Investigation of suppression of <math><mrow><mi mathvariant="normal">Υ</mi><mo>(</mo><mi>n</mi><mi>S</mi><mo>)</mo></mrow></math> in relativistic heavy-ion collisions at <math><mrow><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>200</mn></mrow></math> GeV and 5.02 TeV
- Kim, Junlee et al
- arXiv:2405.11689
 | Initial geometries in the temperature unit with different nuclear thickness parameters in the \trento model for central and peripheral heavy-ion collisions. |
 | Initial geometries in the temperature unit with different nuclear thickness parameters in the \trento model for central and peripheral heavy-ion collisions. |
 | Initial geometries in the temperature unit with different nuclear thickness parameters in the \trento model for central and peripheral heavy-ion collisions. |
 | Initial geometries in the temperature unit with different nuclear thickness parameters in the \trento model for central and peripheral heavy-ion collisions. |
 | Initial geometries in the temperature unit with different nuclear thickness parameters in the \trento model for central and peripheral heavy-ion collisions. |
 | Initial geometries in the temperature unit with different nuclear thickness parameters in the \trento model for central and peripheral heavy-ion collisions. |
 | Initial geometries in the temperature unit with different nuclear thickness parameters in the \trento model for central and peripheral heavy-ion collisions. |
 | Initial geometries in the temperature unit with different nuclear thickness parameters in the \trento model for central and peripheral heavy-ion collisions. |
 | The mean transverse area ($\langle S_T \rangle$) as a function of the number of participants in Pb--Pb collisions and Au--Au collisions for different thickness parameters. |
 | The mean transverse area ($\langle S_T \rangle$) as a function of the number of participants in Pb--Pb collisions and Au--Au collisions for different thickness parameters. |
 | The scaled charged particle multiplicity as a function of the number of participants in Au--Au collisions at $\sqsn=200$~GeV and Pb--Pb collisions at $\sqsn=5.02$~TeV. |
 | Elliptic flow of charged particles in Pb--Pb collisions at $\sqsn=$~5.02~TeV and Au--Au collisions at $\sqsn=$~200~GeV from the simulation and experimental measurements~\cite{ALICE:2018rtz,PHENIX:2009cjr}. The left (right) panels show the results in central (semi-central) collisions. |
 | Elliptic flow of charged particles in Pb--Pb collisions at $\sqsn=$~5.02~TeV and Au--Au collisions at $\sqsn=$~200~GeV from the simulation and experimental measurements~\cite{ALICE:2018rtz,PHENIX:2009cjr}. The left (right) panels show the results in central (semi-central) collisions. |
 | Elliptic flow of charged particles in Pb--Pb collisions at $\sqsn=$~5.02~TeV and Au--Au collisions at $\sqsn=$~200~GeV from the simulation and experimental measurements~\cite{ALICE:2018rtz,PHENIX:2009cjr}. The left (right) panels show the results in central (semi-central) collisions. |
 | Elliptic flow of charged particles in Pb--Pb collisions at $\sqsn=$~5.02~TeV and Au--Au collisions at $\sqsn=$~200~GeV from the simulation and experimental measurements~\cite{ALICE:2018rtz,PHENIX:2009cjr}. The left (right) panels show the results in central (semi-central) collisions. |
 | The nuclear modification factors of \Ups n in Pb--Pb collisions at $\sqsn=$~5.02~TeV. Simulation results using two $p$ parameters in the \trento model are compared with the experimental results by CMS~\cite{CMS:2018zza,CMS:2023lfu}. Statistical and systematic uncertainties of the experimental results are represented as vertical lines and boxes, respectively. |
 | The nuclear modification factors of \Ups n in Au--Au collisions at $\sqsn=$~200~GeV. Simulation results using two $p$ parameters in the \trento model compared with the experimental results by STAR~\cite{STAR:2022rpk}. Statistical and systematic uncertainties of the experimental results are represented as vertical lines and boxes, respectively. |
 | The nuclear modification factor of \Ups n as a function of the number of participants in Pb--Pb collisions at $\sqsn=5.02$~TeV with various formation times. |
 | The nuclear modification factor of \Ups n as a function of the number of participants in Pb--Pb collisions at $\sqsn=5.02$~TeV with various formation times. |
 | The nuclear modification factor of \Ups n as a function of the number of participants in Pb--Pb collisions at $\sqsn=5.02$~TeV with various formation times. |
 | The nuclear modification factor of \Ups n as a function of the number of participants in Au--Au collisions at $\sqsn=200$~GeV with various formation times. |
 | The nuclear modification factor of \Ups n as a function of the number of participants in Au--Au collisions at $\sqsn=200$~GeV with various formation times. |
 | The nuclear modification factor for given nuclear absorption cross-section (\sigabs) as a function of the number of participants in Au--Au collisions. |
 | The nuclear modification factor of \Ups 1 as a function of participants in Au--Au collisions at $\sqsn=200$ GeV, including the nuclear absorption effect. |
 | The nuclear modification factor of \Ups 2 as a function of participants in Au--Au collisions at $\sqsn=200$ GeV, including the nuclear absorption effect. |