Abstract

Numerical results for ground state and excited state properties (energies, double occupancies, and Matsubara-axis self energies) of the single-orbital Hubbard model on a two-dimensional square lattice are presented, in order to provide an assessment of our ability to compute accurate results in the thermodynamic limit. Many methods are employed, including auxiliary field quantum Monte Carlo, bare and bold-line diagrammatic Monte Carlo, method of dual fermions, density matrix embedding theory, density matrix renormalization group, dynamical cluster approximation, diffusion Monte Carlo within a fixed node approximation, unrestricted coupled cluster theory, and multi-reference projected Hartree-Fock. Comparison of results obtained by different methods allows for the identification of uncertainties and systematic errors. The importance of extrapolation to converged thermodynamic limit values is emphasized. Cases where agreement between different methods is obtained establish benchmark results that may be useful in the validation of new approaches and the improvement of existing methods.

Highlights

  • For the fixed-node approximation (FN) technique, a diffusion Monte Carlo calculation based on the nodal structure of a trial wave function obtained with variational Monte Carlo, we show finite-size results for a sequence of 45-degree rotated clusters with size 98, 162, and 242, which have the property of being closed shells at U 1⁄4 0

  • dynamical cluster approximation (DCA) results in the thermodynamic limit are extrapolated from finite clusters; diagrammatic Monte Carlo (DiagMC) results are extrapolated in the expansion order

  • At nonzero T, the data from two types of DiagMC and from DCA in the thermodynamic limit agree within uncertainty

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Summary

Introduction

Systems of large numbers of interacting electrons is one of the grand scientific challenges of the present day. Improved solutions are needed both for the practical problems of materials science and chemistry and for the basic science questions of determining the qualitative behaviors of interacting quantum systems. While many problems of implementation arise, including calculation of the multiplicity of orbitals and interaction matrix elements needed to characterize real materials, the fundamental difficulties are that the dimension of the Hilbert space needed to describe an interacting electron.

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