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Prof. Brian L. Evans Dept. of Electrical and Computer Engineering The University of Texas at Austin. Quadrature Amplitude Modulation (QAM) Transmitter. Introduction.
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Prof. Brian L. Evans Dept. of Electrical and Computer Engineering The University of Texas at Austin Quadrature Amplitude Modulation (QAM) Transmitter
Introduction • Digital Pulse Amplitude Modulation (PAM) modulates digital information onto amplitude of pulse and may be later modulated by sinusoid • Digital Quadrature Amplitude Modulation (QAM) is two-dimensional extension of digital PAM that requires sinusoidal modulation • Digital QAM modulates digital information onto pulses that are modulated onto Amplitudes of a sine and a cosine, or equivalently Amplitude and phase of single sinusoid
Y(w) ½F(w + wc) ½F(w - wc) F(w) ½ 1 w -wc - w1 -wc + w1 wc - w1 wc + w1 0 -wc wc w -w1 w1 0 Review Amplitude Modulation by Cosine • Example:y(t) = f(t) cos(wct) Assume f(t) is an ideal lowpass signal with bandwidth w1 Assume w1 < wc Y(w) is real-valued if F(w) is real-valued • Demodulation: modulation then lowpass filtering • Similar derivation for modulation with sin(w0 t)
Y(w) j ½F(w + wc) -j ½F(w - wc) F(w) j ½ 1 wc wc - w1 wc + w1 w -wc - w1 -wc + w1 -wc w -j ½ -w1 w1 0 Review Amplitude Modulation by Sine • Example: y(t) = f(t) sin(wct) Assume f(t) is an ideal lowpass signal with bandwidth w1 Assume w1 < wc Y(w) is imaginary-valued if F(w) is real-valued • Demodulation: modulation then lowpass filtering
an a*(t) Impulse modulator d[n] Serial/Parallel Map to 2-D constellation bit stream 1 J Impulse modulator bn b*(t) Pulse shaping gT(t) MatchedDelay s(t) + Local Oscillator 90o Pulse shaping gT(t) Matched delay matches delay through 90o phase shifter Digital QAM Modulator
Phase Shift by 90 Degrees • 90o phase shift performed by Hilbert transformer cosine => sine sine => – cosine • Frequency response of idealHilbert transformer:
Magnitude response All pass except at origin For fc > 0 Phase response Piecewise constant For fc < 0 f Hilbert Transformer 90o f -90o
Continuous-time ideal Hilbert transformer Discrete-time ideal Hilbert transformer 1/( t) if t 0 h(t) = 0 if t = 0 h(t) h[n] if n0 t h[n] = n 0 if n=0 Hilbert Transformer Even-indexed samples are zero
Discrete-Time Hilbert Transformer • Approximate by odd-length linear phase FIR filter Truncate response to 2 L + 1 samples: L samples left of origin, L samples right of origin, and origin Shift truncated impulse response by L samples to right to make it causal L is odd because every other sample of impulse response is 0 • Linear phase FIR filter of length N has same phase response as a delay of length (N-1)/2 (N-1)/2 is an integer when N is odd (here N = 2 L + 1) • How would you make sure that delay from local oscillator to sine modulator is equal to delay from local oscillator to cosine modulator?
Performance Analysis of PAM • If we sample matched filter output at correct time instances, nTsym, without any ISI, received signal where the signal component is v(t) output of matched filter Gr() for input ofchannel additive white Gaussian noise N(0; 2) Gr() passes frequencies from -sym/2 to sym/2 ,where sym = 2 fsym = 2 / Tsym • Matched filter has impulse response gr(t) v(nT) ~ N(0; 2/Tsym) 3 d for i = -M/2+1, …, M/2 d -d -3 d 4-PAM
Performance Analysis of PAM Filtered noise T = Tsym Noise power s2d(t1–t2)
O- I I I I I I O+ -7d -5d -3d -d d 3d 5d 7d Performance Analysis of PAM • Decision errorfor inner points • Decision errorfor outer points • Symbol error probability 8-PAM Constellation
Performance Analysis of QAM • Received QAM signal • Information signal s(nT) where i,k { -1, 0, 1, 2 } for 16-QAM • Noise, vI(nT) and vQ(nT) are independent Gaussian random variables ~ N(0; 2/T)
Q 2 2 3 3 1 1 2 2 I 2 2 1 1 3 3 2 2 16-QAM Performance Analysis of QAM • Type 1 correct detection
Q 2 2 3 3 1 1 2 2 I 2 2 1 1 3 3 2 2 16-QAM Performance Analysis of QAM • Type 2 correct detection • Type 3 correct detection
Performance Analysis of QAM • Probability of correct detection • Symbol error probability
Average Power Analysis • PAM and QAM signals are deterministic • For a deterministic signal p(t), instantaneous power is |p(t)|2 • 4-PAM constellation points: { -3 d, -d, d, 3 d } • Total power 9 d2 + d2 + d2 + 9 d2 = 20 d2 • Average power per symbol 5 d2 • 4-QAM constellation points: { d + j d, -d + j d,d – j d, -d – j d } • Total power 2 d2 + 2 d2 + 2 d2 + 2 d2 = 8 d2 • Average power per symbol 2 d2