Particles and Nuclei 1973
DOI: 10.1007/978-1-4684-7550-0_3
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Three-Dimensional Formulation of the Relativistic Two-Body Problem

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Cited by 15 publications
(23 citation statements)
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“…Independently, this idea was developed by A. P. Kotelnikov from the university in Kazan, where N. Lobachevski worked out his geometry [20]. In the scope of the quantum relativistic dynamics the hyperbolic geometry intensively was exploited in, so-called, quasipotential models (see, for instance, [21], [22]). Two-and three-dimensional Euclidean geometries are unique what allow geometric observations.…”
Section: Discussionmentioning
confidence: 99%
“…Independently, this idea was developed by A. P. Kotelnikov from the university in Kazan, where N. Lobachevski worked out his geometry [20]. In the scope of the quantum relativistic dynamics the hyperbolic geometry intensively was exploited in, so-called, quasipotential models (see, for instance, [21], [22]). Two-and three-dimensional Euclidean geometries are unique what allow geometric observations.…”
Section: Discussionmentioning
confidence: 99%
“…In this case, the matrix element of transition from one space to another is the Shapiro function rather than the plane wave [3]. Analogous problem was solved by Kadyshevskii et al [4] who constructed a relativistic configuration space. The same situation arises when implementing the Wigner function formalism in the Lobachevskii curved space [5].…”
Section: Introductionmentioning
confidence: 97%
“…In the present study, an expression for the elastic form factor for a bound relativistic two-particle system is obtained for the case of a vector current by using the relativistic quasipotential (RQP) approach based on the Hamiltonian formulation of quantum field theory [8,9] and by going over to the relativistic configuration representation for interaction between two relativistic spinless particles with arbitrary masses m 1 and m 2 [20,21].…”
Section: Introductionmentioning
confidence: 99%