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Aaij, R.; Beteta, C. Abellán; Adeva, B.; Adinolfi, M.; Aidala, C.; Ajaltouni, Z.; Akar, S.; Albicocco, P.; Albrecht, J.; Alessio, F.; Alexander, M.; Albero, A. Alfonso; Alkhazov, G.; Cartelle, P. Alvarez; Alves, A. A.; Amato, S.; Amhis, Y.; An, L.; Anderlini, L.; Andreassi, G.; Andreotti, M.; Andrews, J. E.; Archilli, F.; Romeu, J. Arnau; Артамонов, А.; Artuso, M.; Arzymatov, K.; Aslanides, E.; Atzeni, M.; Audurier, B.; Bachmann, S.; Back, J. J.; Baker, S.; Balagura, V.; Baldini, W.; Baranov, A.; Barlow, R. J.; Barsuk, S.; Barter, W.; Bartolini, M.; Baryshnikov, F.; Batozskaya, V.; Batsukh, B.; Battig, A.; Battista, V.; Bay, A.; Bedeschi, F.; Bediaga, I.; Beiter, A.; Bel, L. J.; Belin, S.; Beliy, N.; Bellée, V.; Belloli, N.; Belous, K.; Belyaev, I.; Bencivenni, G.; Ben-Haim, E.; Benson, S.; Beranek, S.; Berezhnoy, A.; Bernet, R.; Berninghoff, D.; Bertholet, E.; Bertolin, A.; Betancourt, C.; Betti, F.; Bettler, M. O.; Bezshyiko, Ia.; Bhasin, S.; Bhom, J.; Bieker, M. 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doi:10.1103/physrevlett.123.232001

Cited by 18 publications

(10 citation statements)

References 50 publications

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“…Though jets with larger momenta are more collimated, the net effect is an increase of j T as p T, jet increases. These measurements are consistent with the findings by the ATLAS [19] and LHCb collaborations [20]. 2) handle both the showering process and hadronisation differently.…”

Section: Resultssupporting

confidence: 90%

“…The results showed no clear dependence on the transverse momentum (p T ) of the trigger particle. Jet measurements to study j T were done by the CDF collaboration in pp collisions at √ s = 1.96 TeV [18] at Tevatron, by the ATLAS collaboration in pp at √ s = 7 TeV [19] and by the LHCb collaboration in pp collisions at √ s = 8 TeV [20] at the LHC. The results show a dependence of the width of j T distributions with respect to the p T of jets at the LHC energies.…”

Section: Jhep09(2021)211mentioning

confidence: 99%

See 1 more Smart Citation

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $$ \sqrt{s} $$, $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV

Acharya

Adamová

Adler

et al. 2021

J. High Energ. Phys.

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Jet fragmentation transverse momentum (jT) distributions are measured in proton-proton (pp) and proton-lead (p-Pb) collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ s NN = 5.02 TeV with the ALICE experiment at the LHC. Jets are reconstructed with the ALICE tracking detectors and electromagnetic calorimeter using the anti-kT algorithm with resolution parameter R = 0.4 in the pseudorapidity range |η| < 0.25. The jT values are calculated for charged particles inside a fixed cone with a radius R = 0.4 around the reconstructed jet axis. The measured jT distributions are compared with a variety of parton-shower models. Herwig and Pythia 8 based models describe the data well for the higher jT region, while they underestimate the lower jT region. The jT distributions are further characterised by fitting them with a function composed of an inverse gamma function for higher jT values (called the “wide component”), related to the perturbative component of the fragmentation process, and with a Gaussian for lower jT values (called the “narrow component”), predominantly connected to the hadronisation process. The width of the Gaussian has only a weak dependence on jet transverse momentum, while that of the inverse gamma function increases with increasing jet transverse momentum. For the narrow component, the measured trends are successfully described by all models except for Herwig. For the wide component, Herwig and PYTHIA 8 based models slightly underestimate the data for the higher jet transverse momentum region. These measurements set constraints on models of jet fragmentation and hadronisation.

show abstract

Section: Resultssupporting

confidence: 90%

Section: Jhep09(2021)211mentioning

confidence: 99%

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $$ \sqrt{s} $$, $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV

Acharya

Adamová

Adler

et al. 2021

J. High Energ. Phys.

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“…The measurements are performed integrated over the Z kinematics, so that the charged hadron-in-jet distributions can be studied in three bins of jet p T . Reference [4] describes the analysis procedures and methods in greater detail. Figure 2: Comparisons of the longitudinal momentum fractions of charged hadrons in Z-jet with similar measurements in midrapidity inclusive jets (left) and midrapidity isolated photon-jets (right).…”

Section: Methodsmentioning

confidence: 99%

“…In this talk, new measurements of charged hadron production within jets opposite a Z boson are presented from the LHCb experiment [4]. Previous measurements of hadrons within jets at the Large Hadron Collider (LHC) have been made almost exclusively in the inclusive jet channel [5,6,7].…”

Section: Introductionmentioning

confidence: 99%

Jet hadronization at LHCb

Osborn¹

2019

Proceedings of 13th International Workshop in High pT Physics in the RHIC and LHC Era — PoS(High-pT2019)

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In high energy proton-proton collisions, collimated sprays of particles, called jets, result from hard scattered quarks or gluons. Jets are copiously produced in these collisions; however, the dynamic process through which quarks and gluons, collectively referred to as partons, become bound state hadrons is still not well understood. Jets provide an excellent tool to study this process as they are proxies for the scattered parton; therefore, final-state hadrons can be measured with respect to an observable that is correlated to the scattered parton. The LHCb experiment is in an excellent position to measure hadrons within jets due to its excellent tracking and particle-identification capabilities. In this talk, new measurements of charged hadrons within jets measured opposite a Z boson will be presented from the LHCb collaboration. 13th International Workshop in High pT Physics in the RHIC and LHC Era (High-pT2019) 19

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“…This tagging enriches the jet sample with light-quark jets and depletes the contribution of gluon-jets. Z and γ-tagged jets are harder and more collimated than inclusive jets [19,20]. With preselecting the jet type by this sort of tagging, one can study jet modification in the medium in a more controlled manner.…”

Section: Pos(hardprobes2020)011mentioning

confidence: 99%

A brief walk through: Current status of experimental jet physics

Epple¹

2021

Proceedings of 10th International Conference on Hard and Electromagnetic Probes of High-Energy Nuclear Collisions — PoS(HardPro

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Measurement of Charged Hadron Production in Z -Tagged Jets in Proton-Proton Collisions at s=8 TeV

Cited by 18 publications

References 50 publications

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $$ \sqrt{s} $$, $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $$ \sqrt{s} $$, $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV

Jet hadronization at LHCb

A brief walk through: Current status of experimental jet physics

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