The unfolded dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at forward and midrapidity regions, respectively.

The unfolded dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at backward and midrapidity regions, respectively.

The ratio of unfolded dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with both jets at the midrapidity regions.

The ratio of unfolded dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at midrapidity and forward regions, respectively.

The ratio of unfolded dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at midrapidity and backward regions, respectively.

The ratio of unfolded dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at forward and midrapidity regions, respectively.

The ratio of unfolded dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at backward and midrapidity regions, respectively.

Mean xj ratio, $\langle x_{j} \rangle$, in the range $10-60$ as unfolded for different multiplicities, for different leading and subleading jet combinations for the midrapidity, forward, and backward regions

The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with both jets at the midrapidity regions.

The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at midrapidity and forward regions, respectively.

The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at midrapidity and backward regions, respectively.

The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at forward and midrapidity regions, respectively.

The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at backward and midrapidity regions, respectively.

The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with both jets at the midrapidity regions.

The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at midrapidity and forward regions, respectively.

The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at midrapidity and backward regions, respectively.

The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at forward and midrapidity regions, respectively.

The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at backward and midrapidity regions, respectively.

Mean xj ratio, $\langle x_{j} \rangle$, in the range $10-60$ as reconstructed (raw) for different multiplicities, for different leading and subleading jet combinations for the midrapidity, forward, and backward regions

Data from Figure 2, panel d, upper panel, $v_{0}(p_{T})$ for $\eta_{gap}$ = 1, 0-5% Centrality

Data from Figure 2, panel d, lower panel, $v_{0}(p_{T})$ for $\eta_{gap}$ = 1, 50-60% Centrality

Data from Figure 3, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, 0-5% Centrality, $\eta_{gap}$=0

Data from Figure 3, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, 0-5% Centrality, $\eta_{gap}$=1

Data from Figure 3, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, 0-5% Centrality, $\eta_{gap}$=2

Data from Figure 3, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, 0-5% Centrality, $\eta_{gap}$=3

Data from Figure 3, panel b, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, 60-70% Centrality, $\eta_{gap}$=0

Data from Figure 3, panel b, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, 60-70% Centrality, $\eta_{gap}$=1

Data from Figure 3, panel b, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, 60-70% Centrality, $\eta_{gap}$=2

Data from Figure 3, panel b, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, 60-70% Centrality, $\eta_{gap}$=3

Data from Figure 4, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 0-5% Centrality

Data from Figure 4, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 5-10% Centrality

Data from Figure 4, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 10-20% Centrality

Data from Figure 4, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 20-30% Centrality

Data from Figure 4, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 30-40% Centrality

Data from Figure 4, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 40-50% Centrality

Data from Figure 4, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 50-60% Centrality

Data from Figure 4, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 60-70% Centrality

Data from Figure 4, panel b, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 0-5% Centrality

Data from Figure 4, panel b, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 5-10% Centrality

Data from Figure 4, panel b, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 10-20% Centrality

Data from Figure 4, panel b, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 20-30% Centrality

Data from Figure 4, panel b, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 30-40% Centrality

Data from Figure 4, panel b, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 40-50% Centrality

Data from Figure 4, panel b, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 50-60% Centrality

Data from Figure 4, panel b, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 60-70% Centrality

Data from Figure 5, panel a, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 0-5% Centrality

Data from Figure 5, panel b, $v_{0}(p_{T})/v_{0}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$=1, 0-5% Centrality

Data from Appendix, Figure 6, panel a, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 0-5% Centrality

Data from Appendix, Figure 6, panel b, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 10-20% Centrality

Data from Appendix, Figure 6, panel c, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 30-40% Centrality

Data from Appendix, Figure 6, panel d, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 60-70% Centrality

Data from Appendix, Figure 7, Zero Crossing Point of $v_{0}(p_{T})$ for $\eta_{gap}$ = 1

Data from Appendix, Figure 7, $\left\langle [p_{T}]\right\rangle$ for $p_{T}$ range of 0.5-10 GeV, $\eta_{gap}$ = 1

Data from Appendix, Figure 8, panel a, Closure of Sum Rule 1 for $\eta_{gap}$ = 1

Data from Appendix, Figure 8, panel b, Closure of Sum Rule 2 for $\eta_{gap}$ = 1

Data from Appendix, Figure 9, panel a, $v_{0}$ vs $N_{ch}$ for $\eta_{gap}$ = 1

Data from Appendix, Figure 9, panel b, $v_{0} / v^{5\%}_{0}$ vs $N_{ch}$ for $\eta_{gap}$ = 1

Data from Appendix, Figure 10, panel a, $v_{0}\sqrt{N_{ch}}$ vs $N_{ch}$ for $\eta_{gap}$ = 1

Data from Appendix, Figure 10, panel b, $v_{0}\sqrt{N_{ch}}$ vs Centrality for $\eta_{gap}$ = 1

Data from Appendix, Figure 11, $v_{0}(p_{T})\,\sqrt{\left\langle N_{\mathrm{ch}}\right\rangle}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 0-5% Centrality

Data from Appendix, Figure 11, $v_{0}(p_{T})\,\sqrt{\left\langle N_{\mathrm{ch}}\right\rangle}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 5-10% Centrality

Data from Appendix, Figure 11, $v_{0}(p_{T})\,\sqrt{\left\langle N_{\mathrm{ch}}\right\rangle}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 10-20% Centrality

Data from Appendix, Figure 11, $v_{0}(p_{T})\,\sqrt{\left\langle N_{\mathrm{ch}}\right\rangle}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 20-30% Centrality

Data from Appendix, Figure 11, $v_{0}(p_{T})\,\sqrt{\left\langle N_{\mathrm{ch}}\right\rangle}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 30-40% Centrality

Data from Appendix, Figure 11, $v_{0}(p_{T})\,\sqrt{\left\langle N_{\mathrm{ch}}\right\rangle}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 40-50% Centrality

