Abstract:
The arbitrariness of the choice of the propagator of the Yang–Mills field in the Hamiltonian gauge is considered. Transition from the Coulomb to the Hamiltonian gauge yields a class of propagators that includes both a translationally noninvariant propagator as well as one of the Mandelstam–Leibbrandt type.
Citation:
G. A. Kravtsova, A. A. Slavnov, “Propagator of Yang–Mills field in Hamiltonian Gauge”, TMF, 89:2 (1991), 238–245; Theoret. and Math. Phys., 89:2 (1991), 1181–1187