TY - JOUR
T1 - Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at s√=13s=13 TeV with the ATLAS detector
AU - Clark, Philip James
AU - Leonidopoulos, Christos
AU - Martin, Victoria Jane
AU - Mills, Corrinne
AU - Collaboration, Atlas
AU - Mijovic, Liza
AU - Gao, Yanyan
AU - Farrington, Sinead
PY - 2017/12/15
Y1 - 2017/12/15
N2 - A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb−1 of s√=13s=13 TeV proton-proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via t~1→t(∗)χ~01t~1→t(∗)χ~10 and t~1→bχ~±1→bW(∗)χ~01t~1→bχ~1±→bW(∗)χ~10, where χ 1 0 (χ 1 ± ) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to tχ~01tχ~10, top-squark masses in the range 450–1000 GeV are excluded for χ~01χ~10 masses below 160 GeV. In the case where mt~1∼mt+mχ~01mt~1∼mt+mχ~10, top-squark masses in the range 235–590 GeV are excluded.
AB - A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb−1 of s√=13s=13 TeV proton-proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via t~1→t(∗)χ~01t~1→t(∗)χ~10 and t~1→bχ~±1→bW(∗)χ~01t~1→bχ~1±→bW(∗)χ~10, where χ 1 0 (χ 1 ± ) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to tχ~01tχ~10, top-squark masses in the range 450–1000 GeV are excluded for χ~01χ~10 masses below 160 GeV. In the case where mt~1∼mt+mχ~01mt~1∼mt+mχ~10, top-squark masses in the range 235–590 GeV are excluded.
U2 - 10.1007/JHEP12(2017)085
DO - 10.1007/JHEP12(2017)085
M3 - Article
SN - 1029-8479
VL - 1712
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
M1 - 85
ER -