Data from Appendix, Figure 11, $v_{0}(p_{T})\,\sqrt{\left\langle N_{\mathrm{ch}}\right\rangle}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 50-60% Centrality

Data from Appendix, Figure 11, $v_{0}(p_{T})\,\sqrt{\left\langle N_{\mathrm{ch}}\right\rangle}$ for $p^{ref}_{T}$ = 0.5-2 GeV, $\eta_{gap}$ = 1, 60-70% Centrality

Data from Auxiliary, Figure 1, Top row, Left column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 0-5% Centrality, $\eta_{gap}$=0

Data from Auxiliary, Figure 1, Top row, Left column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 0-5% Centrality, $\eta_{gap}$=1

Data from Auxiliary, Figure 1, Top row, Left column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 0-5% Centrality, $\eta_{gap}$=2

Data from Auxiliary, Figure 1, Top row, Left column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 0-5% Centrality, $\eta_{gap}$=3

Data from Auxiliary, Figure 1, Top row, Right column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 60-70% Centrality, $\eta_{gap}$=0

Data from Auxiliary, Figure 1, Top row, Right column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 60-70% Centrality, $\eta_{gap}$=1

Data from Auxiliary, Figure 1, Top row, Right column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 60-70% Centrality, $\eta_{gap}$=2

Data from Auxiliary, Figure 1, Top row, Right column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 60-70% Centrality, $\eta_{gap}$=3

Data from Auxiliary, Figure 1, Bottom row, Left column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 0-5% Centrality, $\eta_{gap}$=0

Data from Auxiliary, Figure 1, Bottom row, Left column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 0-5% Centrality, $\eta_{gap}$=1

Data from Auxiliary, Figure 1, Bottom row, Left column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 0-5% Centrality, $\eta_{gap}$=2

Data from Auxiliary, Figure 1, Bottom row, Left column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 0-5% Centrality, $\eta_{gap}$=3

Data from Auxiliary, Figure 1, Bottom row, Right column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 60-70% Centrality, $\eta_{gap}$=0

Data from Auxiliary, Figure 1, Bottom row, Right column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 60-70% Centrality, $\eta_{gap}$=1

Data from Auxiliary, Figure 1, Bottom row, Right column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 60-70% Centrality, $\eta_{gap}$=2

Data from Auxiliary, Figure 1, Bottom row, Right column, $v_{0}(p_{T})$ for $p^{ref}_{T}$ = 0.5-5 GeV, 60-70% Centrality, $\eta_{gap}$=3

Data from Auxiliary, Figure 2, $v_{0}(p_{T})$ For $\eta_{gap}$ = 0, and 0-5% Centrality

Data from Auxiliary, Figure 2, $v_{0}(p_{T})$ For $\eta_{gap}$ = 0, and 5-10% Centrality

Data from Auxiliary, Figure 2, $v_{0}(p_{T})$ For $\eta_{gap}$ = 0, and 10-20% Centrality

Data from Auxiliary, Figure 2, $v_{0}(p_{T})$ For $\eta_{gap}$ = 0, and 20-30% Centrality

Data from Auxiliary, Figure 2, $v_{0}(p_{T})$ For $\eta_{gap}$ = 0, and 30-40% Centrality

Data from Auxiliary, Figure 2, $v_{0}(p_{T})$ For $\eta_{gap}$ = 0, and 40-50% Centrality

Data from Auxiliary, Figure 2, $v_{0}(p_{T})$ For $\eta_{gap}$ = 0, and 50-60% Centrality

Data from Auxiliary, Figure 2, $v_{0}(p_{T})$ For $\eta_{gap}$ = 0, and 60-70% Centrality

Data from Auxiliary, Figure 3, $v_{0}(p_{T})$ For $\eta_{gap}$ = 1, and 0-5% Centrality

Data from Auxiliary, Figure 3, $v_{0}(p_{T})$ For $\eta_{gap}$ = 1, and 5-10% Centrality

Data from Auxiliary, Figure 3, $v_{0}(p_{T})$ For $\eta_{gap}$ = 1, and 10-20% Centrality

Data from Auxiliary, Figure 3, $v_{0}(p_{T})$ For $\eta_{gap}$ = 1, and 20-30% Centrality

Data from Auxiliary, Figure 3, $v_{0}(p_{T})$ For $\eta_{gap}$ = 1, and 30-40% Centrality

Data from Auxiliary, Figure 3, $v_{0}(p_{T})$ For $\eta_{gap}$ = 1, and 40-50% Centrality

Data from Auxiliary, Figure 3, $v_{0}(p_{T})$ For $\eta_{gap}$ = 1, and 50-60% Centrality

Data from Auxiliary, Figure 3, $v_{0}(p_{T})$ For $\eta_{gap}$ = 1, and 60-70% Centrality

Data from Auxiliary, Figure 4, $v_{0}(p_{T})$ For $\eta_{gap}$ = 2, and 0-5% Centrality

Data from Auxiliary, Figure 4, $v_{0}(p_{T})$ For $\eta_{gap}$ = 2, and 5-10% Centrality

Data from Auxiliary, Figure 4, $v_{0}(p_{T})$ For $\eta_{gap}$ = 2, and 10-20% Centrality

Data from Auxiliary, Figure 4, $v_{0}(p_{T})$ For $\eta_{gap}$ = 2, and 20-30% Centrality

Data from Auxiliary, Figure 4, $v_{0}(p_{T})$ For $\eta_{gap}$ = 2, and 30-40% Centrality

Data from Auxiliary, Figure 4, $v_{0}(p_{T})$ For $\eta_{gap}$ = 2, and 40-50% Centrality

Data from Auxiliary, Figure 4, $v_{0}(p_{T})$ For $\eta_{gap}$ = 2, and 50-60% Centrality

