2014/02/18 by Peter Staar, Thomas Maier, T. C. Schulthess +1 · 1 citation
Mathematics · Physics and Astronomy · #Advanced Condensed Matter Physics #Cluster (spacecraft) #Combinatorics #Condensed matter physics #Coupling (piping) #Hubbard model #Lattice (music) #Mathematics #Momentum (technical analysis) #Monte Carlo method #Physics #Physics of Superconductivity and Magnetism #Quantum Monte Carlo #Quantum and electron transport phenomena #Quantum mechanics #Statistical physics #Superconductivity #Vertex (graph theory) #cond-mat.str-el
paper · pdf · doi:10.1103/physrevb.89.195133
arxiv created 2014/02/18 · openalex publication_date 2014/05/27 · arxiv updated 2015/06/18 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
The DCA+\phantom\rule0.222222em0exalgorithm was recently introduced by Stear, Maier, and Schulthess [Phys. Rev. B 88, 115101 (2013)] to extend the dynamic cluster approximation (DCA) with a continuous lattice self-energy in order to achieve better convergence with cluster size. Here we extend the DCA+\phantom\rule0.222222em0exalgorithm to the calculation of two-particle correlation functions by introducing irreducible vertex functions with continuous momentum dependence consistent with the DCA+\phantom\rule0.222222em0exself-energy. This enables a significantly more controlled and reliable study of phase transitions than with the DCA. We test the new method by calculating the superconducting transition temperature Tc in the attractive Hubbard model and show that it reproduces previous determinantal quantum Monte Carlo results. We then calculate Tc in the doped repulsive Hubbard model, for which previous DCA calculations could only access the weak-coupling (U=4t) regime for large clusters. We show that the new algorithm provides access to much larger clusters and delivers asymptotically converged results for Tc for both the weak (U=4t) and intermediate (U=7t) coupling regimes, and thereby enables the accurate determination of the exact infinite cluster size result.