Feynman principle for fermions with odd covariant symbol of the Hamiltonian
Teoretičeskaâ i matematičeskaâ fizika, Tome 90 (1992) no. 1, pp. 155-160
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An expression is obtained for the Feynman path integral in the case of Fermi systems with eovariant symbol of the Hamiltonian of arbitrary Grassmaan parity.
@article{TMF_1992_90_1_a13,
author = {V. V. Smirnov},
title = {Feynman principle for fermions with odd covariant symbol of the {Hamiltonian}},
journal = {Teoreti\v{c}eska\^a i matemati\v{c}eska\^a fizika},
pages = {155--160},
publisher = {mathdoc},
volume = {90},
number = {1},
year = {1992},
language = {ru},
url = {http://geodesic.mathdoc.fr/item/TMF_1992_90_1_a13/}
}
TY - JOUR AU - V. V. Smirnov TI - Feynman principle for fermions with odd covariant symbol of the Hamiltonian JO - Teoretičeskaâ i matematičeskaâ fizika PY - 1992 SP - 155 EP - 160 VL - 90 IS - 1 PB - mathdoc UR - http://geodesic.mathdoc.fr/item/TMF_1992_90_1_a13/ LA - ru ID - TMF_1992_90_1_a13 ER -
V. V. Smirnov. Feynman principle for fermions with odd covariant symbol of the Hamiltonian. Teoretičeskaâ i matematičeskaâ fizika, Tome 90 (1992) no. 1, pp. 155-160. http://geodesic.mathdoc.fr/item/TMF_1992_90_1_a13/