JPH0117288B2 - - Google Patents
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- Publication number
- JPH0117288B2 JPH0117288B2 JP56124909A JP12490981A JPH0117288B2 JP H0117288 B2 JPH0117288 B2 JP H0117288B2 JP 56124909 A JP56124909 A JP 56124909A JP 12490981 A JP12490981 A JP 12490981A JP H0117288 B2 JPH0117288 B2 JP H0117288B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- delay
- output
- amplitude
- circuit
- 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
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Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04L—TRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION
- H04L25/00—Baseband systems
- H04L25/02—Details ; arrangements for supplying electrical power along data transmission lines
- H04L25/03—Shaping networks in transmitter or receiver, e.g. adaptive shaping networks
- H04L25/03006—Arrangements for removing intersymbol interference
- H04L25/03012—Arrangements for removing intersymbol interference operating in the time domain
- H04L25/03114—Arrangements for removing intersymbol interference operating in the time domain non-adaptive, i.e. not adjustable, manually adjustable, or adjustable only during the reception of special signals
- H04L25/03133—Arrangements for removing intersymbol interference operating in the time domain non-adaptive, i.e. not adjustable, manually adjustable, or adjustable only during the reception of special signals with a non-recursive structure
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Filters That Use Time-Delay Elements (AREA)
- Filters And Equalizers (AREA)
- Cable Transmission Systems, Equalization Of Radio And Reduction Of Echo (AREA)
Description
【発明の詳細な説明】
この発明は、信号波形の等化を行う波形等化器
に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a waveform equalizer that equalizes signal waveforms.
第1図は本件発明者の開発になる、余弦形の群
遅延特性を周波数軸上で水平方向に所望量ずらせ
ることができる波形等化器を示している。図にお
いて、1は入力端子、2はこの入力端子1に入力
された信号を分岐して出力する分岐回路、3は該
分岐回路2により分岐された信号の位相を90゜回
転する90°移相器、4a〜4dは入力信号を所定
時間T(秒)だけ遅延させて出力する遅延回路、
5は該遅延された信号の位相を反転して出力する
インバータ、6aは上記分岐回路2の出力とイン
バータ5の出力を加算する加算器、6bは90゜移
相器3の出力と遅延回路4dの出力とを加算する
加算器、7a,7bはこの加算器6a,6bのそ
れぞれの出力振幅を調整する振幅調整回路、6c
は該両振幅調整回路7a,7bの出力および遅延
回路4aの出力を加算する加算器、8はその出力
端子である。 FIG. 1 shows a waveform equalizer developed by the inventor of the present invention that can shift the cosine group delay characteristic by a desired amount in the horizontal direction on the frequency axis. In the figure, 1 is an input terminal, 2 is a branching circuit that branches the signal input to this input terminal 1 and outputs it, and 3 is a 90° phase shifter that rotates the phase of the signal branched by the branching circuit 2 by 90°. 4a to 4d are delay circuits that delay the input signal by a predetermined time T (seconds) and output the delayed signal;
5 is an inverter that inverts the phase of the delayed signal and outputs it; 6a is an adder that adds the output of the branch circuit 2 and the output of the inverter 5; 6b is the output of the 90° phase shifter 3 and the delay circuit 4d 7a and 7b are amplitude adjustment circuits that adjust the respective output amplitudes of the adders 6a and 6b; 6c;
is an adder that adds the outputs of both amplitude adjustment circuits 7a and 7b and the output of the delay circuit 4a, and 8 is its output terminal.
なお、上記回路4a,4b,5,6aにより、
上記第1の分岐回路2の出力の一方を時間Tだけ
遅延した主信号と、上記出力とこれを2Tだけ遅
延した反転信号とを加算した加算エコー信号とを
作成する第1の遅延回路網10aを構成してお
り、また上記回路4c,4d,6bにより、上記
移相器3の出力から加算エコー信号を作成する第
2の遅延回路網10bを構成している。 Note that the circuits 4a, 4b, 5, and 6a allow
A first delay circuit network 10a that creates a main signal obtained by delaying one of the outputs of the first branch circuit 2 by a time T, and an added echo signal obtained by adding the above output and an inverted signal obtained by delaying this by 2T. The circuits 4c, 4d, and 6b constitute a second delay circuit network 10b that creates an added echo signal from the output of the phase shifter 3.
