Since thermal (Johnson or Nyquist) noise depends only the resistance, "excess" noise is the only useful parameter that distinguishes resistors from each other in noise performance.
Approximately, the noise spectral density, in W/Hz, is proportional to 1/f, hence the common name "1/f noise" or "pink noise".
In resistors, it is only present when there is a DC current flows through them, and above a "corner" frequency, depending on current, it falls below the inherent Johnson noise and is no longer significant.
Often, it is quantified by a "noise index": NI = 20 x log10 (uV noise per V DC per decade of frequency).
Since the noise density keeps increasisng at lower frequencies, it cannot be eliminated by averaging in the same way as "white noise" from Johnson noise.
Metal foil and wirewound resistors can be better than -30 dB; depending on resistance and construction, carbon can be worse than 0 dB.
One need worry about excess noise in resistors only when there is DC across them, such as bias dividers and emitter resistors.
As is well known, active devices also show excess noise, usually near 1/f.
When I was in grad school, a lab down the hall was investigating excess noise in pure metals and found that even in pure silver, excess noise could be seen if you lowered the temperature (and therefore Johnson noise) to incredibly low values.