${{\mathit t}}{{\overline{\mathit t}}}{{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV

INSPIRE   PDGID:
Q007DT8
VALUE (fb) CL% DOCUMENT ID TECN  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
$<23$ 95 1
AAD
2015AR
 ATLS ${{\mathit \ell}}+\not E_T+{}\geq{}$5j (${}\geq{}$2 ${{\mathit b}}$)
$<70$ 95 2
AAD
2015BY
 ATLS ${}\geq{}2{{\mathit \ell}}+\not E_T+{}\geq{}$2j (${}\geq{}$1 ${{\mathit b}}$)
$<32$ 95 3
KHACHATRYAN
2014R
 CMS ${{\mathit \ell}}+\not E_T+{}\geq{}$6j (${}\geq{}$2 ${{\mathit b}}$)
1  AAD 2015AR based on 20.3 fb${}^{-1}$ of data. A fit to ${{\mathit H}_{{{T}}}}$ distributions in multi-channels classified by the number of jets and of ${{\mathit b}}$-tagged jets is performed.
2  AAD 2015BY based on 20.3 fb${}^{-1}$ of data. A same-sign lepton pair is required. An excess over the SM prediction reaches 2.5${{\mathit \sigma}}$ for hypotheses involving heavy resonances decaying into ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit t}}{{\overline{\mathit t}}}$.
3  Based on 19.6 fb${}^{-1}$ of data, using a multivariate analysis to separate signal from backgrounds. About ${\mathit \sigma (}{{\mathit t}}{{\overline{\mathit t}}}{{\mathit t}}{{\overline{\mathit t}}}{)}$ = 1 fb is expected in the SM.
References