Data from Auxiliary, Figure 4, $v_{0}(p_{T})$ For $\eta_{gap}$ = 2, and 60-70% Centrality

Data from Auxiliary, Figure 5, $v_{0}(p_{T})$ For $\eta_{gap}$ = 3, and 0-5% Centrality

Data from Auxiliary, Figure 5, $v_{0}(p_{T})$ For $\eta_{gap}$ = 3, and 5-10% Centrality

Data from Auxiliary, Figure 5, $v_{0}(p_{T})$ For $\eta_{gap}$ = 3, and 10-20% Centrality

Data from Auxiliary, Figure 5, $v_{0}(p_{T})$ For $\eta_{gap}$ = 3, and 20-30% Centrality

Data from Auxiliary, Figure 5, $v_{0}(p_{T})$ For $\eta_{gap}$ = 3, and 30-40% Centrality

Data from Auxiliary Figure 5, $v_{0}(p_{T})$ For $\eta_{gap}$ = 3, and 40-50% Centrality

Data from Auxiliary Figure 5, $v_{0}(p_{T})$ For $\eta_{gap}$ = 3, and 50-60% Centrality

Data from Auxiliary Figure 5, $v_{0}(p_{T})$ For $\eta_{gap}$ = 3, and 60-70% Centrality

VLL "4321" cross-sections at NLO order of accuracy obtained by MadGraph.

SUSY RPV LQD higgsino cross-sections at NLO + NLL order of accuracy obtained by Resummino.

SUSY RPV LQD wino cross-sections at NLO + NLL order of accuracy obtained by Resummino.

Cutflow of the selection requirements for VLL signals with m_VLL =600, 900, and 1200 GeV. The yields correspond to an integrated luminosity of 126 fb^-1 (140 fb^-1) for the BJET (MST and MSDT) signal regions. The first row refers to unweighted event yields, while the yields presented in other rows are computed after applying event weights according to the selected object reconstruction and identification efficiency scale factors. Dashes (––) refer to requirements that are not applicable.

The expected acceptance times efficiency (including object identification and reconstruction, trigger selection, and event selection) for VLL signal as a function of m_VLL for the combined signal regions as well as for three individual signal region categories: 1τ_had ≥3b MST, 1τ_had ≥3b BJET and ≥2τ_had ≥3b MSDT. The region 1τ_had ≥3b MST refers to the combination of 1τ_had 3b MST and 1τ_had ≥4b MST signal regions, while the region 1τ_had ≥3b BJET refers to the combination of 1τ_had 3b BJET and 1τ_had ≥4b BJET signal regions.

The distributions of the variables used in the simultaneous fit for the SR. The black points with error bars represent the data and their statistical uncertainties, whereas the shaded band represents the predicted uncertainties. The bottom panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction. The last bin of each plot has been extended to include the overflow contribution.

Expected and observed 95% upper limits on the product of the cross section and branching fraction$\sigma(\mathrm{pp} \ ightarrow W\mathrm{a})\mathcal{B}(W ightarrow \ell^{+} v_{\ell})\mathcal{B}(\mathrm{a} \rightarrow Z\gamma)\mathcal{B}(Z \rightarrow \ell^{+} \ell^{-})$ s a function of the ALP mass from 110 to 400 GeV

Expected and observed 95% upper limits on the photophobic ALP model parameter $1/f_{\mathrm{a}}$ as a function of ALP mass reinterpreted from $1/f_{\mathrm{a}}=2~\mathrm{TeV}^{-1}$

Observed 95% CL limits on σ×B for mϕ≠ 125 GeV. The observed limits are consistent with the expected ones within the uncertainties.

Observed 95% CL limits on (σ/σggH)×B for all Higgs boson portal mediator samples where the cross-section is normalized to the SM Higgs boson gluon–gluon fusion production cross-section, σggH = 48.61 pb [97]. The observed limits are consistent with the expected ones within the uncertainties.

Observed 95% CL limits on σ×B for mϕ≠ 125 GeV benchmark samples. The observed limits are consistent with the expected ones within the uncertainties.

Observed 95% CL limits on σ×B for mϕ≠ 125 GeV benchmark samples. The observed limits are consistent with the expected ones within the uncertainties.

Observed 95% CL limits on σ×B for baryogenesis samples for the one-DV analysis. The observed limits are consistent with the expected ones within the uncertainties.

Observed 95% CL limits on σ×B for baryogenesis samples for the one-DV analysis. The observed limits are consistent with the expected ones within the uncertainties.

Observed 95% CL limits on σ×B for baryogenesis samples for the one-DV analysis. The observed limits are consistent with the expected ones within the uncertainties.

Summary of the limits for the Z+ALP model. Comparison between observed and expected 95% CL upper limits on the Z+ALP production cross-section σ×Ba →gg for ma = 40 GeV.

Observed 95% CL upper limits on σ×Ba →gg for all considered ALP mass points.

Comparison between the observed and expected 95% CL limits on (σ/σZH) ×BH →ss for Higgs boson portal mediator and ms=35 GeV for Z-associated H production with one DV.

Observed 95% CL limits on (σ/σZH) ×BH →ss for all Higgs boson portal mediator samples where the cross-section is normalized to the Z(arrow ℓℓ)-associated Higgs boson production cross-section, σZH = 0.089 pb .

Observed 95% CL limits on σ×Bϕ →ss for mϕ≠125 GeV. The observed limits are consistent with the expected ones within the uncertainties.

Observed 95% CL limits on σ×Bϕ →ss for mϕ≠125 GeV. The observed limits are consistent with the expected ones within the uncertainties.

Observed 95% CL upper limits on the σ×BZd →ff production cross-section for dark photon Zd benchmark samples. The observed limits are consistent with the expected ones within the uncertainties.

Observed 95% CL upper limits on the σ×BZd →ff production cross-section for dark photon Zd benchmark samples. The observed limits are consistent with the expected ones within the uncertainties.

