2021
DOI: 10.1103/physrevd.104.112005
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Search for new phenomena in pp collisions in final states with tau leptons, b -jets, and missing transverse momentum with the ATLAS detector

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Cited by 19 publications
(5 citation statements)
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“…Our reinterpretation procedure will make use of the acceptances, efficiencies and upper limits reported by the ATLAS collaboration in the auxiliary material of [76]. We start by noting that ATLAS implicitly assumes that only the bν and tτ channel are open, hence x = BR(S 1 → tτ ) = 1 − BR(S 1 → bν).…”
Section: Jhep02(2022)042mentioning
confidence: 99%
“…Our reinterpretation procedure will make use of the acceptances, efficiencies and upper limits reported by the ATLAS collaboration in the auxiliary material of [76]. We start by noting that ATLAS implicitly assumes that only the bν and tτ channel are open, hence x = BR(S 1 → tτ ) = 1 − BR(S 1 → bν).…”
Section: Jhep02(2022)042mentioning
confidence: 99%
“…The above LQ masses satisfy the constraints from the LQ direct searches. The searches have been performed by studying LQ pair-production channels at the ATLAS [66] (CMS [67])…”
Section: Jhep02(2022)106mentioning
confidence: 99%
“…There are no dedicated searches for jjτ τ and the limits from jjν ν is 1.0 TeV for β = 1. On the other hand, for the TX-II, R 2 dominantly decays to t tτ τ [229], b bτ τ [230,231], jjτ τ , and jjνν each with the branching ratio β 0.24. Here we fix R 2 mass at 1 TeV, which allows the corresponding branching ratio to be as large as β 0.27 (from t tτ τ ).…”
Section: Appendix-iimentioning
confidence: 99%