Improved strong-coupling perturbation theory of the symmetric Anderson impurity model
arXiv:1901.11471 · doi:10.1142/S0217984919503329
Abstract
In a previous work (N. H. Tong, Phys. Rev. B 92, 165126 (2015)), an equation-of-motion based series expansion formalism was used to do the second-order strong-coupling expansion for the single-particle Green function of the Anderson impurity model. In this paper, we improve this theory in two aspects. We first use a more accurate scheme to self-consistently calculate the averages that appear in G1. In the resummation process, we use updated coefficients for the continued fraction, guided by the formally exact continued fraction from the Mori-Zwanzig theory. These changes lead to more accurate impurity spin response to the magnetic bias of the bath. Combined with the dynamical mean-field theory, our theory gives improved description for the antiferromagnetism of Hubbard model at half filling.
11 pages, 4 figures
References in corpus (9)
- Continuous-time Monte Carlo methods for quantum impurity models
- The numerical renormalization group method for quantum impurity systems
- Hierarchical Liouville-space approach for accurate and universal characterization of quantum impurity systems
- Multi-impurity Anderson model for quantum dots coupled in parallel
- Projective Quantum Monte Carlo Method for the Anderson Impurity Model and its Application to Dynamical Mean Field Theory
- Projective Truncation Approximation for Equations of Motion of Two-Time Green's Functions
- Equation of Motion Series Expansion of Double Time Green's Functions
- Controllable Precision of the Projective Truncation Approximation for Green's Functions
- A Standard Basis Operator Equation of Motion Impurity Solver for Dynamical Mean Field Theory