I will present a recently developed continuous-time QMC method for
impurity models [1,2] which is based on a diagrammatic expansion of the
partition function in the impurity-bath hybridization. This algorithm
enables the efficient DMFT-simulation of strongly correlated systems
and I will illustrate its power and flexibility with applications to
Hubbard, Holstein-Hubbard, Kondo-lattice and multi-orbital
models.
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