Searches for third-generation scalar leptoquarks in s√=13 TeV pp collisions with the ATLAS detector
Limits are set on the pair production of scalar leptoquarks, where all possible decays of the leptoquark into a quark (t, b) and a lepton (τ, ν) of the third generation are considered. The limits are presented as a function of the leptoquark mass and the branching ratio into charged leptons for up-t...
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| Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
|---|---|
| Corporate Author: | |
| Format: | Article (Journal) |
| Language: | English |
| Published: |
28 June 2019
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| In: |
Journal of high energy physics
Year: 2019, Issue: 6 |
| ISSN: | 1126-6708 |
| DOI: | 10.1007/JHEP06(2019)144 |
| Online Access: | Verlag, Volltext: https://doi.org/10.1007/JHEP06(2019)144 |
| Author Notes: | the ATLAS Collaboration |
MARC
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| 246 | 3 | 3 | |a Searches for third-generation scalar leptoquarks in square root s = 13 TeV pp collisions with the ATLAS detector |
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| 500 | |a The ATLAS Collaboration: M. Aaboud, G. Aad, B. Abbott, D.C. Abbott, O. Abdinov, D.K. Abhayasinghe, S.H. Abidi, O.S. AbouZeid, N.L. Abraham, H. Abramowicz, H. Abreu, Y. Abulaiti, B.S. Acharya, S. Adachi [und 2879 weitere Personen] | ||
| 500 | |a Im Titel steht der Buchstabe s unter dem Wurzelsymbol | ||
| 500 | |a Im Titel ist pp kursiv dargestellt | ||
| 500 | |a Gesehen am 18.08.2020 | ||
| 520 | |a Limits are set on the pair production of scalar leptoquarks, where all possible decays of the leptoquark into a quark (t, b) and a lepton (τ, ν) of the third generation are considered. The limits are presented as a function of the leptoquark mass and the branching ratio into charged leptons for up-type (LQ 3 u → tν/bτ) and down-type (LQ 3 d → bν/tτ) leptoquarks. Many results are reinterpretations of previously published ATLAS searches. In all cases, LHC proton-proton collision data at a centre-of-mass energy of s√s \sqrt{s} = 13 TeV recorded by the ATLAS detector in 2015 and 2016 are used, corresponding to an integrated luminosity of 36.1 fb−1. Masses below 800 GeV are excluded for both LQ 3 u and LQ 3 d independently of the branching ratio, with masses below about 1 TeV being excluded for the limiting cases of branching ratios equal to zero or unity. Open image in new window | ||
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