Expected and observed limits on (σ/σggH) ×B for the 125 GeV boson benchmark samples for the one-DV search. The cross-section is normalized to the SM Higgs boson gluon–gluon fusion production cross-section, σggH = 48.61 pb.

Expected and observed limits on (σ/σggH) ×B for the 125 GeV boson benchmark samples for the one-DV search. The cross-section is normalized to the SM Higgs boson gluon–gluon fusion production cross-section, σggH = 48.61 pb.

Expected and observed limits on (σ/σggH) ×B for the 125 GeV boson benchmark samples for the one-DV search. The cross-section is normalized to the SM Higgs boson gluon–gluon fusion production cross-section, σggH = 48.61 pb.

Expected and observed 95% CL limits on σ×B for 60 GeV non-SM Higgs boson scalar benchmark samples for the one-DV search.

Expected and observed 95% CL limits on σ×B for 60 GeV non-SM Higgs boson scalar benchmark samples for the one-DV search.

Expected and observed 95% CL limits on σ×B for 200 GeV non-SM Higgs boson scalar benchmark sample for the one-DV search.

Expected and observed 95% CL limits on σ×B for 400 GeV non-SM Higgs boson scalar benchmark sample for the one-DV search.

Expected and observed 95% CL limits on σ×B for 600 GeV non-SM Higgs boson scalar benchmark samples for the one-DV search.

Expected and observed 95% CL limits on σ×B for 600 GeV non-SM Higgs boson scalar benchmark samples for the one-DV search.

Expected and observed 95% CL limits on σ×B for 600 GeV non-SM Higgs boson scalar benchmark samples for the one-DV search.

Expected and observed 95% CL limits on σ×B for 1000 GeV non-SM Higgs boson scalar benchmark samples for the one-DV search.

Expected and observed 95% CL limits on σ×B for 1000 GeV non-SM Higgs boson scalar benchmark samples for the one-DV search.

Expected and observed 95% CL limits on σ×B for 1000 GeV non-SM Higgs boson scalar benchmark samples for the one-DV search.

Expected and observed limits on (σ/σggH) ×B for the 125 GeV boson benchmark samples for the combination of one- and two- DV searches. The cross-section is normalized to the SM Higgs boson gluon–gluon fusion production cross-section, σggH = 48.61 pb.

Expected and observed limits on (σ/σggH) ×B for the 125 GeV boson benchmark samples for the combination of one- and two- DV searches. The cross-section is normalized to the SM Higgs boson gluon–gluon fusion production cross-section, σggH = 48.61 pb.

Expected and observed limits on (σ/σggH) ×B for the 125 GeV boson benchmark samples for the combination of one- and two- DV searches. The cross-section is normalized to the SM Higgs boson gluon–gluon fusion production cross-section, σggH = 48.61 pb.

Expected and observed limits on (σ/σggH) ×B for the 125 GeV boson benchmark samples for the combination of one- and two- DV searches. The cross-section is normalized to the SM Higgs boson gluon–gluon fusion production cross-section, σggH = 48.61 pb.

Expected and observed 95% CL limits on σ×B for 60 GeV non-SM Higgs boson scalar benchmark samples for the combination of one- and two- DV searches.

Expected and observed 95% CL limits on σ×B for 60 GeV non-SM Higgs boson scalar benchmark samples for the combination of one- and two- DV searches.

Expected and observed 95% CL limits on σ×B for 200 GeV non-SM Higgs boson scalar benchmark sample for the combination of one- and two- DV searches.

Expected and observed 95% CL limits on σ×B for 400 GeV non-SM Higgs boson scalar benchmark sample for the combination of one- and two- DV searches.

Expected and observed 95% CL limits on σ×B for 600 GeV non-SM Higgs boson scalar benchmark samples for the combination of one- and two- DV searches.

Expected and observed 95% CL limits on σ×B for 600 GeV non-SM Higgs boson scalar benchmark samples for the combination of one- and two- DV searches.

Expected and observed 95% CL limits on σ×B for 600 GeV non-SM Higgs boson scalar benchmark samples for the combination of one- and two- DV searches.

Expected and observed 95% CL limits on σ×B for 1000 GeV non-SM Higgs boson scalar benchmark samples for the combination of one- and two- DV searches.

Expected and observed 95% CL limits on σ×B for 1000 GeV non-SM Higgs boson scalar benchmark samples for the combination of one- and two- DV searches.

Expected and observed 95% CL limits on σ×B for 1000 GeV non-SM Higgs boson scalar benchmark samples for the combination of one- and two- DV searches.

Expected and observed limits for the baryogenesis benchmark samples (χ →νbb̄ channel) for the one-DV search, where σSM in the plots is cross-section of the SM Higgs boson production.

Expected and observed limits for the baryogenesis benchmark samples (χ →νbb̄ channel) for the one-DV search, where σSM in the plots is cross-section of the SM Higgs boson production.

Expected and observed limits for the baryogenesis benchmark samples (χ →νbb̄ channel) for the one-DV search, where σSM in the plots is cross-section of the SM Higgs boson production.

Expected and observed limits for the baryogenesis benchmark samples (χ →cbs channel) for one-DV search, where σSM in the plots is cross-section of the SM Higgs boson production.

Expected and observed limits for the baryogenesis benchmark samples (χ →cbs channel) for one-DV search, where σSM in the plots is cross-section of the SM Higgs boson production.

Expected and observed limits for the baryogenesis benchmark samples (χ →cbs channel) for one-DV search, where σSM in the plots is cross-section of the SM Higgs boson production.

Expected and observed limits for the baryogenesis benchmark samples (χ →ντ+ τ- channel) for the one-DV search, where σSM in the plots is cross-section of the SM Higgs boson production.

