JP2698979B2 - Carrier recovery method in PSK demodulator - Google Patents

Carrier recovery method in PSK demodulator

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Publication number
JP2698979B2
JP2698979B2 JP63080170A JP8017088A JP2698979B2 JP 2698979 B2 JP2698979 B2 JP 2698979B2 JP 63080170 A JP63080170 A JP 63080170A JP 8017088 A JP8017088 A JP 8017088A JP 2698979 B2 JP2698979 B2 JP 2698979B2
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JP
Japan
Prior art keywords
phase
output
carrier
frequency
phases
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 - Fee Related
Application number
JP63080170A
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Japanese (ja)
Other versions
JPH01253346A (en
Inventor
賢一 藤本
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Japan Radio Co Ltd
Original Assignee
Japan Radio Co Ltd
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Filing date
Publication date
Application filed by Japan Radio Co Ltd filed Critical Japan Radio Co Ltd
Priority to JP63080170A priority Critical patent/JP2698979B2/en
Publication of JPH01253346A publication Critical patent/JPH01253346A/en
Application granted granted Critical
Publication of JP2698979B2 publication Critical patent/JP2698979B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、PSK信号復調器における搬送波再生方式に
関する。
Description: TECHNICAL FIELD The present invention relates to a carrier recovery system in a PSK signal demodulator.

(従来の技術) 従来、一般的なPSK復調回路では信号入力時においてV
COの周波数及び位相が定まっていないため、搬送波再生
用PLLのループ帯域を引き込みの初期段階で広目に設定
して再生動作を開始していた。
(Prior art) Conventionally, in a general PSK demodulation circuit, V
Since the frequency and phase of the CO are not fixed, the loop operation of the PLL for carrier wave reproduction was set to a wide value at the initial stage of pull-in, and the reproduction operation was started.

(本発明が解決しようとする課題) しかし、そのような方式では搬送波を再生し始めて、
トラッキングループが定常状態に到達するまでに要する
時間は、受信波のC/Nが小さい場合にはかなりの長さが
必要であった。
(Problems to be solved by the present invention) However, in such a system, the carrier wave is regenerated,
The time required for the tracking loop to reach the steady state required a considerable length when the C / N of the received wave was small.

(課題を解決するための手段) 本発明はこのような欠点を解決するため、位相制御さ
れた再生搬送波を出力する位相制御用VCOと、この出力
波と受信搬送波の位相を比較する同相(I)、直交
(Q)チャンネルの位相比較回路と、位相比較回路の出
力から雑音等を除去するI、Q両チャンネルの符号間干
渉除去用ローパスフィルタと、フィルタから出力される
I、Q両チャンネルの信号をサンプリングするサンプラ
と、サンプラの出力から再生搬送波の位相誤差を検出す
る位相誤差検出器と、位相誤差信号を平滑して前記位相
制御用VCOに供給するループフィルタとで構成されるPSK
同期形直交復調器において、前記サンプラの出力値から
信号位相空間上での角度を導出する逆正接器と、導出さ
れた角度を相数倍する乗算器と、相数倍された角度に対
応する同相成分と直交成分を導出する正弦余弦成分の計
算器と、導出された同相、直交データをもとに複素フー
リエ変換して強度の最も強い周波数を算出する複素フー
リエ変換器と、算出された周波数を相数で除算し受信搬
送波と再生搬送波との周波数差を得る分周器と、この分
周器の出力と前記逆正接器の出力とから位相差を計算す
る位相推定器とを備えて、搬送波再生の初期において、
前記分周器の出力と前記位相推定器の出力とで位相制御
用VCOを制御することにより、小型化、集積化に有利な
ベースバンド上の処理で、変調波を逓倍してから分周し
て搬送波の周波数と位相を抽出する逓倍法と等価的な効
果を得るようにしたものである。
(Means for Solving the Problems) In order to solve such a drawback, the present invention provides a phase control VCO for outputting a phase-controlled reproduced carrier, and an in-phase (I) for comparing the phase of the output wave with the phase of a received carrier. ), A quadrature (Q) channel phase comparison circuit, a low-pass filter for removing intersymbol interference between I and Q channels for removing noise and the like from the output of the phase comparison circuit, and a I / Q channel output from the filter. A PSK comprising a sampler for sampling a signal, a phase error detector for detecting a phase error of the reproduced carrier from the output of the sampler, and a loop filter for smoothing the phase error signal and supplying the same to the phase control VCO.
In the synchronous quadrature demodulator, an arctangent that derives an angle in a signal phase space from an output value of the sampler, a multiplier that multiplies the derived angle by the number of phases, and an angle corresponding to the angle multiplied by the number of phases. A sine-cosine component calculator for deriving an in-phase component and a quadrature component, a complex Fourier transformer for performing a complex Fourier transform based on the derived in-phase and quadrature data to calculate a frequency having the strongest intensity, and a calculated frequency A frequency divider that divides the number of phases by the number of phases to obtain a frequency difference between the received carrier and the recovered carrier, and a phase estimator that calculates a phase difference from the output of the frequency divider and the output of the arctangent, At the beginning of carrier recovery,
By controlling the phase control VCO with the output of the frequency divider and the output of the phase estimator, processing on the baseband that is advantageous for miniaturization and integration reduces the frequency of the modulated wave before dividing it. Thus, an effect equivalent to the multiplication method for extracting the frequency and phase of the carrier is obtained.

