In a system of interacting fermions, the correlation energy is defined as the difference between the energy of the ground state and the one of the free Fermi gas. We consider N interacting spin 1/2 fermions in the dilute regime, i.e., p << 1 where p is the total density of the system. We rigorously derive a first order upper bound for the correlation energy with an optimal error term of the order O(p7/3) in the thermodynamic limit. Moreover, we improve the lower bound estimate with respect to previous results getting an error O(p2+1/5).& COPY

An optimal upper bound for the dilute Fermi gas in three dimensions / E. Giacomelli. - In: JOURNAL OF FUNCTIONAL ANALYSIS. - ISSN 0022-1236. - 285:8(2023), pp. 110073.1-110073.73. [10.1016/j.jfa.2023.110073]

An optimal upper bound for the dilute Fermi gas in three dimensions

E. Giacomelli
Primo
2023

Abstract

In a system of interacting fermions, the correlation energy is defined as the difference between the energy of the ground state and the one of the free Fermi gas. We consider N interacting spin 1/2 fermions in the dilute regime, i.e., p << 1 where p is the total density of the system. We rigorously derive a first order upper bound for the correlation energy with an optimal error term of the order O(p7/3) in the thermodynamic limit. Moreover, we improve the lower bound estimate with respect to previous results getting an error O(p2+1/5).& COPY
Collective excitations; Fermi gas
Settore MATH-04/A - Fisica matematica
2023
Article (author)
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2434/1157620
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