Abstract
A quasipotential approach to the relativistic two-body problem is developed on the basis of the three-dimensional Hamiltonian formulation of quantum field theory. A relativistic configuration representation is introduced and studied on the basis of a decomposition with respect to matrix elements of irreducible unitary representations of the Lorentz group. A representation is obtained for the quasipotential scattering amplitude at high energies that generalizes the nonrelativistic eikonal formula.
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Kadyshevskii, V.G., Mir-Kasimov, R.M., Skachkov, N.B. (1973). Three-Dimensional Formulation of the Relativistic Two-Body Problem. In: Bogolyubov, N.N., Baldin, A.M., Van Hieu, N., Solov’ev, V.G. (eds) Particles and Nuclei. Springer, Boston, MA. https://doi.org/10.1007/978-1-4684-7550-0_3
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DOI: https://doi.org/10.1007/978-1-4684-7550-0_3
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