以下実施例につき図面により詳細に説明する。 Hereinafter, embodiments will be described in detail with reference to the drawings.

(実施例) 第1図は本発明を0(オフセット)−QPSK(n=2)
復調器に適用した場合の構成図を示す。その原理と動作
につき述べる。なお同図の各部分については、本発明に
関連するものを除き一部説明を略す。
(Embodiment) FIG. 1 shows the present invention as 0 (offset) -QPSK (n = 2).
FIG. 3 shows a configuration diagram when applied to a demodulator. The principle and operation will be described. Note that the description of each part of the drawing is partially omitted except for those related to the present invention.

初期段階では、モード設定スイッチ22は、Sの位置に
セットする。PSK波受信端子1より雑音が付加されてい
ない信号波を受信した場合には、モニタ端子9,10におい
て、それぞれ第2図のI,Qの曲線のような信号波形が観
測される。但し、搬送波と位相制御用VCO2との位相差Δ
ψ次第で、第2図(a)や(b)の例のように様子が違
うため、Δψが逐次変わって行く場合には、たとえ送信
データ・パターンが同じでも、モニタ端子9,10に表われ
る波形はΔψとともに変化して行く。また、雑音、フェ
ージング等が付加された場合は上記I,Qの信号曲線が歪
むことになる。
At the initial stage, the mode setting switch 22 is set to the position S. When a signal wave to which noise is not added is received from the PSK wave receiving terminal 1, signal waveforms such as curves I and Q in FIG. 2 are observed at the monitor terminals 9 and 10, respectively. However, the phase difference Δ between the carrier and the phase control VCO2
Depending on ψ, the appearance is different as in the examples of FIGS. 2 (a) and (b), so if Δψ changes successively, even if the transmission data pattern is the same, the data is displayed on the monitor terminals 9 and 10. The waveform that is displayed changes with Δψ. When noise, fading, and the like are added, the I and Q signal curves are distorted.

