Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description
Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$...
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| Autor*in: |
Singh, Aditya Kumar [verfasserIn] Akhil, Aviral [verfasserIn] Tiwari, Swatantra Kumar [verfasserIn] Pareek, Pooja [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2024 |
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| Anmerkung: |
© The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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| Übergeordnetes Werk: |
Enthalten in: The European physical journal - Springer Berlin Heidelberg, 2011, 139(2024), 6 vom: 06. Juni |
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| Übergeordnetes Werk: |
volume:139 ; year:2024 ; number:6 ; day:06 ; month:06 |
| Links: |
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| DOI / URN: |
10.1140/epjp/s13360-024-05290-0 |
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SPR056146175 |
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10.1140/epjp/s13360-024-05290-0 doi (DE-627)SPR056146175 (SPR)s13360-024-05290-0-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Singh, Aditya Kumar verfasserin aut Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, respectively at Large hadron collider (LHC) energy of $$\sqrt{s_{NN}}$$ = 5.02 TeV. We have also analysed the experimental data of transverse momentum ($$p_T$$) spectra for these identified hadrons at LHC for Pb-Pb as well as for p-Pb collisions. We have used Boltzmann transport equation (BTE) in relaxation time approximation (RTA) for this analysis. The Tsallis statistics is used as an initial distribution function and the Tsallis blast wave (TBW) model is employed as an equilibrium distribution in BTE. The present model fits the measured transverse momentum spectra, $$R_{PbPb}$$, and $$R_{pPb}$$ successfully upto $$p_T$$ = 8 GeV/c with a reasonable $$\chi ^2/ndf$$ for all the considered hadrons at various centralities. The experimental data for $$R_{pPb}$$ are generated using the particle yields at p-Pb and pp collisions where number of binary collisions are taken from Glauber model calculations. We find that the average transverse flow velocity ($$<\beta _r>$$) decreases with the mass as well as when one move from the central collisions to the peripheral collisions. These findings are inline with the results of the hydrodynamics-inspired model calculations. Akhil, Aviral verfasserin aut Tiwari, Swatantra Kumar verfasserin (orcid)0000-0003-4854-8174 aut Pareek, Pooja verfasserin aut Enthalten in The European physical journal Springer Berlin Heidelberg, 2011 139(2024), 6 vom: 06. Juni (DE-627)647653958 (DE-600)2595693-0 2190-5444 nnns volume:139 year:2024 number:6 day:06 month:06 https://dx.doi.org/10.1140/epjp/s13360-024-05290-0 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 139 2024 6 06 06 |
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10.1140/epjp/s13360-024-05290-0 doi (DE-627)SPR056146175 (SPR)s13360-024-05290-0-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Singh, Aditya Kumar verfasserin aut Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, respectively at Large hadron collider (LHC) energy of $$\sqrt{s_{NN}}$$ = 5.02 TeV. We have also analysed the experimental data of transverse momentum ($$p_T$$) spectra for these identified hadrons at LHC for Pb-Pb as well as for p-Pb collisions. We have used Boltzmann transport equation (BTE) in relaxation time approximation (RTA) for this analysis. The Tsallis statistics is used as an initial distribution function and the Tsallis blast wave (TBW) model is employed as an equilibrium distribution in BTE. The present model fits the measured transverse momentum spectra, $$R_{PbPb}$$, and $$R_{pPb}$$ successfully upto $$p_T$$ = 8 GeV/c with a reasonable $$\chi ^2/ndf$$ for all the considered hadrons at various centralities. The experimental data for $$R_{pPb}$$ are generated using the particle yields at p-Pb and pp collisions where number of binary collisions are taken from Glauber model calculations. We find that the average transverse flow velocity ($$<\beta _r>$$) decreases with the mass as well as when one move from the central collisions to the peripheral collisions. These findings are inline with the results of the hydrodynamics-inspired model calculations. Akhil, Aviral verfasserin aut Tiwari, Swatantra Kumar verfasserin (orcid)0000-0003-4854-8174 aut Pareek, Pooja verfasserin aut Enthalten in The European physical journal Springer Berlin Heidelberg, 2011 139(2024), 6 vom: 06. Juni (DE-627)647653958 (DE-600)2595693-0 2190-5444 nnns volume:139 year:2024 number:6 day:06 month:06 https://dx.doi.org/10.1140/epjp/s13360-024-05290-0 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 139 2024 6 06 06 |
