Mostra el registre parcial de l'element
dc.contributor.author | LHCb Collaboration | |
dc.contributor.author | Martínez Vidal, Fernando | |
dc.contributor.author | Oyanguren Campos, Arantza | |
dc.contributor.author | Ruiz Valls, Pablo | |
dc.date.accessioned | 2016-04-20T08:03:50Z | |
dc.date.available | 2016-04-20T08:03:50Z | |
dc.date.issued | 2014 | |
dc.identifier.citation | LHCb Collaboration Martínez Vidal, Fernando Oyanguren Campos, Arantza Ruiz Valls, Pablo 2014 Measurement of Upsilon production in collisions at root s=2.76 TeV European Physical Journal C 74 4 2835-1 2835-11 | |
dc.identifier.uri | http://hdl.handle.net/10550/52847 | |
dc.description.abstract | The production of , and mesons decaying into the dimuon final state is studied with the LHCb detector using a data sample corresponding to an integrated luminosity of collected in proton-proton collisions at a centre-of-mass energy of TeV. The differential production cross-sections times dimuon branching fractions are measured as functions of the transverse momentum and rapidity, over the ranges GeV/ and . The total cross-sections in this kinematic region, assuming unpolarised production, are measured to be sigma (pp -> Upsilon(1S)X) x B(Upsilon(1S) -> mu(+)mu(-)) = 1.111 +/- 0.043 +/- 0.044 nb, sigma (pp -> Upsilon(2S)X) x B(Upsilon(2S) -> mu(+)mu(-)) = 0.264 +/- 0.023 +/- 0.011 nb, sigma (pp -> Upsilon(3S)X) x B(Upsilon(3S) -> mu(+)mu(-))s = 0.159 +/- 0.020 +/- 0.007 nb, where the first uncertainty is statistical and the second systematic. | |
dc.language.iso | eng | |
dc.relation.ispartof | European Physical Journal C, 2014, vol. 74, num. 4, p. 2835-1-2835-11 | |
dc.subject | Física nuclear | |
dc.title | Measurement of Upsilon production in collisions at root s=2.76 TeV | |
dc.type | journal article | es_ES |
dc.date.updated | 2016-04-20T08:03:50Z | |
dc.identifier.doi | 10.1140/epjc/s10052-014-2835-1 | |
dc.identifier.idgrec | 099502 | |
dc.rights.accessRights | open access | es_ES |