Cargando…

A Determination of the Charm Content of the Proton

We present an unbiased determination of the charm content of the proton, in which the charm parton distribution function (PDF) is parametrized on the same footing as the light quarks and the gluon in a global PDF analysis. This determination relies on the calculation of deep-inelastic structure func...

Descripción completa

Detalles Bibliográficos
Autores principales: Ball, Richard D., Bertone, Valerio, Bonvini, Marco, Carrazza, Stefano, Forte, Stefano, Guffanti, Alberto, Hartland, Nathan P., Rojo, Juan, Rottoli, Luca
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1140/epjc/s10052-016-4469-y
http://cds.cern.ch/record/2155124
_version_ 1780950653926899712
author Ball, Richard D.
Bertone, Valerio
Bonvini, Marco
Carrazza, Stefano
Forte, Stefano
Guffanti, Alberto
Hartland, Nathan P.
Rojo, Juan
Rottoli, Luca
author_facet Ball, Richard D.
Bertone, Valerio
Bonvini, Marco
Carrazza, Stefano
Forte, Stefano
Guffanti, Alberto
Hartland, Nathan P.
Rojo, Juan
Rottoli, Luca
author_sort Ball, Richard D.
collection CERN
description We present an unbiased determination of the charm content of the proton, in which the charm parton distribution function (PDF) is parametrized on the same footing as the light quarks and the gluon in a global PDF analysis. This determination relies on the calculation of deep-inelastic structure functions in the FONLL scheme, generalized to account for massive charm-initiated contributions. In contrast to the usual situation in which the charm PDF is assumed to be generated perturbatively by pair radiation off gluons and light quarks, vanishing at a scale set by the value of the charm mass m_c, we find that the fitted charm PDF vanishes within uncertainties at a scale Q~1.5 GeV for all x<~0.1, independent of the value of m_c used in the coefficient functions. We also find some evidence that the charm PDF at large x>~0.1 and low scales does not vanish, but rather has an "intrinsic" component, very weakly scale dependent and almost independent of the value of m_c, carrying about 1% of the total momentum of the proton. The uncertainties in all other PDFs are only slightly increased by the inclusion of fitted charm, while the dependence of these PDFs on m_c is significantly reduced. When the EMC charm structure function dataset is included, it is well described by the fit, and PDF uncertainties in the fitted charm PDF are significantly reduced, though we verify that excluding the EMC data does not qualitatively modify any of our findings. The increased stability with respect to m_c persists at high scales and is the main implication of our results for LHC phenomenology. Fitting the charm PDF modifies the predictions for processes such as high p_T and large rapidity charm pair production and Z+c production, and thus we expect that future LHC data will further constrain the charm content of the proton.
id cern-2155124
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
record_format invenio
spelling cern-21551242022-08-13T02:12:51Zdoi:10.1140/epjc/s10052-016-4469-yhttp://cds.cern.ch/record/2155124engBall, Richard D.Bertone, ValerioBonvini, MarcoCarrazza, StefanoForte, StefanoGuffanti, AlbertoHartland, Nathan P.Rojo, JuanRottoli, LucaA Determination of the Charm Content of the ProtonParticle Physics - PhenomenologyWe present an unbiased determination of the charm content of the proton, in which the charm parton distribution function (PDF) is parametrized on the same footing as the light quarks and the gluon in a global PDF analysis. This determination relies on the calculation of deep-inelastic structure functions in the FONLL scheme, generalized to account for massive charm-initiated contributions. In contrast to the usual situation in which the charm PDF is assumed to be generated perturbatively by pair radiation off gluons and light quarks, vanishing at a scale set by the value of the charm mass m_c, we find that the fitted charm PDF vanishes within uncertainties at a scale Q~1.5 GeV for all x<~0.1, independent of the value of m_c used in the coefficient functions. We also find some evidence that the charm PDF at large x>~0.1 and low scales does not vanish, but rather has an "intrinsic" component, very weakly scale dependent and almost independent of the value of m_c, carrying about 1% of the total momentum of the proton. The uncertainties in all other PDFs are only slightly increased by the inclusion of fitted charm, while the dependence of these PDFs on m_c is significantly reduced. When the EMC charm structure function dataset is included, it is well described by the fit, and PDF uncertainties in the fitted charm PDF are significantly reduced, though we verify that excluding the EMC data does not qualitatively modify any of our findings. The increased stability with respect to m_c persists at high scales and is the main implication of our results for LHC phenomenology. Fitting the charm PDF modifies the predictions for processes such as high p_T and large rapidity charm pair production and Z+c production, and thus we expect that future LHC data will further constrain the charm content of the proton.We present an unbiased determination of the charm content of the proton, in which the charm parton distribution function (PDF) is parametrized on the same footing as the light quarks and the gluon in a global PDF analysis. This