Correlated bosons on a lattice: Dynamical mean-field theory for Bose-Einstein condensed and normal phases
Krzysztof Byczuk, Dieter Vollhardt

TL;DR
This paper introduces a bosonic dynamical mean-field theory (B-DMFT) that accurately models correlated lattice bosons across different phases, including Bose-Einstein condensates, providing a unified framework that extends previous mean-field approaches.
Contribution
The paper develops a comprehensive B-DMFT framework applicable for all coupling strengths and temperatures, treating normal and condensed bosons equally and generalizing existing mean-field theories.
Findings
Local correlations increase condensate density.
B-DMFT reproduces known limits like Beliaev-Popov and Hartree-Fock-Bogoliubov.
The theory predicts an increase in BEC transition temperature T_{BEC}.
Abstract
We formulate a bosonic dynamical mean-field theory (B-DMFT) which provides a comprehensive, thermodynamically consistent framework for the theoretical investigation of correlated lattice bosons. The B-DMFT is applicable for arbitrary values of the coupling parameters and temperature and becomes exact in the limit of high spatial dimensions d or coordination number Z of the lattice. In contrast to its fermionic counterpart the construction of the B-DMFT requires different scalings of the hopping amplitudes with Z depending on whether the bosons are in their normal state or in the Bose-Einstein condensate. A detailed discussion of how this conceptual problem can be overcome by performing the scaling in the action rather than in the Hamiltonian itself is presented. The B-DMFT treats normal and condensed bosons on equal footing and thus includes the effects caused by their dynamic coupling.…
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