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• W2601450132 abstract "We have estimated the limiting branching ratio of the R-parity violating (RPV) decay of the lighter top squark, $tilde t_1 ar l^+ d$ ($l=e$ or $mu $ and d is a down type quark of any flavor), as a function of top squark mass($MST$) for an observable signal in the di-lepton plus di-jet channel at the Tevatron RUN-II experiment with 2 fb$^{-1}$ luminosity. Our simulations indicate that the lepton number violating nature of the underlying decay dynamics can be confirmed via the reconstruction of $MST$. The above decay is interesting in the context of RPV models of neutrino mass where the RPV couplings ($lambda'_{i3j}$) driving the above decay are constrained to be small ($lsim 10^{-3} - 10^{-4} $). If $tilde t_1$ is the next lightest super particle - a theoretically well motivated scenario - then the RPV decay can naturally compete with the R-parity conserving (RPC) modes which also have suppressed widths. The model independent limiting BR can delineate the parameter space in specific supersymmetric models, where the dominating RPV decay is observable and predict the minimum magnitude of the RPV coupling that will be sensitive to Run-II data. We have found it to be in the same ballpark value required by models of neutrino mass, for a wide range of $MST$. A comprehensive future strategy for linking top squark decays with models of neutrino mass is sketched." @default.
• W2601450132 created "2017-04-07" @default.
• W2601450132 creator A5008989193 @default.
• W2601450132 creator A5013666928 @default.
• W2601450132 creator A5021592043 @default.
• W2601450132 date "2004-07-30" @default.
• W2601450132 modified "2023-09-27" @default.
• W2601450132 title "ProbingR-parity violating models of neutrino mass at the Fermilab Tevatron via top squark decays" @default.
• W2601450132 cites W1516587490 @default.
• W2601450132 cites W1555364489 @default.
• W2601450132 cites W1580558097 @default.
• W2601450132 cites W1675984589 @default.
• W2601450132 cites W1805426392 @default.
• W2601450132 cites W1964733056 @default.
• W2601450132 cites W1968589359 @default.
• W2601450132 cites W1968748477 @default.
• W2601450132 cites W1969077320 @default.
• W2601450132 cites W1970077296 @default.
• W2601450132 cites W1974408677 @default.
• W2601450132 cites W1974770733 @default.
• W2601450132 cites W1981406831 @default.
• W2601450132 cites W1983987483 @default.
• W2601450132 cites W1984840579 @default.
• W2601450132 cites W1989572194 @default.
• W2601450132 cites W1994094216 @default.
• W2601450132 cites W1999630440 @default.
• W2601450132 cites W2004660305 @default.
• W2601450132 cites W2006889686 @default.
• W2601450132 cites W2019434046 @default.
• W2601450132 cites W2022547875 @default.
• W2601450132 cites W2023981270 @default.
• W2601450132 cites W2026305137 @default.
• W2601450132 cites W2029139358 @default.
• W2601450132 cites W2029890608 @default.
• W2601450132 cites W2031196171 @default.
• W2601450132 cites W2031268306 @default.
• W2601450132 cites W2036578569 @default.
• W2601450132 cites W2041061282 @default.
• W2601450132 cites W2042711738 @default.
• W2601450132 cites W2046374782 @default.
• W2601450132 cites W2047184962 @default.
• W2601450132 cites W2049568520 @default.
• W2601450132 cites W2050725678 @default.
• W2601450132 cites W2054292573 @default.
• W2601450132 cites W2055101221 @default.
• W2601450132 cites W2058984489 @default.
• W2601450132 cites W2067495348 @default.
• W2601450132 cites W2070893805 @default.
• W2601450132 cites W2075111311 @default.
• W2601450132 cites W2075896356 @default.
• W2601450132 cites W2083182815 @default.
• W2601450132 cites W2088020093 @default.
• W2601450132 cites W2088251440 @default.
• W2601450132 cites W2088868667 @default.
• W2601450132 cites W2089891870 @default.
• W2601450132 cites W2090314870 @default.
• W2601450132 cites W2096544526 @default.
• W2601450132 cites W2102225437 @default.
• W2601450132 cites W2104576071 @default.
• W2601450132 cites W2105605020 @default.
• W2601450132 cites W2115158862 @default.
• W2601450132 cites W2115924910 @default.
• W2601450132 cites W2116355683 @default.
• W2601450132 cites W2118944032 @default.
• W2601450132 cites W2123510857 @default.
• W2601450132 cites W2124635065 @default.
• W2601450132 cites W2126123551 @default.
• W2601450132 cites W2128829202 @default.
• W2601450132 cites W2134803267 @default.
• W2601450132 cites W2149711579 @default.
• W2601450132 cites W2155251936 @default.
• W2601450132 cites W2158398454 @default.
• W2601450132 cites W2160635933 @default.
• W2601450132 cites W2163456024 @default.
• W2601450132 cites W2167762578 @default.
• W2601450132 cites W2172469652 @default.
• W2601450132 cites W2207460949 @default.
• W2601450132 cites W2318491271 @default.
• W2601450132 cites W2417029242 @default.
• W2601450132 cites W3098313849 @default.
• W2601450132 cites W3098349427 @default.
• W2601450132 cites W3100955117 @default.
• W2601450132 cites W3101303819 @default.
• W2601450132 cites W3102209951 @default.
• W2601450132 cites W3103645850 @default.
• W2601450132 cites W3104393593 @default.
• W2601450132 cites W3106386212 @default.
• W2601450132 cites W4230353487 @default.
• W2601450132 cites W63097856 @default.
• W2601450132 doi "https://doi.org/10.1103/physrevd.70.015009" @default.
• W2601450132 hasPublicationYear "2004" @default.
• W2601450132 type Work @default.
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• W2601450132 hasAuthorship W2601450132A5008989193 @default.
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