JPS6233791B2 - - Google Patents
Info
- Publication number
- JPS6233791B2 JPS6233791B2 JP52026530A JP2653077A JPS6233791B2 JP S6233791 B2 JPS6233791 B2 JP S6233791B2 JP 52026530 A JP52026530 A JP 52026530A JP 2653077 A JP2653077 A JP 2653077A JP S6233791 B2 JPS6233791 B2 JP S6233791B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- frequency
- carrier wave
- phase
- 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
Links
- 238000000034 method Methods 0.000 claims description 5
- 238000005259 measurement Methods 0.000 description 16
- 238000001514 detection method Methods 0.000 description 9
- 238000000605 extraction Methods 0.000 description 8
- 238000012937 correction Methods 0.000 description 7
- 230000005540 biological transmission Effects 0.000 description 6
- 238000010586 diagram Methods 0.000 description 2
- 230000008929 regeneration Effects 0.000 description 2
- 238000011069 regeneration method Methods 0.000 description 2
- 230000001360 synchronised effect Effects 0.000 description 2
- 238000004891 communication Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000001934 delay Effects 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 230000001172 regenerating effect Effects 0.000 description 1
- 230000000717 retained effect Effects 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
Landscapes
- Facsimile Transmission Control (AREA)
- Stabilization Of Oscillater, Synchronisation, Frequency Synthesizers (AREA)
- Digital Transmission Methods That Use Modulated Carrier Waves (AREA)
Description
【発明の詳細な説明】
本発明は同期検波方式の復調に関し、その搬送
波再生回路をデイジタル化し、さらに入力信号の
周期測定を位相整合(位相同期のために長い区間
の搬送波送出部分と短い区間の無信号部分とが繰
り返し送られてくる手順)中に行なうことによ
り、測定に用いる発振器の周波数を下げ、LSI化
を計りやすくした搬送波作成方式を提供するもの
である。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to the demodulation of a synchronous detection method, by digitizing its carrier regeneration circuit, and by performing phase matching on the period measurement of the input signal (for phase synchronization, a carrier wave transmission portion in a long period and a portion in a short period are used). By performing this step during the procedure in which the non-signal portion is repeatedly sent, the frequency of the oscillator used for measurement is lowered, thereby providing a carrier wave creation method that makes it easier to integrate into LSI.
一般に電話回線などの帯域の限られた伝送路に
おける通信には残留側波帯伝送が行なわれる。こ
の場合受信側で完全に元の信号を再現するには、
搬送波を再生して同期検波を行なわなければなら
ない。 Generally, vestigial sideband transmission is performed for communication over a transmission path with a limited band, such as a telephone line. In this case, to completely reproduce the original signal on the receiving side,
The carrier wave must be regenerated to perform synchronous detection.
従来、受信側で搬送波を再生する場合、受信信
号から搬送波成分を取出し、それと電圧制御発振
器の出力とを位相比較器で比較し、その位相差に
応じた差信号電圧を出力し、低域フイルタで高周
波分や雑音を取り除き、直流増幅器で増幅して電
圧制御発振器に入力し、受信信号との位相差がな
くなる方向に制御し、それを出力して搬送波を再
生するという様なPLL(フエイズロツクドルー
プ)回路で構成されている。この回路はアナログ
回路であり、IC化する場合、個々の位相比較
器、電圧制御発振器等はIC化されるがどうして
も外付部品が残り、またPLL回路のロツクレンジ
等はループ利得によつて決定されるため、ループ
利得の決め方が微妙であり、ロツクからはずれる
と言う欠点があり、調整箇所およびアナログ信号
処理のためIC化には技術的な困難をともない、
多くの検討を必要とした。 Conventionally, when regenerating a carrier wave on the receiving side, the carrier wave component is extracted from the received signal, and a phase comparator compares it with the output of a voltage controlled oscillator. A difference signal voltage corresponding to the phase difference is output, and a low-pass filter This is a PLL (phase-locked loop) that removes high-frequency components and noise, amplifies it with a DC amplifier, inputs it to a voltage-controlled oscillator, controls it in a direction to eliminate the phase difference with the received signal, and outputs it to regenerate the carrier wave. It consists of a locked loop) circuit. This circuit is an analog circuit, and when integrated into an IC, each phase comparator, voltage controlled oscillator, etc. are integrated into an IC, but external components inevitably remain, and the lock range of the PLL circuit is determined by the loop gain. Therefore, the method of determining the loop gain is delicate, and there are disadvantages in that it may go out of lock, and it is technically difficult to integrate it into an IC because of the adjustment points and analog signal processing.
