- Main
Azimuthal Harmonics in Small and Large Collision Systems at RHIC Top Energies
- Adam, J;
- Adamczyk, L;
- Adams, JR;
- Adkins, JK;
- Agakishiev, G;
- Aggarwal, MM;
- Ahammed, Z;
- Alekseev, I;
- Anderson, DM;
- Aoyama, R;
- Aparin, A;
- Arkhipkin, D;
- Aschenauer, EC;
- Ashraf, MU;
- Atetalla, F;
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- Bunzarov, I;
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- de la Barca Sánchez, M Calderón;
- Cebra, D;
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- Chan, BK;
- Chang, F-H;
- Chang, Z;
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- Horvat, S;
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- Jiang, K;
- Jowzaee, S;
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- Kabana, S;
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- Kalinkin, D;
- Kang, K;
- Kapukchyan, D;
- Kauder, K;
- Ke, HW;
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- Kikoła, DP;
- Kim, C;
- Kinghorn, TA;
- Kisel, I;
- Kisiel, A;
- Kochenda, L;
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- Kumar, L;
- Elayavalli, R Kunnawalkam;
- Kvapil, J;
- Kwasizur, JH;
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- Landgraf, JM;
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- Lebedev, A;
- Lednicky, R;
- Lee, JH;
- Li, C;
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- Li, Y;
- Liang, Y;
- Lidrych, J;
- Lin, T;
- Lipiec, A;
- Lisa, MA;
- Liu, F;
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- Ljubicic, T;
- Llope, WJ;
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- Longacre, RS;
- Luo, S;
- Luo, X;
- L., G;
- Ma, L;
- Ma, R;
- G., Y;
- Magdy, N;
- Majka, R;
- Mallick, D;
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- Markert, C;
- Matis, HS;
- Matonoha, O;
- Mazer, JA;
- Meehan, K;
- Mei, JC;
- Minaev, NG;
- Mioduszewski, S;
- Mishra, D;
- Mohanty, B;
- Mondal, MM;
- Mooney, I;
- Morozov, DA;
- Nasim;
- Negrete, JD;
- Nelson, JM;
- Nemes, DB;
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- Niida, T;
- Nogach, LV;
- Nonaka, T;
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- Oh, K;
- Oh, S;
- Okorokov, VA;
- Olvitt, D;
- Page, BS;
- Pak, R;
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- Pawlik, B;
- Pei, H;
- Perkins, C;
- Pinter, RL;
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- Porter, J;
- Posik, M;
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- Romero, JL;
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- Seger, J;
- Sergeeva, M;
- Seto, R;
- Seyboth, P;
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- Suaide, AAP;
- Sugiura, T;
- Sumbera, M;
- Summa, B;
- Sun, XM;
- Sun, X;
- Sun, Y;
- Surrow, B;
- Svirida, DN;
- Szymanski, P;
- Tang, AH;
- Tang, Z;
- Taranenko, A;
- Tarnowsky, T;
- Thomas, JH;
- Timmins, AR;
- Tlusty, D;
- Todoroki, T;
- Tokarev, M;
- Tomkiel, CA;
- Trentalange, S;
- Tribble, RE;
- Tribedy, P;
- Tripathy, SK;
- Tsai, OD;
- Tu, B;
- Ullrich, T;
- Underwood, DG;
- Upsal, I;
- Van Buren, G;
- Vanek, J;
- Vasiliev, AN;
- Vassiliev, I;
- Videbæk, F;
- Vokal, S;
- Voloshin, SA;
- Vossen, A;
- Wang, F;
- Wang, G;
- Wang, P;
- Wang, Y;
- Wang, Y;
- Webb, JC;
- Wen, L;
- Westfall, GD;
- Wieman, H;
- Wissink, SW;
- Witt, R;
- Wu, Y;
- Xiao, ZG;
- Xie, G;
- Xie, W;
- Xu, J;
- Xu, N;
- Xu, QH;
- Xu, YF;
- Xu, Z;
- Yang, C;
- Yang, Q;
- Yang, S;
- Yang, Y;
- Ye, Z;
- Ye, Z;
- Yi, L;
- Yip, K;
- Yoo, I-K;
- Yu, N;
- Zbroszczyk, H;
- Zha, W;
- Zhang, J;
- Zhang, J;
- Zhang, L;
- Zhang, S;
- Zhang, S;
- Zhang, XP;
- Zhang, Y;
- Zhang, Z;
- Zhao, J;
- Zhong, C;
- Zhou, C;
- Zhu, X;
- Zhu, Z;
- Zyzak, M
- et al.
Published Web Location
https://doi.org/10.1103/physrevlett.122.172301Abstract
The first (v_{1}^{fluc}), second (v_{2}), and third (v_{3}) harmonic coefficients of the azimuthal particle distribution at midrapidity are extracted for charged hadrons and studied as a function of transverse momentum (p_{T}) and mean charged particle multiplicity density ⟨N_{ch}⟩ in U+U (sqrt[s_{NN}]=193 GeV), Au+Au, Cu+Au, Cu+Cu, d+Au, and p+Au collisions at sqrt[s_{NN}]=200 GeV with the STAR detector. For the same ⟨N_{ch}⟩, the v_{1}^{fluc} and v_{3} coefficients are observed to be independent of the collision system, while v_{2} exhibits such a scaling only when normalized by the initial-state eccentricity (ϵ_{2}). The data also show that ln(v_{2}/ϵ_{2}) scales linearly with ⟨N_{ch}⟩^{-1/3}. These measurements provide insight into initial-geometry fluctuations and the role of viscous hydrodynamic attenuation on v_{n} from small to large collision systems.
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