Quarkonium production in heavy ion collisions: coupled Boltzmann transport equations
We develop a set of coupled Boltzmann equations to describe the dynamical evolution of heavy quarks and quarkonia inside the quark-gluon plasma. The quarkonium dissociation and recombination terms are calculated from pNRQCD. Their interplay drives the system to a detailed balance. The heavy quark en...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Yao, Xiaojun [verfasserIn] Ke, Weiyao [verfasserIn] Xu, Yingru [verfasserIn] Bass, Steffen [verfasserIn] Müller, Berndt [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2018 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Nuclear physics |
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| Übergeordnetes Werk: |
volume:982 |
| DOI / URN: |
10.1016/j.nuclphysa.2018.10.005 |
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| Katalog-ID: |
ELV001445022 |
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| 024 | 7 | |a 10.1016/j.nuclphysa.2018.10.005 |2 doi | |
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| 100 | 1 | |a Yao, Xiaojun |e verfasserin |0 (orcid)0000-0002-8377-2203 |4 aut | |
| 245 | 1 | 0 | |a Quarkonium production in heavy ion collisions: coupled Boltzmann transport equations |
| 264 | 1 | |c 2018 | |
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| 337 | |a Computermedien |b c |2 rdamedia | ||
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| 520 | |a We develop a set of coupled Boltzmann equations to describe the dynamical evolution of heavy quarks and quarkonia inside the quark-gluon plasma. The quarkonium dissociation and recombination terms are calculated from pNRQCD. Their interplay drives the system to a detailed balance. The heavy quark energy loss term is necessary for the system to reach kinematic thermalization. By coupling the transport equations with initial particles' momenta generated by Pythia and hydrodynamic medium evolutions, we can describe the R AA of ϒ family at both RHIC and LHC energies. The transverse momentum azimuthal anisotropy of ϒ(1S) in 2.76 TeV peripheral Pb-Pb collisions is also studied. | ||
| 650 | 4 | |a quarkonium production | |
| 650 | 4 | |a heavy ion collision | |
| 650 | 4 | |a Boltzmann equation | |
| 650 | 4 | |a pNRQCD | |
| 650 | 4 | |a detailed balance | |
| 650 | 4 | |a equilibrium | |
| 700 | 1 | |a Ke, Weiyao |e verfasserin |4 aut | |
| 700 | 1 | |a Xu, Yingru |e verfasserin |0 (orcid)0000-0002-3244-3151 |4 aut | |
| 700 | 1 | |a Bass, Steffen |e verfasserin |0 (orcid)0000-0002-9451-0954 |4 aut | |
| 700 | 1 | |a Müller, Berndt |e verfasserin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Nuclear physics <Amsterdam> / A |d Amsterdam : North-Holland Publ. Co., 1967 |g 982 |h Online-Ressource |w (DE-627)266014755 |w (DE-600)1466542-6 |w (DE-576)074959778 |x 1873-1554 |7 nnns |
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| 936 | b | k | |a 33.40 |j Kernphysik |
| 936 | b | k | |a 33.50 |j Physik der Elementarteilchen und Felder: Allgemeines |
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10.1016/j.nuclphysa.2018.10.005 doi (DE-627)ELV001445022 (ELSEVIER)S0375-9474(18)30278-1 DE-627 ger DE-627 rda eng 530 DE-600 33.40 bkl 33.50 bkl Yao, Xiaojun verfasserin (orcid)0000-0002-8377-2203 aut Quarkonium production in heavy ion collisions: coupled Boltzmann transport equations 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We develop a set of coupled Boltzmann equations to describe the dynamical evolution of heavy quarks and quarkonia inside the quark-gluon plasma. The quarkonium dissociation and recombination terms are calculated from pNRQCD. Their interplay drives the system to a detailed balance. The heavy quark energy loss term is necessary for the system to reach kinematic thermalization. By coupling the transport equations with initial particles' momenta generated by Pythia and hydrodynamic medium evolutions, we can describe the R AA of ϒ family at both RHIC and LHC energies. The transverse momentum azimuthal anisotropy of ϒ(1S) in 2.76 TeV peripheral Pb-Pb collisions is also studied. quarkonium production heavy ion collision Boltzmann equation pNRQCD detailed balance equilibrium Ke, Weiyao verfasserin aut Xu, Yingru verfasserin (orcid)0000-0002-3244-3151 aut Bass, Steffen verfasserin (orcid)0000-0002-9451-0954 aut Müller, Berndt verfasserin aut Enthalten in Nuclear physics <Amsterdam> / A Amsterdam : North-Holland Publ. Co., 1967 982 Online-Ressource (DE-627)266014755 (DE-600)1466542-6 (DE-576)074959778 1873-1554 nnns volume:982 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.40 Kernphysik 33.50 Physik der Elementarteilchen und Felder: Allgemeines AR 982 |
