2020
DOI: 10.1016/j.physletb.2020.135465
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Charm and beauty isolation from heavy flavor decay electrons in Au+Au collisions at sNN = 200 GeV at RHIC

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Cited by 12 publications
(10 citation statements)
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“…In previous study, the charm and beauty contributions are separated from the inclusive heavy flavor electrons (HFE) in 200 GeV Au+Au collisions at RHIC [20]. It was found that the electron AA from beauty decays is less suppressed compared to that from charm decays, which is consistent with the mass-dependent energy loss expectation.…”
Section: Introductionsupporting
confidence: 69%
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“…In previous study, the charm and beauty contributions are separated from the inclusive heavy flavor electrons (HFE) in 200 GeV Au+Au collisions at RHIC [20]. It was found that the electron AA from beauty decays is less suppressed compared to that from charm decays, which is consistent with the mass-dependent energy loss expectation.…”
Section: Introductionsupporting
confidence: 69%
“…We adopt the data-driven method developed in Ref. [20] to separate charm and beauty decay contributions from the inclusive HFE spectra [21] in 0-10% and 30-50% central Pb+Pb collisions at √ NN = 5.02 TeV at LHC by taking advantage of the most recent charmed hadron measurements. Different from the previous study at RHIC energy, the HFE measurement [21] from the ALICE experiment was not subtracted by the J∕ contribution (about 5% at 2 < T < 3 GeV/ and much lower in other T regions), and thus, the J∕ → + − contribution is also studied in this work.…”
Section: Transverse Momentum Spectra and Aamentioning
confidence: 99%
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“…In the extremely hot and dense condition created in relativistic heavy-ion collisions, those partons can be liberated via deconfinement to form Quark-Gluon Plasma (QGP) [1,2], which is believed to exist in the early universe around tens of microseconds after the Big Bang. Many experimental evidences show that the QGP is strongly coupled and behaves like a perfect liquid [3][4][5][6][7][8][9]. The Quantum Chromodynamics (QCD) predicts that at large temperature (T ) and small baryon chemical potential (µ B ), it is a smooth crossover from hadronic phase to partonic phase [10].…”
Section: Introductionmentioning
confidence: 99%