次に、動作について説明する。ただし、任意の
信号波形は極めて細いパルスの線型和として表わ
せるので、以下、この極めて細いパルスを入力信
号として取り扱うことにする。 Next, the operation will be explained. However, since any signal waveform can be expressed as a linear sum of extremely thin pulses, we will treat these extremely thin pulses as input signals below.
入力端子1に入力された信号は分岐回路2によ
り2つに分けられ、一方は90゜移相器3を介して、
それぞれ所定の遅延時間Tをもち、信号の減衰を
生じない遅延回路4c,4dに入力される。上記
分岐回路2の出力の他方は、直接遅延回路4a,
4bに入力される。 The signal input to the input terminal 1 is divided into two by the branch circuit 2, and one is sent through the 90° phase shifter 3.
Each signal has a predetermined delay time T and is input to delay circuits 4c and 4d that do not cause signal attenuation. The other output of the branch circuit 2 is a direct delay circuit 4a,
4b.
従つて、上記加算器6aに入力される信号は、
遅延時間ゼロの信号と、遅延時間2Tをもちイン
バータ5によつて位相反転された信号とであり、
該2つの信号が加算された後、振幅調整回路7a
によつて振幅調整され、加算器6cの1つの入力
信号となる。同様に、加算器6bの入力信号とし
ては遅延時間ゼロの信号と遅延時間2Tの信号と
があり、該2つの信号が加算された後、振幅調整
回路7bによつて振幅調整されて加算器6cの1
つの入力信号となる。更に、加算器6cの入力信
号としては、上記のものの他に遅延回路4aのみ
を通ることにより時間Tだけ遅延された信号もあ
り、これは振幅調整されることなく、直接加算器
6cに入力される。以下、この信号を主信号と呼
び、振幅調整回路7a,7bを通過した信号を反
響信号(エコー信号)と呼ぶ。そして、上記加算
器6cで加算された信号は出力端子8から出力さ
れる。 Therefore, the signal input to the adder 6a is:
A signal with a delay time of zero, and a signal with a delay time of 2T whose phase is inverted by the inverter 5.
After the two signals are added, the amplitude adjustment circuit 7a
The amplitude is adjusted by , and becomes one input signal of the adder 6c. Similarly, the input signals of the adder 6b include a signal with a delay time of zero and a signal with a delay time of 2T, and after the two signals are added, the amplitude is adjusted by the amplitude adjustment circuit 7b, and the signal is input to the adder 6c. No. 1
This results in two input signals. Furthermore, in addition to the above input signals to the adder 6c, there is also a signal delayed by a time T by passing only through the delay circuit 4a, and this signal is directly input to the adder 6c without amplitude adjustment. Ru. Hereinafter, this signal will be referred to as a main signal, and the signal that has passed through the amplitude adjustment circuits 7a and 7b will be referred to as an echo signal. The signals added by the adder 6c are output from the output terminal 8.
いま、主信号の振幅を1で正規化し、振幅調整
回路7a,7bによつて調整された振幅値(以下
タツプ係数と呼ぶ)をそれぞれkcosθ0,ksinθ0と
する。ただし、k,θ0は定数であり、kはエコー
信号と主信号との振幅比、θ0は余弦形特性を基準
として周波数軸上で本波形等化器の群遅延又は振
幅特性を水平方向にずらせる量である。 Now, the amplitude of the main signal is normalized by 1, and the amplitude values (hereinafter referred to as tap coefficients) adjusted by the amplitude adjustment circuits 7a and 7b are defined as kcos θ 0 and ksin θ 0 , respectively. However, k and θ 0 are constants, k is the amplitude ratio of the echo signal and the main signal, and θ 0 is the group delay or amplitude characteristic of this waveform equalizer on the frequency axis in the horizontal direction with the cosine characteristic as the reference. This is the amount by which it can be shifted.
この時、等化器全体の伝達関数F1(ω)(ω=
2πf)は、
F1(ω)=1−j2ksin(ωT−θ0) (1)
となり、k≪1のとき振幅及び群遅延特性G1
(ω),τ1(ω)はそれぞれ
となる。 At this time, the transfer function of the entire equalizer F 1 (ω) (ω=
2πf) is F 1 (ω)=1−j2ksin(ωT−θ 0 ) (1), and when k≪1, the amplitude and group delay characteristics G 1
(ω) and τ 1 (ω) are respectively becomes.
