Abstract
Consider a three-body system consisting of one neutral particle 1 and two charged particles characterized by the indices 2 and 3 with charges of opposite sign, i.e., e2e3 < 0. We use the following notation: (x ν , y ν ), v = 1, 2, 3, denotes the (mass-renormalized) coordinate vector within the pair ν, and between the center of mass of the pair ν and particle ν, respectively. The corresponding canonically coniugate momenta are (k ν , p ν ).
Supported by Deutscher Akademischer Austauschdienst and a US DOE Grant of the Harvard-Smithsonian Center for Astrophysics
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S.B. Levin, E.O. Alt, and S.L. Yakovlev: to be published
E.O. Alt and A.M. Mukhamedzhanov: JETP Lett. 56, 435 (1992); Phys. Rev. A47, 2004 (1993)
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Levin, S.B., Alt, E.O., Yakovlev, S.L. (2003). Coulomb Fourier Transformation: Application to a Three-Body Hamiltonian with One Attractive Coulomb Interaction. In: Krivec, R., Rosina, M., Golli, B., Širca, S. (eds) Few-Body Problems in Physics ’02. Few-Body Systems, vol 14. Springer, Vienna. https://doi.org/10.1007/978-3-7091-6728-1_53
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DOI: https://doi.org/10.1007/978-3-7091-6728-1_53
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