Multiplying the frequency of a signal by a factor of N using an ideal frequency multiplier increases the phase noise of the multiplied signal by 20log(N) dB. Similarly dividing a signal frequency by N reduces the phase noise of the output signal by 20log(N) dB.
For the signal
f(t) = cos(ωt + θ)
Frequency multiplication by N multiplies the cosine function argument (ωt + θ) by N.
Consequently any phase noise term in the θ is also multiplied by N. (the phase noise is increased by 20log(N) dB).
For a frequency modulated signal
f(t) = cos (ωct + β sin(ωmt))
for small β
f(t) = cos ( ωct) + (β/2)[ cos( ωc - ωm)t - cos( ωc + ωm)t]
becomes after frequency multiplication by N
f(t) = cos(Nωct + Nβ sin(ωct))
for small Nβ
f(t) = cos(Nωct) + (Nβ/2)[cos(Nωc - ωm)t - cos(Nωc + ωm)t]
1) The sideband amplitude is increased by N. i.e by 20Log(N) dB.
2) The sideband offset from the carrier in the frequency multiplied signal is the same as for the original signal.
For the signal
f(t) = cos(ωt + θ)
Frequency division by N divides the cosine function argument (ωt + θ) by N.
Consequently any phase noise term in the θ is also divided by N. (the phase noise is decreased by 20log(N) dB).
For a frequency modulated signal
f(t) = cos(ωct + βsin(ωmt))
for small β
f(t) = cos(ωct) + (β/2)[cos(ωc - ωm)t - cos(ωc + ωm)t]
becomes after frequency division by N
f(t) = cos((ωc/N)t + (β/N)sin(ωct))
for small β/N
f(t) = cos((ωc/N)t) + (β/2N)[cos(ωc/N - ωm)t - cos(ωc/N + ωm)t]
1) The sideband amplitude is decreased by N. i.e by 20Log(N) dB.
2) The sideband offset from the carrier in the frequency divided signal is the same as for the original signal.
For derivations of the above results for particular frequency multipliers and dividers see:
Derivations using Complex numbers
Derivations using Trigonometric Identities