この時の特性を第2図a,bに示す。この図か
らわかるように、同図aの振幅特性は不変のまま
として同図b破線の余弦形の群遅延特性のみを任
意の周波数θ0/Tだけ水平方向、即ち周波数方向
にずらして実線の特性とすることができ、この等
化器により群遅延の等化を行うことができる。 The characteristics at this time are shown in Figures 2a and b. As can be seen from this figure, while the amplitude characteristic in figure a remains unchanged, only the cosine-shaped group delay characteristic indicated by the broken line in figure b is shifted by an arbitrary frequency θ 0 /T in the horizontal direction, that is, in the frequency direction. This equalizer can perform group delay equalization.
第3図はこの時の時間領域の波形を示す。図に
おいて、aは振幅調整回路7aの出力信号、bは
主信号、cは振幅調整回路7bの出力信号であ
り、上記信号a,bは同相であり、信号cは上記
両信号a,bと90゜の位相差をもつている。 FIG. 3 shows the time domain waveform at this time. In the figure, a is the output signal of the amplitude adjustment circuit 7a, b is the main signal, and c is the output signal of the amplitude adjustment circuit 7b. The signals a and b are in phase, and the signal c is the same as both the signals a and b. It has a phase difference of 90°.
第1図の等化器は以上のように構成されている
ので、波形歪が小さい場合は等化器のタツプ係数
が小さくてすみ、遅延等化を行つても振幅歪を生
ずることはないが、波形歪が大きい場合は(2)式右
辺の近似式が成り立たなくなるため、遅延等化を
行うと振幅歪が発生し、振幅と群遅延の独立性が
保たれず、調整時における収束性が悪いという欠
点があつた。 The equalizer in Figure 1 is configured as described above, so if the waveform distortion is small, the tap coefficient of the equalizer can be small, and even if delay equalization is performed, amplitude distortion will not occur. If the waveform distortion is large, the approximation on the right side of equation (2) no longer holds true, so when delay equalization is performed, amplitude distortion occurs, the independence of amplitude and group delay is not maintained, and the convergence during adjustment is impaired. It had the drawback of being bad.
この発明は上記のような従来のものの欠点を除
去するためになされたもので、遅延等化部により
遅延等化した後の信号を振幅歪補正部に入力し、
かつ振幅歪補正部のタツプ係数と遅延等化部のタ
ツプ係数とに一定の関係をもたせることによつ
て、等化すべき波形の群遅延歪が大きい場合でも
振幅と群遅延の独立性を完全に保つことのできる
波形等化器を提供することを目的としている。 This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and a signal after delay equalization by a delay equalization section is input to an amplitude distortion correction section,
In addition, by establishing a certain relationship between the tap coefficient of the amplitude distortion correction section and the tap coefficient of the delay equalization section, the independence of amplitude and group delay can be completely ensured even when the group delay distortion of the waveform to be equalized is large. The purpose is to provide a waveform equalizer that can maintain
以下、この発明の一実施例を図について説明す
る。 An embodiment of the present invention will be described below with reference to the drawings.
第4図は本発明の一実施例による波形等化器を
示し、図において、10は従来の波形等化器と全
く同一の構成になる遅延等化部、20はこの遅延
等化部10に付加した振幅歪補正部であり、該振
幅歪補正部20の回路要素1b,2b,3b,4
e〜4h,5b,6d〜6f,7c,7d,8b
は遅延等化部10内の対応する回路要素とほとん
ど同一のものである。但しこの振幅歪補正部20
においてはインバータ5bは90゜移相器3bによ
つて位相回転されたエコー信号の側に組み込まれ
ており、また遅延回路4e〜4hの遅延時間は
各々2Tに設定されている。 FIG. 4 shows a waveform equalizer according to an embodiment of the present invention. In the figure, 10 is a delay equalizer having exactly the same configuration as a conventional waveform equalizer, and 20 is a delay equalizer 10. It is an added amplitude distortion correction section, and the circuit elements 1b, 2b, 3b, 4 of the amplitude distortion correction section 20 are
e~4h, 5b, 6d~6f, 7c, 7d, 8b
are almost the same as the corresponding circuit elements in the delay equalizer 10. However, this amplitude distortion correction section 20
In this case, the inverter 5b is installed on the side of the echo signal whose phase has been rotated by the 90° phase shifter 3b, and the delay times of the delay circuits 4e to 4h are each set to 2T.
