Measurement of forward W → eν production in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV

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Fontanelli, F.; Forshaw, D.; Forty, R.; Franco Lima, V.; Frank, M.; Frei, C.; Fu, J.; Furfaro, E.; Färber, C.; Gallas Torreira, A.; Galli, D.; Gallorini, S.; Gambetta, S.; Gandelman, M.; Gandini, P.; Gao, Y.; Garcia Martin, L.; García Pardiñas, J.; Garra Tico, J.; Garrido, L.; Garsed, P.; Gascon, D.; Gaspar, C.; Gavardi, L.; Gazzoni, G.; Gerick, D.; Gersabeck, E.; Gersabeck, M.; Gershon, T.; Ghez, Ph.; Gianì, S.; Gibson, V.; Girard, O.; Giubega, L.; Gizdov, K.; Gligorov, V.; Golubkov, D.; Golutvin, A.; Gomes, A.; Gorelov, I.; Gotti, C.; Grabalosa Gándara, M.; Graciani Diaz, R.; Granado Cardoso, L.; Graugés, E.; Graverini, E.; Graziani, G.; Grecu, A.; Griffith, P.; Grillo, L.; Gruberg Cazon, B.; Grünberg, O.; Gushchin, E.; Guz, Yu.; Gys, T.; Göbel, C.; Hadavizadeh, T.; Hadjivasiliou, C.; Haefeli, G.; Haen, C.; Haines, S.; Hall, S.; Hamilton, B.; Han, X.; Hansmann-Menzemer, S.; Harnew, N.; Harnew, S.; Harrison, J.; Hatch, M.; He, J.; Head, T.; Heister, A.; Hennessy, K.; Henrard, P.; Henry, L.; 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Wyllie, K.; Xie, Y.; Xing, Z.; Xu, Z.; Yang, Z.; Yin, H.; Yu, J.; Yuan, X.; Yushchenko, O.; Zangoli, M.; Zarebski, K.; Zavertyaev, M.; Zhang, L.; Zhang, Y.; Zhang, Y.; Zhelezov, A.; Zheng, Y.; Zhokhov, A.; Zhu, X.; Zhukov, V.; Zucchelli, S.
doi:10.1007/JHEP10(2016)030
Measurement of forward W → eν production in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV

R. Aaij (European Organization for Nuclear Research (CERN), Geneva, Switzerland) ; B. Adeva (Universidad de Santiago de Compostela, Santiago de Compostela, Spain) ; M. Adinolfi (H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom) ; Z. Ajaltouni (Clermont Université, Université Blaise Pascal, CNRS/IN2P3, LPC, Clermont-Ferrand, France) ; S. Akar (CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille, France) ; et al. - Show all 767 authors
A measurement of the cross-section for W → eν production in pp collisions is presented using data corresponding to an integrated luminosity of 2 fb −1 collected by the LHCb experiment at a centre-of-mass energy of s = 8 $$ \sqrt{s}=8 $$ TeV. The electrons are required to have more than 20 GeV of transverse momentum and to lie between 2 . 00 and 4 . 25 in pseudorapidity. The inclusive W production cross-sections, where the W decays to eν , are measured to be σ W + → e + ν e = 1124.4 ± 2.1 ± 21.5 ± 11.2 ± 13.0 p b , $$ {\sigma}_{W^{+}\to {e}^{+}{\nu}_e}=1124.4\pm 2.1\pm 21.5\pm 11.2\pm 13.0\kern0.5em \mathrm{p}\mathrm{b}, $$ σ W − → e − ν ¯ e = 809.0 ± 1.9 ± 18.1 ± 7.0 ± 9.4 p b , $$ {\sigma}_{W^{-}\to {e}^{-}{\overline{\nu}}_e}=809.0\pm 1.9\pm 18.1\pm \kern0.5em 7.0\pm \kern0.5em 9.4\;\mathrm{p}\mathrm{b}, $$ where the first uncertainties are statistical, the second are systematic, the third are due to the knowledge of the LHC beam energy and the fourth are due to the luminosity determination.
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  "titles": [
    {
      "source": "Springer/SISSA", 
      "title": "Measurement of forward W \u2192 e\u03bd production in pp collisions at s = 8 $$ \\sqrt{s}=8 $$ TeV"
    }
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  "copyright": [
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  "abstracts": [
    {
      "source": "Springer/SISSA", 
      "value": "A measurement of the cross-section for W \u2192 e\u03bd production in pp collisions is presented using data corresponding to an integrated luminosity of 2 fb \u22121 collected by the LHCb experiment at a centre-of-mass energy of s = 8 $$ \\sqrt{s}=8 $$ TeV. The electrons are required to have more than 20 GeV of transverse momentum and to lie between 2 . 00 and 4 . 25 in pseudorapidity. The inclusive W production cross-sections, where the W decays to e\u03bd , are measured to be \u03c3 W + \u2192 e + \u03bd e = 1124.4 \u00b1 2.1 \u00b1 21.5 \u00b1 11.2 \u00b1 13.0 p b , $$ {\\sigma}_{W^{+}\\to {e}^{+}{\\nu}_e}=1124.4\\pm 2.1\\pm 21.5\\pm 11.2\\pm 13.0\\kern0.5em \\mathrm{p}\\mathrm{b}, $$ \u03c3 W \u2212 \u2192 e \u2212 \u03bd \u00af e = 809.0 \u00b1 1.9 \u00b1 18.1 \u00b1 7.0 \u00b1 9.4 p b , $$ {\\sigma}_{W^{-}\\to {e}^{-}{\\overline{\\nu}}_e}=809.0\\pm 1.9\\pm 18.1\\pm \\kern0.5em 7.0\\pm \\kern0.5em 9.4\\;\\mathrm{p}\\mathrm{b}, $$ where the first uncertainties are statistical, the second are systematic, the third are due to the knowledge of the LHC beam energy and the fourth are due to the luminosity determination."
    }
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      "date": "2016-10-07", 
      "publisher": "Springer/SISSA"
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}
Published on:: 07 October 2016
Publisher:: Springer/SISSA
Published in:: Journal of High Energy Physics (2016)
DOI:: https://doi.org/10.1007/JHEP10(2016)030
arXiv:: 1608.01484
Copyrights:: The Author(s)
Licence:: CC-BY-4.0
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