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JPS62150507A - Reproducing equalizer - Google Patents

Reproducing equalizer

Info

Publication number
JPS62150507A
JPS62150507A JP29535785A JP29535785A JPS62150507A JP S62150507 A JPS62150507 A JP S62150507A JP 29535785 A JP29535785 A JP 29535785A JP 29535785 A JP29535785 A JP 29535785A JP S62150507 A JPS62150507 A JP S62150507A
Authority
JP
Japan
Prior art keywords
signal
circuit
equalizer
limiter
supplied
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
JP29535785A
Other languages
Japanese (ja)
Inventor
Etsuro Sakamoto
悦朗 坂本
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP29535785A priority Critical patent/JPS62150507A/en
Publication of JPS62150507A publication Critical patent/JPS62150507A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To improve the S/N while preventing the occurrence of an inversion by supplying a reproduced high frequency signal to an addition/subtraction circuit additively via a delay circuit and supplying the signal to the addition/ subtraction circuit subtractingly via a nonlinear circuit. CONSTITUTION:An output of an equalizer 2 is supplied to an addition/ subtraction circuit 11 of a reproducing equalizer 10 via a main transmission line 5, a delay circuit 6 and a variable resistor 7 additively and supplied subtractingly via the 3rd transmission line comprising a limiter 12 as a nonlinear circuit, the 2nd variable resistor 13 and a low pass filter 14 and an output of the reproducing equalizer 10 is fed to a demodulator via a limiter 8. The threshold level of the limiter 12 is set higher than the level of an FM-RF signal when the modulation factor is large, a low side band SL in the FM-RF signal passing through the limiter 12 and the variable resistor 13 is fed to the addition/ subtraction circuit 11 via the low pass filter 14, the intensity of the low side band SL is suppressed to prevent the occurrence of the inversion. Thus, the S/N is improved further while preventing inversion.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はビデオテープレコーダの再生等化器に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a playback equalizer for a video tape recorder.

〔発明の概要〕[Summary of the invention]

本発明は、直接供給される再生RF信号と遅延回路を通
った再生RF信号とを加3E1.て、直線位相特性と傾
斜振幅特性を持たせると共に、非直線回路を通った再生
RF信号を減算するCとにより、再生RF信号の下側帯
波の強調度を高域変調信号の変調指数に応じて制御して
1反転現象を防止しながらいをより一層改善するように
し六ものでおる。
The present invention combines a directly supplied reproduced RF signal and a reproduced RF signal passed through a delay circuit with 3E1. By providing linear phase characteristics and slope amplitude characteristics, and subtracting the reproduced RF signal that has passed through the non-linear circuit, the degree of emphasis of the lower sideband of the reproduced RF signal is adjusted according to the modulation index of the high frequency modulation signal. In order to further improve the performance while preventing the single reversal phenomenon, we have achieved six results.

〔従来の技術〕[Conventional technology]

従来、ビデオテープレコーダ(以下VTRと略称する)
の再生系は1例えば第3図に示すように構成されていた
Conventionally, video tape recorders (hereinafter abbreviated as VTR)
The reproducing system was constructed as shown in FIG. 3, for example.

第3図において、(1)は通常複数とされる回転磁気ヘ
ッドを代表する再生磁気ヘッドであって、再生磁気ヘッ
ド(りの出力、即ち周波数変調された高周波信号(FM
−RF倍信号が、再生増幅器(図示を省略)及びイコラ
イザ(2)を介して、再生等化器(3)に供給される。
In FIG. 3, (1) is a reproducing magnetic head that is representative of a plurality of rotating magnetic heads, and the output of the reproducing magnetic head (i.e., a frequency-modulated high-frequency signal (FM
- The RF multiplied signal is supplied to a regenerative equalizer (3) via a regenerative amplifier (not shown) and an equalizer (2).

