JPS58215156A - Reproducing circuit of carrier wave - Google Patents

Reproducing circuit of carrier wave

Info

Publication number
JPS58215156A
JPS58215156A JP57097957A JP9795782A JPS58215156A JP S58215156 A JPS58215156 A JP S58215156A JP 57097957 A JP57097957 A JP 57097957A JP 9795782 A JP9795782 A JP 9795782A JP S58215156 A JPS58215156 A JP S58215156A
Authority
JP
Japan
Prior art keywords
phase
output
carrier wave
waveform
wave
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
JP57097957A
Other languages
Japanese (ja)
Inventor
Tokihiro Mishiro
御代 時博
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP57097957A priority Critical patent/JPS58215156A/en
Publication of JPS58215156A publication Critical patent/JPS58215156A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04LTRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION
    • H04L27/00Modulated-carrier systems
    • H04L27/18Phase-modulated carrier systems, i.e. using phase-shift keying
    • H04L27/22Demodulator circuits; Receiver circuits
    • H04L27/227Demodulator circuits; Receiver circuits using coherent demodulation
    • H04L27/2271Demodulator circuits; Receiver circuits using coherent demodulation wherein the carrier recovery circuit uses only the demodulated signals
    • H04L27/2273Demodulator circuits; Receiver circuits using coherent demodulation wherein the carrier recovery circuit uses only the demodulated signals associated with quadrature demodulation, e.g. Costas loop

Abstract

PURPOSE:To reproduce a reference carrier wave from a 2-phase modulated wave and to realize the share between 4-phase and 2-phase, by providing a switching circuit to one side of an orthogonal control signal system of a costas type carrier wave reproducing circuit which reproduces a reference carrier wave from a 4-phase modulated wave. CONSTITUTION:An operation same as a conventional costas loop is ensured when a switch 13 is closed. When the switch 13 is opened, the output of an adder 12 is equal to the waveform (C) obtained by obtaining a product through a multiplier 10 between the waveform (B) of an LPF4 and the waveform (A) of a comparator 9'. The output of the adder 12 moves to a point (i) and (j) when the digital value is 0 and pi respectively and has the same function to have the synchronism for the phase of a VCO7' since the place where the value 0 cuts is set in the same phase changing direction. Thus the VCO7' is set under a stable phase synchronizing state. A reference carrier wave is reproduced also from a 2- phase modulated wave with the output of the VCO7'.

Description

【発明の詳細な説明】 Igl  発明の技術分野 本発明は衛星通信等に使用するディジタル4相<S’r
、相変調波から基準搬送波全再生するコスタス型搬送波
再生回路を用い2相4相の位相変調波に対して共用化?
計った搬送波再生回路に関する。
[Detailed Description of the Invention] Igl Technical Field of the Invention The present invention relates to a digital four-phase <S'r
, Can it be shared for 2-phase and 4-phase phase modulated waves using a Costas type carrier wave regeneration circuit that fully recovers the reference carrier from the phase modulated wave?
Regarding the measured carrier wave regeneration circuit.

tbl  技術の背景 従来ディジタル位相変調の伝送路において、変調和数全
かえることはほとんど行なわれていなかった。しかし近
年伝送路の品質が天候等で左右される人工衛星〒径由す
る衛星′A債分野において、回線品質に応じて変調和数
金かえ信号の伝送速度i切替えるよろな通償方式が行な
われ一つつある。
Background of the tbl Technology Conventionally, in a digital phase modulation transmission line, it has been almost impossible to completely change the harmonics. However, in recent years, in the field of satellite 'A bonds' where the quality of the transmission path is influenced by weather etc., various compensation methods have been used to switch the transmission speed of the variable harmonic frequency signal (i) depending on the line quality. There is one.

ディジダル位相変調方式において、4相変訓と2相変1
1114=2比較すると同一の信号帯域中なら4相は2
相に比し2倍の信号音伝送出来るが同一の符号誤り率金
得るためには回線品質が約3db良くなければならない
。従って回線品質の良い晴天時には4相変調により信号
伝送1行にい、回線品質の悪い雨天時等は2相変yA金
行なうことによって通信i確保すること力S出来る。
In the digital phase modulation method, 4 phase change and 2 phase change 1
1114=2 Comparing, if the signal band is the same, 4 phases are 2
It is possible to transmit twice as many signal tones as compared to a phase-based method, but in order to obtain the same code error rate, the line quality must be about 3 db better. Therefore, when the line quality is good and the weather is good, one line of signal transmission is performed using four-phase modulation, and when the line quality is poor, such as on rainy days, a two-phase change is performed to ensure communication.

