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Partition Functions of Strongly Correlated Electron Systems as "Fermionants"

2011/08/11 by Shailesh Chandrasekharan, Chandrasekharan, Shailesh, Uwe-Jens Wiese +1
Physics and Astronomy · #FOS: Physical sciences #High Energy Physics - Lattice (hep-lat) #Strongly Correlated Electrons (cond-mat.str-el) #cond-mat.str-el #hep-lat

paper · pdf · doi:10.48550/arxiv.1108.2461

4 pages, no figures

arxiv created 2011/08/11 · arxiv updated 2011/08/12

Abstract

We introduce a new mathematical object, the "fermionant" FermN(G), of type N of an n × n matrix G. It represents certain n-point functions involving N species of free fermions. When N=1, the fermionant reduces to the determinant. The partition function of the repulsive Hubbard model, of geometrically frustrated quantum antiferromagnets, and of Kondo lattice models can be expressed as fermionants of type N=2, which naturally incorporates infinite on-site repulsion. A computation of the fermionant in polynomial time would solve many interesting fermion sign problems.

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