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10.1140/epjp/s13360-024-05290-0 doi (DE-627)SPR056146175 (SPR)s13360-024-05290-0-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Singh, Aditya Kumar verfasserin aut Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, respectively at Large hadron collider (LHC) energy of $$\sqrt{s_{NN}}$$ = 5.02 TeV. We have also analysed the experimental data of transverse momentum ($$p_T$$) spectra for these identified hadrons at LHC for Pb-Pb as well as for p-Pb collisions. We have used Boltzmann transport equation (BTE) in relaxation time approximation (RTA) for this analysis. The Tsallis statistics is used as an initial distribution function and the Tsallis blast wave (TBW) model is employed as an equilibrium distribution in BTE. The present model fits the measured transverse momentum spectra, $$R_{PbPb}$$, and $$R_{pPb}$$ successfully upto $$p_T$$ = 8 GeV/c with a reasonable $$\chi ^2/ndf$$ for all the considered hadrons at various centralities. The experimental data for $$R_{pPb}$$ are generated using the particle yields at p-Pb and pp collisions where number of binary collisions are taken from Glauber model calculations. We find that the average transverse flow velocity ($$<\beta _r>$$) decreases with the mass as well as when one move from the central collisions to the peripheral collisions. These findings are inline with the results of the hydrodynamics-inspired model calculations. Akhil, Aviral verfasserin aut Tiwari, Swatantra Kumar verfasserin (orcid)0000-0003-4854-8174 aut Pareek, Pooja verfasserin aut Enthalten in The European physical journal Springer Berlin Heidelberg, 2011 139(2024), 6 vom: 06. Juni (DE-627)647653958 (DE-600)2595693-0 2190-5444 nnns volume:139 year:2024 number:6 day:06 month:06 https://dx.doi.org/10.1140/epjp/s13360-024-05290-0 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 139 2024 6 06 06 |
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10.1140/epjp/s13360-024-05290-0 doi (DE-627)SPR056146175 (SPR)s13360-024-05290-0-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Singh, Aditya Kumar verfasserin aut Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, respectively at Large hadron collider (LHC) energy of $$\sqrt{s_{NN}}$$ = 5.02 TeV. We have also analysed the experimental data of transverse momentum ($$p_T$$) spectra for these identified hadrons at LHC for Pb-Pb as well as for p-Pb collisions. We have used Boltzmann transport equation (BTE) in relaxation time approximation (RTA) for this analysis. The Tsallis statistics is used as an initial distribution function and the Tsallis blast wave (TBW) model is employed as an equilibrium distribution in BTE. The present model fits the measured transverse momentum spectra, $$R_{PbPb}$$, and $$R_{pPb}$$ successfully upto $$p_T$$ = 8 GeV/c with a reasonable $$\chi ^2/ndf$$ for all the considered hadrons at various centralities. The experimental data for $$R_{pPb}$$ are generated using the particle yields at p-Pb and pp collisions where number of binary collisions are taken from Glauber model calculations. We find that the average transverse flow velocity ($$<\beta _r>$$) decreases with the mass as well as when one move from the central collisions to the peripheral collisions. These findings are inline with the results of the hydrodynamics-inspired model calculations. Akhil, Aviral verfasserin aut Tiwari, Swatantra Kumar verfasserin (orcid)0000-0003-4854-8174 aut Pareek, Pooja verfasserin aut Enthalten in The European physical journal Springer Berlin Heidelberg, 2011 139(2024), 6 vom: 06. Juni (DE-627)647653958 (DE-600)2595693-0 2190-5444 nnns volume:139 year:2024 number:6 day:06 month:06 https://dx.doi.org/10.1140/epjp/s13360-024-05290-0 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 139 2024 6 06 06 |