determination relies on the NLO calculation of deep-inelastic structure functions in the FONLL scheme, generalized to account for massive charm-initiated contributions. When the EMC charm structure function dataset is included, it is well described by the fit, and PDF uncertainties in the fitted charm PDF are significantly reduced. We then find that the fitted charm PDF vanishes within uncertainties at a scale $Q\sim 1.6$  GeV for all $x\lesssim 0.1$ , independent of the value of $m_c$ used in the coefficient functions. We also find some evidence that the charm PDF at large $x\gtrsim 0.1$ and low scales does not vanish, but rather has an “intrinsic” component, very weakly scale dependent and almost independent of the value of $m_c$ , carrying less than $1\%$ of the total momentum of the proton. The uncertainties in all other PDFs are only slightly increased by the inclusion of fitted charm, while the dependence of these PDFs on $m_c$ is reduced. The increased stability with respect to $m_c$ persists at high scales and is the main implication of our results for LHC phenomenology. Our results show that if the EMC data are correct, then the usual approach in which charm is perturbatively generated leads to biased results for the charm PDF, though at small x this bias could be reabsorbed if the uncertainty due to the charm mass and missing higher orders were included. We show that LHC data for processes, such as high $p_T$ and large rapidity charm pair production and $Z+c$ production, have the potential to confirm or disprove the implications of the EMC data.We present an unbiased determination of the charm content of the proton, in which the charm parton distribution function (PDF) is parametrized on the same footing as the light quarks and the gluon in a global PDF analysis. This determination relies on the calculation of deep-inelastic structure functions in the FONLL scheme, generalized to account for massive charm-initiated contributions. In contrast to the usual situation in which the charm PDF is assumed to be generated perturbatively by pair radiation off gluons and light quarks, vanishing at a scale set by the value of the charm mass m_c, we find that the fitted charm PDF vanishes within uncertainties at a scale Q~1.5 GeV for all x<~0.1, independent of the value of m_c used in the coefficient functions. We also find some evidence that the charm PDF at large x>~0.1 and low scales does not vanish, but rather has an "intrinsic" component, very weakly scale dependent and almost independent of the value of m_c, carrying about 1% of the total momentum of the proton. The uncertainties in all other PDFs are only slightly increased by the inclusion of fitted charm, while the dependence of these PDFs on m_c is significantly reduced. When the EMC charm structure function dataset is included, it is well described by the fit, and PDF uncertainties in the fitted charm PDF are significantly reduced, though we verify that excluding the EMC data does not qualitatively modify any of our findings. The increased stability with respect to m_c persists at high scales and is the main implication of our results for LHC phenomenology. Fitting the charm PDF modifies the predictions for processes such as high p_T and large rapidity charm pair production and Z+c production, and thus we expect that future LHC data will further constrain the charm content of the proton.arXiv:1605.06515EDINBURGH-2016-06CERN-TH-2016-087OUTP-16-03PTIF-UNIMI-2016-3EDINBURGH 2016-06CERN-TH-2016-087OUTP-16-03PTIF-UNIMI-2016-3oai:cds.cern.ch:21551242016-05-20
spellingShingle Particle Physics - Phenomenology
Ball, Richard D.
Bertone, Valerio
Bonvini, Marco
Carrazza, Stefano
Forte, Stefano
Guffanti, Alberto
Hartland, Nathan P.
Rojo, Juan
Rottoli, Luca
A Determination of the Charm Content of the Proton
title A Determination of the Charm Content of the Proton
title_full A Determination of the Charm Content of the Proton
title_fullStr A Determination of the Charm Content of the Proton
title_full_unstemmed A Determination of the Charm Content of the Proton
title_short A Determination of the Charm Content of the Proton
title_sort determination of the charm content of the proton
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1140/epjc/s10052-016-4469-y
http://cds.cern.ch/record/2155124
work_keys_str_mv AT ballrichardd adeterminationofthecharmcontentoftheproton
AT bertonevalerio adeterminationofthecharmcontentoftheproton
AT bonvinimarco adeterminationofthecharmcontentoftheproton
AT carrazzastefano adeterminationofthecharmcontentoftheproton
AT fortestefano adeterminationofthecharmcontentoftheproton
AT guffantialberto adeterminationofthecharmcontentoftheproton
AT hartlandnathanp adeterminationofthecharmcontentoftheproton
AT rojojuan adeterminationofthecharmcontentoftheproton
AT rottoliluca adeterminationofthecharmcontentoftheproton
AT ballrichardd determinationofthecharmcontentoftheproton
AT bertonevalerio determinationofthecharmcontentoftheproton
AT bonvinimarco determinationofthecharmcontentoftheproton
AT carrazzastefano determinationofthecharmcontentoftheproton
AT fortestefano determinationofthecharmcontentoftheproton
AT guffantialberto determinationofthecharmcontentoftheproton
AT hartlandnathanp determinationofthecharmcontentoftheproton
AT rojojuan determinationofthecharmcontentoftheproton
AT rottoliluca determinationofthecharmcontentoftheproton