この阿生等化器(3)の加算回路(4)には、イコライ
ザ(2)の出力が主云送路(5)を介して直接に供給さ
れると共に、遅延時間τの遅延回路(6)及び可変抵抗
器(7)から成る副成送路を介して供給されて、位相特
性が線形とされると共に、振幅特性が直線傾斜の高域抑
圧形とされる。再生等化器(3)の出力がリミッタ(8
)に供給され、リミッタ(8)の出力が図示を省略した
復調回路に供給さ、れて、ビデオ信号に復調される。
The output of the equalizer (2) is directly supplied to the adder circuit (4) of this Ao equalizer (3) via the main transmission path (5), and a delay circuit (6) with a delay time τ is also supplied. ) and a variable resistor (7), the phase characteristic is made linear, and the amplitude characteristic is made into a high-frequency suppressing type with a linear slope. The output of the reproduction equalizer (3) is connected to the limiter (8
), and the output of the limiter (8) is supplied to a demodulation circuit (not shown), where it is demodulated into a video signal.

上述のようなVTRの再生系において、再生磁気ヘッド
(1)からの再生FM−RF fA号は、テープ・ヘッ
ド系の非直線性により、下側帯波が強調されると共に上
側帯波が抑圧されて、下側帯波に比べて、上側帯波のS
/Nが悪くなっている。しかも、この間の位相差は殆ど
差がない。
In the above-mentioned VTR playback system, the lower sideband is emphasized and the upper sideband is suppressed in the reproduced FM-RF fA signal from the readback magnetic head (1) due to the nonlinearity of the tape head system. Therefore, the S of the upper sideband wave is higher than that of the lower sideband wave.
/N is getting worse. Moreover, there is almost no phase difference between them.

ところで、ビデオ信号が黒レベルから白レベルへ急峻に
立上る場合、この立上シ部分にプリエンファシスによる
オーバーシュート(ス/臂イク)が生じ、この部分に対
応するFM−RF傷信号瞬時周波数は非常に高くなる。
By the way, when a video signal rises sharply from the black level to the white level, an overshoot occurs due to pre-emphasis at this rising part, and the instantaneous frequency of the FM-RF flaw signal corresponding to this part is becomes very expensive.

このFM−RF傷信号上述のようなテープ・ヘッド系を
含む伝送系を通過すると。
When this FM-RF flaw signal passes through a transmission system including the tape head system as described above.

スパイク対応部分の振幅が小さくなり、復調器の前段の
リミッタのスライス域をはずれてしまい、リミッタの出
力が欠落する、この欠落は復調器の入力FM−RF信号
の周波数が低くなったことと等価であり、OI調器出力
で黒レベルの信号となる。
The amplitude of the spike-corresponding part becomes smaller and falls outside the slice range of the limiter in the front stage of the demodulator, resulting in a loss of output from the limiter. This loss is equivalent to a lower frequency of the FM-RF signal input to the demodulator. The OI modulator output becomes a black level signal.

この反転現象発生時、 RF信号波形はスパイク対応部
分の零クロス点が欠落している。また、このときのFM
−RF傷信号、第4図の瞬時ベクトル図に示すように、
搬送波C及び上側帯波SUに比べて。
When this reversal phenomenon occurs, the RF signal waveform lacks the zero-crossing point in the spike-corresponding part. Also, the FM at this time
-RF flaw signal, as shown in the instantaneous vector diagram in Figure 4,
Compared to carrier C and upper sideband SU.

下側帯波SLの振幅が大きくなっており、この下側帯波
SLが搬送波C(及び上側帯波SU)と180°近傍の
位相差となる場合、3者を合成しfcRF信号が負の振
幅を有することになる。
If the amplitude of the lower sideband wave SL is large and the phase difference between the lower sideband wave SL and the carrier wave C (and the upper sideband SU) is close to 180°, the fcRF signal will have a negative amplitude by combining the three. will have.

上述のような反転現象の対策として、従来のVTRの再
生系では、イコライザ(2)により、上下側帯波SU及
びSLのレベルを等しくシた後、再生等化器(3)によ
って、S/Nの悪い上側帯波S、Jを抑圧(下側帯波S
Lを強調)してから復調することによシ。
As a countermeasure against the above-mentioned inversion phenomenon, in the conventional VTR playback system, the equalizer (2) equalizes the levels of the upper and lower sidebands SU and SL, and then the playback equalizer (3) adjusts the S/N. Suppresses bad upper sideband waves S and J (lower sideband S
(emphasizes L) and then demodulates.

