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Leading-order anisotropic hydrodynamics for central collisions
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Bottomonium suppression and elliptic flow using Heavy Quarkonium Quantum Dynamics
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Fireball tomography from bottomonia elliptic flow in relativistic heavy-ion collisions
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July 2021 |
Anisotropic hydrodynamic modeling of 2.76 TeV Pb-Pb collisions
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Bottomonium suppression in an open quantum system using the quantum trajectories method
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ϒ production in p–Pb collisions at s NN = 8.16 TeV
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July 2020 |
Nonperturbative potential for the study of quarkonia in QGP
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Static quark-antiquark interactions at nonzero temperature from lattice QCD
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Pseudorapidity distributions of charged hadrons in proton-lead collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ and 8.16 TeV
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Nuclear modification of Y states in pPb collisions at sNN=5.02TeV
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Bottomonium production in Pb + Pb collisions with ATLAS
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Resummed Relativistic Dissipative Hydrodynamics
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Heavy quarkonium suppression in a fireball
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Real time quarkonium transport coefficients in open quantum systems from Euclidean QCD
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May 2013 |
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January 2013 |
Investigating color screening in proton-nucleus collisions with complex potentials*
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February 2019 |
Quasiparticle anisotropic hydrodynamics for central collisions
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March 2017 |
Pion interferometry at 200 GeV using anisotropic hydrodynamics
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December 2020 |
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August 2019 |
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Complex Heavy-Quark Potential at Finite Temperature from Lattice QCD
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August 2021 |
QTRAJ 1.0: A Lindblad equation solver for heavy-quarkonium dynamics
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April 2022 |
Measurement of nuclear modification factors of ϒ(1S), ϒ(2S), and ϒ(3S) mesons in PbPb collisions at s NN = 5.02 TeV
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March 2019 |
Anisotropic escape mechanism and elliptic flow of bottomonia
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Measurement of ϒ ( 1 S ) Elliptic Flow at Forward Rapidity in Pb-Pb Collisions at s N N = 5.02 TeV
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Heavy quarkonium dynamics at next-to-leading order in the binding energy over temperature
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Forward-backward multiplicity correlations in the “wounded nucleon” model
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Υ production in U + U collisions at s N N = 193 GeV measured with the STAR experiment
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Anisotropic hydrodynamic modeling of 200 GeV Au-Au collisions
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Real-time static potential in hot QCD
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Suppression of Excited ϒ States Relative to the Ground State in Pb-Pb Collisions at s NN = 5.02 TeV
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Heavy quarkonium in a weakly-coupled quark-gluon plasma below the melting temperature
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Heavy-quarkonium suppression in p-A collisions from parton energy loss in cold QCD matter
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Quarkonium in-medium transport equation derived from first principles
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Quarkonia in the Quark Gluon Plasma
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Bottomonium suppression at RHIC and LHC in an open quantum system approach
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Bottomonium sequential suppression and strong heavy-quark potential in heavy-ion collisions
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Study of $$\upchi _{{\mathrm {b}}}$$ χ b meson production in $$\mathrm {p} $$ p $$\mathrm {p} $$ p collisions at $$\sqrt{s}=7$$ s = 7 and $$8{\mathrm {\,TeV}} $$ 8 TeV and observation of the decay $$\upchi _{{\mathrm {b}}}\mathrm {(3P)} \rightarrow \Upsilon \mathrm {(3S)} {\upgamma } $$ χ b ( 3 P ) → Υ ( 3 S ) γ
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Charged-particle pseudorapidity density at mid-rapidity in p–Pb collisions at $$\pmb {\sqrt{s_{\scriptscriptstyle {\mathrm{NN}}}}}$$ s NN = 8.16 TeV
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Directed flow in ultrarelativistic heavy-ion collisions
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Model study on Υ(nS) modification in small collision systems
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Quarkonium Production in Hadronic Collisions
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ϒ production and nuclear modification at forward rapidity in Pb–Pb collisions at s NN = 5.02 TeV
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Real and imaginary-time correlators in a thermal medium
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Bottomonium production in heavy-ion collisions using quantum trajectories: Differential observables and momentum anisotropy
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November 2021 |