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10.1140/epjp/s13360-024-05290-0 doi (DE-627)SPR056146175 (SPR)s13360-024-05290-0-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Singh, Aditya Kumar verfasserin aut Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, respectively at Large hadron collider (LHC) energy of $$\sqrt{s_{NN}}$$ = 5.02 TeV. We have also analysed the experimental data of transverse momentum ($$p_T$$) spectra for these identified hadrons at LHC for Pb-Pb as well as for p-Pb collisions. We have used Boltzmann transport equation (BTE) in relaxation time approximation (RTA) for this analysis. The Tsallis statistics is used as an initial distribution function and the Tsallis blast wave (TBW) model is employed as an equilibrium distribution in BTE. The present model fits the measured transverse momentum spectra, $$R_{PbPb}$$, and $$R_{pPb}$$ successfully upto $$p_T$$ = 8 GeV/c with a reasonable $$\chi ^2/ndf$$ for all the considered hadrons at various centralities. The experimental data for $$R_{pPb}$$ are generated using the particle yields at p-Pb and pp collisions where number of binary collisions are taken from Glauber model calculations. We find that the average transverse flow velocity ($$<\beta _r>$$) decreases with the mass as well as when one move from the central collisions to the peripheral collisions. These findings are inline with the results of the hydrodynamics-inspired model calculations. Akhil, Aviral verfasserin aut Tiwari, Swatantra Kumar verfasserin (orcid)0000-0003-4854-8174 aut Pareek, Pooja verfasserin aut Enthalten in The European physical journal Springer Berlin Heidelberg, 2011 139(2024), 6 vom: 06. Juni (DE-627)647653958 (DE-600)2595693-0 2190-5444 nnns volume:139 year:2024 number:6 day:06 month:06 https://dx.doi.org/10.1140/epjp/s13360-024-05290-0 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 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_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 139 2024 6 06 06 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000naa a22002652 4500</leader><controlfield tag="001">SPR056146175</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20240607064713.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">240607s2024 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1140/epjp/s13360-024-05290-0</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR056146175</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s13360-024-05290-0-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Singh, Aditya Kumar</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2024</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, respectively at Large hadron collider (LHC) energy of $$\sqrt{s_{NN}}$$ = 5.02 TeV. We have also analysed the experimental data of transverse momentum ($$p_T$$) spectra for these identified hadrons at LHC for Pb-Pb as well as for p-Pb collisions. We have used Boltzmann transport equation (BTE) in relaxation time approximation (RTA) for this analysis. The Tsallis statistics is used as an initial distribution function and the Tsallis blast wave (TBW) model is employed as an equilibrium distribution in BTE. The present model fits the measured transverse momentum spectra, $$R_{PbPb}$$, and $$R_{pPb}$$ successfully upto $$p_T$$ = 8 GeV/c with a reasonable $$\chi ^2/ndf$$ for all the considered hadrons at various centralities. The experimental data for $$R_{pPb}$$ are generated using the particle yields at p-Pb and pp collisions where number of binary collisions are taken from Glauber model calculations. We find that the average transverse flow velocity ($$<\beta _r>$$) decreases with the mass as well as when one move from the central collisions to the peripheral collisions. 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Singh, Aditya Kumar |
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Singh, Aditya Kumar ddc 530 bkl 33.00 Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description |
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530 VZ 33.00 bkl Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description |
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Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description |
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Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description |
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nuclear modification factor in pb-pb and p-pb collisions at $$\sqrt{s_{nn}}$$ = 5.02 tev at lhc energies using boltzmann transport equation with tsallis blast wave description |
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Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description |
| abstract |
Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, respectively at Large hadron collider (LHC) energy of $$\sqrt{s_{NN}}$$ = 5.02 TeV. We have also analysed the experimental data of transverse momentum ($$p_T$$) spectra for these identified hadrons at LHC for Pb-Pb as well as for p-Pb collisions. We have used Boltzmann transport equation (BTE) in relaxation time approximation (RTA) for this analysis. The Tsallis statistics is used as an initial distribution function and the Tsallis blast wave (TBW) model is employed as an equilibrium distribution in BTE. The present model fits the measured transverse momentum spectra, $$R_{PbPb}$$, and $$R_{pPb}$$ successfully upto $$p_T$$ = 8 GeV/c with a reasonable $$\chi ^2/ndf$$ for all the considered hadrons at various centralities. The experimental data for $$R_{pPb}$$ are generated using the particle yields at p-Pb and pp collisions where number of binary collisions are taken from Glauber model calculations. We find that the average transverse flow velocity ($$<\beta _r>$$) decreases with the mass as well as when one move from the central collisions to the peripheral collisions. These findings are inline with the results of the hydrodynamics-inspired model calculations. © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstractGer |
Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, respectively at Large hadron collider (LHC) energy of $$\sqrt{s_{NN}}$$ = 5.02 TeV. We have also analysed the experimental data of transverse momentum ($$p_T$$) spectra for these identified hadrons at LHC for Pb-Pb as well as for p-Pb collisions. We have used Boltzmann transport equation (BTE) in relaxation time approximation (RTA) for this analysis. The Tsallis statistics is used as an initial distribution function and the Tsallis blast wave (TBW) model is employed as an equilibrium distribution in BTE. The present model fits the measured transverse momentum spectra, $$R_{PbPb}$$, and $$R_{pPb}$$ successfully upto $$p_T$$ = 8 GeV/c with a reasonable $$\chi ^2/ndf$$ for all the considered hadrons at various centralities. The experimental data for $$R_{pPb}$$ are generated using the particle yields at p-Pb and pp collisions where number of binary collisions are taken from Glauber model calculations. We find that the average transverse flow velocity ($$<\beta _r>$$) decreases with the mass as well as when one move from the central collisions to the peripheral collisions. These findings are inline with the results of the hydrodynamics-inspired model calculations. © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstract_unstemmed |
Abstract In this article, we have studied the nuclear modification factor measured in the most central and peripheral Pb-Pb ($$R_{PbPb}$$) and p-Pb collisions ($$R_{pPb}$$) for $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, ($$K^{*0} + \bar{K^{*0}}$$)/2, $$\phi$$ and $$\pi ^{\pm }$$, $$K^{\pm }$$, $$p+\bar{p}$$, respectively at Large hadron collider (LHC) energy of $$\sqrt{s_{NN}}$$ = 5.02 TeV. We have also analysed the experimental data of transverse momentum ($$p_T$$) spectra for these identified hadrons at LHC for Pb-Pb as well as for p-Pb collisions. We have used Boltzmann transport equation (BTE) in relaxation time approximation (RTA) for this analysis. The Tsallis statistics is used as an initial distribution function and the Tsallis blast wave (TBW) model is employed as an equilibrium distribution in BTE. The present model fits the measured transverse momentum spectra, $$R_{PbPb}$$, and $$R_{pPb}$$ successfully upto $$p_T$$ = 8 GeV/c with a reasonable $$\chi ^2/ndf$$ for all the considered hadrons at various centralities. The experimental data for $$R_{pPb}$$ are generated using the particle yields at p-Pb and pp collisions where number of binary collisions are taken from Glauber model calculations. We find that the average transverse flow velocity ($$<\beta _r>$$) decreases with the mass as well as when one move from the central collisions to the peripheral collisions. These findings are inline with the results of the hydrodynamics-inspired model calculations. © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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| title_short |
Nuclear modification factor in Pb-Pb and p-Pb collisions at $$\sqrt{s_{NN}}$$ = 5.02 TeV at LHC energies using Boltzmann transport equation with tsallis blast wave description |
| url |
https://dx.doi.org/10.1140/epjp/s13360-024-05290-0 |
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| author2 |
Akhil, Aviral Tiwari, Swatantra Kumar Pareek, Pooja |
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10.1140/epjp/s13360-024-05290-0 |
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2024-07-03T20:31:46.340Z |
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| score |
7.398299 |