The Parameters of The Tsallis Distribution at the LHC
This talk focuses on fits, using the Tsallis distribution, extending to very large values of the transverse momentum of charged particles in p-p collisions and on the energy dependence of the parameters. A thermodynamically consistent form of the distribution is used for fitting the transverse momen...
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Published in: | EPJ Web of conferences Vol. 137; p. 11004 |
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Abstract | This talk focuses on fits, using the Tsallis distribution, extending to very large values of the transverse momentum of charged particles in p-p collisions and on the energy dependence of the parameters. A thermodynamically consistent form of the distribution is used for fitting the transverse momentum spectra at mid-rapidity. The fits based on the proposed distribution provide a very good description over 14 orders of magnitude. The parameters obtained show a smooth increase in the value of q and a corresponding smooth decrease in the value of T with increasing beam energy. |
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AbstractList | This talk focuses on fits, using the Tsallis distribution, extending to very large values of the transverse momentum of charged particles in p-p collisions and on the energy dependence of the parameters. A thermodynamically consistent form of the distribution is used for fitting the transverse momentum spectra at mid-rapidity. The fits based on the proposed distribution provide a very good description over 14 orders of magnitude. The parameters obtained show a smooth increase in the value of q and a corresponding smooth decrease in the value of T with increasing beam energy. |
Author | Cleymans, J. Azmi, M.D. Teryaev, O.V. Parvan, A.S. |
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CitedBy_id | crossref_primary_10_1140_epja_i2018_12601_8 crossref_primary_10_1103_PhysRevD_109_052008 crossref_primary_10_1088_1361_6471_ab8dcb crossref_primary_10_1007_s41365_023_01307_y crossref_primary_10_1142_S0218301317500719 crossref_primary_10_1142_S0218301319500204 crossref_primary_10_1134_S0021364021090010 crossref_primary_10_1109_ACCESS_2019_2933172 crossref_primary_10_3390_physics4020041 crossref_primary_10_1140_epja_s10050_020_00156_2 crossref_primary_10_3390_particles5020013 crossref_primary_10_1088_1361_6471_ac1393 |
Cites_doi | 10.1007/s12648-015-0747-z 10.1103/PhysRevC.83.064903 10.1007/JHEP03(2015)098 10.1140/epjc/s10052-014-2785-7 10.1007/JHEP08(2011)086 10.1103/PhysRevD.92.074009 10.3390/e17010384 10.1140/epjc/s10052-012-2164-1 10.1103/PhysRevC.79.034909 10.1140/epjc/s10052-014-2794-6 10.1007/BF01016429 10.1103/PhysRevD.87.114007 10.1007/JHEP02(2010)041 10.1140/epjc/s10052-011-1655-9 10.1155/2016/9632126 10.1088/0954-3899/39/2/025006 10.1016/j.physletb.2013.05.029 10.1103/PhysRevD.91.114027 10.1140/epjc/s10052-015-3629-9 10.1140/epja/i2012-12160-0 10.5506/APhysPolB.43.2047 10.1088/1367-2630/13/5/053033 10.1088/0954-3899/41/6/065001 10.1103/PhysRevD.91.054025 |
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