Expected and observed limits for the baryogenesis benchmark samples (χ →ντ+ τ- channel) for the one-DV search, where σSM in the plots is cross-section of the SM Higgs boson production.

Expected and observed limits for the baryogenesis benchmark samples (χ →ντ+ τ- channel) for the one-DV search, where σSM in the plots is cross-section of the SM Higgs boson production.

Expected and observed 95% CL upper limits for the Z+ALP benchmark samples. The observed limits are consistent with the expected ones within the uncertainties.

Expected and observed 95% CL upper limits for the Z+ALP benchmark samples. The observed limits are consistent with the expected ones within the uncertainties.

Expected and observed 95% CL upper limits for the Z+ALP benchmark samples. The observed limits are consistent with the expected ones within the uncertainties.

One-DV barrel trigger 2D efficiency maps as a function of the LLP boost β and transverse decay position Lxy for mϕ=60 GeV, ms=5 GeV, cτsim=0.22 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=60 GeV, ms=5 GeV, cτsim=0.22 m.

One-DV vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=60 GeV, ms=5 GeV, cτsim=0.22 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=60 GeV, ms=5 GeV, cτsim=0.22 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=60 GeV, ms=16 GeV, cτsim=0.66 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=60 GeV, ms=16 GeV, cτsim=0.66 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=60 GeV, ms=16 GeV, cτsim=0.66 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=60 GeV, ms=16 GeV, cτsim=0.66 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=125 GeV, ms=5 GeV, cτsim=0.13 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=125 GeV, ms=5 GeV, cτsim=0.13 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=125 GeV, ms=5 GeV, cτsim=0.13 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=125 GeV, ms=5 GeV, cτsim=0.13 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=125 GeV, ms=5 GeV, cτsim=0.41 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=125 GeV, ms=5 GeV, cτsim=0.41 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=125 GeV, ms=5 GeV, cτsim=0.41 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=125 GeV, ms=5 GeV, cτsim=0.41 m.

One-DV barrel trigger 2D efficiency map for mϕ=125 GeV, ms=16 GeV, cτsim=0.58 m.

One-DV endcap trigger 2D efficiency map for mϕ=125 GeV, ms=16 GeV, cτsim=0.58 m.

One-DV barrel vertex 2D efficiency map for mϕ=125 GeV, ms=16 GeV, cτsim=0.58 m.

One-DV endcap vertex 2D efficiency map for mϕ=125 GeV, ms=16 GeV, cτsim=0.58 m.

One-DV barrel trigger efficiency map for mϕ=125 GeV, ms=35 GeV, cτsim=1.31 m.

One-DV endcap trigger 2D efficiency map for mϕ=125 GeV, ms=35 GeV, cτsim=1.31 m.

One-DV barrel vertex 2D efficiency map for mϕ=125 GeV, ms=35 GeV, cτsim=1.31 m.

One-DV endcap vertex 2D efficiency map for mϕ=125 GeV, ms=35 GeV, cτsim=1.31 m.

One-DV barrel trigger 2D efficiency map for mϕ=125 GeV, ms=35 GeV, cτsim=2.63 m.

One-DV endcap trigger 2D efficiency map for mϕ=125 GeV, ms=35 GeV, cτsim=2.63 m.

One-DV barrel vertex 2D efficiency map for mϕ=125 GeV, ms=35 GeV, cτsim=2.63 m.

One-DV endcap vertex 2D efficiency map for mϕ=125 GeV, ms=35 GeV, cτsim=2.63 m.

One-DV barrel trigger 2D efficiency map for mϕ=125 GeV, ms=55 GeV, cτsim=1.05 m.

One-DV endcap trigger 2D efficiency map for mϕ=125 GeV, ms=55 GeV, cτsim=1.05 m.

One-DV barrel vertex 2D efficiency map for mϕ=125 GeV, ms=55 GeV, cτsim=1.05 m.

One-DV endcap vertex 2D efficiency map for mϕ=125 GeV, ms=55 GeV, cτsim=1.05 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=125 GeV, ms=55 GeV, cτsim=5.32 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=125 GeV, ms=55 GeV, cτsim=5.32 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=125 GeV, ms=55 GeV, cτsim=5.32 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=125 GeV, ms=55 GeV, cτsim=5.32 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=200 GeV, ms=50 GeV, cτsim=1.25 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=200 GeV, ms=50 GeV, cτsim=1.25 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=200 GeV, ms=50 GeV, cτsim=1.25 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=200 GeV, ms=50 GeV, cτsim=1.25 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, ms=100 GeV, cτsim=1.61 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=400 GeV, ms=100 GeV, cτsim=1.61 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, ms=100 GeV, cτsim=1.61 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=400 GeV, ms=100 GeV, cτsim=1.61 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=50 GeV, cτsim=0.59 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=50 GeV, cτsim=0.59 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=50 GeV, cτsim=0.59 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=50 GeV, cτsim=0.59 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=150 GeV, cτsim=1.84 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=150 GeV, cτsim=1.84 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=150 GeV, cτsim=1.84 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=150 GeV, cτsim=1.84 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=150 GeV, cτsim=3.31 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=150 GeV, cτsim=3.31 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=150 GeV, cτsim=3.31 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=150 GeV, cτsim=3.31 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=275 GeV, cτsim=4.29 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=275 GeV, cτsim=4.29 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=275 GeV, cτsim=4.29 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=275 GeV, cτsim=4.29 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=50 GeV, cτsim=0.41 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=50 GeV, cτsim=0.41 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=50 GeV, cτsim=0.41 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=50 GeV, cτsim=0.41 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=275 GeV, cτsim=2.40 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=275 GeV, cτsim=2.40 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=275 GeV, cτsim=2.40 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=275 GeV, cτsim=2.40 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=275 GeV, cτsim=4.33 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=275 GeV, cτsim=4.33 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=275 GeV, cτsim=4.33 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=275 GeV, cτsim=4.33 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=475 GeV, cτsim=6.04 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=475 GeV, cτsim=6.04 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=475 GeV, cτsim=6.04 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=475 GeV, cτsim=6.04 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →bb̄ν channel with mχ=10 GeV and cτsim=0.92 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →bb̄ν channel with mχ=10 GeV and cτsim=0.92 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →bb̄ν channel with mχ=10 GeV and cτsim=0.92 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →bb̄ν channel with mχ=10 GeV and cτsim=0.92 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →cbs channel with mχ=10 GeV and cτsim=0.92 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →cbs channel with mχ=10 GeV and cτsim=0.92 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →cbs channel with mχ=10 GeV and cτsim=0.92 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →cbs channel with mχ=10 GeV and cτsim=0.92 m.