なお上記回路4e,4f,6dにより、上記第
2の分岐回路2bの出力の一方を時間2Tだけ遅
延した主信号と、上記出力とこれを4Tだけ遅延
した信号とを加算した加算エコー信号とを作成す
る第3の遅延回路網20aを構成しており、また
上記回路4g,4h,5b,6eにより、上記移
相器3bの出力から加算エコー信号を作成する第
4の遅延回路網20bを構成している。 Note that the circuits 4e, 4f, and 6d generate a main signal obtained by delaying one of the outputs of the second branch circuit 2b by a time of 2T, and an added echo signal obtained by adding the above output and a signal delayed by 4T. The circuits 4g, 4h, 5b, and 6e constitute a fourth delay circuit network 20b to create an added echo signal from the output of the phase shifter 3b. are doing.
次に、上記のように構成された波形等化器の動
作について、第4図及び第5図を参照して説明す
る。 Next, the operation of the waveform equalizer configured as described above will be explained with reference to FIGS. 4 and 5.
遅延等化部10の出力における振幅及び群遅延
特性を各々G2(ω)、τ2(ω)とすると、これらは
遅延等化部10が従来回路と全く同一の構成であ
るから、(2)式と全く同一の式で、
となる。(3)式からわかるように、振幅歪は−cos2
(ωT−θ0)の形をとることがわかる。 Assuming that the amplitude and group delay characteristics at the output of the delay equalizer 10 are G 2 (ω) and τ 2 (ω), respectively, these are (2 ) is exactly the same as the formula, becomes. As can be seen from equation (3), the amplitude distortion is −cos2
It can be seen that it takes the form (ωT−θ 0 ).
次に振幅歪補正部20の入力端子1bに入力さ
れた遅延等化部10からの信号は、分岐回路2b
によつて2つに分けられ、その一方は90゜移相器
3bに入力された後遅延時間2Tをもち信号の減
衰を生じない遅延回路4g,4hに加えられ、他
方は直接遅延時間2Tをもつ遅延回路4e,4f
に印加される。従つて、加算器6dに入力される
信号は遅延時間ゼロの信号と、遅延時間4Tを持
つ信号であり、これら2つの信号が加算された
後、振幅調整回路7cによつてその出力振幅が
acos2θ0となるよう調整され、加算器6fの入力
信号の1つとなる。同様に、加算器6eに入力す
る信号は、90゜移相器3bを通過した遅延時間ゼ
ロの信号と、遅延時間4Tをもちインバータ5b
によつて位相反転された信号であり、この2つの
信号が加算された後、振幅調整回路7dによつて
その出力振幅がasin2θ0となるよう調整されて加
算器6fの入力の1つとなる。更に、加算器6f
の入力信号としては遅延回路4eのみを通つた遅
延時間2Tを持つ信号があり、これは、振幅調整
されることなく正規化振幅1で直接加算器6fに
入力される。 Next, the signal from the delay equalization section 10 inputted to the input terminal 1b of the amplitude distortion correction section 20 is sent to the branch circuit 2b.
One of them is input to the 90° phase shifter 3b and then added to the delay circuits 4g and 4h which have a delay time of 2T and do not cause signal attenuation, and the other has a delay time of 2T directly. Delay circuits 4e, 4f with
is applied to Therefore, the signals input to the adder 6d are a signal with a delay time of zero and a signal with a delay time of 4T. After these two signals are added, the output amplitude is adjusted by the amplitude adjustment circuit 7c.
It is adjusted so that acos2θ 0 , and becomes one of the input signals of the adder 6f. Similarly, the signal input to the adder 6e is a signal with zero delay time that has passed through the 90° phase shifter 3b, and a signal that has a delay time of 4T and is input to the inverter 5b.
After these two signals are added, the amplitude adjustment circuit 7d adjusts the output amplitude to be asin2θ 0 , and becomes one of the inputs of the adder 6f. Furthermore, adder 6f
As an input signal, there is a signal having a delay time 2T that has passed only through the delay circuit 4e, and is directly inputted to the adder 6f with a normalized amplitude of 1 without amplitude adjustment.
