Comparison between data and background prediction before the fit (Pre-Fit) for the mass of the FCNC top-quark candidate in SR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction before the fit (Pre-Fit) for the mass of the SM top-quark candidate in SR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction before the fit (Pre-Fit) for the transverse momentum of the Z boson candidate in SR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{1}$ discriminant in the mass sideband CR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also separately shown, normalized to 500 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{2}^{u}$ discriminant in the mass sideband CR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also separately shown, normalized to 500 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{1}$ discriminant in SR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also separately shown, normalized to 50 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{2}^{u}$ discriminant in SR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also separately shown, normalized to 50 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZc LH coupling extraction. The distribution is for the $D_{1}$ discriminant in the mass sideband CR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZc LH signals are also separately shown, normalized to 500 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZc LH coupling extraction. The distribution is for the $D_{2}^{c}$ discriminant in the mass sideband CR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZc LH signals are also separately shown, normalized to 500 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZc LH coupling extraction. The distribution is for the $D_{1}$ discriminant in SR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZc LH signals are also separately shown, normalized to 50 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZc LH coupling extraction. The distribution is for the $D_{2}^{c}$ discriminant in SR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZc LH signals are also separately shown, normalized to 50 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the leading lepton $p_{T}$ in the $t\bar{t}$ CR. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also shown separately, normalized to $10^{3}$ times the best fit of the signal yield. The last bin includes the overflow. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the third lepton $p_{T}$ in the $t\bar{t}$ CR. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also shown separately, normalized to $10^{3}$ times the best fit of the signal yield. The last bin includes the overflow. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the leading lepton $p_{T}$ in the $t\bar{t}Z$ CR. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also shown separately, normalized to $10^{3}$ times the best fit of the signal yield. The last bin includes the overflow. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{1}$ discriminant in the $t\bar{t}Z$ CR. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also shown separately, normalized to $10^{3}$ times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0 \leq R_{\mathrm{T}} < 0.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $0.5 \leq R_{\mathrm{T}} < 1.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $1.5 \leq R_{\mathrm{T}} < 2.5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ transverse momentum spectrum for events with $2.5 \leq R_{\mathrm{T}} < 5$ normalised to the $R_{\mathrm{T}}$-integrated spectrum in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 0.5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $0.5 \leq R_{\mathrm{T}} < 1.5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $1.5 \leq R_{\mathrm{T}} < 2.5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $2.5 \leq R_{\mathrm{T}} < 5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 0.5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $0.5 \leq R_{\mathrm{T}} < 1.5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $1.5 \leq R_{\mathrm{T}} < 2.5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $2.5 \leq R_{\mathrm{T}} < 5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 0.5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $0.5 \leq R_{\mathrm{T}} < 1.5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $1.5 \leq R_{\mathrm{T}} < 2.5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{K}^{+}+\mathrm{K}^{-})/(\pi^{+}+\pi^{-})$ for events in the $2.5 \leq R_{\mathrm{T}} < 5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 0.5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $0.5 \leq R_{\mathrm{T}} < 1.5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $1.5 \leq R_{\mathrm{T}} < 2.5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $2.5 \leq R_{\mathrm{T}} < 5$ class in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 0.5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $0.5 \leq R_{\mathrm{T}} < 1.5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $1.5 \leq R_{\mathrm{T}} < 2.5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $2.5 \leq R_{\mathrm{T}} < 5$ class in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $0 \leq R_{\mathrm{T}} < 0.5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $0.5 \leq R_{\mathrm{T}} < 1.5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $1.5 \leq R_{\mathrm{T}} < 2.5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-differential $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ for events in the $2.5 \leq R_{\mathrm{T}} < 5$ class in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ average transverse momentum as a function of $R_{\mathrm{T}}$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ average transverse momentum as a function of $R_{\mathrm{T}}$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\pi^{+}+\pi^{-}$ average transverse momentum as a function of $R_{\mathrm{T}}$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ average transverse momentum as a function of $R_{\mathrm{T}}$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ average transverse momentum as a function of $R_{\mathrm{T}}$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{K}^{+}+\mathrm{K}^{-}$ average transverse momentum as a function of $R_{\mathrm{T}}$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ average transverse momentum as a function of $R_{\mathrm{T}}$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ average transverse momentum as a function of $R_{\mathrm{T}}$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$\mathrm{p} + \mathrm {\overline{p}}$ average transverse momentum as a function of $R_{\mathrm{T}}$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-integrated $(\mathrm{K}^{+} + \mathrm{K}^{-})/(\pi^{+} + \pi^{-})$ as a function of $R_{\mathrm{T}}$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-integrated $(\mathrm{K}^{+} + \mathrm{K}^{-})/(\pi^{+} + \pi^{-})$ as a function of $R_{\mathrm{T}}$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-integrated $(\mathrm{K}^{+} + \mathrm{K}^{-})/(\pi^{+} + \pi^{-})$ as a function of $R_{\mathrm{T}}$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-integrated $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ as a function of $R_{\mathrm{T}}$ in the Toward region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-integrated $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ as a function of $R_{\mathrm{T}}$ in the Away region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

$p_{\mathrm{T}}$-integrated $(\mathrm{p} + \mathrm {\overline{p}})/(\pi^{+} + \pi^{-})$ as a function of $R_{\mathrm{T}}$ in the Transverse region in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$.