総合S/Nを劣化させることなく、反転現象を防止して
いた。
The inversion phenomenon was prevented without deteriorating the overall S/N.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ところが、 VTRのFM−RF傷信号、周知のように
、搬送波C並びに両側帯波S。及びSLの振幅が、m′
!!:変調指数として、それぞれ0次並びに1次のベッ
セル函数J0(rr+)並びにJ 、(m)及びJ−1
(m)で表わされる。
However, as is well known, the FM-RF flaw signal of a VTR is a carrier wave C and both side band waves S. and the amplitude of SL is m′
! ! :0th and 1st order Bessel functions J0(rr+) and J, (m) and J-1 as modulation indices, respectively
(m).

そして、上述のビデオ信号の立」ニジ部分のように。And like the above-mentioned part of the video signal.

高域の変調信号のレベルが大きい場合、変調指数処が犬
きくなって、両側帯波SU及びSLの振幅が増大すると
共に、搬送波Cの振幅が減少する。
When the level of the high-frequency modulation signal is large, the modulation index becomes sharper, the amplitudes of both sideband waves SU and SL increase, and the amplitude of the carrier wave C decreases.

このため、従来の下側帯波強調型の再生等化器では、高
域変調信号による変調指数が大きくなるにつれて、その
出力の搬送波及び両側帯波の振幅が第4図に示したよう
な相対関係に近付いて、反転現象が発生し易くなる。従
って、従来の再生等化器では、下側帯波の強調度が制限
され、これに伴って、S/N改善度も制限されてしまう
という問題があった。
For this reason, in the conventional lower sideband emphasizing type regenerative equalizer, as the modulation index by the high frequency modulation signal increases, the amplitudes of the carrier wave and both sidebands of the output will have a relative relationship as shown in Figure 4. , the reversal phenomenon becomes more likely to occur. Therefore, in the conventional regenerative equalizer, there is a problem in that the degree of emphasis of the lower sideband is limited, and accordingly, the degree of S/N improvement is also limited.

かかる点に鑑み、本発明の目的は、反転現象の発生を防
止しながら、 S/Nをよシ一層改善した再生等化器を
提供するところにあ2)。
In view of this, an object of the present invention is to provide a regenerative equalizer that further improves the S/N ratio while preventing the occurrence of the inversion phenomenon2).

〔問題点を解決するための手段〕[Means for solving problems]

本発明は、再生高周波信号がDW接に供給される加減算
回路と、遅延回路と、非直線回路とを有し。
The present invention includes an addition/subtraction circuit to which a reproduced high-frequency signal is supplied to the DW terminal, a delay circuit, and a nonlinear circuit.

再生高周波信号が遅延回路を介し、て加減算回路に加算
的に供給されると共に、再生高周波信号が非直線回路を
介して加減算回路に減算的に供給されるようにした再生
等化器である。
This is a regenerative equalizer in which a reproduced high-frequency signal is additively supplied to an adder/subtractor circuit via a delay circuit, and a reproduced high-frequency signal is subtractively supplied to an adder/subtracter circuit via a non-linear circuit.

〔作用〕[Effect]

かかる構成によれば、高域変調信号による再生高周波信
号の変調指数に応じて、下側帯波の強調度が変化し、反
転現象が防止されると共に、S/Nがより一層改善され
る。
According to this configuration, the degree of emphasis of the lower sideband changes according to the modulation index of the reproduced high-frequency signal by the high-frequency modulation signal, preventing the inversion phenomenon and further improving the S/N.

〔実施例〕 以下、第1図及び第2図を参照しながら、本発明による
再生等化器の一実施例について説明する。
[Embodiment] An embodiment of the regenerative equalizer according to the present invention will be described below with reference to FIGS. 1 and 2.

本発明の一実施例の構成を第1図に示す。この第1図に
おいて、第3図に対応する部分には同一の符号を付して
重複説明を省略する。
FIG. 1 shows the configuration of an embodiment of the present invention. In FIG. 1, parts corresponding to those in FIG. 3 are designated by the same reference numerals and redundant explanation will be omitted.