従つて、振幅歪補正部20の伝達関数をF3
(ω)とすると、
F3(ω)=1+2acos2(ωT−θ0) (4)
となり、振幅及び群遅延特性G3(ω),τ3(ω)は
それぞれ、
G3(ω)=20log10〔1+2acos2(ωT−θ0)〕
τ3(ω)=O(dB)
(秒) (5)
となる。 Therefore, the transfer function of the amplitude distortion correction section 20 is F 3
(ω), then F 3 (ω) = 1 + 2 a cos2 (ωT - θ 0 ) (4), and the amplitude and group delay characteristics G 3 (ω) and τ 3 (ω) are respectively G 3 (ω) = 20log 10 [1+2acos2(ωT−θ 0 )] τ 3 (ω)=O(dB) (seconds) (5).
即ち、振幅歪補正部20の特性は、群遅延特性
は平担で、振幅特性のみが余弦形に変化すること
がわかる。 That is, it can be seen that the characteristics of the amplitude distortion correction section 20 are that the group delay characteristic is flat and only the amplitude characteristic changes in a cosine shape.
従つて、第4図に示した遅延等化部と振幅歪補
正部とを縦続接続することによつて振幅歪を補正
する場合には、(3)式と(5)式の振幅特性を比較する
ことにより、a=k2/2とした場合に最も振幅歪
が少なくなることがわかる。 Therefore, when correcting amplitude distortion by cascading the delay equalization section and the amplitude distortion correction section shown in Fig. 4, it is necessary to compare the amplitude characteristics of equations (3) and (5). It can be seen that the amplitude distortion is minimized when a=k 2 /2.
この時、第4図全体の振幅特性Gt(ω)は、
Gt(ω)≒10log10〔1+2k2+k4cos2(ωT−θ0)・
{1−3cos2(ωT−θ0)}〕(dB)(6)
となり、振幅歪の項はk4以上の高次項となつて、
振幅歪はきわめて小さくなる。 At this time, the amplitude characteristic Gt(ω) of the entire Figure 4 is Gt(ω)≒10log 10 [1+2k 2 +k 4 cos2(ωT−θ 0 )・
{1−3cos2(ωT−θ 0 )}](dB)(6), and the amplitude distortion term becomes a higher order term of k4 or higher,
Amplitude distortion becomes extremely small.
このようにa=k2/2としたときの第4図の回
路の各種の周波数特性を第5図に示す。即ち、同
図aは遅延等化部10の群遅延特性を、図bは遅
延等化部10に発生する振幅歪を、図cは振幅歪
補正部20における振幅特性を、図dは上記遅延
等化部10と上記振幅歪補正部20とを縦続接続
した時の総合の振幅特性をそれぞれ示す。 FIG. 5 shows various frequency characteristics of the circuit shown in FIG. 4 when a=k 2 /2. That is, Figure a shows the group delay characteristic of the delay equalizer 10, Figure b shows the amplitude distortion generated in the delay equalizer 10, Figure c shows the amplitude characteristic in the amplitude distortion corrector 20, and Figure d shows the above delay. The overall amplitude characteristics when the equalization section 10 and the amplitude distortion correction section 20 are connected in cascade are shown.
但し、同図において、破線は周波数軸方向のず
れが零(すなわちθ0=0)の場合であり、実線は
一般の場合(θ0≠0)を示している。 However, in the figure, the broken line indicates the case where the deviation in the frequency axis direction is zero (ie, θ 0 =0), and the solid line indicates the general case (θ 0 ≠0).
なお、上記実施例では遅延等化部及び振幅歪補
正部として主信号の前後各1個ずつのエコー信号
を用いた場合について説明したが、本発明はこの
場合のみに限定されるものではなく、主信号の前
後に複数個のエコー信号を用いて等化することも
でき、この場合、振幅歪を補正しつつ、更に複雑
な群遅延特性の等化を行うことが可能となる。 In the above embodiment, a case has been described in which one echo signal before and after the main signal is used as the delay equalization section and the amplitude distortion correction section, but the present invention is not limited to only this case. Equalization can also be performed using a plurality of echo signals before and after the main signal, and in this case, it is possible to perform more complex equalization of group delay characteristics while correcting amplitude distortion.
また、上記実施例回路は振幅調整回路とインバ
ータを別々に構成したが、これらは極性反転機能
をもつ利得調整回路によつても構成できる。ま
た、遅延回路としては、タツプ付遅延線やシフト
レジスタあるいはケーブル等を用いることもでき
る。 Further, although the above-described embodiment circuit has the amplitude adjustment circuit and the inverter configured separately, these can also be configured with a gain adjustment circuit having a polarity inversion function. Further, as the delay circuit, a delay line with taps, a shift register, a cable, etc. can also be used.