本発明はこの様な通信システムの受信側復+!II器に
使用するものである。
The present invention is designed to restore the receiving side of such a communication system! It is used for II equipment.

tel  従来技術と問題点 ディジタル位相変w4波から規準搬送波?再生する手段
としてはいわゆるコスタス型搬送波再生回路(コスタス
ループ)が知られており4相2,2相の夫々の位相変調
波を再生するためには従来第1図、第2図に示すよろな
専用独立の回路紮使用していた。
tel Conventional technology and problems Digital phase change from W4 wave to standard carrier wave? A so-called Costas type carrier wave regeneration circuit (Costas loop) is known as a regeneration means, and in order to regenerate each of the 4-phase 2 and 2-phase phase modulated waves, the conventional methods shown in Figs. 1 and 2 are used. A dedicated independent circuit was used.

第1図は従来例の2相コスタスlレ一プ回路のブロック
図、yp、 2 図pt rti例の4相コス7スlレ
一グ回路の10ツク図、準3図は第1図の場合のコスダ
スIレーグの安定点を説明する波形のタイム千ヤードで
(へ)は削(t)(こOe、 (1?’+−θO)の波
形?示【御坊バー′flLSin 2 (Rl−Rn 
) ノn1.形k 示ス、N 4 図(・21丁2図の
場合のコスタスループの安定点全説明j−る波形のタイ
ム千ヤードで(Nけ低v、P波器(以′1:l」PFと
称す)4′の出力波形、(Rは比較器9小出力波形、(
(−IけL P P 7’の出力波形、fl)は比較器
9′の出力波形、(弓はt算器1oの出力波形、(Dけ
1、算器11の出力波形、(Gけ加nR% 12の出力
波形を示す。
Figure 1 is a block diagram of a conventional 2-phase Costas L-1 circuit; The time of the waveform to explain the stable point of Kosdas I leg in the case of 1000 yards shows the waveform of (1?'+-θO)? Rn
) nonn1. Form k shows, N 4 Figure (・Complete explanation of the stable point of the Costas loop in the case of 21-2 Figures j) At the time of 1,000 yards of the waveform (N ke low v, P wave device (hereinafter '1:l' PF ) 4' output waveform, (R is the comparator 9 small output waveform, (
(-I digit L P P 7' output waveform, fl) is the output waveform of comparator 9', (bow is the output waveform of t calculator 1o, (D digit 1, output waveform of calculator 11, (G digit The output waveform of Add nR% 12 is shown.

(ゾ中1.l’、:’1,5.5’、1(1,11は奪
算器、2 、4 、2’ 、 4’はLPF 、 6 
、6’はループフィlレダ、7.7′は電圧制御型発振
器(以下VCOと称す)、lFt’h9oz位相器、g
、g’H比v器、12は加轡器ケ示す。
(1.l', :'1, 5.5', 1 (1, 11 are detractors, 2, 4, 2', 4' are LPF, 6
, 6' is a loop filter, 7.7' is a voltage controlled oscillator (hereinafter referred to as VCO), 1Ft'h9oz phase shifter, g
, g'H ratio v, 12 indicates the adder.

先づ第1図とiA3図?用いて2相コスタスlレープの
動作を説明する。入力信号の2相位相変調波’it m
(tl s’n (Wr tl61)(但しm(11は
振巾i示す)としVCO7の出力Q2SIn(w、(+
θ0)とすると隼算器lにでこれらの象算金行いLPF
2紮通った信号ハm (11(:o q(θニー〇〇)
とかる。又VCO7の出力?90度位相器8にで90度
位相?ずらした信号2Cos (w、 tl00)と入
力信号と1聚算器5にて?jl−行いLPF’4 ?通
ツタ信号はm(tl 5in(θl−00)と力る。こ
のLPF2及び4の出力の信号w#、J器3にて々3算
1行うとその出力信号はキーS1n 2(θ1−θ0)
となる。この信号をルーグツィルタ6紮介してVCO7
に加えて位相差(θ1−θO)が0にとるよ−”1Vc
O7の位相全かえるよろにして(,1Z、。
First, Figure 1 and Figure iA3? The operation of the two-phase Costas I rape will be explained using the following. Two-phase phase modulated wave of input signal 'it m
(tl s'n (Wr tl61) (however, m (11 indicates the amplitude i) and the output of VCO7 Q2SIn(w, (+
θ0), these quadrant calculations are performed in Hayabusa calculator LPF
Signal hum that passed 2 times (11(:o q(θ knee〇〇)
Tokaru. Also, the output of VCO7? 90 degree phase with 90 degree phase shifter 8? Shifted signal 2Cos (w, tl00) and input signal and 1 in multiplier 5? jl-do LPF'4? The output signal is inputted as m(tl 5in(θl-00). When the signal w# of the output of LPF2 and 4 is calculated by 3 in J unit 3, the output signal becomes key S1n 2(θ1-θ0 )
becomes. This signal is passed to the VCO7 via the Lugsirter 6.
In addition to that, the phase difference (θ1-θO) is set to 0-"1Vc
The phase of O7 is completely changed (,1Z,.

