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The inelastic hadronic cross section in proton–lead collisions at a centre-of-mass energy per nucleon pair of 5.02 TeV is measured with the CMS detector at the LHC. The data sample, corresponding to an integrated luminosity of L=12.6±0.4nb−1, has been collected with an unbiased trigger for inclusive particle production. The cross section is obtained from the measured number of proton–lead collisions with hadronic activity produced in the pseudorapidity ranges 3<5 and/or −5<−3, corrected for photon-induced contributions, experimental acceptance, and other instrumental effects. The inelastic cross section is measured to be σinel(pPb)=2061 ± 3(stat) ±34(syst) ±72(lumi) mb. Various Monte Carlo generators, commonly used in heavy ion and cosmic ray physics, are found to reproduce the data within uncertainties. The value of σinel(pPb) is compatible with that expected from the proton–proton cross section at 5.02 TeV scaled up within a simple Glauber approach to account for multiple scatterings in the lead nucleus, indicating that further net nuclear corrections are small.
(2016). Measurement of the inelastic cross section in proton–lead collisions at √sNN=5.02TeV [journal article - articolo]. In PHYSICS LETTERS. SECTION B. Retrieved from http://hdl.handle.net/10446/140666
Measurement of the inelastic cross section in proton–lead collisions at √sNN=5.02TeV
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Camporesi;G. Cerminara;S. Colafranceschi;M. D'Alfonso;D. d'Enterria;A. Dabrowski;V. Daponte;A. David;M. De Gruttola;F. De Guio;A. De Roeck;S. De Visscher;E. Di Marco;M. Dobson;M. Dordevic;T. du Pree;N. Dupont;A. Elliott-Peisert;G. Franzoni;W. Funk;D. Gigi;K. Gill;D. Giordano;M. Girone;F. Glege;R. Guida;S. Gundacker;M. Guthoff;J. Hammer;M. Hansen;P. Harris;J. Hegeman;V. Innocente;P. Janot;H. Kirschenmann;M. J. Kortelainen;K. Kousouris;K. Krajczar;P. Lecoq;C. Lourenço;M. T. Lucchini;N. Magini;L. Malgeri;M. Mannelli;A. Martelli;L. Masetti;F. Meijers;S. Mersi;E. Meschi;F. Moortgat;S. Morovic;M. Mulders;M. V. Nemallapudi;H. Neugebauer;S. Orfanelli;L. Orsini;L. Pape;E. Perez;A. Petrilli;G. Petrucciani;A. Pfeiffer;D. Piparo;A. Racz;G. Rolandi;M. Rovere;M. Ruan;H. Sakulin;C. Schäfer;C. Schwick;A. Sharma;P. Silva;M. Simon;P. Sphicas;D. Spiga;J. Steggemann;B. Stieger;M. Stoye;Y. Takahashi;D. Treille;A. Triossi;A. Tsirou;G. I. Veres;N. Wardle;H. K. Wöhri;A. Zagozdzinska;W. D. Zeuner;W. Bertl;K. 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2016-01-01
Abstract
The inelastic hadronic cross section in proton–lead collisions at a centre-of-mass energy per nucleon pair of 5.02 TeV is measured with the CMS detector at the LHC. The data sample, corresponding to an integrated luminosity of L=12.6±0.4nb−1, has been collected with an unbiased trigger for inclusive particle production. The cross section is obtained from the measured number of proton–lead collisions with hadronic activity produced in the pseudorapidity ranges 3<5 and/or −5<−3, corrected for photon-induced contributions, experimental acceptance, and other instrumental effects. The inelastic cross section is measured to be σinel(pPb)=2061 ± 3(stat) ±34(syst) ±72(lumi) mb. Various Monte Carlo generators, commonly used in heavy ion and cosmic ray physics, are found to reproduce the data within uncertainties. The value of σinel(pPb) is compatible with that expected from the proton–proton cross section at 5.02 TeV scaled up within a simple Glauber approach to account for multiple scatterings in the lead nucleus, indicating that further net nuclear corrections are small.
Khachatryan, V.; Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Asilar, E.; Bergauer, T.; Brandstetter, J.; Brondolin, E.; Dragicevic, M.; Erö, J.; Flechl, ...espandi
(2016). Measurement of the inelastic cross section in proton–lead collisions at √sNN=5.02TeV [journal article - articolo]. In PHYSICS LETTERS. SECTION B. Retrieved from http://hdl.handle.net/10446/140666
Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/10446/140666
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simulazione ASN
Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande.
La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.