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Catalogo dei prodotti della ricerca
The Y(1S), Y(2S), and Y(3S) production cross sections in proton-proton collisions at root s = 7 TeV are measured using a data sample collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 3.1 +/- 0.3 pb(-1). Integrated over the rapidity range vertical bar y vertical bar < 2, we find the product of the Y(1S) production cross section and branching fraction to dimuons to be sigma(pp -> Y(1S)X) center dot B(Y(1S) -> mu(+)mu(-)) = 7.37 +/- 0.13(-0.42)(+0.61) +/- 0.81 nb, where the first uncertainty is statistical, the second is systematic, and the third is associated with the estimation of the integrated luminosity of the data sample. This cross section is obtained assuming unpolarized Y(1S) production. With the assumption of fully transverse or fully longitudinal production polarization, the measured cross section changes by about 20%. We also report the measurement of the Y(1S), Y(2S), and Y(3S) differential cross sections as a function of transverse momentum and rapidity.
Upsilon production cross section in pp collisions at root s=7 TeV / V., K., A. M., S., A., T., W., A., T., B., M., D., J., E., C., F., M., F., R., F., V. M., G., J., H., S., H., C., H., M., H., N., H., J., H., M., J., G., K., W., K., et al.. - In: PHYSICAL REVIEW D, PARTICLES, FIELDS, GRAVITATION, AND COSMOLOGY. - ISSN 1550-7998. - 83:(2011), p. 112004. [10.1103/physrevd.83.112004]
Upsilon production cross section in pp collisions at root s=7 TeV
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H. Chang;K. H. Chen;W. T. Chen;S. Dutta;A. Go;C. M. Kuo;S. W. Li;W. Lin;M. H. Liu;Z. K. Liu;Y. J. Lu;J. H. Wu;S. S. Yu;P. Bartalini;P. Chang;Y. H. Chang;Y. W. Chang;Y. Chao;K. F. Chen;W. S. Hou;Y. Hsiung;K. Y. Kao;Y. J. Lei;R. S. Lu;J. G. Shiu;Y. M. Tzeng;M. Wang;A. Adiguzel;M. N. Bakirci;S. Cerci;C. Dozen;I. Dumanoglu;E. Eskut;S. Girgis;G. Gokbulut;Y. Guler;E. Gurpinar;I. Hos;E. E. Kangal;T. Karaman;A. K. Topaksu;A. Nart;G. Onengut;K. Ozdemir;S. Ozturk;A. Polatoz;K. Sogut;B. Tali;H. Topakli;D. Uzun;L. N. Vergili;M. Vergili;C. Zorbilmez;I. V. Akin;T. Aliev;S. Bilmis;M. Deniz;H. Gamsizkan;A. M. Guler;K. Ocalan;A. Ozpineci;M. Serin;R. Sever;U. E. Surat;E. Yildirim;M. Zeyrek;M. Deliomeroglu;D. Demir;E. Gulmez;A. Halu;B. Isildak;M. Kaya;O. Kaya;S. Ozkorucuklu;N. Sonmez;L. Levchuk;P. Bell;F. Bostock;J. J. Brooke;T. L. Cheng;E. Clement;D. Cussans;R. Frazier;J. Goldstein;M. Grimes;M. Hansen;D. Hartley;G. P. Heath;H. F. Heath;B. Huckvale;J. Jackson;L. Kreczko;S. Metson;D. M. Newbold;K. 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Milstene;A. Sakharov;M. Anderson;M. Bachtis;J. N. Bellinger;D. Carlsmith;S. Dasu;J. Efron;L. Gray;K. S. Grogg;M. Grothe;R. Hall Wilton;M. Herndon;P. Klabbers;J. Klukas;A. Lanaro;C. Lazaridis;J. Leonard;D. Lomidze;R. Loveless;A. Mohapatra;D. Reeder;I. Ross;A. Savin;W. H. Smith;J. Swanson;M. Weinberg
2011
Abstract
The Y(1S), Y(2S), and Y(3S) production cross sections in proton-proton collisions at root s = 7 TeV are measured using a data sample collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 3.1 +/- 0.3 pb(-1). Integrated over the rapidity range vertical bar y vertical bar < 2, we find the product of the Y(1S) production cross section and branching fraction to dimuons to be sigma(pp -> Y(1S)X) center dot B(Y(1S) -> mu(+)mu(-)) = 7.37 +/- 0.13(-0.42)(+0.61) +/- 0.81 nb, where the first uncertainty is statistical, the second is systematic, and the third is associated with the estimation of the integrated luminosity of the data sample. This cross section is obtained assuming unpolarized Y(1S) production. With the assumption of fully transverse or fully longitudinal production polarization, the measured cross section changes by about 20%. We also report the measurement of the Y(1S), Y(2S), and Y(3S) differential cross sections as a function of transverse momentum and rapidity.
01 Pubblicazione su rivista::01a Articolo in rivista
Upsilon production cross section in pp collisions at root s=7 TeV / V., K., A. M., S., A., T., W., A., T., B., M., D., J., E., C., F., M., F., R., F., V. M., G., J., H., S., H., C., H., M., H., N., H., J., H., M., J., G., K., W., K., et al.. - In: PHYSICAL REVIEW D, PARTICLES, FIELDS, GRAVITATION, AND COSMOLOGY. - ISSN 1550-7998. - 83:(2011), p. 112004. [10.1103/physrevd.83.112004]
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11573/385421
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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.