即ち位相同期回路となっている。この時のm1tlco
sなる。2相位相変調波はディシダIし値により位相差
(θl−θO)が0又けπに変化する。これによりm 
(11Co s (θI−θO)は(2)のイ点又は0
点に移動し、trIIf tl −T−81n 2 (θ1−00)は山のハ点又は二点
に移動するつしかしハ点と二点は位相の変化方向が同一
であるのでVC07i位相同期さすのに位相がかわって
も同じょ肖に働きVCO7y位相差(θ1−00)いる
。尚m((l Cos (θ1−θ0)の信号to、1
の判別回路(図示してない)に送り上記イ点ロ点に示す
最大損中点の振巾方向によII)0.li判定するよ)
にしている。
In other words, it is a phase locked circuit. m1tlco at this time
It becomes s. The phase difference (θl−θO) of the two-phase phase modulated wave changes from 0 to π depending on the decider I value. This results in m
(11Cos (θI−θO) is the point A in (2) or 0
trIIf tl -T-81n 2 (θ1-00) moves to point C or two points of the mountain. However, since the direction of phase change is the same at point C and two points, VC07i phase synchronization is performed. Even if the phase changes, the VCO7y works in the same way and there is a phase difference (θ1-00). Note that the signal to, 1 of m((l Cos (θ1−θ0))
II) 0. I will judge li)
I have to.

次に@2図第4図紮用いて4相コスタスループの動作?
説明する。LPF2’ 、LPF4’の出力迄け2相コ
スダスルーズの場合と同じである。よってLPF’2’
の出力波形業示すと囚の如くなり又LPF4’の出力波
形は(qの如くなる。
Next, how does the 4-phase Costas loop work using Figure 2 and Figure 4?
explain. The process up to the outputs of LPF2' and LPF4' is the same as in the two-phase cosda loose case. Therefore, LPF'2'
The output waveform of LPF 4' is as shown below, and the output waveform of LPF 4' is as shown in (q).

