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Nuclear matter equation of state with single particle correlations
Affiliation:1. Dipartimento di Fisica, Università di Catania, Italy;2. INFN, Sezione di Catania, Corso Italia 57, I-95129 Catania, Italy;1. Theoretical Division, Los Alamos National Laboratory, Los Alamos, NM 87545, United States;2. Yukawa Institute for Theoretical Physics, Kyoto University, Kyoto 606-8502, Japan;3. RIKEN Nishina Center, Wako 351-0198, Japan;4. Center for Mathematics and Physics University of Aizu, Aizu Wakamatsu, Fukushima 965-0001, Japan;1. Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany;2. Department of Physics and Astronomy, University of Tennessee, Knoxville, TN 37996, USA;3. Physics Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA;1. School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China;2. Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100190, China;3. Facility for Rare Isotope Beams, Michigan State University, East Lansing, MI 48824, USA;4. Department of Physics and Astronomy, Vanderbilt University, Nashville, TN 37235, USA
Abstract:
Symmetrical nuclear matter at finite temperature is studied in the framework of the Brueckner-Hartree-Fock approximation extended to include single-particle correlations. A liquid-vapor phase transition is observed, wtih a critical temperature of about 20 MeV, in close similarity with Skyrme force calculations. The inclusion of single-particle correlations introduces a significant temperature dependence in the single-particle potential as well as in the nucleon effective mass. In this scheme the Hughenholtz-Van Hove theorem is well satisfied throughout the range of density and temperature considered.
Keywords:
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