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AM vs FM; error probability of coherent ASK

Short answer

AM has variable transmitted power, requires linear amplifiers, FOM ≤ 1/3, and simple envelope detection. FM has constant power, allows efficient class C amplifiers, FOM = 1.5β², but needs wider bandwidth and complex limiter/discriminator receivers. Coherent ASK error probability is P_e = ½erfc(√(E_b/2N_0)) = Q(√(E_b/N_0)), identical to BFSK and 3 dB worse than BPSK.

Compare A.M and F.M in terms of power efficiency and system complexity. Calculate the error probability of coherent ASK.

AM vs FM: power efficiency and complexity

PointAM (DSB-FC)FM
Transmitted powerVaries with modulation, Pc(1+μ2/2)P_c(1+\mu^2/2)Constant, Ac2/2A_c^2/2, independent of modulation
Useful (sideband) powerAt most 1/3 of total for a single tone (μ=1\mu=1)All power is useful; carrier power is redistributed to sidebands
Power amplifierLinear (class A/B) amplifiers needed after low-level modulation, lower efficiency (class C only in high-level modulation)Class C (non-linear), high efficiency, since envelope is constant
Noise performanceFOM ≤1/3\le 1/3 for a single toneFOM =32β2=\frac32\beta^2; much better for β>0.5\beta>0.5
Bandwidth2W2W2(β+1)W2(\beta+1)W (Carson), much wider
Transmitter complexitySimple (high-level collector/plate modulation)More complex (VCO, AFC/frequency stabilisation, multipliers)
Receiver complexityVery simple (diode envelope detector)Needs limiter, discriminator/PLL, de-emphasis
Noise immunityAmplitude noise directly affects outputLimiter removes amplitude noise; capture effect

So FM is more power efficient (better SNR per watt and efficient class C amplifiers) but uses more bandwidth and more complex circuits; AM is simpler and cheaper but wastes power in the carrier.

Error probability of coherent ASK

ASK (on–off keying) signals over 0≤t≤Tb0\le t\le T_b:

s1(t)=Acos⁡ωct  (bit 1),s2(t)=0  (bit 0)s_1(t)=A\cos\omega_ct\ \ (\text{bit }1),\qquad s_2(t)=0\ \ (\text{bit }0)

Coherent receiver (correlator = matched filter):

 r(t) -->(x)--> integrate --> sample --> y > lam ? 1 : 0
          ^       0..Tb       t=Tb
          |
       cos(wc t)  (local carrier, in phase)

Correlator output at t=Tbt=T_b, with r(t)=si(t)+w(t)r(t)=s_i(t)+w(t):

y=∫0Tbr(t)cos⁡ωct dt=ai+ny=\int_0^{T_b}r(t)\cos\omega_ct\,dt=a_i+n
  • Bit 1: a1=∫0TbAcos⁡2ωct dt=ATb2a_1=\int_0^{T_b}A\cos^2\omega_ct\,dt=\frac{AT_b}{2} (for fcf_c an integer multiple of 1/Tb1/T_b).
  • Bit 0: a2=0a_2=0.
  • Noise: n=∫0Tbw(t)cos⁡ωct dtn=\int_0^{T_b}w(t)\cos\omega_ct\,dt is Gaussian, mean 0, variance
σ2=∫0Tb ⁣ ⁣∫0TbN02δ(t−u)cos⁡ωctcos⁡ωcu dt du=N02⋅Tb2=N0Tb4\sigma^2=\int_0^{T_b}\!\!\int_0^{T_b}\frac{N_0}{2}\delta(t-u)\cos\omega_ct\cos\omega_cu\,dt\,du=\frac{N_0}{2}\cdot\frac{T_b}{2}=\frac{N_0T_b}{4}

Threshold midway: λ=ATb4\lambda=\frac{AT_b}{4}. Using the binary result Pe=12erfc⁡(a1−a222σ)P_e=\frac12\operatorname{erfc}\left(\frac{a_1-a_2}{2\sqrt2\sigma}\right):

a1−a222 σ=ATb/222N0Tb/4=ATb22N0=A2Tb8N0\begin{aligned} \frac{a_1-a_2}{2\sqrt2\,\sigma} &= \frac{AT_b/2}{2\sqrt2\sqrt{N_0T_b/4}}=\frac{A\sqrt{T_b}}{2\sqrt{2N_0}}=\sqrt{\frac{A^2T_b}{8N_0}} \end{aligned}

Energy of a "1" pulse is E1=A2Tb2E_1=\frac{A^2T_b}{2}; the average energy per bit (half the bits are 0) is Eb=E12=A2Tb4E_b=\frac{E_1}{2}=\frac{A^2T_b}{4}. Hence A2Tb8N0=Eb2N0\frac{A^2T_b}{8N_0}=\frac{E_b}{2N_0} and

Pe(ASK)=12erfc⁡(Eb2N0)=Q(EbN0)P_e(\text{ASK})=\frac12\operatorname{erfc}\left(\sqrt{\frac{E_b}{2N_0}}\right)=Q\left(\sqrt{\frac{E_b}{N_0}}\right)

(In terms of peak energy E1E_1: Pe=12erfc⁡E1/4N0P_e=\frac12\operatorname{erfc}\sqrt{E_1/4N_0}.)

✓ Answer checked by Claude Opus 5.5 (high effort)

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