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   <dc:title>Measurement of the exclusive Υ production cross-section in pp collisions at √{s}=7 TeV and 8 TeV</dc:title>
   <dc:creator>Badalov, Alexey</dc:creator>
   <dc:creator>Casanova Mohr, Raimon</dc:creator>
   <dc:creator>Garrido Beltrán, Lluís</dc:creator>
   <dc:creator>Gascón Fora, David</dc:creator>
   <dc:creator>Graciani Díaz, Ricardo</dc:creator>
   <dc:creator>Graugés Pous, Eugeni</dc:creator>
   <dc:creator>Mann Benito, Carla</dc:creator>
   <dc:creator>Picatoste Olloqui, Eduardo</dc:creator>
   <dc:creator>Rives Molina, Vicente José</dc:creator>
   <dc:creator>Ruiz, Hugo (Ruiz Pérez)</dc:creator>
   <dc:creator>LHCb collaboration</dc:creator>
   <dc:subject>Hadrons</dc:subject>
   <dc:subject>Gran Col·lisionador d'Hadrons</dc:subject>
   <dc:subject>Física de partícules</dc:subject>
   <dc:subject>Experiments</dc:subject>
   <dc:subject>Hadrons</dc:subject>
   <dc:subject>Large Hadron Collider (France and Switzerland)</dc:subject>
   <dc:subject>Particle physics</dc:subject>
   <dc:subject>Experiments</dc:subject>
   <dcterms:abstract>A study is presented of central exclusive production of Υ(nS) states, where the Υ(nS) resonances decay to the µ +µ − final state, using pp collision data recorded by the LHCb experiment. The cross-section is measured in the rapidity range 2 &lt; y(Υ) &lt; 4.5 where the muons are reconstructed in the pseudorapidity range 2 &lt; η(µ ±) &lt; 4.5. The data sample corresponds to an integrated luminosity of 2.9 fb−1 and was collected at centre-of-mass energies of 7 TeV and 8 TeV. The measured Υ(1S) and Υ(2S) production cross-sections are σ(pp → pΥ(1S)p) = 9.0 ± 2.1 ± 1.7 pb and σ(pp → pΥ(2S)p) = 1.3 ± 0.8 ± 0.3 pb, where the first uncertainties are statistical and the second are systematic. The Υ(1S) cross-section is also measured as a function of rapidity and is found to be in good agreement with Standard Model predictions. An upper limit is set at 3.4 pb at the 95% confidence level for the exclusive Υ(3S) production cross-section, including possible contamination from χb(3P) → Υ(3S)γ decays.</dcterms:abstract>
   <dcterms:issued>2022-05-19T14:10:39Z</dcterms:issued>
   <dcterms:issued>2022-05-19T14:10:39Z</dcterms:issued>
   <dcterms:issued>2015-09-14</dcterms:issued>
   <dcterms:issued>2022-05-19T14:10:39Z</dcterms:issued>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:relation>Reproducció del document publicat a: https://doi.org/10.1007/JHEP09(2015)084</dc:relation>
   <dc:relation>Journal of High Energy Physics, 2015, vol. 2015, num. 84, p. 1-21</dc:relation>
   <dc:relation>https://doi.org/10.1007/JHEP09(2015)084</dc:relation>
   <dc:rights>cc-by (c) Badalov, A. et al., 2015</dc:rights>
   <dc:rights>https://creativecommons.org/licenses/by/4.0/</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:publisher>Springer Verlag</dc:publisher>
   <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
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