Searching for small droplets of hydrodynamic fluid in proton–proton collisions at the LHC
Abstract In this paper, we investigate the hydrodynamic collectivity in proton-proton collisions at $$\sqrt{s}=$$ s = 13 TeV, using iEBE-VISHNU with three different initial conditions, namely, HIJING, super-MC and TRENTo. With properly tuned parameters, hydrodynamics gives reasonable descriptions of...
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2020-09-01
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doaj-bff7d835d55b48bab711f9bf9e28125b2020-11-25T01:56:09ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522020-09-0180911110.1140/epjc/s10052-020-8376-xSearching for small droplets of hydrodynamic fluid in proton–proton collisions at the LHCWenbin Zhao0You Zhou1Koichi Murase2Huichao Song3Department of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking UniversityNiels Bohr Institute, University of CopenhagenCenter for High Energy Physics, Peking UniversityDepartment of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking UniversityAbstract In this paper, we investigate the hydrodynamic collectivity in proton-proton collisions at $$\sqrt{s}=$$ s = 13 TeV, using iEBE-VISHNU with three different initial conditions, namely, HIJING, super-MC and TRENTo. With properly tuned parameters, hydrodynamics gives reasonable descriptions of the measured two-particle correlations, including the integrated and $$p_\mathrm{T}$$ p T -differential flow. However, the hydrodynamic simulations fail to describe the negative four-particle cumulant $$c_2^v\{4\}$$ c 2 v { 4 } as measured in experiments. The four-particle cumulant $$c_2^v\{4\}$$ c 2 v { 4 } is always positive after hydrodynamic evolutions. Further investigations show that the non-linear response between the final $$v_2$$ v 2 and the initial $$\varepsilon _2$$ ε 2 becomes significant in p-p systems. This leads to a large deviation from linear eccentricity scaling and generates additional flow fluctuations, which results in a positive $$c_2^v\{4\}$$ c 2 v { 4 } even with a negative $$c_2^\varepsilon \{4\}$$ c 2 ε { 4 } from the initial state. We also presented the first hydrodynamic calculations of mixed harmonic azimuthal correlations in p-p collisions. Although many qualitative features are reproduced by the hydrodynamic simulations, the measured negative normalized Symmetric-Cumulant $$nsc_{2,3}\{4\}$$ n s c 2 , 3 { 4 } cannot be reproduced. Obviously hydrodynamic calculations have a general difficulty to describe the data. It triggers that whether hydrodynamics with a new initial state could solve this puzzle, or hydrodynamics itself is not the appreciated mechanism of the observed collectivity, and the non-hydrodynamic modes become important in p-p collisions at the LHC.http://link.springer.com/article/10.1140/epjc/s10052-020-8376-x |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Wenbin Zhao You Zhou Koichi Murase Huichao Song |
spellingShingle |
Wenbin Zhao You Zhou Koichi Murase Huichao Song Searching for small droplets of hydrodynamic fluid in proton–proton collisions at the LHC European Physical Journal C: Particles and Fields |
author_facet |
Wenbin Zhao You Zhou Koichi Murase Huichao Song |
author_sort |
Wenbin Zhao |
title |
Searching for small droplets of hydrodynamic fluid in proton–proton collisions at the LHC |
title_short |
Searching for small droplets of hydrodynamic fluid in proton–proton collisions at the LHC |
title_full |
Searching for small droplets of hydrodynamic fluid in proton–proton collisions at the LHC |
title_fullStr |
Searching for small droplets of hydrodynamic fluid in proton–proton collisions at the LHC |
title_full_unstemmed |
Searching for small droplets of hydrodynamic fluid in proton–proton collisions at the LHC |
title_sort |
searching for small droplets of hydrodynamic fluid in proton–proton collisions at the lhc |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2020-09-01 |
description |
Abstract In this paper, we investigate the hydrodynamic collectivity in proton-proton collisions at $$\sqrt{s}=$$ s = 13 TeV, using iEBE-VISHNU with three different initial conditions, namely, HIJING, super-MC and TRENTo. With properly tuned parameters, hydrodynamics gives reasonable descriptions of the measured two-particle correlations, including the integrated and $$p_\mathrm{T}$$ p T -differential flow. However, the hydrodynamic simulations fail to describe the negative four-particle cumulant $$c_2^v\{4\}$$ c 2 v { 4 } as measured in experiments. The four-particle cumulant $$c_2^v\{4\}$$ c 2 v { 4 } is always positive after hydrodynamic evolutions. Further investigations show that the non-linear response between the final $$v_2$$ v 2 and the initial $$\varepsilon _2$$ ε 2 becomes significant in p-p systems. This leads to a large deviation from linear eccentricity scaling and generates additional flow fluctuations, which results in a positive $$c_2^v\{4\}$$ c 2 v { 4 } even with a negative $$c_2^\varepsilon \{4\}$$ c 2 ε { 4 } from the initial state. We also presented the first hydrodynamic calculations of mixed harmonic azimuthal correlations in p-p collisions. Although many qualitative features are reproduced by the hydrodynamic simulations, the measured negative normalized Symmetric-Cumulant $$nsc_{2,3}\{4\}$$ n s c 2 , 3 { 4 } cannot be reproduced. Obviously hydrodynamic calculations have a general difficulty to describe the data. It triggers that whether hydrodynamics with a new initial state could solve this puzzle, or hydrodynamics itself is not the appreciated mechanism of the observed collectivity, and the non-hydrodynamic modes become important in p-p collisions at the LHC. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-020-8376-x |
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