Semideterministic and stochastic sampling of Feynman diagrams with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mrow><mml:mn>1</mml:mn><mml:mo>/</mml:mo><mml:mi>N</mml:mi></mml:mrow><mml:mi>f</mml:mi></mml:msub></mml:math>

We introduce a family of (semi)-bold-line series, assisted with <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:mn>1</a:mn><a:mo>/</a:mo><a:msub><a:mi>N</a:mi><a:mi>f</a:mi></a:msub></a:mrow></a:math> expansions, with <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:msub><b:mi>N</b:mi><b:mi>f</b:mi></b:msub></b:math> being the number of fermion flavors. If there is no additional <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:msub><c:mi>N</c:mi><c:mi>f</c:mi></c:msub></c:math> cut, the series reduces to the random phase approximation series in the density-density channel, complementary to the particle-hole and particle-particle channels introduced in . To address the very localized integrands in diagrammatic Monte Carlo, we introduced an innovative VEGAS-RG-MCMC sampling method, where we found a significant decrease of autocorrelation time without the usage of the state-of-the-art many-configuration MCMC (MCMCMC) method while the combination of both is also straightforward. We performed extensive benchmarks for density, energy, and pressure with the <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:mrow><d:mi>t</d:mi><d:mtext>−</d:mtext><d:msup><d:mrow><d:mi>t</d:mi></d:mrow><d:mo>′</d:mo></d:msup></d:mrow><d:mo> </d:mo><d:mrow><d:mi>SU</d:mi><d:mo>(</d:mo><d:msub><d:mi>N</d:mi><d:mi>f</d:mi></d:msub><d:mo>)</d:mo></d:mrow></d:math> Hubbard model on a square lattice and honeycomb lattices over a wide range of numerical methods. For benchmark purposes, we also implement bare-<e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:mi mathvariant="normal">U</e:mi></e:math> symmetry-broken perturbation series for the two-dimensional SU(2) Hubbard model on the honeycomb lattice, where we found encouraging results from weak to intermediate couplings.

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Publication Details

Journal
Physical Review Research
Published
2025-05-22
DOI
https://doi.org/10.1103/physrevresearch.7.023177
Primary Topic
Quantum many-body systems
Type
article
Field-Weighted Citation Impact
0.00

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article

Semideterministic and stochastic sampling of Feynman diagrams with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mrow><mml:mn>1</mml:mn><mml:mo>/</mml:mo><mml:mi>N</mml:mi></mml:mrow><mml:mi>f</mml:mi></mml:msub></mml:math>

Boyuan Shi
Physical Review Research
Quantum many-body systems
article

Semideterministic and stochastic sampling of Feynman diagrams with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mrow><mml:mn>1</mml:mn><mml:mo>/</mml:mo><mml:mi>N</mml:mi></mml:mrow><mml:mi>f</mml:mi></mml:msub></mml:math>

Boyuan Shi
article en

Abstract

We introduce a family of (semi)-bold-line series, assisted with <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:mn>1</a:mn><a:mo>/</a:mo><a:msub><a:mi>N</a:mi><a:mi>f</a:mi></a:msub></a:mrow></a:math> expansions, with <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:msub><b:mi>N</b:mi><b:mi>f</b:mi></b:msub></b:math> being the number of fermion flavors. If there is no additional <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:msub><c:mi>N</c:mi><c:mi>f</c:mi></c:msub></c:math> cut, the series reduces to the random phase approximation series in the density-density channel, complementary to the particle-hole and particle-particle channels introduced in . To address the very localized integrands in diagrammatic Monte Carlo, we introduced an innovative VEGAS-RG-MCMC sampling method, where we found a significant decrease of autocorrelation time without the usage of the state-of-the-art many-configuration MCMC (MCMCMC) method while the combination of both is also straightforward. We performed extensive benchmarks for density, energy, and pressure with the <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:mrow><d:mi>t</d:mi><d:mtext>−</d:mtext><d:msup><d:mrow><d:mi>t</d:mi></d:mrow><d:mo>′</d:mo></d:msup></d:mrow><d:mo> </d:mo><d:mrow><d:mi>SU</d:mi><d:mo>(</d:mo><d:msub><d:mi>N</d:mi><d:mi>f</d:mi></d:msub><d:mo>)</d:mo></d:mrow></d:math> Hubbard model on a square lattice and honeycomb lattices over a wide range of numerical methods. For benchmark purposes, we also implement bare-<e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:mi mathvariant="normal">U</e:mi></e:math> symmetry-broken perturbation series for the two-dimensional SU(2) Hubbard model on the honeycomb lattice, where we found encouraging results from weak to intermediate couplings.

Physical Review ResearchVol. 7(2)
Imperial College London (GB)
Imperial College London
Openalex Percentile: Top 91%
Quantum many-body systems
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