One-DV barrel trigger 2D efficiency maps as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →τ+τ-ν channel with mχ=10 GeV and cτsim=0.92 m.

One-DV endcap trigger 2D efficiency maps as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →τ+τ-ν channel with mχ=10 GeV and cτsim=0.92 m.

One-DV barrel vertex 2D efficiency maps as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →τ+τ-ν channel with mχ=10 GeV and cτsim=0.92 m.

One-DV endcap vertex 2D efficiency maps as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →τ+τ-ν channel with mχ=10 GeV and cτsim=0.92 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →bb̄ν channel with mχ=55 GeV and cτsim=5.55 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →bb̄ν channel with mχ=55 GeV and cτsim=5.55 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →bb̄ν channel with mχ=55 GeV and cτsim=5.55 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →bb̄ν channel with mχ=55 GeV and cτsim=5.55 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →cbs channel with mχ=55 GeV and cτsim=5.55 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →cbs channel with mχ=55 GeV and cτsim=5.55 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →cbs channel with mχ=55 GeV and cτsim=5.55 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →cbs channel with mχ=55 GeV and cτsim=5.55 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →τ+τ-ν channel with mχ=55 GeV and cτsim=5.55 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →τ+τ-ν channel with mχ=55 GeV and cτsim=5.55 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →τ+τ-ν channel with mχ=55 GeV and cτsim=5.55 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →τ+τ-ν channel with mχ=55 GeV and cτsim=5.55 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →bb̄ν channel with mχ=100 GeV and cτsim=3.50 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →bb̄ν channel with mχ=100 GeV and cτsim=3.50 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →bb̄ν channel with mχ=100 GeV and cτsim=3.50 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →bb̄ν channel with mχ=100 GeV and cτsim=3.50 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →cbs channel with mχ=100 GeV and cτsim=3.50 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →cbs channel with mχ=100 GeV and cτsim=3.50 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →cbs channel with mχ=100 GeV and cτsim=3.50 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →cbs channel with mχ=100 GeV and cτsim=3.50 m.

One-DV barrel trigger 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →τ+τ-ν channel with mχ=100 GeV and cτsim=3.50 m.

One-DV endcap trigger 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →τ+τ-ν channel with mχ=100 GeV and cτsim=3.50 m.

One-DV barrel vertex 2D efficiency map as a function of the LLP boost β and transverse decay position Lxy for baryogenesis χ →τ+τ-ν channel with mχ=100 GeV and cτsim=3.50 m.

One-DV endcap vertex 2D efficiency map as a function of the LLP boost β and longitudinal decay position Lz for baryogenesis χ →τ+τ-ν channel with mχ=100 GeV and cτsim=3.50 m.

One-DV barrel trigger efficiency for Z+ALP samples in the lepton-triggered region for mALP=0.1 GeV and cτsim=0.003 m.

One-DV endcap trigger efficiency for Z+ALP samples in the lepton-triggered region for mALP=0.1 GeV and cτsim=0.003 m.

One-DV barrel vertex efficiency for Z+ALP samples in the lepton-triggered region for mALP=0.1 GeV and cτsim=0.003 m.

One-DV endcap vertex efficiency for Z+ALP samples in the lepton-triggered region for mALP=0.1 GeV and cτsim=0.003 m.

One-DV barrel trigger efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mALP=1 GeV and cτsim=0.031 m.

One-DV endcap trigger efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mALP=1 GeV and cτsim=0.031 m.

One-DV barrel vertex efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mALP=1 GeV and cτsim=0.031 m.

One-DV endcap vertex efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mALP=1 GeV and cτsim=0.031 m.

One-DV barrel trigger efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mALP=10 GeV and cτsim=0.31 m.

One-DV endcap trigger efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mALP=10 GeV and cτsim=0.31 m.

One-DV barrel vertex efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mALP=10 GeV and cτsim=0.31 m.

One-DV endcap vertex efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mALP=10 GeV and cτsim=0.31 m.

One-DV barrel trigger efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mALP=40 GeV and cτsim=0.48 m.

One-DV endcap trigger efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mALP=40 GeV and cτsim=0.48 m.

One-DV barrel vertex efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mALP=40 GeV and cτsim=0.48 m.

