TY - JOUR
T1 - Comparison of heavy-ion transport simulations
T2 - Collision integral with pions and ∆ resonances in a box
AU - Ono, Akira
AU - Xu, Jun
AU - Colonna, Maria
AU - Danielewicz, Pawel
AU - Ko, Che Ming
AU - Tsang, Manyee Betty
AU - Wang, Yong Jia
AU - Wolter, Hermann
AU - Zhang, Ying Xun
AU - Chen, Lie Wen
AU - Cozma, Dan
AU - Elfner, Hannah
AU - Feng, Zhao Qing
AU - Ikeno, Natsumi
AU - Li, Bao An
AU - Mallik, Swagata
AU - Nara, Yasushi
AU - Ogawa, Tatsuhiko
AU - Ohnishi, Akira
AU - Oliinychenko, Dmytro
AU - Su, Jun
AU - Song, Taesoo
AU - Zhang, Feng Shou
AU - Zhang, Zhen
N1 - Publisher Copyright:
Copyright © 2019, The Authors. All rights reserved.
Copyright:
Copyright 2020 Elsevier B.V., All rights reserved.
PY - 2019/4/5
Y1 - 2019/4/5
N2 - Background: Simulations by transport codes are indispensable for extracting valuable physical information from heavy-ion collisions. Pion observables such as the π−/π+ yield ratio are expected to be sensitive to the symmetry energy at high densities. Purpose: To evaluate, understand and reduce the uncertainties in transport-code results originating from different approximations in handling the production of ∆ resonances and pions. Methods: We compare ten transport codes under controlled conditions for a system confined in a box, with periodic boundary conditions, and initialized with nucleons at saturation density and at 60 MeV temperature. The reactions NN ↔ N∆ and ∆ ↔ Nπ are implemented, but the Pauli blocking and the mean-field potential are deactivated in the present comparison. Thus these are cascade calculations including pions and ∆ resonances. Results are compared to those from the two reference cases of a chemically equilibrated ideal gas mixture and of the rate equation. Results: For the numbers of ∆ and π, deviations from the reference values are observed in many codes, and they depend significantly on the size of the time step. These deviations are tied to different ways in ordering the sequence of reactions, such as collisions and decays, that take place in the same time step. Better agreements with the reference values are seen in the reaction rates and the number ratios among the isospin species of ∆ and π. Both the reaction rates and the number ratios are, however, affected by the correlations between particle positions, which are absent in the Boltzmann equation, but are induced by the way particle scatterings are treated in many of the transport calculations. The uncertainty in the transport-code predictions of the π−/π+ ratio, after letting the existing ∆ resonances decay, is found to be within a few percent for the system initialized at n/p = 1.5. Conclusions: The uncertainty in the final π−/π+ ratio in this simplified case of particles in a box is sufficiently small so that it does not strongly impact constraining the high-density symmetry energy from heavy-ion collisions. Most of the sources of uncertainties have been understood, and individual codes may be further improved in future applications. This investigation will be extended in the future to heavy-ion collisions to ensure the problems identified here remain under control.
AB - Background: Simulations by transport codes are indispensable for extracting valuable physical information from heavy-ion collisions. Pion observables such as the π−/π+ yield ratio are expected to be sensitive to the symmetry energy at high densities. Purpose: To evaluate, understand and reduce the uncertainties in transport-code results originating from different approximations in handling the production of ∆ resonances and pions. Methods: We compare ten transport codes under controlled conditions for a system confined in a box, with periodic boundary conditions, and initialized with nucleons at saturation density and at 60 MeV temperature. The reactions NN ↔ N∆ and ∆ ↔ Nπ are implemented, but the Pauli blocking and the mean-field potential are deactivated in the present comparison. Thus these are cascade calculations including pions and ∆ resonances. Results are compared to those from the two reference cases of a chemically equilibrated ideal gas mixture and of the rate equation. Results: For the numbers of ∆ and π, deviations from the reference values are observed in many codes, and they depend significantly on the size of the time step. These deviations are tied to different ways in ordering the sequence of reactions, such as collisions and decays, that take place in the same time step. Better agreements with the reference values are seen in the reaction rates and the number ratios among the isospin species of ∆ and π. Both the reaction rates and the number ratios are, however, affected by the correlations between particle positions, which are absent in the Boltzmann equation, but are induced by the way particle scatterings are treated in many of the transport calculations. The uncertainty in the transport-code predictions of the π−/π+ ratio, after letting the existing ∆ resonances decay, is found to be within a few percent for the system initialized at n/p = 1.5. Conclusions: The uncertainty in the final π−/π+ ratio in this simplified case of particles in a box is sufficiently small so that it does not strongly impact constraining the high-density symmetry energy from heavy-ion collisions. Most of the sources of uncertainties have been understood, and individual codes may be further improved in future applications. This investigation will be extended in the future to heavy-ion collisions to ensure the problems identified here remain under control.
UR - http://www.scopus.com/inward/record.url?scp=85094735817&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85094735817&partnerID=8YFLogxK
M3 - Article
AN - SCOPUS:85094735817
JO - [No source information available]
JF - [No source information available]
ER -