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Please use this identifier to cite or link to this item: https://olympias.lib.uoi.gr/jspui/handle/123456789/17148
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dc.contributor.authorAllanach, B. C.en
dc.contributor.authorBaer, H.en
dc.contributor.authorBanerjee, S.en
dc.contributor.authorBerger, Edmond L.en
dc.contributor.authorChertok, M.B.en
dc.contributor.authorCheung, King-manen
dc.contributor.authorde Campos, F.en
dc.contributor.authorDedes, A.en
dc.contributor.authorDiaz, M.A.en
dc.contributor.authorDreiner, Herbert K.en
dc.contributor.authorEboli, Oscar J.P.en
dc.contributor.authorGunion, John F.en
dc.contributor.authorHarris, B.W.en
dc.contributor.authorHewett, J.L.en
dc.contributor.authorMagro, M.B.en
dc.contributor.authorMondal, N.K.en
dc.contributor.authorNarasimham, V.S.en
dc.contributor.authorNavarro, L.en
dc.contributor.authorParua, N.en
dc.contributor.authorPorod, W.en
dc.contributor.authorRestrepo, D.A.en
dc.contributor.authorRichardson, P.en
dc.contributor.authorRizzo, T.en
dc.contributor.authorSeymour, M.H.en
dc.contributor.authorSullivan, Z.en
dc.contributor.authorValle, J.W.F.en
dc.date.accessioned2015-11-24T18:35:52Z-
dc.date.available2015-11-24T18:35:52Z-
dc.identifier.urihttps://olympias.lib.uoi.gr/jspui/handle/123456789/17148-
dc.rightsDefault Licence-
dc.titleSearching for R parity violation at Run II of the Tevatronen
heal.typejournalArticle-
heal.type.enJournal articleen
heal.type.elΆρθρο Περιοδικούel
heal.accesscampus-
heal.recordProviderΠανεπιστήμιο Ιωαννίνων. Σχολή Επιστημών και Τεχνολογιών. Τμήμα Βιολογικών Εφαρμογών και Τεχνολογιώνel
heal.publicationDate1999-
heal.abstractWe present an outlook for possible discovery of supersymmetry with broken R-parity at Run II of the Tevatron. We first present a review of the literature and an update of the experimental bounds. In turn we then discuss the following processes: 1. Resonant slepton production followed by R-parity violating decay, (a) via $LQD^c$ and (b) via $LLE^c$. 2. How to distinguish resonant slepton production from $Z'$ or $W'$ production. 3. Resonant slepton production followed by the decay to neutralino LSP, which decays via $LQD^c$. 4. Resonant stop production followed by the decay to a chargino, which cascades to the neutralino LSP. 5. Gluino pair production followed by the cascade decay to charm squarks which decay directly via $L_1Q_2D^c_1$. 6. Squark pair production followed by the cascade decay to the neutralino LSP which decays via $L_1Q_2D^c_1$. 7. MSSM pair production followed by the cascade decay to the LSP which decays (a) via $LLE^c$, (b) via $LQD^c$, and (c) via $U^cD^cD^c$, respectively. 8. Top quark and top squark decays in spontaneous R-parity violation.en
heal.journalTypepeer reviewed-
heal.fullTextAvailabilityTRUE-
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