TY - JOUR
T1 - Measurement of the primary Lund jet plane density in proton-proton collisions at √s = 13 TeV
AU - The CMS Collaboration
AU - Hayrapetyan, A.
AU - Tumasyan, A.
AU - Adam, W.
AU - Forthomme, Laurent
AU - Kirschenmann, H.
AU - Österberg, K.
AU - Voutilainen, M.
AU - Bharthuar, Shudhashil
AU - Brücken, Erik
AU - Garcia, F.
AU - Havukainen, J.
AU - Heikkilä, Jaana
AU - Kallonen, Kimmo
AU - Kim, Minsuk
AU - Kinnunen, R.
AU - Lampén, T.
AU - Lassila-Perini, K.
AU - Laurila, S.
AU - Lehti, S.
AU - Lindén, T.
AU - Lotti, Mikko
AU - Luukka, P.
AU - Martikainen, Laura
AU - Myllymäki, Mikael Erkki Johannes
AU - Pekkanen, Juska
AU - Rantanen, Milla-Maarit
AU - Siikonen, H.
AU - Tuominen, E.
AU - Tuominiemi, J.
AU - Viinikainen, Jussi
AU - Petrow, H.
AU - Tuuva, T.
PY - 2024/5/10
Y1 - 2024/5/10
N2 - A measurement is presented of the primary Lund jet plane (LJP) density in inclusive jet production in proton-proton collisions. The analysis uses 138 fb(-1) of data collected by the CMS experiment at root s = 13TeV. The LJP, a representation of the phase space of emissions inside jets, is constructed using iterative jet declustering. The transverse momentum kT and the splitting angle Delta R of an emission relative to its emitter are measured at each step of the jet declustering process. The average density of emissions as function of ln( k(T)/GeV) and ln( R/Delta R) is measured for jets with distance parameters R = 0.4 or 0.8, transverse momentum p(T) > 700 GeV, and rapidity |y| < 1.7. The jet substructure is measured using the charged-particle tracks of the jet. The measured distributions, unfolded to the level of stable charged particles, are compared with theoretical predictions from simulations and with perturbative quantum chromodynamics calculations. Due to the ability of the LJP to factorize physical effects, these measurements can be used to improve different aspects of the physics modeling in event generators.
AB - A measurement is presented of the primary Lund jet plane (LJP) density in inclusive jet production in proton-proton collisions. The analysis uses 138 fb(-1) of data collected by the CMS experiment at root s = 13TeV. The LJP, a representation of the phase space of emissions inside jets, is constructed using iterative jet declustering. The transverse momentum kT and the splitting angle Delta R of an emission relative to its emitter are measured at each step of the jet declustering process. The average density of emissions as function of ln( k(T)/GeV) and ln( R/Delta R) is measured for jets with distance parameters R = 0.4 or 0.8, transverse momentum p(T) > 700 GeV, and rapidity |y| < 1.7. The jet substructure is measured using the charged-particle tracks of the jet. The measured distributions, unfolded to the level of stable charged particles, are compared with theoretical predictions from simulations and with perturbative quantum chromodynamics calculations. Due to the ability of the LJP to factorize physical effects, these measurements can be used to improve different aspects of the physics modeling in event generators.
KW - 114 Physical sciences
U2 - 10.1007/JHEP05(2024)116
DO - 10.1007/JHEP05(2024)116
M3 - Article
SN - 1029-8479
VL - 2024
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 5
M1 - 116
ER -