Transverse momentum spectra for the jet region, obtained as toward-transverse. Events with a leading track with PT>5 GEV at midrapidity are selected. The spectrum is shown in Figure 1 (right panel).

Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the underlying event (transverse region). Events with a leading track with PT>5 GEV at midrapidity are selected. The B2 is shown in Figure 2 (both panels).

Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the jet (transverse-toward region). Events with a leading track with PT>5 GEV at midrapidity are selected. The B2 is shown in Figure 2 (both panels).

$p_{\rm T}$-differential density of $\Xi^{\pm}$ in jets and the underlying event in pp collisions at $\sqrt{s} = 13$ TeV.

$p_{\rm T}$-differential density of inclusive $\Omega^{\pm}$ in pp collisions at $\sqrt{s} = 13$ TeV.

$p_{\rm T}$-differential density of $\Omega^{\pm}$ in jets and the underlying event in pp collisions at $\sqrt{s} = 13$ TeV.

$p_{\rm T}$-differential $(\Lambda + \overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ ratio of inclusive particles in pp collisions at $\sqrt{s} = 13$ TeV.

$p_{\rm T}$-differential $(\Lambda + \overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ ratio in jets and the underlying event in pp collisions at $\sqrt{s} = 13$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / 2{\rm K}_{\rm S}^{0}$ and $(\Xi^{-} + \Xi^{+}) / (\Lambda + \overline{\Lambda})$ ratios of inclusive particles in pp collisions at $\sqrt{s} = 13$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / 2{\rm K}_{\rm S}^{0}$ and $(\Xi^{-} + \Xi^{+}) / (\Lambda + \overline{\Lambda})$ ratios in jets and the underlying event in pp collisions at $\sqrt{s} = 13$ TeV.

$p_{\rm T}$-differential $(\Omega^{-} + \Omega^{+}) / 2{\rm K}_{\rm S}^{0}$, $(\Omega^{-} + \Omega^{+}) / (\Lambda + \overline{\Lambda})$ and $(\Omega^{-} + \Omega^{+}) / (\Xi^{-} + \Xi^{+})$ ratios of inclusive particles in pp collisions at $\sqrt{s} = 13$ TeV.

$p_{\rm T}$-differential $(\Omega^{-} + \Omega^{+}) / 2{\rm K}_{\rm S}^{0}$, $(\Omega^{-} + \Omega^{+}) / (\Lambda + \overline{\Lambda})$ and $(\Omega^{-} + \Omega^{+}) / (\Xi^{-} + \Xi^{+})$ ratios in jets and the underlying event in pp collisions at $\sqrt{s} = 13$ TeV.

$p_{\rm T}$-differential density of inclusive ${\rm K}_{\rm S}^{0}$ and $\Lambda$ ($\overline{\Lambda}$) in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential densities of ${\rm K}_{\rm S}^{0}$ and $\Lambda$ ($\overline{\Lambda}$) in jets and the underlying event in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of inclusive $\Xi^{\pm}$ in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of $\Xi^{\pm}$ in jets and the underlying event in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of inclusive $\Omega^{\pm}$ in p-Pb collisions at $\sqrt{s} = 5.02$ TeV.

