TY - JOUR
T1 - Measurement of the cross-section for electroweak production of dijets in association with a Z boson in pp collisions at s=13TeV with the ATLAS detector
AU - ATLAS Collaboration
AU - Bethani, Agni
AU - Bielski, Rafal
AU - Connelly, Ian
AU - Cox, Brian
AU - Da Via, Cinzia
AU - Dann, Nicholas
AU - Forcolin, Giulio
AU - Forti, Alessandra
AU - Howarth, James
AU - Loebinger, Frederick
AU - Marsden, Stephen
AU - Masik, Jiri
AU - Menary, Stephen
AU - Munoz Sanchez, Francisca
AU - Oh, Alexander
AU - Pater, Joleen
AU - Peters, Yvonne
AU - Pilkington, Andrew
AU - Pin, Arnaud
AU - Price, Darren
AU - Qin, Yang
AU - Raine, John
AU - Rawling, Jacob
AU - Roberts, Rhys
AU - H, Schweiger
AU - Shaw, Savanna
AU - Tomlinson, Lee
AU - Watts, Stephen
AU - Wilk, Fabian
AU - Wyatt, Terence
AU - Lack, David
PY - 2017
Y1 - 2017
N2 - The cross-section for the production of two jets in association with a leptonically decaying Z boson (Zjj ) is measured in proton–proton collisions at a centre-of-mass energy of 13 TeV, using data recorded with the ATLAS detector at the Large Hadron Collider, corresponding to an integrated luminosity of 3.2 fb−1. The electroweak Zjj cross-section is extracted in a fiducial region chosen to enhance the electroweak contribution relative to the dominant Drell–Yan Zjj process, which is constrained using a data-driven approach. The measured fiducial electroweak cross-section is σEWZjj = 119±16(stat.)±20(syst.)±2(lumi.) fb for dijet invariant mass greater than 250 GeV, and 34.2±5.8(stat.)±5.5(syst.)±0.7(lumi.) fb for dijet invariant mass greater than 1 TeV. Standard Model predictions are in agreement with the measurements. The inclusive Zjj cross-section is also measured in six different fiducial regions with varying contributions from electroweak and Drell–Yan Zjj production.
AB - The cross-section for the production of two jets in association with a leptonically decaying Z boson (Zjj ) is measured in proton–proton collisions at a centre-of-mass energy of 13 TeV, using data recorded with the ATLAS detector at the Large Hadron Collider, corresponding to an integrated luminosity of 3.2 fb−1. The electroweak Zjj cross-section is extracted in a fiducial region chosen to enhance the electroweak contribution relative to the dominant Drell–Yan Zjj process, which is constrained using a data-driven approach. The measured fiducial electroweak cross-section is σEWZjj = 119±16(stat.)±20(syst.)±2(lumi.) fb for dijet invariant mass greater than 250 GeV, and 34.2±5.8(stat.)±5.5(syst.)±0.7(lumi.) fb for dijet invariant mass greater than 1 TeV. Standard Model predictions are in agreement with the measurements. The inclusive Zjj cross-section is also measured in six different fiducial regions with varying contributions from electroweak and Drell–Yan Zjj production.
U2 - 10.1016/j.physletb.2017.10.040
DO - 10.1016/j.physletb.2017.10.040
M3 - Article
SN - 0370-2693
JO - Physics Letters. Section B: Nuclear, Elementary Particle and High-Energy Physics
JF - Physics Letters. Section B: Nuclear, Elementary Particle and High-Energy Physics
ER -