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(3+1)-dimensional dissipative relativistic fluid dynamics at non-zero net baryon density

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arxiv 1906.11181 v2 pith:BRVXA2NE submitted 2019-06-26 nucl-th hep-phnucl-exphysics.comp-ph

classification nucl-thhep-phnucl-exphysics.comp-ph
keywords baryoncodeevolutionbeshydrocurrentsdensitydimensionaldissipative
verification ladder T0 review T1 audit T2 compute T3 formal
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Heavy-ion collisions at center-of-mass energies between 1 and 100 GeV/nucleon are essential to understand the phase diagram of QCD and search for its critical point. At these energies the net baryon density of the system can be high, and simulating its evolution becomes an indispensable part of theoretical modeling. We here present the (3+1)-dimensional diffusive relativistic hydrodynamic code BEShydro which solves the equations of motion of second-order Denicol-Niemi-Molnar-Rischke (DNMR) theory, including bulk and shear viscous currents and baryon diffusion currents. BEShydro features a modular structure that allows to easily turn on and off baryon evolution and different dissipative effects and thus to study their physical effects on the dynamical evolution individually. An extensive set of test protocols for the code, including several novel tests of the precision of baryon transport that can also be used to test other such codes, is documented here and supplied as a permanent part of the code package.

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Cited by 2 Pith papers

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

  1. Critical net-proton number fluctuations with hydrodynamics

    nucl-th 2026-07 conditional novelty 6.0 of 10

    fRG critical fluctuations on hydrodynamic freeze-out hypersurfaces yield non-monotonic net-proton C4/C2 versus collision energy, absent in the HRG baseline.

  2. Attractor of hydrodynamic attractors

    nucl-th 2025-09 conditional novelty 6.0 of 10

    Second- and higher-order hydrodynamic attractors converge to the same universal curve before the Navier-Stokes limit, with the leading correction controlled only by second-order coefficients.

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