It required a lot of consideration.
本発明は前記従来技術に鑑み、搬送波再生回路
をデイジタル回路で構成することのできる新規な
搬送波作成方式を提供するものである。 In view of the above-mentioned prior art, the present invention provides a new carrier wave generation method in which the carrier wave regeneration circuit can be configured with a digital circuit.
以下本発明の実施例を図面によつて説明する。
フアクシミリ装置において原稿を送る場合、まず
位相整合を行ない、位相整合終了後は画信号が送
り出される。第1図においてAは位相整合時の送
出信号で走査周波数の周期aごとに長い区間の連
続な搬送波送出部分と短い区間の無信号部分が繰
り返し送出される。Bは画信号中の信号でbの位
相信号の部分b′の画信号の部分から成つている。
第2図および第3図において、1は入力信号端子
で、位相整合中は第1図Aの波形が画信号中は第
1図Bの波形が受信される。2はゼロクロス点検
出回路で入力信号イのゼロクロス点を検出してロ
に示す矩形波に変換し、さらにその矩形波ロの立
上りおよび立下りを検出して2倍の周波数の矩形
波ハを作り出す。 Embodiments of the present invention will be described below with reference to the drawings.
When sending a document in a facsimile machine, phase matching is first performed, and after the phase matching is completed, an image signal is sent out. In FIG. 1, A is a transmission signal during phase matching, and a long section of continuous carrier wave transmission part and a short section of no signal part are repeatedly sent out every period a of the scanning frequency. B is a signal in the image signal and consists of a phase signal portion of b and an image signal portion of b'.
In FIGS. 2 and 3, 1 is an input signal terminal, and the waveform shown in FIG. 1A is received during phase matching, and the waveform shown in FIG. 1B is received during the image signal. 2 is a zero-crossing point detection circuit that detects the zero-crossing point of input signal A and converts it into the rectangular wave shown in B, and then detects the rising and falling edges of the rectangular wave B to create a rectangular wave C with twice the frequency. .
位相整合中、コントロール回路4において、入
力端子3からの位相整合中で、かつ搬送波が送出
されている区間を示す位相整合波取出信号ニとゼ
ロクロス点検出回路2の出力信号ハとによつてゲ
ート信号ホの立上りを決める。信号ホがHレベル
の間、カウンタ8が動作し、固定発振器7のクロ
ツクヌのパルス数をカウントし始める。同時にゲ
ート5はゲート信号ホがHレベルのとき点Xと点
Zとが接続され、ゼロクロス点検出回路2からの
信号ハをカウンタ6に印加する。カウンタ6はゼ
ロクロス点検出回路2の出力信号ハをn+1個カ
ウントするとコントロール回路4に桁上げ信号を
送る。コントロール回路4はカウンタ6からの桁
上げ信号によつてゲート信号ホの立下りを決め
る。この立下りによつてカウンタ8は動作をスト
ツプし、その内容を保持しておく。ゲート信号ホ
は入力信号イの2倍の周波数の信号ハのn波の期
間Hレベルとなる信号で、その期間固定発振器7
のパルス数を測定する。この動作は位相整合中に
1回行えばよく、例えば最初に長い区間の搬送波
が送出されてくる時に行なう。9は除算器で、カ
ウンタ8が測定した固定発振器7のパルス数をm
とすると、測定終了後は除算器9によつてmを固
定発振器7のパルス数を測定する期間の信号ハの
波数nで割り算し、この商をk、余りをlとして
この結果を保持しておく。上記の測定する期間の
信号ハの波数nは固定値としてカウンタ6及び除
算器9に保持されている。第3図ハ,ホ,ヘに示
した例ではn=8、m=83で、k=10、l=3と
なる。一方、カウンタ10はゲート信号ホのLレ
ベル期間動作し、固定発振器7のクロツクヌス数
をカウントする。11は比較回路で、除算器9の
商kとカウンタ10の内容が一致した時パルスの
出力を出す。12は遅延回路で、13は余り補正
回路である。遅延回路12は余り補正回路13の
出力が2値のレベルでHの時、比較回路11の出
力を固定発振器7の1クロツク分遅延させ、余り
補正回路13の出力が2値のレベルでLの時、比
較回路11の出力をそのまま出力する。又同時に
ゲート信号ホのLレベルの期間ゲート5は点Yと
点Zが接続され、遅延回路12の出力信号をカウ
ンタ6に印加する。カウンタ6はそれを0〜(n
−1)まで順にカウンタする。余り補正回路13
はカウンタ6の内容と余りlに応じて、カウンタ
6がカウントされるごとに出力信号を変化させ、
n回中l回は2値のレベルでHの信号を残り(n
−l)回はLの信号を出力して遅延回路12を制
御する。 During phase matching, the control circuit 4 uses the phase matching wave extraction signal D indicating the section from the input terminal 3 during phase matching and the carrier wave is being sent out, and the output signal C of the zero cross point detection circuit 2 to perform a gate operation. Determines the rise of signal E. While the signal H is at H level, the counter 8 operates and starts counting the number of clock pulses of the fixed oscillator 7. At the same time, the gate 5 connects the points X and Z when the gate signal E is at H level, and applies the signal C from the zero-cross point detection circuit 2 to the counter 6. The counter 6 sends a carry signal to the control circuit 4 after counting n+1 output signals C from the zero crossing point detection circuit 2. The control circuit 4 determines the fall of the gate signal E based on the carry signal from the counter 6. Due to this fall, the counter 8 stops its operation and holds its contents. Gate signal E is a signal that is at H level for a period of n waves of signal C, which has twice the frequency of input signal A, and the fixed oscillator 7
