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An Analysis of the Inclusive $\Upsilon (1S) \to \eta^\prime X$ Decay and Constraints on the $\eta^\prime$-Meson Distribution Amplitudes

We calculate the $\eta^\prime$-meson energy spectrum in the $\Upsilon (1S) \to \eta^\prime g g g \to \eta^\prime X$ decay in the leading-order perturbative QCD in the static-quark limit for the orthoquarkonium.Our principal result is the extraction of parameters of the $\eta^\prime g^* g$ effective...

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Detalles Bibliográficos
Autores principales: Ali, Ahmed, Parkhomenko, A.Ya.
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:https://dx.doi.org/10.1140/epjcd/s2003-03-215-1
http://cds.cern.ch/record/678166
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author Ali, Ahmed
Parkhomenko, A.Ya.
author_facet Ali, Ahmed
Parkhomenko, A.Ya.
author_sort Ali, Ahmed
collection CERN
description We calculate the $\eta^\prime$-meson energy spectrum in the $\Upsilon (1S) \to \eta^\prime g g g \to \eta^\prime X$ decay in the leading-order perturbative QCD in the static-quark limit for the orthoquarkonium.Our principal result is the extraction of parameters of the $\eta^\prime g^* g$ effective vertex function (EVF) involving a virtual and a real gluon from the available data on the hard part of the $\eta^\prime$-meson energy spectrum. The perturbative-QCD based framework provides a good description of the available CLEO data, allowing one to constrain the lowest Gegenbauer coefficients $B^{(q)}_2$ and $B^{(g)}_2$ of the quark-antiquark and gluonic distribution amplitudes of the $\eta^\prime$-meson. The resulting constraints are combined with the existing ones on these coefficients from an analysis of the $\eta^\prime - \gamma$ transition form factor and the requirement of positivity of the EVF, yielding $B^{(q)}_2 (\mu_0^2) = -0.008 \pm 0.054$ and $B^{(g)}_2 (\mu_0^2) = 4.6 \pm 2.5$ for $\mu_0^2 = 2 GeV^2$. This reduces significantly the current uncertainty on these coefficients.
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institution Organización Europea para la Investigación Nuclear
language eng
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spelling cern-6781662023-03-14T18:49:22Zdoi:10.1140/epjcd/s2003-03-215-1http://cds.cern.ch/record/678166engAli, AhmedParkhomenko, A.Ya.An Analysis of the Inclusive $\Upsilon (1S) \to \eta^\prime X$ Decay and Constraints on the $\eta^\prime$-Meson Distribution AmplitudesParticle Physics - PhenomenologyWe calculate the $\eta^\prime$-meson energy spectrum in the $\Upsilon (1S) \to \eta^\prime g g g \to \eta^\prime X$ decay in the leading-order perturbative QCD in the static-quark limit for the orthoquarkonium.Our principal result is the extraction of parameters of the $\eta^\prime g^* g$ effective vertex function (EVF) involving a virtual and a real gluon from the available data on the hard part of the $\eta^\prime$-meson energy spectrum. The perturbative-QCD based framework provides a good description of the available CLEO data, allowing one to constrain the lowest Gegenbauer coefficients $B^{(q)}_2$ and $B^{(g)}_2$ of the quark-antiquark and gluonic distribution amplitudes of the $\eta^\prime$-meson. The resulting constraints are combined with the existing ones on these coefficients from an analysis of the $\eta^\prime - \gamma$ transition form factor and the requirement of positivity of the EVF, yielding $B^{(q)}_2 (\mu_0^2) = -0.008 \pm 0.054$ and $B^{(g)}_2 (\mu_0^2) = 4.6 \pm 2.5$ for $\mu_0^2 = 2 GeV^2$. This reduces significantly the current uncertainty on these coefficients.We calculate the $\eta^\prime$-meson energy spectrum in the $\Upsilon (1S) \to \eta^\prime g g g \to \eta^\prime X$ decay in the leading-order perturbative QCD in the static-quark limit for the orthoquarkonium.Our principal result is the extraction of parameters of the $\eta^\prime g^* g$ effective vertex function (EVF) involving a virtual and a real gluon from the available data on the hard part of the $\eta^\prime$-meson energy spectrum. The perturbative-QCD based framework provides a good description of the available CLEO data, allowing one to constrain the lowest Gegenbauer coefficients $B^{(q)}_2$ and $B^{(g)}_2$ of the quark-antiquark and gluonic distribution amplitudes of the $\eta^\prime$-meson. The resulting constraints are combined with the existing ones on these coefficients from an analysis of the $\eta^\prime - \gamma$ transition form factor and the requirement of positivity of the EVF, yielding $B^{(q)}_2 (\mu_0^2) = -0.008 \pm 0.054$ and $B^{(g)}_2 (\mu_0^2) = 4.6 \pm 2.5$ for $\mu_0^2 = 2 GeV^2$. This reduces significantly the current uncertainty on these coefficients.hep-ph/0310256CERN-TH-2003-254CERN-TH-2003-254oai:cds.cern.ch:6781662003-10-21
spellingShingle Particle Physics - Phenomenology
Ali, Ahmed
Parkhomenko, A.Ya.
An Analysis of the Inclusive $\Upsilon (1S) \to \eta^\prime X$ Decay and Constraints on the $\eta^\prime$-Meson Distribution Amplitudes
title An Analysis of the Inclusive $\Upsilon (1S) \to \eta^\prime X$ Decay and Constraints on the $\eta^\prime$-Meson Distribution Amplitudes
title_full An Analysis of the Inclusive $\Upsilon (1S) \to \eta^\prime X$ Decay and Constraints on the $\eta^\prime$-Meson Distribution Amplitudes
title_fullStr An Analysis of the Inclusive $\Upsilon (1S) \to \eta^\prime X$ Decay and Constraints on the $\eta^\prime$-Meson Distribution Amplitudes
title_full_unstemmed An Analysis of the Inclusive $\Upsilon (1S) \to \eta^\prime X$ Decay and Constraints on the $\eta^\prime$-Meson Distribution Amplitudes
title_short An Analysis of the Inclusive $\Upsilon (1S) \to \eta^\prime X$ Decay and Constraints on the $\eta^\prime$-Meson Distribution Amplitudes
title_sort analysis of the inclusive $\upsilon (1s) \to \eta^\prime x$ decay and constraints on the $\eta^\prime$-meson distribution amplitudes
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1140/epjcd/s2003-03-215-1
http://cds.cern.ch/record/678166
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