これ等の波形全比較器9′、9にて比較し正か負か?判
定して出力さすとtBl(+))に示す正負の矩形波と
なる。この(均に示す比較器9′の出力の矩形波信号と
((−1に示す波形のT、PF4’の出力信号との積を
東算G1oVCで求めるとその信号の波形は(均に示す
如くなる。又(口に示す比較器9の出力の矩形波信号と
囚に示す波形のL P F 2’の出力信号とのflf
kI算器itにて求めるとその信号の波形は(稍に示す
如くなる。この東算器10と11の出力信号の差孕加算
器12にて求めるとこの信号の波形は(0に示−を如く
入力信号波形の位相が2に変化する間に、()を切る所
が同じ位相の変化方向に90度間隔にホ、へ、ト、千の
如く4個所生ずる。この+(1に示すyI号?ループフ
ィルタ6′?介し直流電子に変換してV (: 07/
に印加して(qに示す信号が0点になるよう(でVCO
7’の位相全かえるようにしている。4相f\γ相変調
波はディジダル値により入力信号とV (207’の出
力信号との位相差がO,r/2゜”+3/2gになるよ
う変化する。しかしこの回路では、このよ′1に変化し
ても(qに示す加算器12の出力はπ/2間隔のホ、へ
、ト、千の付近゛液移動しいづれもOt切る所が同じ位
相の変化方向であるのでVCO7J7位相同期さすのに
同じょう罠働きVCO7J:安定した同期位相に引込む
。このようにしてVCO7’の出力にで規準搬送波全再
生するようにしている。尚LPF2’及び41の出力?
0.1判別回路(図示してない)に送りLPF2’及び
4′の出力の基準搬送波全基準にして、入力した信号が
+側にあるか一側にあるが又位相差がいくらかにより入
力信号全変調したディジダル値?求めているっ しかし第1図に示す2相コスタスル一プ回路ケ2相位相
変調の時しか使用出来ず又第2図に示す4相コスダスル
一プ回路け4相位相変調のときしか使用出来ないため4
相及び2相の位相変調を共に使用する場合は2つの回路
會持つ必要があり回路規模が大きく々り高価となり又2
つ回路?使用するので信頼性が悪くなる欠点がある。
Are these waveforms compared by all comparators 9' and 9, and are they positive or negative? When determined and output, it becomes a positive and negative rectangular wave shown as tBl(+)). When the product of the rectangular wave signal of the output of the comparator 9' shown in ((-1) and the output signal of T, PF4' of the waveform shown in (-1) is calculated using Tosan G1oVC, the waveform of the signal is Also, (flf of the rectangular wave signal of the output of the comparator 9 shown on the left and the output signal of L P F 2' with the waveform shown on the left)
When calculated using the kI calculator it, the waveform of the signal is as shown in the figure below.When calculated using the adder 12, the waveform of this signal is shown as (0). While the phase of the input signal waveform changes to 2 as shown in , there are four places where ( ) is cut at 90 degree intervals in the direction of the same phase change, such as E, H, G, and 1000. It is converted into DC electrons through the yI?loop filter 6'?V (: 07/
(so that the signal shown at q becomes 0 point) (so that the VCO
The phase of 7' is completely changed. The 4-phase f\γ-phase modulated wave changes depending on the digital value so that the phase difference between the input signal and the output signal of V (207') becomes O,r/2°''+3/2g. Even if the output of the adder 12 shown in q changes to 1, the output of the adder 12 is near E, H, G, and 1000 at π/2 intervals. The same trap works to achieve phase synchronization.VCO7J: Pulls into a stable synchronization phase.In this way, the reference carrier wave is fully regenerated at the output of VCO7'.In addition, the outputs of LPF2' and 41?
The input signal is sent to a 0.1 discriminator circuit (not shown), and depending on whether the input signal is on the + side or on the one side, based on the reference carrier of the output of LPF 2' and 4', depending on the phase difference. Fully modulated digital value? However, the two-phase Kosda loop circuit shown in Figure 1 can only be used for two-phase phase modulation, and the four-phase Kosda loop circuit shown in Figure 2 can only be used for four-phase phase modulation. Tame 4
When phase modulation and two-phase phase modulation are used together, it is necessary to have two circuits, which results in a large and expensive circuit.
One circuit? Since it is used, it has the disadvantage of poor reliability.

(由 発明の目的 本発明の目的は上記の欠点をなくするために、4相のコ
スダス型搬送波再生回路を2相位相変調波の場合にも共
用出来るようにし小形化低価格化が可能で信頼性の高い
搬送波再生回路の提供にある。
(Object of the Invention) In order to eliminate the above-mentioned drawbacks, the purpose of the present invention is to make it possible to use a four-phase Cosdas type carrier wave regeneration circuit also in the case of a two-phase phase modulated wave, thereby making it possible to reduce the size, cost, and reliability. The objective is to provide a carrier wave regeneration circuit with high performance.

te+  発明の構成 本発明は上記の目的全達成するために4相位相変Fil
i波から基準搬送波全再生するコスダス型搬送波再生回
路の直交制御信号系の一方にスイッチ回路全般けこのス
イッチ全所にすることにより2相位相変調波から基準搬
送波全再生すること全可能とし4相2相の共用化7計っ
たことを特徴とするつげ)発明の男施例 以下本発明の1実施例につま図に従って説明する。
te+ Structure of the Invention In order to achieve all of the above objects, the present invention provides a four-phase phase change filter.
By installing the entire switch circuit on one side of the orthogonal control signal system of the Cosdas type carrier wave regeneration circuit that fully regenerates the reference carrier from the i-wave, it is possible to fully regenerate the reference carrier from the two-phase phase modulated wave, making it possible to fully regenerate the reference carrier from the two-phase phase modulated wave. 7) Embodiment of the Invention One embodiment of the present invention will be described below with reference to the drawings.

