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Hard Quasi-real Photo-production of Charged Hadrons at COMPASS energies

The Common Muon Proton Apparatus for Structure and Spectroscopy (COMPASS) at CERN with its use of beams of naturally polarized muons scattered of a polarized deuteron target, provides an environment of hard scattering between quasi-real photons and partons. Hard hadron quasi-real photo-production wi...

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Autor principal: Morreale, Astrid
Lenguaje:eng
Publicado: 2010
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1742-6596/295/1/012110
http://cds.cern.ch/record/1314129
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author Morreale, Astrid
author_facet Morreale, Astrid
author_sort Morreale, Astrid
collection CERN
description The Common Muon Proton Apparatus for Structure and Spectroscopy (COMPASS) at CERN with its use of beams of naturally polarized muons scattered of a polarized deuteron target, provides an environment of hard scattering between quasi-real photons and partons. Hard hadron quasi-real photo-production with polarized initial states is sensitive to the polarized gluon distribution $\Delta$G through $\gamma$-gluon($g$) direct channels as well as $q$-$g$ resolved processes. Comparisons of unpolarized differential cross section measurements to next-to-leading order (NLO) pQCD calculations are essential to develop our understanding of proton-proton and lepton-nucleon scattering at varying center of mass energies. These measurements are important to asses the applicability of NLO pQCD in interpreting polarized processes. In this talk we will discuss unidentified charged separated hadron production at low $Q^{2}$ (Q$^{2}<0.1 GeV^{2}/c^{2}$) and high transverse momenta (p$_{T}>1.0\,GeV/c$). $<p_{T}^2>$ spectra of charged hadrons at $Q^{2}>1 GeV^{2}/c^{2}$ will also be discussed.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2010
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spelling cern-13141292022-08-17T13:29:51Zdoi:10.1088/1742-6596/295/1/012110http://cds.cern.ch/record/1314129engMorreale, AstridHard Quasi-real Photo-production of Charged Hadrons at COMPASS energiesParticle Physics - ExperimentThe Common Muon Proton Apparatus for Structure and Spectroscopy (COMPASS) at CERN with its use of beams of naturally polarized muons scattered of a polarized deuteron target, provides an environment of hard scattering between quasi-real photons and partons. Hard hadron quasi-real photo-production with polarized initial states is sensitive to the polarized gluon distribution $\Delta$G through $\gamma$-gluon($g$) direct channels as well as $q$-$g$ resolved processes. Comparisons of unpolarized differential cross section measurements to next-to-leading order (NLO) pQCD calculations are essential to develop our understanding of proton-proton and lepton-nucleon scattering at varying center of mass energies. These measurements are important to asses the applicability of NLO pQCD in interpreting polarized processes. In this talk we will discuss unidentified charged separated hadron production at low $Q^{2}$ (Q$^{2}<0.1 GeV^{2}/c^{2}$) and high transverse momenta (p$_{T}>1.0\,GeV/c$). $<p_{T}^2>$ spectra of charged hadrons at $Q^{2}>1 GeV^{2}/c^{2}$ will also be discussed.The Common Muon Proton Apparatus for Structure and Spectroscopy (COMPASS) at CERN with its use of beams of naturally polarized muons scattered of a polarized deuteron target, provides an environment of hard scattering between quasi-real photons and partons. Hard hadron quasi-real photo-production with polarized initial states is sensitive to the polarized gluon distribution $\Delta$G through $\gamma$-gluon($g$) direct channels as well as $q$-$g$ resolved processes. Comparisons of unpolarized differential cross section measurements to next-to-leading order (NLO) pQCD calculations are essential to develop our understanding of proton-proton and lepton-nucleon scattering at varying center of mass energies. These measurements are important to asses the applicability of NLO pQCD in interpreting polarized processes. In this talk we will discuss unidentified charged separated hadron production at low $Q^{2}$ (Q$^{2}<0.1 GeV^{2}/c^{2}$) and high transverse momenta (p$_{T}>1.0\,GeV/c$). $<p_{T}^2>$ spectra of charged hadrons at $Q^{2}>1 GeV^{2}/c^{2}$ will also be discussed.arXiv:1012.2796oai:cds.cern.ch:13141292010-12-14
spellingShingle Particle Physics - Experiment
Morreale, Astrid
Hard Quasi-real Photo-production of Charged Hadrons at COMPASS energies
title Hard Quasi-real Photo-production of Charged Hadrons at COMPASS energies
title_full Hard Quasi-real Photo-production of Charged Hadrons at COMPASS energies
title_fullStr Hard Quasi-real Photo-production of Charged Hadrons at COMPASS energies
title_full_unstemmed Hard Quasi-real Photo-production of Charged Hadrons at COMPASS energies
title_short Hard Quasi-real Photo-production of Charged Hadrons at COMPASS energies
title_sort hard quasi-real photo-production of charged hadrons at compass energies
topic Particle Physics - Experiment
url https://dx.doi.org/10.1088/1742-6596/295/1/012110
http://cds.cern.ch/record/1314129
work_keys_str_mv AT morrealeastrid hardquasirealphotoproductionofchargedhadronsatcompassenergies