One-DV endcap vertex efficiency for Z+ALP samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mALP=40 GeV and cτsim=0.48 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, mZd=5 GeV, cτsim=0.6 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, mZd=5 GeV, cτsim=0.6 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, mZd=5 GeV, cτsim=0.6 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, mZd=5 GeV, cτsim=0.6 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, mZd=15 GeV, cτsim=1.6 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, mZd=15 GeV, cτsim=1.6 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, mZd=15 GeV, cτsim=1.6 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, mZd=15 GeV, cτsim=1.6 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, mZd=15 GeV, cτsim=3.0 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, mZd=15 GeV, cτsim=3.0 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, mZd=15 GeV, cτsim=3.0 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, mZd=15 GeV, cτsim=3.0 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=250 GeV, mZd=50 GeV, cτsim=1.6 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=250 GeV, mZd=50 GeV, cτsim=1.6 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=250 GeV, mZd=50 GeV, cτsim=1.6 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=250 GeV, mZd=50 GeV, cτsim=1.6 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=250 GeV, mZd=100 GeV, cτsim=3.4 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=250 GeV, mZd=100 GeV, cτsim=3.4 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=250 GeV, mZd=100 GeV, cτsim=3.4 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=250 GeV, mZd=100 GeV, cτsim=3.4 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, mZd=100 GeV, cτsim=1.6 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudial decay position Lz for mϕ=400 GeV, mZd=100 GeV, cτsim=1.6 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, mZd=100 GeV, cτsim=1.6 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=400 GeV, mZd=100 GeV, cτsim=1.6 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, mZd=200 GeV, cτsim=4.0 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=400 GeV, mZd=200 GeV, cτsim=4.0 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, mZd=200 GeV, cτsim=4.0 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=400 GeV, mZd=200 GeV, cτsim=4.0 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, mZd=150 GeV, cτsim=1.6 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, mZd=150 GeV, cτsim=1.6 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, mZd=150 GeV, cτsim=1.6 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, mZd=150 GeV, cτsim=1.6 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, mZd=150 GeV, cτsim=4.0 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, mZd=150 GeV, cτsim=4.0 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, mZd=150 GeV, cτsim=4.0 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, mZd=150 GeV, cτsim=4.0 m.

One-DV barrel trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, mZd=400 GeV, cτsim=4.6 m.

One-DV endcap trigger efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, mZd=400 GeV, cτsim=4.6 m.

One-DV barrel vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, mZd=400 GeV, cτsim=4.6 m.

One-DV endcap vertex efficiency for HZZd samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, mZd=400 GeV, cτsim=4.6 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=60 GeV, ms=5 GeV, cτsim=0.12 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=60 GeV, ms=5 GeV, cτsim=0.12 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=60 GeV, ms=5 GeV, cτsim=0.12 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=60 GeV, ms=5 GeV, cτsim=0.12 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=60 GeV, ms=15 GeV, cτsim=0.25 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=60 GeV, ms=15 GeV, cτsim=0.25 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=60 GeV, ms=15 GeV, cτsim=0.25 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=60 GeV, ms=15 GeV, cτsim=0.25 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=5 GeV, cτsim=0.1 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=5 GeV, cτsim=0.1 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=5 GeV, cτsim=0.1 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=5 GeV, cτsim=0.1 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=5 GeV, cτsim=0.3 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=5 GeV, cτsim=0.3 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=5 GeV, cτsim=0.3 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=5 GeV, cτsim=0.3 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=16 GeV, cτsim=0.3 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=16 GeV, cτsim=0.3 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=16 GeV, cτsim=0.3 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=16 GeV, cτsim=0.3 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=35 GeV, cτsim=0.75 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=35 GeV, cτsim=0.75 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=35 GeV, cτsim=0.75 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=35 GeV, cτsim=0.75 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=35 GeV, cτsim=2.5 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=35 GeV, cτsim=2.5 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=35 GeV, cτsim=2.5 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=35 GeV, cτsim=2.5 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=55 GeV, cτsim=1.0 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=55 GeV, cτsim=1.0 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=55 GeV, cτsim=1.0 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=55 GeV, cτsim=1.0 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=55 GeV, cτsim=3.5 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=55 GeV, cτsim=3.5 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mH=125 GeV, ms=55 GeV, cτsim=3.5 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mH=125 GeV, ms=55 GeV, cτsim=3.5 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=200 GeV, ms=50 GeV, cτsim=1.25 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=200 GeV, ms=50 GeV, cτsim=1.25 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=200 GeV, ms=50 GeV, cτsim=1.25 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=200 GeV, ms=50 GeV, cτsim=1.25 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=200 GeV, ms=80 GeV, cτsim=2.0 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=200 GeV, ms=80 GeV, cτsim=2.0 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=200 GeV, ms=80 GeV, cτsim=2.0 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=200 GeV, ms=80 GeV, cτsim=2.0 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, ms=100 GeV, cτsim=1.25 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=400 GeV, ms=100 GeV, cτsim=1.25 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, ms=100 GeV, cτsim=1.25 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=400 GeV, ms=100 GeV, cτsim=1.25 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, ms=175 GeV, cτsim=2.5 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=400 GeV, ms=175 GeV, cτsim=2.5 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=400 GeV, ms=175 GeV, cτsim=2.5 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=400 GeV, ms=175 GeV, cτsim=2.5 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=50 GeV, cτsim=0.4 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=50 GeV, cτsim=0.4 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=50 GeV, cτsim=0.4 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=50 GeV, cτsim=0.4 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=150 GeV, cτsim=1.5 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=150 GeV, cτsim=1.5 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=150 GeV, cτsim=1.5 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=150 GeV, cτsim=1.5 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=150 GeV, cτsim=3.5 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=150 GeV, cτsim=3.5 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=150 GeV, cτsim=3.5 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=150 GeV, cτsim=3.5 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=275 GeV, cτsim=2.5 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=275 GeV, cτsim=2.5 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=600 GeV, ms=275 GeV, cτsim=2.5 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=600 GeV, ms=275 GeV, cτsim=2.5 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=50 GeV, cτsim=0.3 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=50 GeV, cτsim=0.3 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=50 GeV, cτsim=0.3 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=50 GeV, cτsim=0.3 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=275 GeV, cτsim=1.5 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=275 GeV, cτsim=1.5 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=275 GeV, cτsim=1.5 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=275 GeV, cτsim=1.5 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=275 GeV, cτsim=3.5 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=275 GeV, cτsim=3.5 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=275 GeV, cτsim=3.5 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=275 GeV, cτsim=3.5 m.

One-DV barrel trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=475 GeV, cτsim=4.5 m.

One-DV endcap trigger efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=475 GeV, cτsim=4.5 m.

