2006 Fortieth Asilomar Conference on Signals, Systems and Computers 2006
DOI: 10.1109/acssc.2006.354795
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A Bandwidth Efficient Constant Envelope Modulation

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Cited by 4 publications
(5 citation statements)
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“…Other techniques for designing the pulse shaping filters that have been reported are based on optimization techniques with a specific objective function such as maximizing the robustness against timing jitter [2,3,[8][9][10] minimizing the duration of the impulse response [11][12][13] or minimizing the peak to average power ratio (PAPR) at the transmitter filter output [14]. Besides the complex way of calculating 2 EURASIP Journal on Advances in Signal Processing the filter coefficients, filters that are obtained by optimization techniques are usually of nonlinear phase [11,12] or they cannot be directly partitioned into matched filter pairs [2,3,[8][9][10][15][16][17] having linear phase characteristic. The same holds true for the IIR Nyquist filters as discussed in [17,18].…”
Section: Introductionmentioning
confidence: 99%
“…Other techniques for designing the pulse shaping filters that have been reported are based on optimization techniques with a specific objective function such as maximizing the robustness against timing jitter [2,3,[8][9][10] minimizing the duration of the impulse response [11][12][13] or minimizing the peak to average power ratio (PAPR) at the transmitter filter output [14]. Besides the complex way of calculating 2 EURASIP Journal on Advances in Signal Processing the filter coefficients, filters that are obtained by optimization techniques are usually of nonlinear phase [11,12] or they cannot be directly partitioned into matched filter pairs [2,3,[8][9][10][15][16][17] having linear phase characteristic. The same holds true for the IIR Nyquist filters as discussed in [17,18].…”
Section: Introductionmentioning
confidence: 99%
“…Since (5) implies that p(t -nT)p* (t) = 0 for all t whenever 1n2 > g, (10) yields g -1 distinct complex constraints and one real constraint on the coefficients ck [Note: (10) for n is redundant with (10) for -n]. These constraints are:…”
Section: B Zero Intersymbol Interferencementioning
confidence: 99%
“…p(t) = 0 V/t , [-gT/2, gT/2] where g is chosen to be a positive integer. The Fourier series supplies a sufficiently general way to express such a pulse shape: p(t) = p(t)rect (iT) (5) Therefore, (5) and (7) imply that the Fourier Transform of p(t) can be written as kmax P(f) = gT E cksinc(gTf -k) (8) k:=-kTnax Note that (8) implies that the first positive null in the pulse's spectrum occurs at f = (kmax + 1)/gT. Therefore, we can control the width of the central lobe of the spectrum by proper choice of kmax.…”
Section: A Pulse Durationmentioning
confidence: 99%
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