Projected sensitivities of the search for RPV supersymmetric neutralinos decaying semileptonically [6] and produced through a Higgs boson exotic decay. The results are extrapolated from Run 1 results (top left), for luminosities of 23 $\text{ fb} ^{-1}$ (top right), 50 $\text{ fb} ^{-1}$ (bottom left) and 300 $\text{ fb} ^{-1}$ (bottom right). The results are presented in terms of the excluded parameter space of the neutralinos for different upper limits at 95% C.L. on the branching fractions of the Higgs boson decay.

Comparison of projected sensitivities in the search for RPV supersymmetric neutralinos decaying semileptonically [6] and produced through a Higgs boson exotic decay. The sensitivities are extrapolated from Run 1 results, and the figure compares parameter regions where the branching fraction of the Higgs boson decay to a $\tilde{\chi}^{0}_{1} \tilde{\chi}^{0}_{1}$ pair is constrained to be smaller than 2% (left) and 0.5% (right) at 95% CL.

Projected sensitivities of the search for HV pions decaying hadronically [5] and produced through a Higgs boson exotic decay. The results are extrapolated from Run 1 results (top left), for luminosities of 23 $\text{ fb} ^{-1}$ (top right), 50 $\text{ fb} ^{-1}$ (bottom left) and 300 $\text{ fb} ^{-1}$ (bottom right). The results are presented in terms of the excluded parameter space of the HV pions for different upper limits at 95% C.L. on the branching fractions of the Higgs boson decay.

Comparison of projected sensitivities in the search for HV pions decaying hadronically [5] and produced through a Higgs boson exotic decay. The sensitivities are extrapolated from Run 1 results, and the figure compares parameter regions where the branching fraction of the Higgs boson decay to a $\pi_v\pi_v$ pair is constrained to be smaller than 20% (left) and 2% (right) at 95% CL.

Animated gif made out of all figures.

Assumptions for the integrated luminosity used in this document.

Examples of the acceptance and total efficiencies assumed to detect a $\tilde{\chi}^{0}_{1}$ decaying semileptonically at a $pp$ collision energy of $\sqrt{s}=13$ TeV at the LHCb detector. Background yields at an integrated luminosity of 1.7 $\text{ fb} ^{-1}$ are also presented. Differences in these yields are due to the effect of a multivariate classifier which is trained differently for each mass-lifetime case.

Background yields assumed for the HV pion analysis at an integrated luminosity of 23 $\text{ fb} ^{-1}$ . The yields are divided in bins of $R_{xy}=\sqrt{x^2+y^2}$, where $x,y$ are the coordinates of the $\pi_v$ particle decay vertex position. Values are extrapolated from Ref. [5].

Examples of the acceptance and total efficiencies assumed to detect a $\pi_v$ particle decaying to a pair of jets at a $pp$ collision energy $\sqrt{s}=14$ TeV at the LHCb detector. The main inefficiencies arise from the requirements to have $\pi_v$ particle in the VELO and to have the decay products in the LHCb acceptance and from the reconstruction of the secondary vertex. More details can be found in Ref. [5].