数
fYが外乱等によシ増加(又は減少)した場合に、前記
電圧制御型発振器の発振周波数が増加(又は減少)する
ように制御をかけるようにしたことを特徴とする前記特
許請求の範囲第1項記載の磁気再生装置。
(3) The frequency of the reproduced signal is fY1, the oscillation frequency of the voltage-controlled oscillator is f, and the demodulation means (f-fY
), when the frequency fY of the reproduced signal increases (or decreases) due to disturbance etc., control is performed so that the oscillation frequency of the voltage controlled oscillator increases (or decreases). 2. The magnetic reproducing device according to claim 1, wherein the magnetic reproducing device is configured such that the magnetic reproducing device has a magnetic reproducing device.
(4)高城変換後に弾性表面波フィルタを用いて再生信
号の周波数特性補正を行なうようにしたことを特徴とす
る請求範囲第1項記載の磁気再生装置。
(4) The magnetic reproducing apparatus according to claim 1, wherein the frequency characteristics of the reproduced signal are corrected using a surface acoustic wave filter after the Takagi transformation.
JP59022820A 1984-02-13 1984-02-13 Magnetic reproducing device Pending JPS60169286A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59022820A JPS60169286A (en) 1984-02-13 1984-02-13 Magnetic reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59022820A JPS60169286A (en) 1984-02-13 1984-02-13 Magnetic reproducing device

Publications (1)

Publication Number Publication Date
JPS60169286A true JPS60169286A (en) 1985-09-02

Family

ID=12093324

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59022820A Pending JPS60169286A (en) 1984-02-13 1984-02-13 Magnetic reproducing device

Country Status (1)

Country Link
JP (1) JPS60169286A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01318377A (en) * 1988-06-17 1989-12-22 Sharp Corp Time base correcting device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01318377A (en) * 1988-06-17 1989-12-22 Sharp Corp Time base correcting device

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