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Efficient computations of continuous action densities of states for lattice models
The Logarithmic Linear Relaxation (LLR) algorithm is an efficient method for computing densities of states for systems with a continuous spectrum. A key feature of this method is exponential error reduction, which allows us to evaluate the density of states of a system over hundreds of thousands of...
Autores principales: | , , , , |
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Lenguaje: | eng |
Publicado: |
2022
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1088/1742-6596/2207/1/012052 http://cds.cern.ch/record/2789459 |
_version_ | 1780972180449787904 |
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author | Lucini, Biagio Francesconi, Olmo Holzmann, Markus Lancaster, David Rago, Antonio |
author_facet | Lucini, Biagio Francesconi, Olmo Holzmann, Markus Lancaster, David Rago, Antonio |
author_sort | Lucini, Biagio |
collection | CERN |
description | The Logarithmic Linear Relaxation (LLR) algorithm is an efficient method for computing densities of states for systems with a continuous spectrum. A key feature of this method is exponential error reduction, which allows us to evaluate the density of states of a system over hundreds of thousands of orders of magnitude with a fixed level of relative accuracy. As a consequence of exponential error reduction, the LLR method provides a robust alternative to traditional Monte Carlo calculations in cases in which states suppressed by the Boltzmann weight play nevertheless a relevant role, e.g., as transition regions between dominant configuration sets. After reviewing the algorithm, we will show an application in U(1) Lattice Gauge Theory that has enabled us to obtain the most accurate estimate of the critical coupling with modest computational resources, defeating exponential tunneling times between metastable vacua. As a further showcase, we will then present an application of the LLR method to the decorrelation of the topological charge in SU(3) Lattice Gauge Theory near the continuum limit. Finally, we will review in general applications of the LLR algorithm to systems affected by a strong sign problem and discuss the case of the Bose gas at finite chemical potential. |
id | cern-2789459 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2022 |
record_format | invenio |
spelling | cern-27894592023-06-29T04:31:21Zdoi:10.1088/1742-6596/2207/1/012052http://cds.cern.ch/record/2789459engLucini, BiagioFrancesconi, OlmoHolzmann, MarkusLancaster, DavidRago, AntonioEfficient computations of continuous action densities of states for lattice modelscond-mat.str-elcond-mat.stat-mechhep-latParticle Physics - LatticeThe Logarithmic Linear Relaxation (LLR) algorithm is an efficient method for computing densities of states for systems with a continuous spectrum. A key feature of this method is exponential error reduction, which allows us to evaluate the density of states of a system over hundreds of thousands of orders of magnitude with a fixed level of relative accuracy. As a consequence of exponential error reduction, the LLR method provides a robust alternative to traditional Monte Carlo calculations in cases in which states suppressed by the Boltzmann weight play nevertheless a relevant role, e.g., as transition regions between dominant configuration sets. After reviewing the algorithm, we will show an application in U(1) Lattice Gauge Theory that has enabled us to obtain the most accurate estimate of the critical coupling with modest computational resources, defeating exponential tunneling times between metastable vacua. As a further showcase, we will then present an application of the LLR method to the decorrelation of the topological charge in SU(3) Lattice Gauge Theory near the continuum limit. Finally, we will review in general applications of the LLR algorithm to systems affected by a strong sign problem and discuss the case of the Bose gas at finite chemical potential.The Logarithmic Linear Relaxation (LLR) algorithm is an efficient method for computing densities of states for systems with a continuous spectrum. A key feature of this method is exponential error reduction, which allows us to evaluate the density of states of a system over hundreds of thousands of orders of magnitude with a fixed level of relative accuracy. As a consequence of exponential error reduction, the LLR method provides a robust alternative to traditional Monte Carlo calculations in cases in which states suppressed by the Boltzmann weight play nevertheless a relevant role, e.g., as transition regions between dominant configuration sets. After reviewing the algorithm, we will show an application in U(1) Lattice Gauge Theory that has enabled us to obtain the most accurate estimate of the critical coupling with modest computational resources, defeating exponential tunneling times between metastable vacua. As a further showcase, we will then present an application of the LLR method to the decorrelation of the topological charge in SU(3) Lattice Gauge Theory near the continuum limit. Finally, we will review in general applications of the LLR algorithm to systems affected by a strong sign problem and discuss the case of the Bose gas at finite chemical potential.arXiv:2111.00353oai:cds.cern.ch:27894592022 |
spellingShingle | cond-mat.str-el cond-mat.stat-mech hep-lat Particle Physics - Lattice Lucini, Biagio Francesconi, Olmo Holzmann, Markus Lancaster, David Rago, Antonio Efficient computations of continuous action densities of states for lattice models |
title | Efficient computations of continuous action densities of states for lattice models |
title_full | Efficient computations of continuous action densities of states for lattice models |
title_fullStr | Efficient computations of continuous action densities of states for lattice models |
title_full_unstemmed | Efficient computations of continuous action densities of states for lattice models |
title_short | Efficient computations of continuous action densities of states for lattice models |
title_sort | efficient computations of continuous action densities of states for lattice models |
topic | cond-mat.str-el cond-mat.stat-mech hep-lat Particle Physics - Lattice |
url | https://dx.doi.org/10.1088/1742-6596/2207/1/012052 http://cds.cern.ch/record/2789459 |
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