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Di-jet production in photon-photon collisions at √see from 189 to 209 GeV

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Di-jet production in photon-photon collisions at √see from 189 to 209 GeV. / OPAL Collaboration.

In: European Physical Journal C: Particles and Fields, Vol. 31, No. 3, 11.2003, p. 307-325.

Research output: Contribution to journalJournal articlepeer-review

Harvard

OPAL Collaboration 2003, 'Di-jet production in photon-photon collisions at √see from 189 to 209 GeV', European Physical Journal C: Particles and Fields, vol. 31, no. 3, pp. 307-325. https://doi.org/10.1140/epjc/s2003-01360-8

APA

OPAL Collaboration (2003). Di-jet production in photon-photon collisions at √see from 189 to 209 GeV. European Physical Journal C: Particles and Fields, 31(3), 307-325. https://doi.org/10.1140/epjc/s2003-01360-8

Vancouver

OPAL Collaboration. Di-jet production in photon-photon collisions at √see from 189 to 209 GeV. European Physical Journal C: Particles and Fields. 2003 Nov;31(3):307-325. https://doi.org/10.1140/epjc/s2003-01360-8

Author

OPAL Collaboration. / Di-jet production in photon-photon collisions at √see from 189 to 209 GeV. In: European Physical Journal C: Particles and Fields. 2003 ; Vol. 31, No. 3. pp. 307-325.

Bibtex

@article{9a45bdd42889448e834183ee035cfd77,
title = "Di-jet production in photon-photon collisions at √see from 189 to 209 GeV",
abstract = "Di-jet production is studied in collisions of quasi-real photons at e+ e- centre-of-mass energies √see from 189 to 209 GeV at LEP. The data were collected with the OPAL detector. Jets are reconstructed using an inclusive k⊥-clustering algorithm for all cross-section measurements presented. A cone jet algorithm is used in addition to study the different structure of the jets resulting from either of the algorithms. The inclusive di-jet cross-section is measured as a function of the mean transverse energy E¯jetT of the two leading jets, and as a function of the estimated fraction of the photon momentum carried by the parton entering the hard sub-process, xγ, for different regions of E¯jetT. Angular distributions in di-jet events are measured and used to demonstrate the dominance of quark and gluon initiated processes in different regions of phase space. Furthermore the inclusive di-jet cross-section as a function of ηjet and Δηjet is presented, where ηjetcntr is the jet pseudo-rapidity. Different regions of the x+γ - x−γ -space are explored to study and control the influence of an underlying event. The results are compared to next-to-leading order perturbative QCD calculations and to the predictions of the leading order Monte Carlo generator PYTHIA.",
author = "Bailey, {Ian Richard} and Vakhtang Kartvelishvili and {OPAL Collaboration}",
year = "2003",
month = nov,
doi = "10.1140/epjc/s2003-01360-8",
language = "English",
volume = "31",
pages = "307--325",
journal = "European Physical Journal C: Particles and Fields",
issn = "1434-6044",
publisher = "SPRINGER",
number = "3",

}

RIS

TY - JOUR

T1 - Di-jet production in photon-photon collisions at √see from 189 to 209 GeV

AU - Bailey, Ian Richard

AU - Kartvelishvili, Vakhtang

AU - OPAL Collaboration

PY - 2003/11

Y1 - 2003/11

N2 - Di-jet production is studied in collisions of quasi-real photons at e+ e- centre-of-mass energies √see from 189 to 209 GeV at LEP. The data were collected with the OPAL detector. Jets are reconstructed using an inclusive k⊥-clustering algorithm for all cross-section measurements presented. A cone jet algorithm is used in addition to study the different structure of the jets resulting from either of the algorithms. The inclusive di-jet cross-section is measured as a function of the mean transverse energy E¯jetT of the two leading jets, and as a function of the estimated fraction of the photon momentum carried by the parton entering the hard sub-process, xγ, for different regions of E¯jetT. Angular distributions in di-jet events are measured and used to demonstrate the dominance of quark and gluon initiated processes in different regions of phase space. Furthermore the inclusive di-jet cross-section as a function of ηjet and Δηjet is presented, where ηjetcntr is the jet pseudo-rapidity. Different regions of the x+γ - x−γ -space are explored to study and control the influence of an underlying event. The results are compared to next-to-leading order perturbative QCD calculations and to the predictions of the leading order Monte Carlo generator PYTHIA.

AB - Di-jet production is studied in collisions of quasi-real photons at e+ e- centre-of-mass energies √see from 189 to 209 GeV at LEP. The data were collected with the OPAL detector. Jets are reconstructed using an inclusive k⊥-clustering algorithm for all cross-section measurements presented. A cone jet algorithm is used in addition to study the different structure of the jets resulting from either of the algorithms. The inclusive di-jet cross-section is measured as a function of the mean transverse energy E¯jetT of the two leading jets, and as a function of the estimated fraction of the photon momentum carried by the parton entering the hard sub-process, xγ, for different regions of E¯jetT. Angular distributions in di-jet events are measured and used to demonstrate the dominance of quark and gluon initiated processes in different regions of phase space. Furthermore the inclusive di-jet cross-section as a function of ηjet and Δηjet is presented, where ηjetcntr is the jet pseudo-rapidity. Different regions of the x+γ - x−γ -space are explored to study and control the influence of an underlying event. The results are compared to next-to-leading order perturbative QCD calculations and to the predictions of the leading order Monte Carlo generator PYTHIA.

U2 - 10.1140/epjc/s2003-01360-8

DO - 10.1140/epjc/s2003-01360-8

M3 - Journal article

VL - 31

SP - 307

EP - 325

JO - European Physical Journal C: Particles and Fields

JF - European Physical Journal C: Particles and Fields

SN - 1434-6044

IS - 3

ER -