pith. machine review for the scientific record. sign in

arxiv: 1704.00131 · v2 · submitted 2017-04-01 · ❄️ cond-mat.str-el · hep-lat· physics.comp-ph· quant-ph

Recognition: unknown

The ALF (Algorithms for Lattice Fermions) project release 1.0. Documentation for the auxiliary field quantum Monte Carlo code

Authors on Pith no claims yet
classification ❄️ cond-mat.str-el hep-latphysics.comp-phquant-ph
keywords latticemodelcodefieldoperatorssingle-bodyalgorithmsauxiliary
0
0 comments X
read the original abstract

The Algorithms for Lattice Fermions package provides a general code for the finite temperature auxiliary field quantum Monte Carlo algorithm. The code is engineered to be able to simulate any model that can be written in terms of sums of single-body operators, of squares of single-body operators and single-body operators coupled to an Ising field with given dynamics. We provide predefined types that allow the user to specify the model, the Bravais lattice as well as equal time and time displaced observables. The code supports an MPI implementation. Examples such as the Hubbard model on the honeycomb lattice and the Hubbard model on the square lattice coupled to a transverse Ising field are provided and discussed in the documentation. We furthermore discuss how to use the package to implement the Kondo lattice model and the $SU(N)$-Hubbard-Heisenberg model. One can download the code from our Git instance at https://alf.physik.uni-wuerzburg.de and sign in to file issues.

This paper has not been read by Pith yet.

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Analyzing the two-dimensional doped Hubbard model with the Worldvolume HMC method

    hep-lat 2026-05 conditional novelty 6.0

    WV-HMC successfully simulates the doped 2D Hubbard model on 8x8 lattices at U/t=8 and T/t≈0.156 with controlled statistical errors.