Measure the number of pulses. This operation only needs to be performed once during phase matching, for example, when a long section carrier wave is first sent out. 9 is a divider which divides the number of pulses of the fixed oscillator 7 measured by the counter 8 into m
Then, after the measurement is completed, the divider 9 divides m by the wave number n of the signal C during the period during which the number of pulses of the fixed oscillator 7 is measured, and this result is retained with the quotient as k and the remainder as l. put. The wave number n of the signal C during the above measurement period is held as a fixed value in the counter 6 and the divider 9. In the example shown in FIGS. 3C, 3E, and 3E, n=8, m=83, k=10, and l=3. On the other hand, the counter 10 operates during the L level period of the gate signal H and counts the number of clock pulses of the fixed oscillator 7. 11 is a comparison circuit which outputs a pulse when the quotient k of the divider 9 and the contents of the counter 10 match. 12 is a delay circuit, and 13 is a remainder correction circuit. The delay circuit 12 delays the output of the comparator circuit 11 by one clock of the fixed oscillator 7 when the output of the remainder correction circuit 13 is at a binary level and is L. At this time, the output of the comparator circuit 11 is output as is. At the same time, during the period when the gate signal E is at L level, the points Y and Z of the gate 5 are connected, and the output signal of the delay circuit 12 is applied to the counter 6. Counter 6 calculates it from 0 to (n
-1). Remainder correction circuit 13
changes the output signal every time the counter 6 counts according to the contents of the counter 6 and the remainder l,
For l times out of n times, the signal is H at a binary level and the rest (n
-l) times, the delay circuit 12 is controlled by outputting an L signal.
18は位相信号取出し信号トの入力端子で、1
4は位相信号取出回路である。信号トは位相整合
中は搬送波が送出される区間がHレベル、画信号
中は位相信号、すなわち搬送波を送出する区間
(第1図Bのb)がHレベルである。位相信号取
出回路14は信号トを用いて信号トがHレベルに
なつた後の最初のゼロクロス点検出回路2からの
信号ハを1波取出す。すなわち、入力信号イの搬
送波成分の2倍の周波数の信号が1波取出され
る。さらに位相信号取出回路14において、信号
チを用いてこの信号チがHレベルとなつた後の最
初の固定発振器7の1クロツク分を取出す。リは
信号チを用いて取出された固定発振器7の1クロ
ツク分の信号である。 18 is an input terminal for the phase signal extraction signal G;
4 is a phase signal extraction circuit. During phase matching, the signal G is at H level in the section where the carrier wave is sent out, and during the image signal, the phase signal, that is, the section where the carrier wave is sent out (b in FIG. 1B) is at H level. The phase signal extraction circuit 14 uses the signal G to extract one wave of the signal C from the first zero cross point detection circuit 2 after the signal G becomes H level. That is, one wave of a signal having a frequency twice that of the carrier wave component of input signal A is extracted. Furthermore, the phase signal extraction circuit 14 uses the signal CH to extract one clock of the first fixed oscillator 7 after the signal CH becomes H level. 1 is a signal for one clock of the fixed oscillator 7 extracted using the signal chi.
