Fig. 5.

Expected (open dots and 1$\mathit{\sigma }$ and 2$\mathit{\sigma }$ bands) and observed (full dots) cross-section times branching fraction upper limits (95% CL) for the processes indicated in the bottom left corner of each plot, ${\mathit{\tau }}_{\mathrm{LLP}}$ is always 10$\mathrm{ps}$. The results correspond to the 8 TeV dataset. a Upper limits as a function of the LLP mass for process $PA$; b as a function of the LLP mass for process $PB$, with $m_{\text{``}\tilde{\mathrm{g}}\text{''}}=100$ $\mathrm{GeV}/c^2$; c as a function of $m_{{\mathrm{h}}^0}$ for process $PC$ for $m_{\mathrm{LLP}}$ of 20, 40, and 60 $\mathrm{GeV}/c^2$, from top to bottom (the single point at 130 $\mathrm{GeV}/c^2$ with $m_{\mathrm{LLP}}=60\mathrm{GeV}/c^2$ has been shifted to the right for visualisation); d upper limits as a function of the LLP mass for process $PD$ with $m_{\tilde{\mathrm{q}}}=60$ $\mathrm{GeV}/c^2$