Abstract:
For a system of two relativistic particles described in the Logunov–Tavkhelidze one-time approach the dependence of the quasipotential of one-boson exchange on the total energy of the system is calculated. It is shown that despite the nonlocal form of the obtained quasipotential
the three-dimensional equations for the wave function can be reduced by a partial expansion to one-dimensional equations. The influence of the energy dependence of the quasipotential on its behavior in the coordinate representation is discussed.
Citation:
V. N. Kapshai, V. I. Savrin, N. B. Skachkov, “Dependence of the quasipotential on the total energy of a two-particle system”, TMF, 69:3 (1986), 400–410; Theoret. and Math. Phys., 69:3 (1986), 1226–1233
\Bibitem{KapSavSka86}
\by V.~N.~Kapshai, V.~I.~Savrin, N.~B.~Skachkov
\paper Dependence of the quasipotential on the total energy of a~two-particle system
\jour TMF
\yr 1986
\vol 69
\issue 3
\pages 400--410
\mathnet{http://mi.mathnet.ru/tmf5239}
\transl
\jour Theoret. and Math. Phys.
\yr 1986
\vol 69
\issue 3
\pages 1226--1233
\crossref{https://doi.org/10.1007/BF01017621}
\isi{https://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=Publons&SrcAuth=Publons_CEL&DestLinkType=FullRecord&DestApp=WOS_CPL&KeyUT=A1986J423400007}
Linking options:
https://www.mathnet.ru/eng/tmf5239
https://www.mathnet.ru/eng/tmf/v69/i3/p400
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