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Forward Jets and Forward-Central Jets at CMS

We report on cross section measurements for inclusive forward jet production and for the simultaneous production of a forward and a central jet in sqrt{s} = 7 TeV pp-collisions. Data collected in 2010, corresponding to an integrated luminosity of 3.14 pb^{-1}, is used for the measurements. Jets in t...

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Autor principal: Sen, Niladri
Lenguaje:eng
Publicado: 2011
Materias:
Acceso en línea:https://dx.doi.org/10.1063/1.3700687
http://cds.cern.ch/record/1401592
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author Sen, Niladri
author_facet Sen, Niladri
author_sort Sen, Niladri
collection CERN
description We report on cross section measurements for inclusive forward jet production and for the simultaneous production of a forward and a central jet in sqrt{s} = 7 TeV pp-collisions. Data collected in 2010, corresponding to an integrated luminosity of 3.14 pb^{-1}, is used for the measurements. Jets in the transverse momentum range pT = 35 - 140 GeV/c are reconstructed with the anti-kT (R = 0.5) algorithm. The extended coverage of large pseudo-rapidities is provided by the Hadronic Forward calorimeter (3.2 < \eta < 4.7), while central jets are limited to \eta < 2.8, covered by the main detector components. The two differential cross sections are presented as a function of the jet transverse momentum. Comparisons to next-to-leading order perturbative calculations, and predictions from event generators based on different parton showering mechanisms (PYTHIA and HERWIG) and parton dynamics (CASCADE) are shown.
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institution Organización Europea para la Investigación Nuclear
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publishDate 2011
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spelling cern-14015922019-09-30T06:29:59Zdoi:10.1063/1.3700687http://cds.cern.ch/record/1401592engSen, NiladriForward Jets and Forward-Central Jets at CMSParticle Physics - ExperimentWe report on cross section measurements for inclusive forward jet production and for the simultaneous production of a forward and a central jet in sqrt{s} = 7 TeV pp-collisions. Data collected in 2010, corresponding to an integrated luminosity of 3.14 pb^{-1}, is used for the measurements. Jets in the transverse momentum range pT = 35 - 140 GeV/c are reconstructed with the anti-kT (R = 0.5) algorithm. The extended coverage of large pseudo-rapidities is provided by the Hadronic Forward calorimeter (3.2 < \eta < 4.7), while central jets are limited to \eta < 2.8, covered by the main detector components. The two differential cross sections are presented as a function of the jet transverse momentum. Comparisons to next-to-leading order perturbative calculations, and predictions from event generators based on different parton showering mechanisms (PYTHIA and HERWIG) and parton dynamics (CASCADE) are shown.We report on cross section measurements for inclusive forward jet production and for the simultaneous production of a forward and a central jet in s = 7 TeV pp-collisions. Data collected in 2010, corresponding to an integrated luminosity of 3.14 pb−1, is used for the measurements. Jets in the transverse momentum range pT = 35 - 140 GeV/c are reconstructed with the anti-kT (R = 0.5) algorithm. The extended coverage of large pseudo-rapidities is provided by the Hadronic Forward calorimeter (3.2 < |η| < 4.7), while central jets are limited to |η| < 2.8, covered by the main detector components. The two differential cross sections are presented as a function of the jet transverse momentum. Comparisons to next-to-leading order perturbative calculations, and predictions from event generators based on different parton showering mechanisms (PYTHIA and HERWIG) and parton dynamics (CASCADE) are shown.We report on cross section measurements for inclusive forward jet production and for the simultaneous production of a forward and a central jet in sqrt{s} = 7 TeV pp-collisions. Data collected in 2010, corresponding to an integrated luminosity of 3.14 pb^{-1}, is used for the measurements. Jets in the transverse momentum range pT = 35 - 140 GeV/c are reconstructed with the anti-kT (R = 0.5) algorithm. The extended coverage of large pseudo-rapidities is provided by the Hadronic Forward calorimeter (3.2 < \eta < 4.7), while central jets are limited to \eta < 2.8, covered by the main detector components. The two differential cross sections are presented as a function of the jet transverse momentum. Comparisons to next-to-leading order perturbative calculations, and predictions from event generators based on different parton showering mechanisms (PYTHIA and HERWIG) and parton dynamics (CASCADE) are shown.arXiv:1111.5410oai:cds.cern.ch:14015922011-11-24
spellingShingle Particle Physics - Experiment
Sen, Niladri
Forward Jets and Forward-Central Jets at CMS
title Forward Jets and Forward-Central Jets at CMS
title_full Forward Jets and Forward-Central Jets at CMS
title_fullStr Forward Jets and Forward-Central Jets at CMS
title_full_unstemmed Forward Jets and Forward-Central Jets at CMS
title_short Forward Jets and Forward-Central Jets at CMS
title_sort forward jets and forward-central jets at cms
topic Particle Physics - Experiment
url https://dx.doi.org/10.1063/1.3700687
http://cds.cern.ch/record/1401592
work_keys_str_mv AT senniladri forwardjetsandforwardcentraljetsatcms