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Title: Heavy-quark production and elliptic flow in Au+Au collisions at √s NN=62.4 GeV

In this study, we present measurements of electrons and positrons from the semileptonic decays of heavy-flavor hadrons at midrapidity (|y|< 0.35) in Au+Au collisions at √s NN = 62.4 GeV. The data were collected in 2010 by the PHENIX experiment that included the new hadron-blind detector. The invariant yield of electrons from heavy-flavor decays is measured as a function of transverse momentum in the range 1 < p e T < 5 GeV/c. The invariant yield per binary collision is slightly enhanced above the p+p reference in Au+Au 0%–20%, 20%–40%, and 40%–60% centralities at a comparable level. At this low beam energy this may be a result of the interplay between initial-state Cronin effects, final-state flow, and energy loss in medium. The v₂ of electrons from heavy-flavor decays is nonzero when averaged between 1.3 < p e T < 2.5 GeV/c for 0%–40% centrality collisions at √s NN = 62.4 GeV. For 20%–40% centrality collisions, the v₂ at √s NN = 62.4 GeV is smaller than that for heavy-flavor decays at √s NN = 200 GeV. The v₂ of the electrons from heavy-flavor decay at the lower beam energy is also smaller than v₂ for pions. Both results indicate thatmore » the heavy-quarks interact with the medium formed in these collisions, but they may not be at the same level of thermalization with the medium as observed at √s NN = 200 GeV.« less
Authors:
 [1]
  1. Univ. of Colorado, Boulder, CO (United States). et al.
Publication Date:
Report Number(s):
BNL-108103-2015-JA
Journal ID: ISSN 0556-2813; PRVCAN; KB0201021
Grant/Contract Number:
SC00112704; AC05-00OR22725
Type:
Accepted Manuscript
Journal Name:
Physical Review. C, Nuclear Physics
Additional Journal Information:
Journal Volume: 91; Journal Issue: 4; Journal ID: ISSN 0556-2813
Publisher:
American Physical Society (APS)
Research Org:
Brookhaven National Laboratory (BNL), Upton, NY (United States); Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
Sponsoring Org:
USDOE Office of Science (SC), High Energy Physics (HEP) (SC-25)
Country of Publication:
United States
Language:
English
Subject:
73 NUCLEAR PHYSICS AND RADIATION PHYSICS; heavy-quark; elliptic; Au+Au; collisions; 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
OSTI Identifier:
1213358
Alternate Identifier(s):
OSTI ID: 1180932; OSTI ID: 1338502

Adare, A. Heavy-quark production and elliptic flow in Au+Au collisions at √sNN=62.4 GeV. United States: N. p., Web. doi:10.1103/PhysRevC.91.044907.
Adare, A. Heavy-quark production and elliptic flow in Au+Au collisions at √sNN=62.4 GeV. United States. doi:10.1103/PhysRevC.91.044907.
Adare, A. 2015. "Heavy-quark production and elliptic flow in Au+Au collisions at √sNN=62.4 GeV". United States. doi:10.1103/PhysRevC.91.044907. https://www.osti.gov/servlets/purl/1213358.
@article{osti_1213358,
title = {Heavy-quark production and elliptic flow in Au+Au collisions at √sNN=62.4 GeV},
author = {Adare, A.},
abstractNote = {In this study, we present measurements of electrons and positrons from the semileptonic decays of heavy-flavor hadrons at midrapidity (|y|< 0.35) in Au+Au collisions at √sNN = 62.4 GeV. The data were collected in 2010 by the PHENIX experiment that included the new hadron-blind detector. The invariant yield of electrons from heavy-flavor decays is measured as a function of transverse momentum in the range 1 < peT < 5 GeV/c. The invariant yield per binary collision is slightly enhanced above the p+p reference in Au+Au 0%–20%, 20%–40%, and 40%–60% centralities at a comparable level. At this low beam energy this may be a result of the interplay between initial-state Cronin effects, final-state flow, and energy loss in medium. The v₂ of electrons from heavy-flavor decays is nonzero when averaged between 1.3 < peT < 2.5 GeV/c for 0%–40% centrality collisions at √sNN = 62.4 GeV. For 20%–40% centrality collisions, the v₂ at √sNN = 62.4 GeV is smaller than that for heavy-flavor decays at √sNN = 200 GeV. The v₂ of the electrons from heavy-flavor decay at the lower beam energy is also smaller than v₂ for pions. Both results indicate that the heavy-quarks interact with the medium formed in these collisions, but they may not be at the same level of thermalization with the medium as observed at √sNN = 200 GeV.},
doi = {10.1103/PhysRevC.91.044907},
journal = {Physical Review. C, Nuclear Physics},
number = 4,
volume = 91,
place = {United States},
year = {2015},
month = {4}
}