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Relaxation-Time Boltzmann Solutions Without Truncations
Abstract
The relaxation-time Boltzmann equation governs relativistic matter far from equilibrium, but existing approaches rely on finite-order truncations that break down in this regime. We introduce ShARK (Stochastic Advection Relaxation Kinetics), the first fully 3D Monte Carlo kinetic framework to capture exact, far-from-equilibrium ultrarelativistic dynamics for arbitrary initial conditions while directly enforcing target transport coefficients, converging to the exact Anderson-Witting solution. Validated against the Bjorken and Gubser flows, the framework reproduces the exact kinetic result where truncated methods fail.
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BibTeX
@misc{silva2026relaxationtime,
title = {{Relaxation-Time Boltzmann Solutions Without Truncations}},
author = {Tiago Nunes da Silva and Jadna L. Barauna and Giorgio Torrieri},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.35164},
eprint = {2609.35164},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.35164},
}
RIS
TY - UNPB
TI - Relaxation-Time Boltzmann Solutions Without Truncations
AU - Tiago Nunes da Silva
AU - Jadna L. Barauna
AU - Giorgio Torrieri
PY - 2026
DA - 2026/09/28
PB - arXiv
DO - 10.48550/arxiv.2609.35164
UR - https://arxiv.org/abs/2609.35164
AB - The relaxation-time Boltzmann equation governs relativistic matter far from equilibrium, but existing approaches rely on finite-order truncations that break down in this regime. We introduce ShARK (Stochastic Advection Relaxation Kinetics), the first fully 3D Monte Carlo kinetic framework to capture exact, far-from-equilibrium ultrarelativistic dynamics for arbitrary initial conditions while directly enforcing target transport coefficients, converging to the exact Anderson-Witting solution. Validated against the Bjorken and Gubser flows, the framework reproduces the exact kinetic result where truncated methods fail.
ER -