| Table of contents | |
| Detection (Demodulation) of DSB-SC | |
| Power and bandwidth considerations | |
| Advantages | |
| Disadvantages | |
| Applications | |
| Practical notes and concluding remarks |
DSB-SC stands for Double Sideband Suppressed Carrier. It is an amplitude-modulation scheme in which the two sidebands that carry the information are transmitted but the carrier component is intentionally not transmitted (it is suppressed). The carrier contains no information; transmitting it wastes transmitter power. By suppressing the carrier, the available transmitter power is concentrated in the sidebands that carry the modulating information, improving power efficiency.
A common method to generate a DSB-SC signal is by using a product (multiplier) modulator. The modulated signal is the product of the baseband (modulating) signal and a sinusoidal carrier.

If the baseband (message) signal is x(t) and the carrier is cos(ωct), the transmitted DSB-SC signal is produced by multiplying these two signals. Using the frequency-shifting property of the Fourier transform, multiplication in time corresponds to frequency translation (convolution) in the frequency domain.
By the frequency-shifting property of the Fourier transform:

The result of multiplication with a cosine carrier places copies of the baseband spectrum around +ωc and -ωc, producing only the two sidebands and no carrier impulse at ω = 0.

Consider a sinusoidal message (for clarity of algebra) and a sinusoidal carrier:
x(t) = Ax cos(2πfxt)
c(t) = Ac cos(2πfct)
The product at the modulator output is s(t) = x(t)·c(t).
Derivation (each step on a separate line):
Ax cos(2πfxt) · Ac cos(2πfct)
= AxAc · cos(2πfxt) cos(2πfct)
= (AxAc/2) · [cos 2π(fc + fx)t + cos 2π(fc - fx)t]
Thus the modulated signal consists of two sinusoidal components at frequencies fc + fx (upper sideband) and fc - fx (lower sideband).

From the frequency locations:
fmax = fc + fx
fmin = fc - fx
Bandwidth, BW = fmax - fmin = 2 fx
Hence, for a baseband signal whose highest frequency is fx, the DSB-SC transmission occupies a total bandwidth of 2 fx, symmetrically placed about the carrier frequency.
To remove the carrier while preserving the sidebands, a balanced modulator (balanced mixer) is commonly used. The principle is that a nonlinear device produces products (sum and difference frequencies) when two signals are applied; a balanced arrangement cancels the carrier terms while retaining the desired product terms that give the sidebands.
A balanced modulator can be implemented using diodes, transistors or FETs in a bridge/transformer arrangement so that carrier components cancel at the output.

In the diode balanced modulator shown, the message x(t) is applied such that the two diode legs see the carrier with opposite phase for the message component. The instantaneous inputs at the two diode legs may be written as:
v1 = cos ωct + x(t)
v2 = cos ωct - x(t)
Each diode is a nonlinear device. Represent its I-V characteristic by a power series (Taylor expansion) about the operating point:
i(v) = a v + b v² + higher-order terms
The diode currents are therefore (writing the first two nonzero terms):
i1 = a [cos ωct + x(t)] + b [cos ωct + x(t)]² + ...

i2 = a [cos ωct - x(t)] + b [cos ωct - x(t)]² + ...

The output voltage across the load R is proportional to the difference of these diode currents:
vo = R [i1 - i2]
On expanding and cancelling identical terms the even powers of the carrier that are common to i1 and i2 are removed, while terms odd in x(t) remain. Keeping the dominant terms gives:
vo = 2 a R x(t) + 4 b R x(t) cos ωct + higher-order products
Interpretation:
The unwanted baseband feedthrough is usually removed by a band-pass filter (tuned LC network) centred at the carrier frequency, leaving the DSB-SC output:
vo ≈ K x(t) cos ωct, where K = 4 b R
Because the carrier is suppressed, envelope detectors (which rely on a carrier envelope) cannot recover the message from DSB-SC. Synchronous (coherent) detection is required; this means the receiver must multiply the received DSB-SC signal by a locally generated carrier having the same frequency and phase as the transmitter carrier, then low-pass filter the product to obtain the baseband.
Suppose the received DSB-SC signal is r(t) = K x(t) cos ωct (noise and channel effects omitted). The receiver multiplies r(t) by a locally generated carrier cos(ωct + φ):
r(t) · cos(ωct + φ) = K x(t) cos ωct · cos(ωct + φ)
= (K/2) x(t) [cos φ + cos(2 ωct + φ)]
After passing this product through a low-pass filter, the high-frequency term cos(2 ωct + φ) is removed and the recovered baseband is:
(K/2) x(t) cos φ
Therefore demodulation requires the receiver carrier to be phase-synchronised with the transmitter carrier (φ ≈ 0). A phase error reduces recovered amplitude by a factor cos φ and can even invert polarity for large phase errors. Practical receivers use carrier-recovery techniques such as Costas loops or pilot carriers where available.
Power: in DSB-SC all transmitted power appears in the sidebands that carry information; the carrier component carries no power because it is not transmitted. This is why DSB-SC is often described as having very high modulation efficiency: none of the transmitted power is wasted on an uninformative carrier.
Bandwidth: the DSB-SC signal occupies a bandwidth equal to twice the highest frequency present in the baseband (BW = 2 fm,max). This is the same occupied bandwidth as a DSB-FC system (DSB-SC simply removes the carrier spectral line but leaves the sidebands unchanged in width).
DSB-SC is a fundamental modulation technique taught in communication systems because it illustrates multiplication in time, spectral translation, and the need for coherent detection. It offers better power efficiency than conventional AM but at the expense of receiver complexity. Balanced modulators and mixers are practical implementations that cancel unwanted carrier components while producing the desired sideband products. Understanding DSB-SC prepares one for related techniques such as single-sideband (SSB) modulation and coherent digital modulation schemes.
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