$p_{\rm T}$-differential density of $\Omega^{\pm}$ in jets and the underlying event in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Lambda + \overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ ratio in jets for various event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / 2{\rm K}_{\rm S}^{0}$ and $(\Xi^{-} + \Xi^{+}) / (\Lambda + \overline{\Lambda})$ ratios in jets for various event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Omega^{-} + \Omega^{+}) / 2{\rm K}_{\rm S}^{0}$, $(\Omega^{-} + \Omega^{+}) / (\Lambda + \overline{\Lambda})$ and $(\Omega^{-} + \Omega^{+}) / (\Xi^{-} + \Xi^{+})$ ratios in jets in MB p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of inclusive ${\rm K}_{\rm S}^{0}$ and $\Lambda$ ($\overline{\Lambda}$) for $0$-$10\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential densities of ${\rm K}_{\rm S}^{0}$ and $\Lambda$ ($\overline{\Lambda}$) in jets and the underlying event for $0$-$10\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of inclusive $\Xi^{\pm}$ for $0$-$10\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of $\Xi^{\pm}$ in jets and the underlying event for $0$-$10\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of inclusive ${\rm K}_{\rm S}^{0}$ and $\Lambda$ ($\overline{\Lambda}$) for $10$-$40\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential densities of ${\rm K}_{\rm S}^{0}$ and $\Lambda$ ($\overline{\Lambda}$) in jets and the underlying event for $10$-$40\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of inclusive $\Xi^{\pm}$ for $10$-$40\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of $\Xi^{\pm}$ in jets and the underlying event for $10$-$40\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of inclusive ${\rm K}_{\rm S}^{0}$ and $\Lambda$ ($\overline{\Lambda}$) for $40$-$100\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential densities of ${\rm K}_{\rm S}^{0}$ and $\Lambda$ ($\overline{\Lambda}$) in jets and the underlying event for $40$-$100\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of inclusive $\Xi^{\pm}$ for $40$-$100\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential density of $\Xi^{\pm}$ in jets and the underlying event for $40$-$100\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Lambda + \overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ ratio of inclusive particles for various event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Lambda + \overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ ratio in the underlying event for various event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Lambda + \overline{\Lambda})/2{\rm K}_{\rm S}^{0}$ ratio in jets for various event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / 2{\rm K}_{\rm S}^{0}$ ratio of inclusive particles for various event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / 2{\rm K}_{\rm S}^{0}$ ratio in the underlying event for $0$-$10\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / 2{\rm K}_{\rm S}^{0}$ ratio in the underlying event for $10$-$40\%$ and $40$-$100\%$ event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / 2{\rm K}_{\rm S}^{0}$ ratio in jets for various event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / (\Lambda + \overline{\Lambda})$ ratio of inclusive particles for various event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / (\Lambda + \overline{\Lambda})$ ratio in the underlying event for $0$-$10\%$ event activity class in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / (\Lambda + \overline{\Lambda})$ ratio in the underlying event for $10$-$40\%$ and $40$-$100\%$ event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

$p_{\rm T}$-differential $(\Xi^{-} + \Xi^{+}) / (\Lambda + \overline{\Lambda})$ ratio in jets for various event activity classes in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Probability of finding at least one TAR jet, where the p_T-leading TAR jet passes the m_Wcand and D₂^&beta;=1 requirements, as a function of m_s. The probability is determined in a sample of signal events with m_Z'=2100 GeV, with the preselections applied.

Probability of finding a W_had candidate reconstructed as a pair of R=0.4 PFlow jets, as a function of m_s. The probability is determined in a sample of signal events with m_Z'=500 GeV, with the preselections applied that do not pass the requirements of the merged category.

Probability of finding a W_had candidate reconstructed as a pair of R=0.4 PFlow jets, as a function of m_s. The probability is determined in a sample of signal events with m_Z'=1000 GeV, with the preselections applied that do not pass the requirements of the merged category.

Probability of finding a W_had candidate reconstructed as a pair of R=0.4 PFlow jets, as a function of m_s. The probability is determined in a sample of signal events with m_Z'=1700 GeV, with the preselections applied that do not pass the requirements of the merged category.

Probability of finding a W_had candidate reconstructed as a pair of R=0.4 PFlow jets, as a function of m_s. The probability is determined in a sample of signal events with m_Z'=2100 GeV, with the preselections applied that do not pass the requirements of the merged category.

Observed exclusion contour at 95&#37; C.L. for the dark Higgs model in the (m_Z', m_s) plane for g_q=0.25, g_&chi;=1, m_&chi;=200 GeV, and sin&theta;=0.01.

Expected exclusion contour at 95&#37; C.L. for the dark Higgs model in the (m_Z', m_s) plane for g_q=0.25, g_&chi;=1, m_&chi;=200 GeV, and sin&theta;=0.01.

Expected+1&sigma; exclusion contour at 95&#37; C.L. for the dark Higgs model in the (m_Z', m_s) plane for g_q=0.25, g_&chi;=1, m_&chi;=200 GeV, and sin&theta;=0.01.

Expected-1&sigma; exclusion contour at 95&#37; C.L. for the dark Higgs model in the (m_Z', m_s) plane for g_q=0.25, g_&chi;=1, m_&chi;=200 GeV, and sin&theta;=0.01.

Expected+2&sigma; exclusion contour at 95&#37; C.L. for the dark Higgs model in the (m_Z', m_s) plane for g_q=0.25, g_&chi;=1, m_&chi;=200 GeV, and sin&theta;=0.01.

Expected-2&sigma; exclusion contour at 95&#37; C.L. for the dark Higgs model in the (m_Z', m_s) plane for g_q=0.25, g_&chi;=1, m_&chi;=200 GeV, and sin&theta;=0.01.