第5図eよ不発明の実施例の搬送波再生回路のブロック
図である。
FIG. 5e is a block diagram of a carrier recovery circuit according to an embodiment of the present invention.

図中第2図と同一機能のものは同一記号で示す。Components in the figure that have the same functions as those in FIG. 2 are indicated by the same symbols.

13けスイノ(孕示す。13ke Suino (pregnant).

第5図は、第2図の従来例の4相コスタスループの回路
のダーW器11と加算612の間にスイッチ134設け
たものである。従っ゛Cスイッチ]3が接続状態の時は
従来の4相コスダスIレーブト同シである。このスイッ
チ13t−断とするさ、加算器12の出力はスイッチ1
3側から像号がこガいので、第4図紮用いて説、明する
と、第2図の場合で説明し、た山に示す家3v器10の
出力信号が其の侭出力づれる。この信号Th11−ブー
フイルダ6′を介してV C()7’に印加L2て山に
示す信号がi点になるよ%VT:07’の位相が制御さ
れる。2相変調波はディジダル値により人力信号とVC
O7’の出力信号の位相差ブISOにkつたりπになっ
たり変化する。
FIG. 5 shows a circuit in which a switch 134 is provided between the DW circuit 11 and the adder 612 in the conventional four-phase Costas loop circuit shown in FIG. Therefore, when the [C switch] 3 is in the connected state, it is the same as the conventional 4-phase cosda I control. When this switch 13t is turned off, the output of the adder 12 is
Since the image signal is high from the 3rd side, we will explain it using Figure 4.The case of Figure 2 will be explained, and the output signal of the 3V device 10 shown in the left side will be shifted from its side output. The phase of %VT:07' is controlled such that the signal Th11 is applied to V C ()7' via the boo fielder 6' and the signal shown at the peak becomes the point i. The two-phase modulated wave is divided into human signal and VC by digital value.
The phase difference of the output signal of O7' changes from k to π.

【7かし第5図の回路で嬬加脛器12の出力は、0の時
は第4図(ト)のり点、πの時はヌ点付近に移動し、い
ずれも0の切る所が同じ位相の変化方向であるのでVC
(17/の位相全同期烙すのに同じよう姓−働きVC0
7’2安定した位相回期状態に引込む。
[7] However, in the circuit shown in Fig. 5, the output of the oscillator 12 moves to the glue point (G) in Fig. 4 when it is 0, and to the vicinity of the N point when it is π; Since the direction of change in phase is the same, VC
(17/ phase all synchronization
7'2 Draw into a stable phase rotation state.

こねによりVC07′の出力にて2相位相変調波からも
基準搬送波が再生される。尚lヨPF:、”、4’の出
力2o、を判別回路に送っているか、この場合け■、P
F2’の出力が十最大の場合(位相差0)及び−最大の
場合(位相差π)けLPF、s’の出力は共に()であ
るのでこの十最大の場合及び−最大の場合で入力信号?
変調した子ィジタルPを求めることが出来る。以上の如
く、スイッチ13を接続状卵(CすれIi4相(XT相
変勲波用の搬送波再生回路となりスイッチi3を断にす
れ(ば2相位相変調波の間に入れた場合tit 1加W
器12の出力は第4図(弓に示す如くになり、入力信号
とVCO7’の位相が0の1痔はル点πの時はオ点付近
に移動しいづれもOi切る所が同じ位相変化方向である
のでVCO7’の位相全回期シすのには同じよらに働き
VCO7’會安デした位相同量状態に引込む。従ってこ
のようにしてもよい。
By kneading, the reference carrier wave is also reproduced from the two-phase phase modulated wave at the output of VC07'. In addition, whether the output 2o of PF:,",4' is sent to the discrimination circuit, in this case,
When the output of F2' is 10 maximum (phase difference 0) and - maximum (phase difference π), the output of LPF and s' are both (), so input in the case of 10 maximum and -maximum. signal?
The modulated child digital P can be obtained. As described above, when the switch 13 is connected to the carrier wave regeneration circuit for the 4-phase (XT phase-modulated wave), the switch 13 is turned off (if it is inserted between the 2-phase phase modulated waves
The output of the device 12 is as shown in Fig. 4 (arrow), and when the phase of the input signal and the VCO 7' is 0, it moves to the vicinity of the O point when the input signal and the VCO 7' are at the Le point π. Since it is in the same direction, it works in the same way to complete all the phase cycles of the VCO 7' and pull the VCO 7' into a stable phase-equal state.Therefore, it may be done in this manner.

