TY - JOUR
T1 - Measurement of inclusive jet and dijet cross-sections in proton-proton collisions at \sqrt{s}=13 TeV 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 - Lack, David
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 - Price, Darren
AU - Qin, Yang
AU - Raine, John
AU - Rawling, Jacob
AU - Roberts, Rhys
AU - Schweiger, H.
AU - Shaw, Savanna
AU - Tomlinson, Lee
AU - Wilk, Fabian
AU - Wyatt, Terence
PY - 2018/5/30
Y1 - 2018/5/30
N2 - Inclusive jet and dijet cross-sections are measured in proton-proton collisions at a centre-of-mass energy of 13 TeV. The measurement uses a dataset with an integrated luminosity of 3.2 fb−1 recorded in 2015 with the ATLAS detector at the Large Hadron Collider. Jets are identified using the anti-kt algorithm with a radius parameter value of R = 0.4. The inclusive jet cross-sections are measured double-differentially as a function of the jet transverse momentum, covering the range from 100 GeV to 3.5 TeV, and the absolute jet rapidity up to |y| = 3. The double-differential dijet production cross-sections are presented as a function of the dijet mass, covering the range from 300 GeV to 9 TeV, and the half absolute rapidity separation between the two leading jets within |y| < 3, y∗, up to y∗ = 3. Next-to-leading-order, and next-to-next-to-leading-order for the inclusive jet measurement, perturbative QCD calculations corrected for non-perturbative and electroweak effects are compared to the measured cross-sections.
AB - Inclusive jet and dijet cross-sections are measured in proton-proton collisions at a centre-of-mass energy of 13 TeV. The measurement uses a dataset with an integrated luminosity of 3.2 fb−1 recorded in 2015 with the ATLAS detector at the Large Hadron Collider. Jets are identified using the anti-kt algorithm with a radius parameter value of R = 0.4. The inclusive jet cross-sections are measured double-differentially as a function of the jet transverse momentum, covering the range from 100 GeV to 3.5 TeV, and the absolute jet rapidity up to |y| = 3. The double-differential dijet production cross-sections are presented as a function of the dijet mass, covering the range from 300 GeV to 9 TeV, and the half absolute rapidity separation between the two leading jets within |y| < 3, y∗, up to y∗ = 3. Next-to-leading-order, and next-to-next-to-leading-order for the inclusive jet measurement, perturbative QCD calculations corrected for non-perturbative and electroweak effects are compared to the measured cross-sections.
U2 - 10.1007/JHEP05(2018)195
DO - 10.1007/JHEP05(2018)195
M3 - Article
SN - 1126-6708
JO - The Journal of High Energy Physics
JF - The Journal of High Energy Physics
ER -