さらに、エコー信号の個数は必ずしも主信号の
前後で同数である必要はなく、遅延等化部と振幅
歪補正部とで同じ個数である必要もない。 Furthermore, the number of echo signals does not necessarily need to be the same before and after the main signal, nor does it need to be the same number in the delay equalization section and the amplitude distortion correction section.
以上のように、この発明によれば、遅延等化部
と、該遅延等化部が発生する振幅歪を補正する振
幅歪補正部とを縦続接続し、かつその各々のタツ
プ係数に一定の関係を持たせるように構成したの
で、振幅歪なしに群遅延の大きな歪を等化するこ
とができ、かつ、振幅と群遅延の独立性が保たれ
るので調整が容易になるという効果がある。 As described above, according to the present invention, the delay equalization section and the amplitude distortion correction section that corrects the amplitude distortion generated by the delay equalization section are connected in cascade, and the tap coefficients of each of them have a certain relationship. Since the structure is configured to have a large group delay distortion without amplitude distortion, it is possible to equalize distortion with a large group delay, and since the independence of the amplitude and group delay is maintained, adjustment is facilitated.
第1図は本件発明者の開発になる波形等化器の
ブロツク構成図、第2図は第1図の波形等化器の
周波数特性図、第3図は第1図の波形等化器の時
間領域特性図、第4図は本発明の一実施例による
波形等化器のブロツク構成図、第5図は本発明の
一実施例による波形等化器の各種の周波数特性図
であり、図aは遅延等化部の群遅延特性図、図b
は該遅延等化部の振幅歪特性図、図cは振幅歪補
正部の振幅特性図、図dは総合振幅特性図であ
る。
10…遅延等化部、20…振幅歪補正部、2…
第1の分岐回路、3…90゜移相器(第1の移相
器)、4a〜4d…遅延回路、5…インバータ、
6a,6b…加算器、10a,10b…第1、第
2の遅延回路網、7a,7b…第1、第2の振幅
調整回路、6c…加算器(第1の加算回路)、2
b…第2の分岐回路、3b…90゜移相器(第2の
移相器)、4e〜4h…遅延回路、5b…インバ
ータ、6d,6e…加算器、20a,20b…第
3、第4の遅延回路網、7c,7d…第3、第4
の振幅調整回路、6f…加算器(第1の加算回
路)。なお、図中同一符号は同一又は相当部分を
示す。
Figure 1 is a block diagram of a waveform equalizer developed by the inventor of the present invention, Figure 2 is a frequency characteristic diagram of the waveform equalizer of Figure 1, and Figure 3 is a diagram of the waveform equalizer of Figure 1. 4 is a block configuration diagram of a waveform equalizer according to an embodiment of the present invention, and FIG. 5 is a diagram of various frequency characteristics of a waveform equalizer according to an embodiment of the present invention. Figure a is the group delay characteristic diagram of the delay equalization section, Figure b
is an amplitude distortion characteristic diagram of the delay equalization section, FIG. c is an amplitude characteristic diagram of the amplitude distortion correction section, and FIG. d is a total amplitude characteristic diagram. 10... Delay equalization section, 20... Amplitude distortion correction section, 2...
1st branch circuit, 3... 90° phase shifter (first phase shifter), 4a to 4d... delay circuit, 5... inverter,
6a, 6b...Adder, 10a, 10b...First and second delay circuit networks, 7a, 7b...First and second amplitude adjustment circuits, 6c...Adder (first addition circuit), 2
b...Second branch circuit, 3b...90° phase shifter (second phase shifter), 4e to 4h...Delay circuit, 5b...Inverter, 6d, 6e...Adder, 20a, 20b...Third, third 4 delay circuit networks, 7c, 7d...third, fourth
amplitude adjustment circuit, 6f...adder (first addition circuit). Note that the same reference numerals in the figures indicate the same or equivalent parts.