第1図において、再生等化器αQの加減算回路α◇には
、イコライザ(2)の出力が、主伝送路(5)並びに遅
延回路(6)及び可変抵抗器(7)を介して、加算的に
供給されると共に、非直線回路としてのリミッタ(6)
、第2の可変抵抗器(至)及び低域フィルタα→から成
る第3の伝送路を介して減算的に供給される。
In Fig. 1, the output of the equalizer (2) is added to the addition/subtraction circuit α◇ of the regenerative equalizer αQ via the main transmission path (5), delay circuit (6), and variable resistor (7). limiter (6) as a non-linear circuit.
, a second variable resistor (to) and a low-pass filter α→.

この再生等化器αQの出力が、リミッタ(8)を介して
The output of this regenerative equalizer αQ is passed through a limiter (8).

図示を省略した復調器に供給される。The signal is supplied to a demodulator (not shown).

なお、低域フィルタ04の遮断特性はFM−RF倍信号
搬送波周波数を中心として点対称となるような緩傾斜で
あることが好ましい。
Note that it is preferable that the cutoff characteristic of the low-pass filter 04 has a gentle slope that is point symmetrical about the FM-RF multiplied signal carrier frequency.

次に、第2図をも参照しながら1本実施例の動作につい
て説明する。
Next, the operation of this embodiment will be explained with reference to FIG.

再生FM−RF倍信号小振幅の場合、可変抵抗器(7)
及び(至)の伝送係数をα7及びα13として、再生等
化器叫の振幅特性A((ロ)は次の(1)式のように表
わされる。
For small amplitude reproduced FM-RF multiplied signal, variable resistor (7)
Letting the transmission coefficients of and (to) be α7 and α13, the amplitude characteristic A ((b) of the reproduced equalizer signal is expressed as the following equation (1).

本実施例において対象とするJi’M−RF倍信号振幅
が小さくなるのは、前述のように、高域変調信号による
変調指数mが大きい場合であって、再生等化器α1の入
力側のFM−RF 9号は、第2図Aに示すように、両
側帯波SU及びSLの振幅が大きく、搬送波Cの振幅が
小さくなって、反転現象の発生に対する余裕度が小さい
。このため、本実施例においては、リミッタ(2)のス
レショルドレベルが変調指数が大きい場合のFM−RF
倍信号レベルよpも高く設定され、リミッタ(2)及び
可変抵抗器α3を通過しfCFM−RF傷信号中下側帯
波SLが低域フィルタα棒を通って加減算回路α溌に供
給され、前出(1)式に従って、下側帯波SLの強調度
が抑えられ1反転現象の発生が防止される。
In this embodiment, the target Ji'M-RF signal amplitude becomes small when the modulation index m by the high-frequency modulation signal is large, and the amplitude of the Ji'M-RF multiplied signal becomes small as described above. In FM-RF No. 9, as shown in FIG. 2A, the amplitudes of both sideband waves SU and SL are large, and the amplitude of the carrier wave C is small, so that there is little margin for occurrence of an inversion phenomenon. Therefore, in this embodiment, the threshold level of the limiter (2) is set to FM-RF when the modulation index is large.
P is also set higher than the double signal level, and the middle lower sideband wave SL of the fCFM-RF flaw signal passes through the limiter (2) and variable resistor α3, and is supplied to the adder/subtractor circuit α through the low-pass filter α rod, and then According to equation (1), the degree of emphasis of the lower sideband wave SL is suppressed and the occurrence of the 1-inversion phenomenon is prevented.

逆に、FM−RF倍信号振幅が大きくなるのは、高域変
調信号による変調指数が小さい場合であって。
Conversely, the FM-RF multiplied signal amplitude becomes large when the modulation index by the high frequency modulation signal is small.

再生等化器αQの入力側の信号は、第2図Bに実線で示
すように、両搬送波SU及びSLの振幅が小さく。
In the signal on the input side of the regenerative equalizer αQ, as shown by the solid line in FIG. 2B, the amplitudes of both carrier waves SU and SL are small.

搬送波Cの振幅が大きくなって、反転現象の発生に対す
る余裕度が大きい。
Since the amplitude of the carrier wave C becomes large, there is a large margin for occurrence of an inversion phenomenon.

