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The $K^{0}_{s}K^{0}_{s}$ Final State in Two-Photon Collisions and Some Implications for Glueball Searches

The K0sK0s final state in two-photon collisions is studied with the L3 detector at LEP using data at centre of mass energies from 91 GeV to 183 GeV. The K0sK0s mass spectrum is dominated by the formation of the f_2'(1525) tensor meson whose two-photon partial width is measured. Clear evidence f...

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Autor principal: Braccini, Saverio
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0375-9474(99)00194-3
http://cds.cern.ch/record/370727
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author Braccini, Saverio
author_facet Braccini, Saverio
author_sort Braccini, Saverio
collection CERN
description The K0sK0s final state in two-photon collisions is studied with the L3 detector at LEP using data at centre of mass energies from 91 GeV to 183 GeV. The K0sK0s mass spectrum is dominated by the formation of the f_2'(1525) tensor meson whose two-photon partial width is measured. Clear evidence for destructive f_2-a_2 interference is observed. No signal is present in the region around 2.2 GeV. An upper limit for the two-photon partial width times the K0sK0s branching ratio of the \xi(2230) glueball candidate is then derived. An enhancement is observed around 1750 MeV. It may be due to the formation of a radial recurrence of the f_2'(1525) or to the s\bar{s} member of the 0++ meson nonet.
id cern-370727
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1999
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spelling cern-3707272021-10-08T02:19:15Zdoi:10.1016/S0375-9474(99)00194-3http://cds.cern.ch/record/370727engBraccini, SaverioThe $K^{0}_{s}K^{0}_{s}$ Final State in Two-Photon Collisions and Some Implications for Glueball SearchesParticle Physics - ExperimentThe K0sK0s final state in two-photon collisions is studied with the L3 detector at LEP using data at centre of mass energies from 91 GeV to 183 GeV. The K0sK0s mass spectrum is dominated by the formation of the f_2'(1525) tensor meson whose two-photon partial width is measured. Clear evidence for destructive f_2-a_2 interference is observed. No signal is present in the region around 2.2 GeV. An upper limit for the two-photon partial width times the K0sK0s branching ratio of the \xi(2230) glueball candidate is then derived. An enhancement is observed around 1750 MeV. It may be due to the formation of a radial recurrence of the f_2'(1525) or to the s\bar{s} member of the 0++ meson nonet.The K0sK0s final state in two-photon collisions is studied with the L3 detector at LEP using data at centre of mass energies from 91 GeV to 183 GeV. The K0sK0s mass spectrum is dominated by the formation of the f_2'(1525) tensor meson whose two-photon partial width is measured. Clear evidence for destructive f_2-a_2 interference is observed. No signal is present in the region around 2.2 GeV. An upper limit for the two-photon partial width times the K0sK0s branching ratio of the \xi(2230) glueball candidate is then derived. An enhancement is observed around 1750 MeV. It may be due to the formation of a radial recurrence of the f_2'(1525) or to the s\bar{s} member of the 0++ meson nonet.The K0sK0s final state in two-photon collisions is studied with the L3 detector at LEP using data at centre of mass energies from 91 GeV to 183 GeV. The K0sK0s mass spectrum is dominated by the formation of the f_2'(1525) tensor meson whose two-photon partial width is measured. Clear evidence for destructive f_2-a_2 interference is observed. No signal is present in the region around 2.2 GeV. An upper limit for the two-photon partial width times the K0sK0s branching ratio of the \xi(2230) glueball candidate is then derived. An enhancement is observed around 1750 MeV. It may be due to the formation of a radial recurrence of the f_2'(1525) or to the s\bar{s} member of the 0++ meson nonet.The K s 0 K s 0 final state in two-photon collisions is studied with the L3 detector at LEP using data at centre of mass energies from 91 GeV to 183 GeV. The K s 0 K s 0 mass spectrum is dominated by the formation of the f 2 ′(1525) tensor meson whose two-photon partial width is measured. Clear evidence for destructive f 2 -a 2 interference is observed. No signal is present in the region around 2.2 GeV. An upper limit for the two-photon partial width times the K s 0 K s 0 branching ratio of the ξ(2230) glueball candidate is then derived. An enhancement is observed around 1750 MeV. It may be due to the formation of a radial recurrence of the f 2 ′(1525) or to the s s member of the 0 ++ meson nonet.hep-ex/9811017oai:cds.cern.ch:3707271999
spellingShingle Particle Physics - Experiment
Braccini, Saverio
The $K^{0}_{s}K^{0}_{s}$ Final State in Two-Photon Collisions and Some Implications for Glueball Searches
title The $K^{0}_{s}K^{0}_{s}$ Final State in Two-Photon Collisions and Some Implications for Glueball Searches
title_full The $K^{0}_{s}K^{0}_{s}$ Final State in Two-Photon Collisions and Some Implications for Glueball Searches
title_fullStr The $K^{0}_{s}K^{0}_{s}$ Final State in Two-Photon Collisions and Some Implications for Glueball Searches
title_full_unstemmed The $K^{0}_{s}K^{0}_{s}$ Final State in Two-Photon Collisions and Some Implications for Glueball Searches
title_short The $K^{0}_{s}K^{0}_{s}$ Final State in Two-Photon Collisions and Some Implications for Glueball Searches
title_sort $k^{0}_{s}k^{0}_{s}$ final state in two-photon collisions and some implications for glueball searches
topic Particle Physics - Experiment
url https://dx.doi.org/10.1016/S0375-9474(99)00194-3
http://cds.cern.ch/record/370727
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