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Nuclear core dynamics and rearrangement energy for hypernuclei
Institution:1. Department of Applied Physics, Coherence and Quantum Technology Group, Eindhoven University of Technology, P.O. Box 513, 5600, MB Eindhoven, Netherlands;2. Thermo Fisher Scientific, Achtseweg Noord 5, 5651, GG Eindhoven, Netherlands;1. Departamento de Fisiologia e Farmacologia, Universidade Federal de Santa Maria (UFSM), Santa Maria, RS, Brazil;2. Departamento de Biología, Facultad de Ciencias del Mar y Ambientales, Campus de Excelencia Internacional del Mar (CEI-MAR), Universidad de Cádiz, Puerto Real, Cádiz, Spain;3. Instituto de Biodiversidade e Florestas, Universidade Federal do Oeste do Pará (UFOPA), Santarém, PA, Brazil;4. Instituto de Ciencias Marinas de Andalucía, Consejo Superior de Investigaciones Científicas (CSIC), Puerto Real, Cádiz, Spain;5. Nutrigenomics and Fish Growth Endocrinology Group, Institute of Aquaculture Torre de la Sal (IATS-CSIC), Ribera de Cabanes, Castellón, Spain.
Abstract:The effect of the nuclear core dynamics on the binding energies of Λ hypernuclei is studied in the framework of variational correlated wave functions. In addition to the core energy and to a Λ single-particle contribution ?ν, we exhibit a rearrangement energy ER which in particular depends on the ΛN correlations F and on the difference δφN between the core wave function and its exact ground-state value. ER is nonzero only if there are both ΛN correlations (F ≠ 1) and if δφN ≠ 0. The latter can result from core polarization by the Λ or from errors in the ground-state variational wave function of the core. ER varies linearly with δφN for small δφN. Detailed numerical results for central ΛN and NN potentials with repulsive cores confirm these general features. For a give core wave function ΛN correlations reduce the radius of the core nucleons relative to their c.m.; however ER leads to an expansion of the core rather than to a contraction with only ?ν. The core polarization eneegy is quite small ? 0.4 MeV. We study the effects of errors in the variational core wave function by detuning this as a function of one of the variational parameters.
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