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Quenched charmonium spectrum
We study charmonium using the standard relativistic formalism in the quenched approximation, on a set of lattices with isotropic lattice spacings ranging from 0.1 to 0.04 fm. We concentrate on the calculation of the hyperfine splitting between eta_c and J/psi, aiming for a controlled continuum extra...
Autores principales: | , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2003
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1088/1126-6708/2003/08/022 http://cds.cern.ch/record/627247 |
_version_ | 1780900550906216448 |
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author | Choe, S. de Forcrand, P. Garcia Perez, M. Liu, Y. Nakamura, A. Stamatescu, I.O. Takaishi, T. Umeda, T. |
author_facet | Choe, S. de Forcrand, P. Garcia Perez, M. Liu, Y. Nakamura, A. Stamatescu, I.O. Takaishi, T. Umeda, T. |
author_sort | Choe, S. |
collection | CERN |
description | We study charmonium using the standard relativistic formalism in the quenched approximation, on a set of lattices with isotropic lattice spacings ranging from 0.1 to 0.04 fm. We concentrate on the calculation of the hyperfine splitting between eta_c and J/psi, aiming for a controlled continuum extrapolation of this quantity. The splitting extracted from the non-perturbatively improved clover Dirac operator shows very little dependence on the lattice spacing for $a leq 0.1$ fm. The dependence is much stronger for Wilson and tree-level improved clover operators, but they still yield consistent extrapolations if sufficiently fine lattices, $a leq 0.07$ fm ($a M(eta_c) leq 1$), are used. Our result for the hyperfine splitting is 77(2)(6) MeV (where Sommer's parameter, r_0, is used to fix the scale). This value remains about 30% below experiment. Dynamical fermions and OZI-forbidden diagrams both contribute to the remainder. Results for the eta_c and J/psi wave functions are also presented. |
id | cern-627247 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2003 |
record_format | invenio |
spelling | cern-6272472023-03-14T20:26:31Zdoi:10.1088/1126-6708/2003/08/022http://cds.cern.ch/record/627247engChoe, S.de Forcrand, P.Garcia Perez, M.Liu, Y.Nakamura, A.Stamatescu, I.O.Takaishi, T.Umeda, T.Quenched charmonium spectrumParticle Physics - LatticeWe study charmonium using the standard relativistic formalism in the quenched approximation, on a set of lattices with isotropic lattice spacings ranging from 0.1 to 0.04 fm. We concentrate on the calculation of the hyperfine splitting between eta_c and J/psi, aiming for a controlled continuum extrapolation of this quantity. The splitting extracted from the non-perturbatively improved clover Dirac operator shows very little dependence on the lattice spacing for $a leq 0.1$ fm. The dependence is much stronger for Wilson and tree-level improved clover operators, but they still yield consistent extrapolations if sufficiently fine lattices, $a leq 0.07$ fm ($a M(eta_c) leq 1$), are used. Our result for the hyperfine splitting is 77(2)(6) MeV (where Sommer's parameter, r_0, is used to fix the scale). This value remains about 30% below experiment. Dynamical fermions and OZI-forbidden diagrams both contribute to the remainder. Results for the eta_c and J/psi wave functions are also presented.We study charmonium using the standard relativistic formalism in the quenched approximation, on a set of lattices with isotropic lattice spacings ranging from 0.1 to 0.04 fm. We concentrate on the calculation of the hyperfine splitting between eta_c and J/psi, aiming for a controlled continuum extrapolation of this quantity. The splitting extracted from the non-perturbatively improved clover Dirac operator shows very little dependence on the lattice spacing for $a \leq 0.1$ fm. The dependence is much stronger for Wilson and tree-level improved clover operators, but they still yield consistent extrapolations if sufficiently fine lattices, $a \leq 0.07$ fm ($a M(\eta_c) \leq 1$), are used. Our result for the hyperfine splitting is 77(2)(6) MeV (where Sommer's parameter, r_0, is used to fix the scale). This value remains about 30% below experiment. Dynamical fermions and OZI-forbidden diagrams both contribute to the remainder. Results for the eta_c and J/psi wave functions are also presented.hep-lat/0307004IFT-UAM-CSIC-03-24CERN-TH-2002-243CERN-TH-2002-243IFT-UAM-CSIC-2003-24oai:cds.cern.ch:6272472003-07-03 |
spellingShingle | Particle Physics - Lattice Choe, S. de Forcrand, P. Garcia Perez, M. Liu, Y. Nakamura, A. Stamatescu, I.O. Takaishi, T. Umeda, T. Quenched charmonium spectrum |
title | Quenched charmonium spectrum |
title_full | Quenched charmonium spectrum |
title_fullStr | Quenched charmonium spectrum |
title_full_unstemmed | Quenched charmonium spectrum |
title_short | Quenched charmonium spectrum |
title_sort | quenched charmonium spectrum |
topic | Particle Physics - Lattice |
url | https://dx.doi.org/10.1088/1126-6708/2003/08/022 http://cds.cern.ch/record/627247 |
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