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DSB-AM, DSB-SC and SSB spectra; synchronous detection

Short answer

DSB-AM transmits carrier and both sidebands (BW=2W, envelope detection). DSB-SC suppresses carrier (BW=2W, coherent detection). SSB transmits one sideband (BW=W, coherent). DSB-SC detection is synchronous because the receiver must regenerate a carrier locked in frequency and phase to the suppressed carrier; any phase error reduces output by cosφ, and 90° error gives zero output.

Compare the basics of DSB-AM, DSB-SC and SSB modulations with their respective spectrum? Why DSB-SC detection is known as synchronous detection, explain with required details?

Comparison of DSB-AM, DSB-SC and SSB

For message spectrum M(f)M(f) band-limited to WW:

PointDSB-AM (FC)DSB-SCSSB
ExpressionAc[1+kam(t)]cos⁡ωctA_c[1 + k_am(t)]\cos\omega_ctAcm(t)cos⁡ωctA_cm(t)\cos\omega_ctAc2[mcos⁡ωct∓m^sin⁡ωct]\frac{A_c}{2}[m\cos\omega_ct \mp \hat m\sin\omega_ct]
CarrierPresentAbsentAbsent
Bandwidth2W2W2W2WWW
Efficiency≤ 33.3%100%100%
DetectionEnvelopeCoherentCoherent

Spectra

 DSB-AM:          carrier
          LSB      |      USB
         /////     |     \\\\\
 -------+-----+----+----+-----+------> f
      fc-W        fc         fc+W

 DSB-SC:  LSB    (no carrier)   USB
         /////                 \\\\\
 -------+-----+----+----+-----+------> f
      fc-W        fc         fc+W

 SSB (USB):                    USB
                              \\\\\
 ------------------+----------+------> f
                  fc         fc+W

Why DSB-SC detection is synchronous

DSB-SC has no carrier, and its envelope is ∣m(t)∣|m(t)|, not m(t)m(t); the carrier phase reverses each time m(t)m(t) crosses zero. So an envelope detector would give ∣m(t)∣|m(t)| (distorted). The message can be recovered only by multiplying with a local carrier that is synchronised in frequency and phase with the transmitter carrier, hence "synchronous detection".

 s(t) --->( X )---> LPF ---> vo(t)
            ^
     cos(wc t + phi)   (from carrier recovery)
vo(t)=LPF{Acm(t)cos⁡ωctcos⁡(ωct+ϕ)}=Ac2m(t)cos⁡ϕv_o(t) = \text{LPF}\{A_cm(t)\cos\omega_ct\cos(\omega_ct + \phi)\} = \frac{A_c}{2}m(t)\cos\phi
  • ϕ=0\phi = 0: output Ac2m(t)\tfrac{A_c}{2}m(t), ideal.
  • ϕ≠0\phi \ne 0: attenuation by cos⁡ϕ\cos\phi; at ϕ=90∘\phi = 90^\circ the output vanishes (quadrature null).
  • Frequency error Δω\Delta\omega: output ∝m(t)cos⁡Δωt\propto m(t)\cos\Delta\omega t, a beating distortion.

Hence exact synchronisation is required, provided by a pilot carrier, squaring loop or Costas loop.

✓ Answer checked by Claude Opus 5.5 (high effort)

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