| spelling |
10.1016/j.nuclphysa.2018.10.005 doi (DE-627)ELV001445022 (ELSEVIER)S0375-9474(18)30278-1 DE-627 ger DE-627 rda eng 530 DE-600 33.40 bkl 33.50 bkl Yao, Xiaojun verfasserin (orcid)0000-0002-8377-2203 aut Quarkonium production in heavy ion collisions: coupled Boltzmann transport equations 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We develop a set of coupled Boltzmann equations to describe the dynamical evolution of heavy quarks and quarkonia inside the quark-gluon plasma. The quarkonium dissociation and recombination terms are calculated from pNRQCD. Their interplay drives the system to a detailed balance. The heavy quark energy loss term is necessary for the system to reach kinematic thermalization. By coupling the transport equations with initial particles' momenta generated by Pythia and hydrodynamic medium evolutions, we can describe the R AA of ϒ family at both RHIC and LHC energies. The transverse momentum azimuthal anisotropy of ϒ(1S) in 2.76 TeV peripheral Pb-Pb collisions is also studied. quarkonium production heavy ion collision Boltzmann equation pNRQCD detailed balance equilibrium Ke, Weiyao verfasserin aut Xu, Yingru verfasserin (orcid)0000-0002-3244-3151 aut Bass, Steffen verfasserin (orcid)0000-0002-9451-0954 aut Müller, Berndt verfasserin aut Enthalten in Nuclear physics <Amsterdam> / A Amsterdam : North-Holland Publ. Co., 1967 982 Online-Ressource (DE-627)266014755 (DE-600)1466542-6 (DE-576)074959778 1873-1554 nnns volume:982 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.40 Kernphysik 33.50 Physik der Elementarteilchen und Felder: Allgemeines AR 982 |
| allfields_unstemmed |
10.1016/j.nuclphysa.2018.10.005 doi (DE-627)ELV001445022 (ELSEVIER)S0375-9474(18)30278-1 DE-627 ger DE-627 rda eng 530 DE-600 33.40 bkl 33.50 bkl Yao, Xiaojun verfasserin (orcid)0000-0002-8377-2203 aut Quarkonium production in heavy ion collisions: coupled Boltzmann transport equations 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We develop a set of coupled Boltzmann equations to describe the dynamical evolution of heavy quarks and quarkonia inside the quark-gluon plasma. The quarkonium dissociation and recombination terms are calculated from pNRQCD. Their interplay drives the system to a detailed balance. The heavy quark energy loss term is necessary for the system to reach kinematic thermalization. By coupling the transport equations with initial particles' momenta generated by Pythia and hydrodynamic medium evolutions, we can describe the R AA of ϒ family at both RHIC and LHC energies. The transverse momentum azimuthal anisotropy of ϒ(1S) in 2.76 TeV peripheral Pb-Pb collisions is also studied. quarkonium production heavy ion collision Boltzmann equation pNRQCD detailed balance equilibrium Ke, Weiyao verfasserin aut Xu, Yingru verfasserin (orcid)0000-0002-3244-3151 aut Bass, Steffen verfasserin (orcid)0000-0002-9451-0954 aut Müller, Berndt verfasserin aut Enthalten in Nuclear physics <Amsterdam> / A Amsterdam : North-Holland Publ. Co., 1967 982 Online-Ressource (DE-627)266014755 (DE-600)1466542-6 (DE-576)074959778 1873-1554 nnns volume:982 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.40 Kernphysik 33.50 Physik der Elementarteilchen und Felder: Allgemeines AR 982 |
| allfieldsGer |
