Abstract:
For the solution of a quasipotential equation, a representation is obtained in the form of a
Feynman integral in phase space, a method of finite approximation of this integral being
specified. The representation is used to investigate the high-energy asymptotic behavior
of the quasipotential amplitude.
Citation:
V. N. Pervushin, “Solution of a quasipotential equation in the form of a Feynman integral”, TMF, 14:3 (1973), 332–341; Theoret. and Math. Phys., 14:3 (1973), 246–252
\Bibitem{Per73}
\by V.~N.~Pervushin
\paper Solution of a quasipotential equation in the form of a Feynman integral
\jour TMF
\yr 1973
\vol 14
\issue 3
\pages 332--341
\mathnet{http://mi.mathnet.ru/tmf3391}
\transl
\jour Theoret. and Math. Phys.
\yr 1973
\vol 14
\issue 3
\pages 246--252
\crossref{https://doi.org/10.1007/BF01029306}
Linking options:
https://www.mathnet.ru/eng/tmf3391
https://www.mathnet.ru/eng/tmf/v14/i3/p332
This publication is cited in the following 1 articles:
A. V. Bogdanov, G. V. Dubrovskiy, “Path integral representation for inelastic scattering amplitude and its quasiclassical approximations”, Theoret. and Math. Phys., 30:2 (1977), 146–152
Citation in format AMSBIB
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