I think it's a bit more complicated than that.
The CCIR 468 standard mandates a weighting curve that, contrary to A-weighting, actually provides a gain of up to 12+ dB in a bandwidth which have been found to be critical for the subjective annoyance of noise:
View attachment 396712
And the standard also mandates the use of a special detector circuit (the electronic circuit which convert the instantaneous noise voltage to average values to be used for computing the displayed noise voltage) which has characteristics designed to give a certain weight to noise spikes inside very high crest factor average signal contents.
As a result, if "simple" A-weighting applied to RMS noise level measurements usually produces more impressive figures (say a 95 dB unweighted signal to noise ratio over a 20 Hz - 20 kHz bandwidth becomes 101 dBA), CCIR 468 actually produces
less high figures (say the same 95 dB becomes something as 87 dBqps, dBqps being the metrics used to show CCIR weighted noise measurements).
For specific purposes, the CCIR 468 standard also specified an unweighted measurement, using the same special detector circuit, which has a flat frequency response from 22.4 Hz to 22.4 kHz.
This standard has not been amended since several decades : it is a very well-established method of noise measurement.
I have at my disposal a Rohde & Schwarz psophometer which incorporates both CCIR compliant circuits and flat band-limited RMS noise measurement circuits. It is very enlightening to measure and compare the noise levels of various devices obtained with both methods.
By the way, I think the CCIR noise measurement standard shows in itself why noise-shaped dither can be interesting to improve the subjective performances of a digital chain in certain conditions.