10.1016/j.nuclphysa.2018.10.005 doi (DE-627)ELV001445022 (ELSEVIER)S0375-9474(18)30278-1 DE-627 ger DE-627 rda eng 530 DE-600 33.40 bkl 33.50 bkl Yao, Xiaojun verfasserin (orcid)0000-0002-8377-2203 aut Quarkonium production in heavy ion collisions: coupled Boltzmann transport equations 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We develop a set of coupled Boltzmann equations to describe the dynamical evolution of heavy quarks and quarkonia inside the quark-gluon plasma. The quarkonium dissociation and recombination terms are calculated from pNRQCD. Their interplay drives the system to a detailed balance. The heavy quark energy loss term is necessary for the system to reach kinematic thermalization. By coupling the transport equations with initial particles' momenta generated by Pythia and hydrodynamic medium evolutions, we can describe the R AA of ϒ family at both RHIC and LHC energies. The transverse momentum azimuthal anisotropy of ϒ(1S) in 2.76 TeV peripheral Pb-Pb collisions is also studied. quarkonium production heavy ion collision Boltzmann equation pNRQCD detailed balance equilibrium Ke, Weiyao verfasserin aut Xu, Yingru verfasserin (orcid)0000-0002-3244-3151 aut Bass, Steffen verfasserin (orcid)0000-0002-9451-0954 aut Müller, Berndt verfasserin aut Enthalten in Nuclear physics <Amsterdam> / A Amsterdam : North-Holland Publ. Co., 1967 982 Online-Ressource (DE-627)266014755 (DE-600)1466542-6 (DE-576)074959778 1873-1554 nnns volume:982 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.40 Kernphysik 33.50 Physik der Elementarteilchen und Felder: Allgemeines AR 982 |
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marc |
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2018 |
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zzz |
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Yao, Xiaojun Ke, Weiyao Xu, Yingru Bass, Steffen Müller, Berndt |
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Elektronische Aufsätze |
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Yao, Xiaojun |
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10.1016/j.nuclphysa.2018.10.005 |
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530 |
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verfasserin |
| title_sort |
quarkonium production in heavy ion collisions: coupled boltzmann transport equations |
| title_auth |
Quarkonium production in heavy ion collisions: coupled Boltzmann transport equations |
| abstract |
We develop a set of coupled Boltzmann equations to describe the dynamical evolution of heavy quarks and quarkonia inside the quark-gluon plasma. The quarkonium dissociation and recombination terms are calculated from pNRQCD. Their interplay drives the system to a detailed balance. The heavy quark energy loss term is necessary for the system to reach kinematic thermalization. By coupling the transport equations with initial particles' momenta generated by Pythia and hydrodynamic medium evolutions, we can describe the R AA of ϒ family at both RHIC and LHC energies. The transverse momentum azimuthal anisotropy of ϒ(1S) in 2.76 TeV peripheral Pb-Pb collisions is also studied. |
| abstractGer |
We develop a set of coupled Boltzmann equations to describe the dynamical evolution of heavy quarks and quarkonia inside the quark-gluon plasma. The quarkonium dissociation and recombination terms are calculated from pNRQCD. Their interplay drives the system to a detailed balance. The heavy quark energy loss term is necessary for the system to reach kinematic thermalization. By coupling the transport equations with initial particles' momenta generated by Pythia and hydrodynamic medium evolutions, we can describe the R AA of ϒ family at both RHIC and LHC energies. The transverse momentum azimuthal anisotropy of ϒ(1S) in 2.76 TeV peripheral Pb-Pb collisions is also studied. |
| abstract_unstemmed |
We develop a set of coupled Boltzmann equations to describe the dynamical evolution of heavy quarks and quarkonia inside the quark-gluon plasma. The quarkonium dissociation and recombination terms are calculated from pNRQCD. Their interplay drives the system to a detailed balance. The heavy quark energy loss term is necessary for the system to reach kinematic thermalization. By coupling the transport equations with initial particles' momenta generated by Pythia and hydrodynamic medium evolutions, we can describe the R AA of ϒ family at both RHIC and LHC energies. The transverse momentum azimuthal anisotropy of ϒ(1S) in 2.76 TeV peripheral Pb-Pb collisions is also studied. |
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| title_short |
Quarkonium production in heavy ion collisions: coupled Boltzmann transport equations |
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Ke, Weiyao Xu, Yingru Bass, Steffen Müller, Berndt |
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