Measurements of jet multiplicity and jet transverse momentum in multijet events in proton–proton collisions at √s = 13 TeV
Abstract Multijet events at large transverse momentum ( $$p_{\textrm{T}}$$ p T...
| Main Authors: | , , , , , , , , , , , , , , , , , , , |
|---|---|
| Other Authors: | |
| Format: | Article |
| Language: | English |
| Published: |
Springer Berlin Heidelberg
2023
|
| Online Access: | https://hdl.handle.net/1721.1/152209 |
| Summary: | Abstract
Multijet events at large transverse momentum (
$$p_{\textrm{T}}$$
p
T
) are measured at
$$\sqrt{s}=13\,\text {TeV} $$
s
=
13
TeV
using data recorded with the CMS detector at the LHC, corresponding to an integrated luminosity of
$$36.3{\,\text {fb}^{-1}} $$
36.3
fb
-
1
. The multiplicity of jets with
$$p_{\textrm{T}} >50\,\text {GeV} $$
p
T
>
50
GeV
that are produced in association with a high-
$$p_{\textrm{T}}$$
p
T
dijet system is measured in various ranges of the
$$p_{\textrm{T}}$$
p
T
of the jet with the highest transverse momentum and as a function of the azimuthal angle difference
$$\varDelta \phi _{1,2}$$
Δ
ϕ
1
,
2
between the two highest
$$p_{\textrm{T}}$$
p
T
jets in the dijet system. The differential production cross sections are measured as a function of the transverse momenta of the four highest
$$p_{\textrm{T}}$$
p
T
jets. The measurements are compared with leading and next-to-leading order matrix element calculations supplemented with simulations of parton shower, hadronization, and multiparton interactions. In addition, the measurements are compared with next-to-leading order matrix element calculations combined with transverse-momentum dependent parton densities and transverse-momentum dependent parton shower. |
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