この信号波は、クロック再生器8から出力されるサン
プリング・クロックのタイミング調整により、信号位相
空間上の情報をもつ各々のデータスロットの中点でサン
プリングされるようにする。このサンプラ11,12の出力
を毎回逆正接器13に入力して(1)式の計算を行ない、
信号位相空間上の角度ψを求める。但しこの際にはI,
Qの2系列のデータ符号を考慮し、0≦ψ<2πの範
囲内で求める。第3図(a)にこの様子を示す。
This signal wave is sampled at the midpoint of each data slot having information on the signal phase space by adjusting the timing of the sampling clock output from the clock regenerator 8. The outputs of the samplers 11 and 12 are input to the arctangent 13 each time, and the equation (1) is calculated.
Determining the angle [psi K on the signal phase space. However, in this case, I,
In consideration of the data codes of the two sequences of Q, it is determined within the range of 0 ≦ ψ K <2π. FIG. 3A shows this state.

ψ=tan-1(QK/IK),0≦ψ<2π ……(1) しかし、この状態では(a)に示すようにI,Qの2系
列データ・パターンによる4通りの位相不確定性がある
ので、位相ψを乗算器(4倍器)14で4倍し、第3図
(b)のようにパターン依存性を除いた形にする。
ψ K = tan −1 (Q K / I K ), 0 ≦ ψ K <2π (1) However, in this state, as shown in FIG. since there is a phase ambiguity, the phase [psi K multiplier (4 doubler) 14 4 multiplies, in the form except for the pattern dependence as FIG. 3 (b).

次に、この4倍した位相4ψに対応する時間軸上の
同相成分I′K,直交成分Q′を同相、直交成分計算器
15で(2)式により求める。
Then, in-phase component I 'K, quadrature component Q' on the time axis corresponding to the 4 times the phase 4Pusai K phase of K, quadrature component calculator
In step 15, the value is obtained by equation (2).

I′=cos(4ψ),Q′=sin(4ψ) ……(2) 4倍位相の回転周波数は複素フーリエ変換によって求
めるので、必要とする周波数分解能を保証する個数(M
個)分のサンプリング・データに対して、(1)式,
(2)式の処理を行なってI′K,Q′をメモリにスト
アする。
I 'K = cos (4ψ K ), Q' since the rotational frequency of K = sin (4ψ K) ...... (2) 4 -fold phase determined by a complex Fourier transformation, the number to ensure frequency resolution requires (M
Equation (1),
By performing the processing of the equation (2), I ' K and Q' K are stored in the memory.

複素フーリエ変換器16では(3)式のような形で各Δ
f′に対して計算し、強度Aの最も強い周波数Δf′を
選出する。
In the complex Fourier transformer 16, each Δ
Calculation is performed on f ′, and the frequency Δf ′ having the highest intensity A is selected.

求めたΔf′は、搬送波と位相制御用VCO2との周波数
差の4倍になっているので、(4)式のような操作を行
なう。即ち、1/4倍器17に通して所望のビート周波数Δ
fを得る。
Since the obtained Δf ′ is four times the frequency difference between the carrier and the phase control VCO 2, the operation shown in equation (4) is performed. That is, the desired beat frequency Δ
Get f.

Δf=1/4・Δf′ ……(4) また、位相推定器18では(5)式の計算を行ない、サ
ンプリング期間の最終時点での位相差Δψを、サンプリ
ング期間中の各位相情報ψと位相回転速度Δfとから
導出する。但し、計算はmadulo−2πで行なう。
Δf = 1/4 · Δf ′ (4) Further, the phase estimator 18 calculates the expression (5), and calculates the phase difference Δψ at the end of the sampling period by each phase information K K during the sampling period. And the phase rotation speed Δf. However, the calculation is performed with madulo-2π.

上式でπ/4を引くのは、信号点の位相と基準の軸がπ
/4だけシフトしていることによる。
Subtracting π / 4 in the above equation means that the phase of the signal point and the reference axis are π
Due to shifting by / 4.