Claims (1)
延して主信号を作成するとともに上記分岐回路の
一方の出力とこれを時間2Tだけ遅延した信号の
反転信号とを加算してエコー信号を作成する第1
の遅延回路網、 上記分岐回路の他方の出力を90゜移相する第1
の移相器、 この移相器の出力とこれを時間2Tだけ遅延し
た信号とを加算してエコー信号を作成する第2の
遅延回路網、 エコー信号と主信号との振幅比をk、余弦形特
性を基準として周波数軸上で本波形等化器の群遅
延特性を水平方向にずらせる量をθ0としたとき、
上記第1、第2の遅延回路網のエコー信号出力に
kcosθ0,ksinθ0なる重みを付けて振幅調整する第
1、第2の振幅調整回路、 この両振幅調整回路の出力と上記第1の遅延回
路網の主信号出力とを加算する第1の加算回路を
備えた遅延等化部と、 該遅延等化部の出力を入力信号とし該入力信号
を分岐する第2の分岐回路、 この分岐回路の一方の出力を所定時間2Tだけ
遅延して主信号を作成するとともに上記分岐回路
の一方の出力とこれを時間4Tだけ遅延した信号
を加算してエコー信号を作成する第3の遅延回路
網、 上記分岐回路の他方の出力を90゜移相する第2
の移相器、 この移相器の出力とこれを時間4Tだけ遅延し
た信号の反転信号とを加算してエコー信号を作成
する第4の遅延回路網、 上記第3、第4の遅延回路網のエコー信号出力
に(k2/2)cos2θ0,(k2/2)sin2θ0なる重み
を付けて振幅調整する第3、第4の振幅調整回
路、 この両振幅調整回路の出力と上記第3の遅延回
路網の主信号出力とを加算する第2の加算回路を
備た振幅歪補正部とを備え、 上記遅延等化部で群遅延歪の等化を行なう際に
発生する振幅歪を、群遅延が平坦で余弦形の振幅
特性を呈する上記振幅歪補正部で補正することを
特徴とする波形等化器。[Scope of Claims] 1. A first branch circuit that branches an input signal; one output of this branch circuit is delayed by a predetermined time T to create a main signal, and the output of one of the branch circuits and this main signal are The first step is to create an echo signal by adding the inverted signal of the signal delayed by 2T.
a delay network, a first phase shifting the other output of the branch circuit by 90°;
A second delay circuit that creates an echo signal by adding the output of this phase shifter and a signal delayed by a time of 2T, and the amplitude ratio of the echo signal and the main signal is expressed as k, cosine When the amount by which the group delay characteristics of this waveform equalizer is shifted in the horizontal direction on the frequency axis based on the waveform characteristics as a reference is θ 0 ,
To the echo signal output of the first and second delay circuit networks above.
First and second amplitude adjustment circuits that adjust the amplitude with weights of kcosθ 0 and ksinθ 0 , and a first addition that adds the outputs of both amplitude adjustment circuits and the main signal output of the first delay circuit network. a delay equalization section including a circuit; a second branch circuit that takes the output of the delay equalization section as an input signal and branches the input signal; one output of this branch circuit is delayed by a predetermined time of 2T to produce a main signal; and a third delay network that creates an echo signal by adding the output of one of the branch circuits and a signal delayed by a time of 4T, and a third delay circuit that shifts the phase of the other output of the branch circuit by 90°. 2
a phase shifter, a fourth delay circuit network that creates an echo signal by adding the output of this phase shifter and an inverted signal of a signal delayed by time 4T, and the third and fourth delay circuit networks described above. third and fourth amplitude adjustment circuits that adjust the amplitude by adding weights of (k 2 /2) cos2θ 0 and (k 2 /2) sin2θ 0 to the echo signal output of and an amplitude distortion correction section equipped with a second addition circuit that adds the main signal output of the delay circuit network No. 3, and the amplitude distortion correction section that is provided with a second addition circuit that adds the main signal output of the delay circuit network No. 3. . A waveform equalizer, characterized in that the amplitude distortion correction unit performs correction with the amplitude distortion correction section having a flat group delay and a cosine-shaped amplitude characteristic.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56124909A JPS5850814A (en) | 1981-08-07 | 1981-08-07 | waveform equalizer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56124909A JPS5850814A (en) | 1981-08-07 | 1981-08-07 | waveform equalizer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5850814A JPS5850814A (en) | 1983-03-25 |
| JPH0117288B2 true JPH0117288B2 (en) | 1989-03-29 |
Family
ID=14897104
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56124909A Granted JPS5850814A (en) | 1981-08-07 | 1981-08-07 | waveform equalizer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5850814A (en) |
-
1981
- 1981-08-07 JP JP56124909A patent/JPS5850814A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5850814A (en) | 1983-03-25 |
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