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RESEARCH PRODUCT

Coulomb Fourier Transformation: Application to a Three-Body Hamiltonian with One Attractive Coulomb Interaction

E. O. AltS. L. YakovlevS. B. LevinS. B. Levin

subject

Physicssymbols.namesakeFourier transformQuantum mechanicsCoulomb wave functionCoulombsymbolsCoordinate vectorCoulomb barrierNeutral particleHamiltonian (quantum mechanics)Charged particle

description

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 ).

yearjournalcountryeditionlanguage
2003-01-01
https://doi.org/10.1007/978-3-7091-6728-1_53