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Scaling properties of fractional momentum loss of high-$$p_T$$ hadrons in nucleus-nucleus collisions at $$sqrt{s_{NN}}$$ from 62.4 GeV to 2.76 TeV

$$sqrt{s_{NN}}$$が62.4GeV 2.76TeVまでの原子核-原子核衝突における高横運動量粒子の運動量損失についてのスケーリング性

Adare, A.*; 長谷川 勝一   ; 今井 憲一; 永宮 正治; 佐甲 博之   ; 佐藤 進  ; 谷田 聖   ; PHENIX Collaboration*; 他623名*

Adare, A.*; Hasegawa, Shoichi; Imai, Kenichi; Nagamiya, Shoji; Sako, Hiroyuki; Sato, Susumu; Tanida, Kiyoshi; PHENIX Collaboration*; 623 of others*

Measurements of the fractional momentum loss ($$S_{rm loss}=delta p_T/p_T$$) of high-transverse-momentum-identified hadrons in heavy-ion collisions are presented. Using $$pi^0$$ in Au+Au and Cu+Cu collisions at $$sqrt{s_{NN}}$$ = 62.4 and 200 GeV measured by the PHENIX experiment at the Relativistic Heavy Ion Collider and and charged hadrons in Pb+Pb collisions measured by the ALICE experiment at the Large Hadron Collider, we studied the scaling properties of $$S_{rm loss}$$ as a function of a number of variables: the number of participants, $$N_{rm part}$$, the number of quark participants, $$N_{qp}$$, the charged-particle density, $$dN_{rm ch}/deta$$, and the Bjorken energy density times the equilibration time, $$epsilon_{Bj}tau_0$$. We find that the $$p_T$$, where $$S_{rm loss}$$ has its maximum, varies both with centrality and collision energy. Above the maximum, $$S_{rm loss}$$ tends to follow a power-law function with all four scaling variables. The data at $$sqrt{s_{NN}}$$ = 200 and 2.76 TeV, for sufficiently high particle densities, have a common scaling of $$S_{rm loss}$$ with $$dN_{rm ch}/deta$$ and $$epsilon_{Bj}tau_0$$, lending insight into the physics of parton energy loss.

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パーセンタイル:75.78

分野:Physics, Nuclear

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