Mixtures of correlated bosons and fermions: Dynamical mean‐field theory for normal and condensed phases

• Published in: Annalen der Physik Vol. 521; no. 9; pp. 622 - 633
• Main Authors: Byczuk, K., Vollhardt, D.
• Format: Journal Article
• Language: English
• Published: Berlin WILEY‐VCH Verlag 16-09-2009
• Subjects: Correlated lattice fermions and bosons; dynamical mean‐field theory
• ISSN: 0003-3804; 1521-3889
• DOI: 10.1002/andp.20095210904

We derive a dynamical mean‐field theory for mixtures of interacting bosons and fermions on a lattice (BF‐DMFT). The BF‐DMFT is a comprehensive, thermodynamically consistent framework for the theoretical investigation of Bose‐Fermi mixtures and is applicable for arbitrary values of the coupling parameters and temperatures. It becomes exact in the limit of high spatial dimensions d or coordination number Z of the lattice. In particular, the BF‐DMFT treats normal and condensed bosons on equal footing and thus includes the effects caused by their dynamic coupling. Using the BF‐DMFT we investigate two different interaction models of correlated lattice bosons and fermions, one where all particles are spinless (model I) and one where fermions carry a spin one‐half (model II). In model I the local, repulsive interaction between bosons and fermions can give rise to an attractive effective interaction between the bosons. In model II it can also lead to an attraction between the fermions.
A dynamical mean‐field theory for mixtures of interacting bosons and fermions on a lattice (BF‐DMFT) is derived. The BF‐DMFT is a comprehensive, thermodynamically consistent framework for the theoretical investigation of Bose‐Fermi mixtures and is applicable for arbitrary values of the coupling parameters and temperatures. It becomes exact in the limit of high spatial dimensions d or coordination number Z of the lattice. In particular, the BF‐DMFT treats normal and condensed bosons on equal footing and thus includes the effects caused by their dynamic coupling. Using the BF‐DMFT two different interaction models of correlated lattice bosons and fermions are investigated, one where all particles are spinless (model I) and one where fermions carry a spin one‐half (model II). In model I the local, repulsive interaction between bosons and fermions can give rise to an attractive effective interaction between the bosons. In model II it can also lead to an attraction between the fermions.