One-DV barrel vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and transverse decay position Lxy for mϕ=1000 GeV, ms=475 GeV, cτsim=4.5 m.

One-DV endcap vertex efficiency for ZH samples in the lepton-triggered region as a function of the LLP boost β and longitudinal decay position Lz for mϕ=1000 GeV, ms=475 GeV, cτsim=4.5 m.

Upper limits at $95\%$ CL on the LQ-fermion couplings, $|y_{e u}|$, versus $S_{e u}$ mass for scalar LQs coupled to electrons.

Observed and Expected UL exclusions on the $BR(H\to S)$ of generic signals with $m_{A'} = 1.0\;GeV$ and $BR(A' \rightarrow \pi\pi) = 1.0$.

The observed data in the dielectron channel and the fitted signal-plus-background templates, shown for the $S_{e d}$ scenario with a candidate LQ mass of 2.5 TeV. Distributions of events are binned in the reconstructed dilepton mass, rapidity, and cosine theta.

Observed and Expected UL exclusions on the number of 'signal' yields in sideband A from the model agnostic fit, assuming no 'SUEP-like' signal contamination in the CRs.

Upper limits at $95\%$ CL on the LQ-fermion couplings, $|y_{e d}|$, versus $S_{e d}$ mass for scalar LQs coupled to electrons.

Postfit values for SR in the B-Only CR+SR and CR-Only fits with the prefit signal overlayed for reference

The observed data in the dimuon channel and the fitted signal-plus-background templates, shown for the $S_{\mu u}$ scenario with a candidate LQ mass of 2.5 TeV. Distributions of events are binned in the reconstructed dilepton mass, rapidity, and cosine theta.

Postfit values for PR in the B-Only CR+SR and CR-Only fits with the prefit signal overlayed for reference

Upper limits at $95\%$ CL on the LQ-fermion couplings, $|y_{\mu u}|$, versus $S_{\mu u}$ mass for scalar LQs coupled to muons.

Postfit values for CRDY in the B-Only CR+SR and CR-Only fits with the prefit signal overlayed for reference

The observed data in the dimuon channel and the fitted signal-plus-background templates, shown for the $S_{\mu d}$ scenario with a candidate LQ mass of 2.5 TeV. Distributions of events are binned in the reconstructed dilepton mass, rapidity, and cosine theta.

Postfit values for CRTT in the B-Only CR+SR and CR-Only fits with the prefit signal overlayed for reference

Upper limits at $95\%$ CL on the LQ-fermion couplings, $|y_{\mu d}|$, versus $S_{\mu d}$ mass for scalar LQs coupled to muons.

Per-selection efficiencies on Generic - $m_{A'} = 1.0\;GeV$ $BR(A' \rightarrow \pi\pi) = 1.0$ Hadronic - $m_{A'} = 0.7\;GeV$ and $BR(A' \rightarrow ee) = BR(A' \rightarrow \mu\mu) = 0.15$ $BR(A' \rightarrow \pi\pi) = 0.7$ Leptonic - $m_{A'} = 0.5\;GeV$ and $BR(A' \rightarrow ee) = BR(A' \rightarrow \mu\mu) = 0.2$ and $BR(A' \rightarrow \pi\pi) = 0.6$ samples. Selections: 2 OSSF leptons, one SUEP cluster, $60\leq Z_{m}\leq 120$ GeV, $p_{T}^Z\geq 25$ GeV, veto events with b-tagged jets, $p_{T}^{SUEP} > 60\;GeV$, and $dR^{Ak4}_{Ak15} < 1.5$. Efficiencies are the ratio of the histogram size at the selection step to the previous step (except twoLepton vs. initial). The final column is the total cumulative efficiency (dR vs. initial). Note that these selection numbers were all calculated using samples generated with 600,000 events for each signal point considered.

The observed data in the dielectron channel and the fitted signal-plus-background templates, shown for the $V_{e u}$ scenario with a candidate LQ mass of 2.5 TeV. Distributions of events are binned in the reconstructed dilepton mass, rapidity, and cosine theta.

Interpolated observed and expected UL exclusions on $BR(H\to S) = 1$ for generic signals with $m_{A'} = 1.0\;GeV$ and $BR(A' \rightarrow \pi\pi) = 1.0$. The discreate heatmap points can be found in the UL Generic (Observed & Expected) figure in this sandbox

Upper limits at $95\%$ CL on the LQ-fermion couplings, $|g_{e u}|$, versus $V_{e u}$ mass for vector LQs coupled to electrons.

The observed data in the dielectron channel and the fitted signal-plus-background templates, shown for the $V_{e d}$ scenario with a candidate LQ mass of 2.5 TeV. Distributions of events are binned in the reconstructed dilepton mass, rapidity, and cosine theta.

Upper limits at $95\%$ CL on the LQ-fermion couplings, $|g_{e d}|$, versus $V_{e d}$ mass for vector LQs coupled to electrons.

The observed data in the dimuon channel and the fitted signal-plus-background templates, shown for the $V_{\mu u}$ scenario with a candidate LQ mass of 2.5 TeV. Distributions of events are binned in the reconstructed dilepton mass, rapidity, and cosine theta.

Upper limits at $95\%$ CL on the LQ-fermion couplings, $|g_{\mu u}|$, versus $V_{\mu u}$ mass for vector LQs coupled to muons.

The observed data in the dimuon channel and the fitted signal-plus-background templates, shown for the $V_{\mu d}$ scenario with a candidate LQ mass of 2.5 TeV. Distributions of events are binned in the reconstructed dilepton mass, rapidity, and cosine theta.

Upper limits at $95\%$ CL on the LQ-fermion couplings, $|g_{\mu d}|$, versus $V_{\mu d}$ mass for vector LQs coupled to muons.

Systematic covariance matrix for the differential cross-section distribution.