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Aaij, R, Adeva, B, Adinolfi, M, Ajaltouni, Z, Akar, S, Albrecht, J, Alessio, F, Alexander, M, Alfonso Albero, A, Ali, S et al (show 774 more authors) , Alkhazov, G, Cartelle, P Alvarez, Alves, AA Jr, Amato, S, Amerio, S, Amhis, Y, An, L, Anderlini, L, Andreassi, G, Andreotti, M, Andrews, JE, Appleby, RB, Archilli, F, d'Argent, P, Romeu, J Arnau, Artamonov, A, Artuso, M, Aslanides, E, Atzeni, M, Auriemma, G, Bachmann, S, Back, JJ, Baesso, C, Baker, S, Balagura, V, Baldini, W, Baranov, A, Barlow, RJ, Barsuk, S, Barter, W, Baryshnikov, F, Batozskaya, V, Battista, V, Bay, A, Beddow, J, Bedeschi, F, Bediaga, I, Beiter, A, Bel, LJ, Beliy, N, Bellee, V, Belloli, N, Belous, K, Belyaev, I, Ben-Haim, E, Bencivenni, G, Benson, S, Beranek, S, Berezhnoy, A, Bernet, R, Berninghoff, D, Bertholet, E, Bertolin, A, Betancourt, C, Betti, F, Bettler, MO, van Beuzekom, M, Bezshyiko, Ia, Bifani, S, Billoir, P, Birnkraut, A, Bizzeti, A, Bjorn, M, Blake, T, Blanc, F, Blusk, S, Bocci, V, Boettcher, T, Bondar, 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(2018)
Measurement of Υ production in pp collisions at √s=13 TeV.
JOURNAL OF HIGH ENERGY PHYSICS, 2018 (7).
2025-.
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Abstract
<jats:title>A<jats:sc>bstract</jats:sc></jats:title><jats:p>The production cross-sections of<jats:italic>ϒ</jats:italic>(1<jats:italic>S</jats:italic>),<jats:italic>ϒ</jats:italic>(2<jats:italic>S</jats:italic>) and<jats:italic>ϒ</jats:italic>(3<jats:italic>S</jats:italic>) mesons in proton-proton collisions at<jats:inline-formula><jats:alternatives><jats:tex-math>$$ \sqrt{s}=13 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo>=</mml:mo><mml:mn>13</mml:mn></mml:math></jats:alternatives></jats:inline-formula>TeV are measured with a data sample corresponding to an integrated luminosity of 277 ± 11 pb<jats:sup>−1</jats:sup>recorded by the LHCb experiment in 2015. The<jats:italic>ϒ</jats:italic>mesons are reconstructed in the decay mode<jats:italic>ϒ</jats:italic>→<jats:italic>μ</jats:italic><jats:sup>+</jats:sup><jats:italic>μ</jats:italic><jats:sup>−</jats:sup>. The differential production cross-sections times the dimuon branching fractions are measured as a function of the<jats:italic>ϒ</jats:italic>transverse momentum,<jats:italic>p</jats:italic><jats:sub>T</jats:sub>, and rapidity,<jats:italic>y</jats:italic>, over the range 0<jats:italic>< p</jats:italic><jats:sub>T</jats:sub><jats:italic><</jats:italic>30 GeV<jats:italic>/c</jats:italic>and 2<jats:italic>.</jats:italic>0<jats:italic>< y <</jats:italic>4<jats:italic>.</jats:italic>5. The ratios of the cross-sections with respect to the LHCb measurement at<jats:inline-formula><jats:alternatives><jats:tex-math>$$ \sqrt{s}=8 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo>=</mml:mo><mml:mn>8</mml:mn></mml:math></jats:alternatives></jats:inline-formula>TeV are also determined. The measurements are compared with theoretical predictions based on NRQCD.</jats:p>