TY - JOUR
T1 - Monte Carlo event generator for initial conditions of conserved charges in nuclear geometry
AU - Carzon, Patrick
AU - Martinez, Mauricio
AU - Sievert, Matthew D.
AU - Wertepny, Douglas E.
AU - Noronha-Hostler, Jacquelyn
N1 - Funding Information:
The authors thank G. Denicol, A. Dumitru, J. Jalilian-Marian, Y. Kovchegov, M. Luzum, J. Nagle, P. Romatschke, T. Schaefer, V. Skokov, P. Sorensen, and P. Tribedy for useful discussions. We thank G. Denicol for elucidating the useful order-of-magnitude estimate in Appendix . The authors thank the anonymous referees for their excellent feedback which helped us to refine our original approach. M.M. acknowledges support from the U.S.-DOE Nuclear Science Grant No. DE-FG02-03ER41260 and the BEST (Beam Energy Scan Theory) DOE Topical Collaboration. M.D.S. acknowledges support from a startup grant from New Mexico State University. D.E.W. acknowledges previous support from the Zuckerman STEM Leadership Program. J.N.H. acknowledges the support from the U.S.-DOE Nuclear Science Grant No. DE-SC0020633, and from the Illinois Campus Cluster, a computing resource that is operated by the Illinois Campus Cluster Program (ICCP) in conjunction with the National Center for Supercomputing Applications (NCSA), and which is supported by funds from the University of Illinois at Urbana-Champaign.
Publisher Copyright:
© 2022 American Physical Society.
PY - 2022/3
Y1 - 2022/3
N2 - At top collider energies where baryon stopping is negligible, the initial state of heavy-ion collisions is overall charge neutral and predominantly composed of gluons. Nevertheless, there can also be significant local fluctuations of the baryon number, strangeness, and electric charge densities about zero, perturbatively corresponding to the production of quark/antiquark pairs. These previously ignored local charge fluctuations can permit the study of charge diffusion in the quark-gluon plasma (QGP), even at top collider energies. In this paper we present a new model denoted ICCING (initial conserved charges in nuclear geometry) which can reconstruct the initial conditions of conserved charges in the QGP by sampling a (g→qq¯) splitting probability over the initial energy density. We find that the new charge distributions generally differ from the bulk energy density; in particular, the strangeness distribution is significantly more eccentric than standard bulk observables and appears to be associated with the geometry of hot spots in the initial state. The new information provided by these conserved charges opens the door to studying a wealth of new charge-and flavor-dependent correlations in the initial state and ultimately the charge transport parameters of the QGP.
AB - At top collider energies where baryon stopping is negligible, the initial state of heavy-ion collisions is overall charge neutral and predominantly composed of gluons. Nevertheless, there can also be significant local fluctuations of the baryon number, strangeness, and electric charge densities about zero, perturbatively corresponding to the production of quark/antiquark pairs. These previously ignored local charge fluctuations can permit the study of charge diffusion in the quark-gluon plasma (QGP), even at top collider energies. In this paper we present a new model denoted ICCING (initial conserved charges in nuclear geometry) which can reconstruct the initial conditions of conserved charges in the QGP by sampling a (g→qq¯) splitting probability over the initial energy density. We find that the new charge distributions generally differ from the bulk energy density; in particular, the strangeness distribution is significantly more eccentric than standard bulk observables and appears to be associated with the geometry of hot spots in the initial state. The new information provided by these conserved charges opens the door to studying a wealth of new charge-and flavor-dependent correlations in the initial state and ultimately the charge transport parameters of the QGP.
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U2 - 10.1103/PhysRevC.105.034908
DO - 10.1103/PhysRevC.105.034908
M3 - Article
AN - SCOPUS:85127490230
SN - 2469-9985
VL - 105
JO - Physical Review C
JF - Physical Review C
IS - 3
M1 - 034908
ER -