ゲート15は、遅延回路12からの出力信号と
位相信号取出回路14からの出力信号を加え合わ
せるORゲートである。ルはゲート15からの出
力信号で、信号ル中のdは位相信号取出回路14
からの信号すなわち信号リ、eは遅延回路12か
らの信号である。ゲート15からの信号ルによつ
て、カウンタ10はクリアされ、固定発振器7の
クロツクを始めからカウントし直す。測定後、以
上の動作をくり返し行なうと、信号ルは固定発振
器7のクロツクをn回中(n−l)回にk分周、
残りl回は(k+1)分周し、周期aごとに新た
にセツトし直した信号に相当する。第3図に示し
た例では、m=83、n=8でk=10、l=3であ
るから、その分周比を例えば10、11、10、11、
10、10、11、10と定め、これをくり返し用いてい
る。16フリツプフロツプで構成される分周回路
でゲート15の信号ルを半分に分周する。17は
出力端子である。以上の動作によつて出力端子1
7からは送信側の搬送波とほとんど同周波数、同
位相の連続波オを得ることができる。なお測定す
る際、測定する期間の信号ハの波数nが2の指数
乗個、n=2i(iは正の整数)とすると、2進
表示でカウンタ8の内容の下iビツトは余り、残
りの上位の桁は商となり、除算器9は不要とな
る。 Gate 15 is an OR gate that adds the output signal from delay circuit 12 and the output signal from phase signal extraction circuit 14. is the output signal from the gate 15, and d in the signal is the phase signal extraction circuit 14.
The signals from the delay circuit 12, that is, the signals li and e, are the signals from the delay circuit 12. A signal from gate 15 clears counter 10 and causes fixed oscillator 7 to start counting again. After the measurement, by repeating the above operation, the signal divides the clock of the fixed oscillator 7 by k out of n times (n-l),
The remaining l times correspond to a signal that is frequency-divided by (k+1) and newly set every period a. In the example shown in Fig. 3, m = 83, n = 8, k = 10, l = 3, so the frequency division ratio is set to, for example, 10, 11, 10, 11,
It is set as 10, 10, 11, 10 and is used repeatedly. A frequency divider circuit consisting of 16 flip-flops divides the frequency of the gate 15 signal in half. 17 is an output terminal. By the above operation, output terminal 1
7, it is possible to obtain a continuous wave signal having almost the same frequency and phase as the carrier wave on the transmitting side. When measuring, if the wave number n of the signal C during the measurement period is an exponential number of 2, and n = 2 i (i is a positive integer), the lower i bit of the contents of the counter 8 in binary representation is the remainder, The remaining high-order digits become the quotient, and the divider 9 becomes unnecessary.
以上のように本発明はゼロクロス点検出回路の
部分を除いて純デイジタル回路で構成されている
から、容易にLSI化することができる。また、例
えば、前記実施例において、固定発振器7の周波
数を500KHz(周期2μs)とし、第1図に示し
た位相整合時の搬送波送出部分と無信号部分の繰
り返し周波数が9Hz、すなわち1/a=9Hz、搬
送波の周波数が2.1KHzの時、位相整合中に搬送
波の2倍の周波数の信号で256波取出し、その間
の固定発振器のパルスをカウントする。パルスを
用いてデイジタル化した測定を行うと、誤差とし
て最大1パルス分の測定誤差が生じる。従つて、
256波取出してカウントした値に対して最大1パ
ルス分のカウント誤差が生じている。測定結果を
くり返し利用すると再生搬送波に測定誤差が累積
するが、本実施例では、画信号中の位相信号(搬
送波が送出されてくる)を用いて位相補正を行つ
ており、1/a=9Hzより、9Hzごとに位相が補
正される。9Hz中に4.2KHzの波の個数は約467
(1/9/1/4.2×103≒467)個であり、256波
のカウント
結果を用いて再生した搬送波は、もとの搬送波に
対して最大約2(467/256≒2)クロツクの振
れ、すなわち最大4μsの振れが生じる。これを
度数に直すと約3゜((4×10-6/1/2.1×103
)×
360゜=3.024゜)の振れである。また測定を位相
整合中に行ない画信号中位相信号ごとに補正する
だけである。従つて、位相整合中の長い区間の搬
送波送出部分を利用し、測定期間を長くして(十
分多くの入力信号を取出して)固定発振器のパル
スをカウントすることができる。測定誤差は測定
期間で最大1パルス分であり、この測定結果をく
り返し利用して搬送波を再生すると誤差が累積す
るが画信号中の位相信号部分の搬送波を利用して
補正をかけるので固定発振器の周波数を下げるこ
とが可能である。さらに、電話回線のように搬送
回路を何回も伝送された信号では、搬送時の変復
調にともなう周波数ずれが存在し、送信時の搬送
波周波数と、受信時の搬送波周波数は、ふつう異
るものである。従来方法のPLL回路等では引込み
範囲を大きく取つてかつ安定動作のために回路が
複雑となり、またその調整も微妙であり、多大の
労力を必要としたが、本発明では受信機側の固定
発振器出力を分周するため、周波数の安定度は固
定発振器の安定度であり、水晶発振器などの安定
な発振器を使用すると簡単に10-5ぐらいいの安定
度が得られ、かつ引込み範囲の下限は、カウンタ
8のビツト数で制限され、例えば、先の例(固定
発振器の周波数500KHz、測定期間は搬送波の2
倍の成分で256波、1/a=9Hz)の場合、カウ
ンタ8を16ビツトとすると、カウンタ8がオーバ
ーフローすることなく測定出来る搬送波の2倍の
周波数xHzは、方程式(500×103/x)256=216
−1を解くことによつて得られ、x≒1953Hzとな
る。上限は最大位相誤差を定めることによつて定
まり、例として最大位相誤差を6゜とすると、搬
送波の2倍の周波数yHzは、方程式1/500×103
×
y/9/256=1/y/2×6/360を解くことに
よつて得られ、y≒
6196Hzとなる。もとの搬送波2100Hzに対して2100
−1123.5Hz〜2100+998Hz(1953/2〜6196/2
