TY - JOUR
T1 - Searches for third-generation scalar leptoquarks in s=13 TeV pp collisions with the ATLAS detector
AU - Aaboud, M.
AU - Aad, G.
AU - Abbott, B.
AU - Abbott, DC
AU - Abdinov, O.
AU - Abhayasinghe, DK
AU - Abidi, S.H.
AU - AbouZeid, Ossama Sherif Alexander
AU - Abraham, NL
AU - Abramowicz, H.
AU - Abreu, H.
AU - Abulaiti, Y.
AU - Acharya, B.S.
AU - Adachi, Sosuke
AU - Adam, Luise
AU - Adamczyk, L.
AU - Adamek, L.
AU - Adelman, J.
AU - Adersberger, M.
AU - Adiguzel, A.
AU - Besjes, Geert-Jan
AU - Alonso Diaz, Alejandro
AU - Camplani, Alessandra
AU - Dam, Mogens
AU - Bajic, Milena
AU - Hansen, Peter Henrik
AU - Hansen, Jørn Dines
AU - Galster, Gorm Aske Gram Krohn
AU - Hansen, Jørgen Beck
AU - Monk, James William
AU - de Almeida Dias, Flavia
AU - hqz214, hqz214
AU - Petersen, Troels Christian
AU - Stark, Simon Holm
AU - Ignazzi, Rosanna
AU - Wiglesworth, Graig
AU - Xella, Stefania
AU - ATLAS
PY - 2019/6/1
Y1 - 2019/6/1
N2 - 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 (LQ3 u → tν/bτ) and down-type (LQ3 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 = 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 LQ3 u and LQ3 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.[Figure not available: see fulltext.].
AB - 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 (LQ3 u → tν/bτ) and down-type (LQ3 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 = 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 LQ3 u and LQ3 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.[Figure not available: see fulltext.].
U2 - 10.1007/JHEP06(2019)144
DO - 10.1007/JHEP06(2019)144
M3 - Journal article
SN - 1126-6708
VL - 2019
JO - Journal of High Energy Physics (Online)
JF - Journal of High Energy Physics (Online)
IS - 6
M1 - 144
ER -