以上のように、初期周波数差Δfと初期位相差Δψを
求めて、電圧変換器19でVCO初期設定用制御電圧に変換
した後、モード設定スイッチ22をIの位置にして初期化
をする。その後は、スイッチ22をTの位置にしてトラッ
キングモードに切り換え、I,Q両系列のサンプリング・
データから直接に位相誤差を位相誤差検出器20で検出
し、ループフィルタ21で平均化するPLL動作を開始す
る。
As described above, after the initial frequency difference Δf and the initial phase difference Δψ are obtained and converted into the VCO initial setting control voltage by the voltage converter 19, the mode setting switch 22 is set to the position I for initialization. Thereafter, the switch 22 is switched to the T position to switch to the tracking mode, and sampling and sampling of both I and Q sequences are performed.
The phase error is directly detected from the data by the phase error detector 20 and the PLL operation for averaging by the loop filter 21 is started.

なお、上記の説明では、オフセット−QPSK(n=2)
の復調器を例にとったが、本発明はこれに限るものでは
なく、2相PSK、4相PSK、8相PSK等に対してもそれぞ
れn=1,2,3とした上で、同様の手法が適用できる。
In the above description, offset-QPSK (n = 2)
Although the present invention is not limited to this, the present invention is not limited to this, and it is assumed that n = 1, 2, and 3 for 2-phase PSK, 4-phase PSK, 8-phase PSK, etc. Can be applied.

(発明の効果) 以上述べたように、直交するI,Q両チャンネルのサン
プリング信号の位相空間上の位置が示す角度を、変調デ
ータパターンによる位相不確定性を取り除くために2n
した後にその回転周波数を計算して1/2n倍することによ
り、PSK変調がかかった信号状態のまま受信信号の搬送
波とローカルVCOの周波数ずれと位相ずれを、小型化、
集積化に有利なベースバンド上の処理で精度良く導出で
き、トラッキングによる定常的復調状態に到るまでの所
要時間の短縮が可能となる。
(Effects of the Invention) As described above, the angle indicated by the position in the phase space of the sampling signals of the orthogonal I and Q channels is multiplied by 2 n in order to remove the phase uncertainty due to the modulation data pattern. By calculating the rotation frequency and multiplying by 1/2 n , the frequency shift and phase shift between the carrier of the received signal and the local VCO can be reduced while maintaining the signal state with PSK modulation.
It is possible to accurately derive by baseband processing which is advantageous for integration, and it is possible to reduce the time required until a steady demodulation state by tracking is reached.