Hz)の範囲で引込む。 As described above, since the present invention is constructed of purely digital circuits except for the zero-crossing point detection circuit, it can be easily implemented as an LSI. For example, in the above embodiment, the frequency of the fixed oscillator 7 is 500 KHz (period: 2 μs), and the repetition frequency of the carrier wave sending part and the no-signal part during phase matching shown in FIG. 1 is 9 Hz, that is, 1/a= When the frequency of the carrier wave is 9Hz and the frequency of the carrier wave is 2.1KHz, 256 waves of a signal with twice the frequency of the carrier wave are extracted during phase matching, and the pulses of the fixed oscillator are counted during the phase matching. When digitized measurements are made using pulses, a measurement error of up to one pulse occurs as an error. Therefore,
There is a maximum count error of one pulse with respect to the value obtained by extracting and counting 256 waves. If measurement results are used repeatedly, measurement errors will accumulate in the reproduced carrier wave, but in this example, phase correction is performed using the phase signal in the image signal (from which the carrier wave is transmitted), and 1/a = 9 Hz. Therefore, the phase is corrected every 9 Hz. The number of 4.2KHz waves in 9Hz is approximately 467
(1/9/1/4.2×10 3 ≒467), and the carrier wave reproduced using the count result of 256 waves is a maximum of about 2 (467/256≒2) with respect to the original carrier wave. Clock swings, ie, swings of up to 4 μs, occur. Converting this into degrees is approximately 3° ((4×10 -6 /1/2.1×10 3
) x 360° = 3.024°). Further, the measurement is performed during phase matching, and correction is only made for each phase signal in the image signal. Therefore, it is possible to take advantage of the long carrier wave delivery part during phase matching and to lengthen the measurement period (by taking out a sufficiently large number of input signals) to count the pulses of the fixed oscillator. The measurement error is a maximum of one pulse during the measurement period, and if this measurement result is used repeatedly to reproduce the carrier wave, the error will accumulate, but since the correction is made using the carrier wave of the phase signal part of the image signal, it is difficult to use a fixed oscillator. It is possible to lower the frequency. Furthermore, in a signal that is transmitted over a carrier circuit many times, such as on a telephone line, there is a frequency shift due to modulation and demodulation during the carrier, and the carrier wave frequency at the time of transmission and the carrier wave frequency at the time of reception are usually different. be. In conventional PLL circuits, etc., the pull-in range is large and the circuit is complicated to achieve stable operation, and the adjustment is delicate and requires a lot of effort.However, in the present invention, the fixed oscillator on the receiver side Since the output is divided, the frequency stability is that of a fixed oscillator.If you use a stable oscillator such as a crystal oscillator, you can easily obtain a stability of about 10 -5 , and the lower limit of the pull-in range is , is limited by the number of bits of counter 8, for example, in the previous example (fixed oscillator frequency 500KHz, measurement period is 2
If the counter 8 is 16 bits, the frequency xHz that is twice the carrier wave that the counter 8 can measure without overflowing is calculated using the equation (500×10 3 /x )256=2 16
-1, and x≈1953Hz. The upper limit is determined by determining the maximum phase error. For example, if the maximum phase error is 6°, the frequency yHz, which is twice the carrier wave, is determined by the equation 1/500×10 3
It is obtained by solving ×y/9/256=1/y/2×6/360, and y≈6196Hz. 2100 for the original carrier 2100Hz
-1123.5Hz~2100+998Hz (1953/2~6196/2
Hz) range.
