Under , the transition amplitude changes to first order by an insertionIfwith the corresponding condition on the bra, the two terms vanish after moving to the external states. The amplitude is then independent of the gauge-fixing choice.
Conversely, invariance for arbitrary changes of the gauge-fixing fermion requires physical external states to be BRST closed. States differing by a BRST-exact state have identical matrix elements against closed states, so the physical state space is the cohomology
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