上述のようなリミッタ(6)のスレショルドレベルはこ
の場合のFM−RF倍信号レベルよりも低くなシ、リミ
ッタ(6)から低域フィルタ(14までの第3の伝送路
を介して加減算回路C1,)に供給される下側帯波SL
の相対値が減少する。これは前出(1)式におQするα
15の減少と等価であって、F’M−RF倍信号レベル
がリミッタ(6)のスレショルドレベルを超える場合は
、第2図Bに破線で示すように、反転現象の発生に対し
て余裕を保ちながら、′F側帯波Sl、liを強調する
ことができて、汐をより一層改善することができる。
The threshold level of the limiter (6) as described above is lower than the FM-RF multiplied signal level in this case. , ) is supplied to the lower sideband SL
The relative value of decreases. This is α, which is Q to equation (1) above.
If the F'M-RF multiplied signal level exceeds the threshold level of the limiter (6), as shown by the broken line in Figure 2B, there is a margin for the occurrence of the inversion phenomenon. It is possible to emphasize the 'F sideband waves Sl and li while maintaining the same, and it is possible to further improve the tide.

以上の説明では、再生等化器(10の特性を制御するた
めにリミッタ(6)を用い穴が、圧縮回路、対数増幅回
路のような非直線回路を使用することもできる。
In the above description, the limiter (6) is used to control the characteristics of the regenerative equalizer (10), but a non-linear circuit such as a compression circuit or a logarithmic amplification circuit may also be used.

〔発明の効果〕〔Effect of the invention〕

以上詳述のように、本発明によれば、高域変調信号によ
る変調指数に応じて、再生U信号の下側帯波の強調度を
制御することができて、反転現象を防止しながら、S/
Nをより 一層改善することのできる再生等化器が得ら
れる。
As described in detail above, according to the present invention, it is possible to control the degree of emphasis of the lower sideband of the reproduced U signal according to the modulation index of the high frequency modulation signal, and to prevent the inversion phenomenon while /
A regenerative equalizer that can further improve N is obtained.

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

第1図は本発明による再生等化器の一実施例の構成を示
すブロック図、第2図tよ第1図の実施例の動作を説明
するためのベクトル図、第3図は従来の再生等化器の構
成例を示すブロック図、第4図は本発明の説明に供する
ベクトル図である。 (3)及びαQは再生等化器、(6ンは遅延回路、αη
は加減算回路、(6)はlJミッタ(非直線回路)であ
る。
FIG. 1 is a block diagram showing the configuration of an embodiment of a regenerative equalizer according to the present invention, FIG. 2 is a vector diagram for explaining the operation of the embodiment of FIG. FIG. 4 is a block diagram showing an example of the configuration of the equalizer, and is a vector diagram for explaining the present invention. (3) and αQ are regenerative equalizers, (6 is a delay circuit, αη
is an addition/subtraction circuit, and (6) is an lJ mitter (nonlinear circuit).

Claims (1)

【特許請求の範囲】 再生高周波信号が直接に供給される加減算回路と、遅延
回路と、非直線回路とを有し、 上記再生高周波信号が上記遅延回路を介して上記加減算
回路に加算的に供給されると共に、上記再生高周波信号
が上記非直線回路を介して上記加減算回路に減算的に供
給されるようにしたことを特徴とする再生等化器。
[Claims] An adder/subtractor circuit to which a reproduced high-frequency signal is directly supplied, a delay circuit, and a non-linear circuit, wherein the reproduced high-frequency signal is additively supplied to the adder/subtracter circuit via the delay circuit. and the reproduced high-frequency signal is subtractively supplied to the addition/subtraction circuit via the non-linear circuit.
JP29535785A 1985-12-25 1985-12-25 Reproducing equalizer Pending JPS62150507A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29535785A JPS62150507A (en) 1985-12-25 1985-12-25 Reproducing equalizer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29535785A JPS62150507A (en) 1985-12-25 1985-12-25 Reproducing equalizer

Publications (1)

Publication Number Publication Date
JPS62150507A true JPS62150507A (en) 1987-07-04

Family

ID=17819569

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29535785A Pending JPS62150507A (en) 1985-12-25 1985-12-25 Reproducing equalizer

Country Status (1)

Country Link
JP (1) JPS62150507A (en)

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