Anticommuting scalar Grassmann fields (Faddeev–Popov ghosts, c, c̄) introduced to make gauge-fixed path integrals unitary. BRST charge nilpotency Q²=0 enforces gauge symmetry.
Anticommuting scalar Grassmann fields (Faddeev–Popov ghosts, c, c̄) introduced to make gauge-fixed path integrals unitary. BRST charge nilpotency Q²=0 enforces gauge symmetry.