| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $\text{none 600 - 3400}$ |
95 |
1 |
|
CMS |
|
|
2 |
|
CMS |
| $\text{none 150 - 287}$ |
95 |
3 |
|
ATLS |
|
1
SIRUNYAN 2018BO search for color octet scalar boson produced through gluon fusion process in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit above assumes ${{\mathit S}_{{8gg}}}$ coupling ${{\mathit k}_{{s}}^{2}}$ = 1/2.
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2
KHACHATRYAN 2015AV search for pair productions of neutral color-octet weak-triplet scalar particles (${{\mathit \Theta}^{0}}$), decaying to ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit Z}}{{\mathit g}}$ or ${{\mathit \gamma}}{{\mathit g}}$ , in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The ${{\mathit \Theta}^{0}}$ particle is often predicted in coloron (${{\mathit G}^{\,'}}$, color-octet gauge boson) models and appear in the ${{\mathit p}}{{\mathit p}}$ collisions through ${{\mathit G}^{\,'}}$ $\rightarrow$ ${{\mathit \Theta}^{0}}{{\mathit \Theta}^{0}}$ decays. Assuming B( ${{\mathit \Theta}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ) = 0.5, they give limits ${\mathit m}_{{{\mathit \Theta}^{0}}}$ $>$ 623 GeV (426 GeV) for ${\mathit m}_{{{\mathit G}^{\,'}}}$ = 2.3 ${\mathit m}_{{{\mathit \Theta}^{0}}}$ (${\mathit m}_{{{\mathit G}^{\,'}}}$ = 5 ${\mathit m}_{{{\mathit \Theta}^{0}}}$).
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3
AAD 2013K search for pair production of color-octet scalar particles in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV. Cross section limits are interpreted as mass limits on scalar partners of a Dirac gluino.
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