Definition of Single Sideband Phase
Noise
Signal generators, voltage controlled
oscillators and other signal sources often come with a phase noise
specification such as shown in Figure 1.2 
Figure 1.2 VCO Phase Noise
This
happens to be the phase noise of one of our VCO designs at
450MHz. The view on a spectrum analyzer is given below in
Figure 1.3. The
SSB Phase Noise, often given the symbol Lf(fm),
is a power ratio. It is the ratio of the power in a 1Hz
bandwidth a frequency fm away from the
carrier, to the power in the carrier itself. As it
is a power ratio, to convert to dBc/Hz, use 10log10(Lf(fm)) Example:
Looking at Figure 1.2, we see that the SSB phase noise at an
offset frequency of 10kHz is about -120dBc/Hz, ( Lf(10kHz)
= 10-12 ). This means that if the VCO was
producing 0dBm at 450MHz, a 1Hz wide filter at 450.01MHz would
receive -120dBm, and a second filter at 449.99MHz would also receive
-120dBm. Note that the definition
of phase noise implicitly assumes that the spectrum is symmetric, as
it is for a signal that has only phase noise and no amplitude
noise. Signals with asymmetric spectrum (i.e. spectrum at fc
+ fm is different to spectrum at fc
- fm ), have a combination
of amplitude and phase noise, and it is necessary to remove the
amplitude noise before measuring Lf(fm)
on a spectrum analyser. Although
SSB Phase Noise is conventionally defined in a 1Hz bandwidth,
in use it is necessary to determine the noise power in other
bandwidths. If the SSB Phase Noise is approximately constant
over the bandwidth of interest then Noise
Power in bandwidth B Hz centered a distance fm
from the carrier (i.e. centered at fc +
fm or fc -
fm ) is approximately given by Power
in B Hz = B Lf(fm)
Pc where Pc
is the power in the carrier. It is generally more convenient
to work in dB's, the corresponding equation is Power
in B Hz [dBm] = 10 log10(B) + Lf(fm)
[dBc/Hz] + Pc [dBm]
..
(1.10)
Example: Looking at Figure 1.2
again, and noting that the SSB phase noise at an offset frequency of
10kHz is -120dBc/Hz. If the VCO was producing 0dBm at
450MHz, then a 3kHz wide filter at 450.01MHz would receive
approximately -85dBm, and a second filter (also 3kHz wide) at
449.99MHz would also receive around -85dBm. This is indicated
by the following (simulated) spectrum analyzer display for the VCO with
phase noise given in Figure 1.2, where the resolution bandwidth is
3kHz. This spectrum analyzer display shows the power
received by a 3kHz wide filter as the filter center frequency is varied
over the display sweep range. 
Figure 1.3 Spectrum Analyser display of VCO
The
accuracy of (1.10) degrades as the bandwidth B increases, as
the phase noise slope is not linear (it appears linear in Figure 1.2 but
that has logarithmic scales, it is typically varying as 1/fm2).
To accurately determine the power in adjacent channels, it is
necessary to integrate the phase noise curve. If you
have measurements of phase noise you can integrate them numerically,
if you are designing a synthesizer then using a simulation tool like
SimPLL can do this automatically.
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