第1図は受信側に入る入力信号例を示す図、第
2図は本発明の一実施例による搬送波作成方式の
ブロツク図、第3図は第2図の動作説明用のタイ
ミングチヤートである。
1,18……入力端子、2……ゼロクロス点検
出回路、4……コントロール回路、5,15……
ゲート、6……カウンタ、7……固定発振器、
8,10……カウンタ、9……除算器、11……
比較回路、12……遅延回路、13……余り補正
回路、14……位相信号取出回路、16……分周
回路、17……出力端子。
FIG. 1 is a diagram showing an example of an input signal entering the receiving side, FIG. 2 is a block diagram of a carrier wave generation system according to an embodiment of the present invention, and FIG. 3 is a timing chart for explaining the operation of FIG. 1, 18... Input terminal, 2... Zero cross point detection circuit, 4... Control circuit, 5, 15...
Gate, 6...Counter, 7...Fixed oscillator,
8, 10... Counter, 9... Divider, 11...
Comparison circuit, 12... Delay circuit, 13... Remainder correction circuit, 14... Phase signal extraction circuit, 16... Frequency dividing circuit, 17... Output terminal.
Claims (1)
に、搬送波からその周波数の2倍の周波数の信号
を作成する手段と、前記2倍の周波数信号のn波
の期間に、内蔵する固定発振器のクロツク数をカ
ウントする手段と、前記カウントした結果を前記
nで除算して商kと余りlを求める手段と、前記
n波の期間と等長の期間において前記固定発振器
のクロツクを(n−l)回はk分周、残りl回は
(k+1)分周する分周器と、前記長い区間の連
続搬送波の受信後は画信号中から位相信号を抽出
して位相を定める信号を作り出し、この位相を定
める信号にもとずいて前記分周器をリセツトする
手段と、前記分周器の出力信号を2分周する手段
を有し、送出されてくる搬送波と同周波数、同位
相の連続波を作成することを特徴とする搬送波作
成方式。1. Means for creating a signal with a frequency twice the frequency of the carrier wave during a period when a continuous carrier wave of a long period is transmitted, and a built-in fixed oscillator clock during the period of n waves of the double frequency signal. means for counting a number; means for dividing the counted result by the n to obtain a quotient k and a remainder l; A frequency divider divides the frequency by k times, and divides the frequency by (k+1) for the remaining l times.After receiving the continuous carrier wave of the long section, a phase signal is extracted from the image signal to create a signal that determines the phase. means for resetting the frequency divider based on a signal that determines the frequency divider, and means for dividing the output signal of the frequency divider by two, so as to generate a continuous wave having the same frequency and the same phase as the transmitted carrier wave. A carrier wave creation method characterized by creating a carrier wave.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2653077A JPS53111267A (en) | 1977-03-09 | 1977-03-09 | Generation system for continuous wave |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2653077A JPS53111267A (en) | 1977-03-09 | 1977-03-09 | Generation system for continuous wave |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS53111267A JPS53111267A (en) | 1978-09-28 |
| JPS6233791B2 true JPS6233791B2 (en) | 1987-07-22 |
Family
ID=12196027
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2653077A Granted JPS53111267A (en) | 1977-03-09 | 1977-03-09 | Generation system for continuous wave |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS53111267A (en) |
-
1977
- 1977-03-09 JP JP2653077A patent/JPS53111267A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS53111267A (en) | 1978-09-28 |
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