Coulomb problem in momentum space without screening

N. J. Upadhyay, V. Eremenko, L. Hlophe, F. M. Nunes, Ch Elster, G. Arbanas, J. E. Escher, I. J. Thompson

Research output: Contribution to journalArticlepeer-review

12 Scopus citations

Abstract

Background: The repulsive Coulomb force poses severe challenges when solving the three-body problem for (d,p) reactions on intermediate mass and heavy nuclei. Recently, a new approach based on the Coulomb-distorted basis in momentum space was proposed. Purpose: In this work, we demonstrate the feasibility of using the Coulomb-distorted basis in momentum space for calculating matrix elements expected in a wide range of nuclear reactions. Method: We discuss the analytic forms of the Coulomb wave function in momentum space. We analyze the singularities in the Coulomb-distorted form factors and the required regularization techniques. Employing a separable interaction derived from a realistic nucleon-nucleus optical potential, we compute and study the Coulomb-distorted form factors for a wide range of cases, including charge, angular momentum, and energy dependence. We also investigate in detail the precision of our calculations. Results: The Coulomb-distorted form factors differ significantly from the nuclear form factors except for the very highest momenta. Typically, the structure of the form factor is shifted away from zero momentum due to the Coulomb interaction. Unlike the Yamaguchi forms typically used in three-body methods, our realistic form factors have a short high-momentum tail, which allows for a safe and efficient truncation of the momentum grid. Conclusions: Our results show that the Coulomb-distorted basis can be effectively implemented.

Original languageEnglish
Article number014615
JournalPhysical Review C - Nuclear Physics
Volume90
Issue number1
DOIs
StatePublished - Jul 28 2014

Funding

FundersFunder number
National Science FoundationPHY-0800026
U.S. Department of EnergyDE-FG02-93ER40756, DE-SC0004084, DE-AC0500OR22725, DE-AC02-05CH11231, DE-SC0004087, DE-FG52-08NA28552, DE-AC52-07NA27344

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