par Khachatryan, Vardan;Barria, Patrizia 
;Caillol, Cécile ;Clerbaux, Barbara ;De Lentdecker, Gilles ;Delannoy, Hugo ;Fasanella, Giuseppe ;Favart, Laurent ;Gay, Arnaud ;Grebenyuk, Anastasia ;Karapostoli, Georgia ;Lenzi, Thomas ;Maerschalk, Thierry ;Marinov, Audrey ;Randle-Conde, Aidan Sean ;Reis, Thomas ;Seva, Tomislav ;Vander Velde, Catherine ;Vanlaer, Pascal ;Yonamine, Ryo ;Zenoni, Florian ;Leonard, Alexandre ;Pernie, Luca ;Zhang, Fengwangdong
Référence Journal of High Energy Physics, 2016, 8, 139
Publication Publié, 2016
;Caillol, Cécile ;Clerbaux, Barbara ;De Lentdecker, Gilles ;Delannoy, Hugo ;Fasanella, Giuseppe ;Favart, Laurent ;Gay, Arnaud ;Grebenyuk, Anastasia ;Karapostoli, Georgia ;Lenzi, Thomas ;Maerschalk, Thierry ;Marinov, Audrey ;Randle-Conde, Aidan Sean ;Reis, Thomas ;Seva, Tomislav ;Vander Velde, Catherine ;Vanlaer, Pascal ;Yonamine, Ryo ;Zenoni, Florian ;Leonard, Alexandre ;Pernie, Luca ;Zhang, Fengwangdong Référence Journal of High Energy Physics, 2016, 8, 139
Publication Publié, 2016
Article révisé par les pairs
| Résumé : | The decorrelation in the azimuthal angle between the most forward and the most backward jets (Mueller-Navelet jets) is measured in data collected in pp collisions with the CMS detector at the LHC at s=7 TeV. The measurement is presented in the form of distributions of azimuthal-angle differences, Δϕ, between the Mueller-Navelet jets, the average cosines of (π − Δϕ), 2(π − Δϕ), and 3(π − Δϕ), and ratios of these cosines. The jets are required to have transverse momenta, pT, in excess of 35 GeV and rapidities, |