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

第1図は本発明の搬送波再生方式によるPSK復調器の一
実施例を示す構成図、第2図は第1図のモニタ端子9,10
で観測される時間波形図で、(a)は搬送波とVCOの位
相差Δψが0、(b)はΔψ>0の場合の図、第3図
(a)は逆正接計算器13の出力ψの信号位相空間上で
の不確定を示す説明図、第3図(b)は2n倍器(n=
2)の出力4ψが一義性を示す説明図である。 1……PSK波受信端子、2……位相制御用VCO、3……π
/2移相器、4,5……位相検波器、6,7……符号間干渉除去
用ローパスフィルタ、8……クロック再生器、13……逆
正接器、14……2n倍器、15……同相、直交成分計算器、
16……複素フーリエ変換器、17……1/2n倍器、18……位
相推定器、22……モード設定スイッチ。
FIG. 1 is a block diagram showing an embodiment of a PSK demodulator using a carrier recovery system according to the present invention, and FIG. 2 is a diagram showing monitor terminals 9, 10 in FIG.
(A) is a diagram when the phase difference Δψ between the carrier and the VCO is 0, (b) is a diagram when Δψ> 0, and FIG. 3 (a) is an output の of the arctangent calculator 13. K explanatory diagram showing the uncertainty on the signal phase space, FIG. 3 (b) is 2 n multiplier (n =
Output 4Pusai K 2) is an explanatory view showing an unambiguous. 1 ... PSK wave receiving terminal, 2 ... VCO for phase control, 3 ... π
1/2 phase shifter, 4,5 phase detector, 6,7 low-pass filter for removing intersymbol interference, 8 clock regenerator, 13 arctangent, 14 2n multiplier, 15 ... In-phase, quadrature component calculator,
16: Complex Fourier transformer, 17: 1 / 2n multiplier, 18: Phase estimator, 22: Mode setting switch.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】位相制御された再生搬送波を出力する位相
制御用VCOと、この出力波と受信搬送波の位相を比較す
る同相(I)チャンネル及び直交(Q)チャンネルの位
相比較回路と、両位相比較回路の出力から雑音等を除去
するI、Q両チャンネルの符号間干渉除去用ローパスフ
ィルタと、両フィルタから出力されるI、Q両チャンネ
ルの信号をサンプリングするサンプラと、両サンプラの
出力から再生搬送波の位相誤差を検出する位相誤差検出
器と、この位相誤差信号を平滑して前記位相制御用VCO
に供給するループフィルタとで構成されるPSK同期形直
交復調器において、 前記両サンプラの出力値から信号位相空間上での角度を
導出する逆正接器と、導出された角度を相数倍する乗算
器と、相数倍された角度に対応する同相成分と直交成分
を導出する正弦余弦成分の計算器と、導出された同相、
直交両データをもとに複素フーリエ変換して強度の最も
強い周波数を算出する複素フーリエ変換器と、算出され
た周波数を相数で除算し受信搬送波と再生搬送波との周
波数差を得る分周器と、この分周器の出力と前記逆正接
器の出力とから位相差を計算する位相推定器とを備え
て、 搬送波再生の初期において前記ループフィルタからの出
力に代え、前記分周器の出力と前記位相推定器の出力と
で前記位相制御用VCOを制御して初期化するようにしたP
SK復調器における搬送波再生方式。
A phase control VCO for outputting a phase-controlled reproduced carrier, a phase comparison circuit for an in-phase (I) channel and a quadrature (Q) channel for comparing the phases of the output wave and a received carrier, A low-pass filter for removing inter-symbol interference of I and Q channels for removing noise and the like from the output of the comparison circuit, a sampler for sampling signals of both I and Q channels output from both filters, and reproduction from outputs of both samplers A phase error detector for detecting a phase error of a carrier, and a phase control VCO for smoothing the phase error signal.
A PSK-synchronous quadrature demodulator composed of a loop filter and an inverse tangent device that derives an angle in a signal phase space from output values of the two samplers, and a multiplication that multiplies the derived angle by the number of phases. And a calculator of a sine cosine component for deriving an in-phase component and a quadrature component corresponding to the angle multiplied by the number of phases, and the derived in-phase,
A complex Fourier transformer that calculates the highest frequency by performing a complex Fourier transform based on both orthogonal data, and a frequency divider that divides the calculated frequency by the number of phases to obtain a frequency difference between a received carrier and a reproduced carrier. And a phase estimator for calculating a phase difference from the output of the frequency divider and the output of the arctangent, and the output of the frequency divider replaces the output from the loop filter at the beginning of carrier wave recovery. And the output of the phase estimator controls and initializes the phase control VCO.
Carrier recovery method in SK demodulator.
JP63080170A 1988-03-31 1988-03-31 Carrier recovery method in PSK demodulator Expired - Fee Related JP2698979B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63080170A JP2698979B2 (en) 1988-03-31 1988-03-31 Carrier recovery method in PSK demodulator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63080170A JP2698979B2 (en) 1988-03-31 1988-03-31 Carrier recovery method in PSK demodulator

Publications (2)

Publication Number Publication Date
JPH01253346A JPH01253346A (en) 1989-10-09
JP2698979B2 true JP2698979B2 (en) 1998-01-19

Family

ID=13710856

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63080170A Expired - Fee Related JP2698979B2 (en) 1988-03-31 1988-03-31 Carrier recovery method in PSK demodulator

Country Status (1)

Country Link
JP (1) JP2698979B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01254040A (en) * 1988-04-01 1989-10-11 Sharp Corp Phase error detector for polyphase modulation wave

Also Published As

Publication number Publication date
JPH01253346A (en) 1989-10-09

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