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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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Lenguaje: | eng |
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1999
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Acceso en línea: | https://dx.doi.org/10.1016/S0375-9474(99)00194-3 http://cds.cern.ch/record/370727 |
_version_ | 1780893100253642752 |
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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 |
record_format | invenio |
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 |
work_keys_str_mv | AT braccinisaverio thek0sk0sfinalstateintwophotoncollisionsandsomeimplicationsforglueballsearches AT braccinisaverio k0sk0sfinalstateintwophotoncollisionsandsomeimplicationsforglueballsearches |