(釦 発明の効用 以」二詳細に説明せる如く本発明により 4相のコスタ
ス型子送波再生回路t2相の位相変調波から基準搬送波
全再生する回路に共用出来るので小形化出来る乏共に低
価格化が実現出来又回路規模がホ嘱く々るので高信頼化
が実現出来る効果がある。
(Button: Effects of the Invention) As explained in detail in 2, the present invention provides a 4-phase Costas-type slave transmission regeneration circuit.It can be used in common with the circuit that fully regenerates the reference carrier wave from the phase modulated wave of the 2-phase, so it can be made smaller and less expensive. This has the effect of realizing high reliability because the circuit scale is large.

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

第1図は従来例の2相のコスダスループ回路のブロック
図、第2図は従来例の4相コスタス!レ一プ回路のブロ
ック図、第3図は第1図の場合のコスダスループの安定
点全説明する波形のタイム千−−ト、第4図は第2図の
場合のコスタスループの安定点全説明する波形のダイム
チヤード、WJS図は本発明の実施例の搬送波再生回路
のブロック図である。 図中1.1’、:’1,5.5’、10.11は東算器
、2゜4.2’、4’は低域r波器、6,6′はループ
フィtレダ、7.7′は電圧制御型発振器、8,8/は
90度位相器、9.9′は比較器、12は加算器、13
はスイッチ?示す。 ]絡− ヤラ尼
Figure 1 is a block diagram of a conventional 2-phase Kosda loop circuit, and Figure 2 is a conventional 4-phase Kosda loop circuit. A block diagram of the loop circuit. Figure 3 is a time chart of the waveform that explains all the stable points of the Kostas loop in the case of Figure 1. Figure 4 shows all the stable points of the Costas loop in the case of Figure 2. The Dimechard and WJS diagram of the waveform shown in FIG. In the figure, 1.1', :'1, 5.5', 10.11 are Tosaiki, 2゜4.2', 4' are low-frequency r wave generators, 6, 6' are loop fit radars, 7 .7' is a voltage controlled oscillator, 8,8/ is a 90 degree phase shifter, 9.9' is a comparator, 12 is an adder, 13
Is it a switch? show. ] Connection - Yara-ni

Claims (1)

【特許請求の範囲】[Claims] 4相位相変調波から基準搬送波i再生するコスタス型搬
送波再生回路の直交制御信号系の一方にスイッチ回路を
設けこのスイッチ全所とすることKより2相位相変調波
から基準搬送波を再生すること?可能とし六−こと全特
徴とする搬送波再生回路っ
Is it possible to provide a switch circuit on one side of the orthogonal control signal system of a Costas-type carrier wave regeneration circuit that regenerates a reference carrier wave i from a four-phase phase modulated wave, and to use this switch at all locations?Is it possible to regenerate a reference carrier wave from a two-phase phase modulated wave from K? A carrier wave regeneration circuit with all six features
JP57097957A 1982-06-08 1982-06-08 Reproducing circuit of carrier wave Pending JPS58215156A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57097957A JPS58215156A (en) 1982-06-08 1982-06-08 Reproducing circuit of carrier wave

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57097957A JPS58215156A (en) 1982-06-08 1982-06-08 Reproducing circuit of carrier wave

Publications (1)

Publication Number Publication Date
JPS58215156A true JPS58215156A (en) 1983-12-14

Family

ID=14206142

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57097957A Pending JPS58215156A (en) 1982-06-08 1982-06-08 Reproducing circuit of carrier wave

Country Status (1)

Country Link
JP (1) JPS58215156A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63234759A (en) * 1987-03-24 1988-09-30 Hitachi Ltd Carrier recovery device
JPH022769A (en) * 1988-06-17 1990-01-08 Oki Electric Ind Co Ltd Demodulation circuit
JP2016500217A (en) * 2012-10-01 2016-01-07 パーク、ジョシュアPARK,Joshua RF carrier synchronization and phase alignment method and system

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63234759A (en) * 1987-03-24 1988-09-30 Hitachi Ltd Carrier recovery device
JPH022769A (en) * 1988-06-17 1990-01-08 Oki Electric Ind Co Ltd Demodulation circuit
JP2016500217A (en) * 2012-10-01 2016-01-07 パーク、ジョシュアPARK,Joshua RF carrier synchronization and phase alignment method and system

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