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000620274 0247_ $$2arXiv$$aarXiv:2406.01430
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000620274 245__ $$aThe azimuthal correlation between the leading jet and the scattered lepton in deep inelastic scattering at HERA
000620274 260__ $$aHeidelberg$$bSpringer$$c2024
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000620274 520__ $$aThe azimuthal correlation angle, $\Delta \phi $, between the scattered lepton and the leading jet in deep inelastic $e^{\pm }p$ scattering at HERA has been studied using data collected with the ZEUS detector at a centre-of-mass energy of $\sqrt{s} = 318 {\,\text {Ge}\hspace{-0.66666pt}\text {V}}$, corresponding to an integrated luminosity of $326 \,\text {pb}^{-1}$. A measurement of jet cross sections in the laboratory frame was made in a fiducial region corresponding to photon virtuality $10 {\,\text {Ge}\hspace{-0.66666pt}\text {V}}^2< Q^2 < 350 {\,\text {Ge}\hspace{-0.66666pt}\text {V}}^2$, inelasticity $0.04< y < 0.7$, outgoing lepton energy $E_e > 10 {\,\text {Ge}\hspace{-0.66666pt}\text {V}}$, lepton polar angle $140^\circ< \theta _e < 180^\circ $, jet transverse momentum $2.5 {\,\text {Ge}\hspace{-0.66666pt}\text {V}}< p_\textrm{T,jet} < 30 {\,\text {Ge}\hspace{-0.66666pt}\text {V}}$, and jet pseudorapidity $-1.5< \eta _\textrm{jet} < 1.8$. Jets were reconstructed using the $k_\textrm{T}$ algorithm with the radius parameter $R = 1$. The leading jet in an event is defined as the jet that carries the highest $p_\textrm{T,jet}$. Differential cross sections, $d\sigma /d\Delta \phi $, were measured as a function of the azimuthal correlation angle in various ranges of leading-jet transverse momentum, photon virtuality and jet multiplicity. Perturbative calculations at $\mathcal {O}(\alpha _{s}^2)$ accuracy successfully describe the data within the fiducial region, although a lower level of agreement is observed near $\Delta \phi \rightarrow \pi $ for events with high jet multiplicity, due to limitations of the perturbative approach in describing soft phenomena in QCD. The data are equally well described by Monte Carlo predictions that supplement leading-order matrix elements with parton showering.
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000620274 650_7 $$2INSPIRE$$apositron p: deep inelastic scattering
000620274 650_7 $$2INSPIRE$$ajet: transverse momentum
000620274 650_7 $$2INSPIRE$$ajet: multiplicity
000620274 650_7 $$2INSPIRE$$alepton: energy
000620274 650_7 $$2INSPIRE$$ajet: multiplicity: high
000620274 650_7 $$2INSPIRE$$aperturbation theory: higher-order
000620274 650_7 $$2INSPIRE$$ahigher-order: 0
000620274 650_7 $$2INSPIRE$$ajet: rapidity
000620274 650_7 $$2INSPIRE$$aangular correlation
000620274 650_7 $$2INSPIRE$$aelectron p: deep inelastic scattering
000620274 650_7 $$2INSPIRE$$aphoton
000620274 650_7 $$2INSPIRE$$aDESY HERA Stor
000620274 650_7 $$2INSPIRE$$anumerical calculations: Monte Carlo
000620274 650_7 $$2INSPIRE$$aquantum chromodynamics: perturbation theory
000620274 650_7 $$2INSPIRE$$aZEUS
000620274 650_7 $$2INSPIRE$$aparton
000620274 650_7 $$2INSPIRE$$adifferential cross section: measured
000620274 650_7 $$2INSPIRE$$aangular dependence
000620274 650_7 $$2INSPIRE$$atransverse momentum dependence
000620274 650_7 $$2INSPIRE$$amultiplicity: dependence
000620274 650_7 $$2INSPIRE$$aexperimental results
000620274 650_7 $$2INSPIRE$$a318 GeV-cms
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