Observed upper limits at 95&#37; C.L. on &sigma;(pp &rarr; s &chi;&chi;) &times; B(s &rarr; W^&pm; W^&mp;) for m_Z'=0.5 TeV as a function of m_s. The expected limits, varied up and down by one and two standard deviations, are shown as green and yellow bands, respectively. The observed and expected limits are compared to the theoretical LO cross section for the &sigma;(pp &rarr; s &chi;&chi;) &times; B(s &rarr; W^&pm; W^&mp;) process for m_Z'=0.5 TeV, shown in dashed blue.

Observed upper limits at 95&#37; C.L. on &sigma;(pp &rarr; s &chi;&chi;) &times; B(s &rarr; W^&pm; W^&mp;) for m_Z'=1 TeV as a function of m_s. The expected limits, varied up and down by one and two standard deviations, are shown as green and yellow bands, respectively. The observed and expected limits are compared to the theoretical LO cross section for the &sigma;(pp &rarr; s &chi;&chi;) &times; B(s &rarr; W^&pm; W^&mp;) process for m_Z'=1 TeV, shown in dashed blue.

Observed upper limits at 95&#37; C.L. on &sigma;(pp &rarr; s &chi;&chi;) &times; B(s &rarr; W^&pm; W^&mp;) for m_Z'=1.7 TeV as a function of m_s. The expected limits, varied up and down by one and two standard deviations, are shown as green and yellow bands, respectively. The observed and expected limits are compared to the theoretical LO cross section for the &sigma;(pp &rarr; s &chi;&chi;) &times; B(s &rarr; W^&pm; W^&mp;) process for m_Z'=1.7 TeV, shown in dashed blue.

Observed upper limits at 95&#37; C.L. on &sigma;(pp &rarr; s &chi;&chi;) &times; B(s &rarr; W^&pm; W^&mp;) for m_Z'=2.1 TeV as a function of m_s. The expected limits, varied up and down by one and two standard deviations, are shown as green and yellow bands, respectively. The observed and expected limits are compared to the theoretical LO cross section for the &sigma;(pp &rarr; s &chi;&chi;) &times; B(s &rarr; W^&pm; W^&mp;) process for m_Z'=2.1 TeV, shown in dashed blue.

Data overlaid on SM background yields stacked in each SR and CR category after the fit to data ('Post-fit'). The yields in the SR are broken down into their contributions to the individual bins. The maximum-likelihood estimators are set to the conditional values of the CR-only fit, and propagated to SR and CRs.

Dominant sources of uncertainty for three dark Higgs scenarios after the fit to data. The uncertainties are quantified in terms of their contribution to the fitted signal uncertainty that is expressed relative to the theory prediction. Three representative dark Higgs signal scenarios with g_q=0.25, g_&chi;=1.0, sin&theta;=0.01 and m_&chi;=200 GeV are considered, which are indicated using the (m_Z', m_s) format in units of GeV in the table columns.

Cumulative efficiencies in the merged category for three representative dark Higgs signal scenarios with g_q=0.25, g_&chi;=1.0, sin&theta;=0.01, m_Z' = 1 TeV, and m_&chi;=200 GeV considering s&rarr;W(&ell;&nu;)W(qq) decays only.

Cumulative efficiencies in the resolved category for three representative dark Higgs signal scenarios with g_q=0.25, g_&chi;=1.0, sin&theta;=0.01, m_Z' = 1 TeV, and m_&chi;=200 GeV considering s&rarr;W(&ell;&nu;)W(qq) decays only.

Theoretical cross section for &sigma;(pp &rarr; s&chi;&chi;) &times; B(s &rarr; W^&plusmn;W^&#8723;) for each of the dark Higgs signal points at m_Z′ ={300, 350, 400, 500, 750} GeV, with g_q = 0.25, g<sub>&chi; = 1.0, sin&theta; = 0.01, m_Z′ = 1 TeV , and m_&chi; = 200 GeV. Also shown are experimentally excluded cross sections of &sigma;(pp &rarr; s&chi;&chi;) &times; B(s &rarr; W^&plusmn;W^&#8723;) (Obs.) together with the expectations (Exp.) varied up and down by one standard deviation (&plusmn;1&sigma;).

Theoretical cross section for &sigma;(pp &rarr; s&chi;&chi;) &times; B(s &rarr; W^&plusmn;W^&#8723;) for each of the dark Higgs signal points at m_Z′ ={1000, 1700} GeV, with g_q = 0.25, g<sub>&chi; = 1.0, sin&theta; = 0.01, m_Z′ = 1 TeV , and m_&chi; = 200 GeV. Also shown are experimentally excluded cross sections of &sigma;(pp &rarr; s&chi;&chi;) &times; B(s &rarr; W^&plusmn;W^&#8723;) (Obs.) together with the expectations (Exp.) varied up and down by one standard deviation (&plusmn;1&sigma;).

Theoretical cross section for &sigma;(pp &rarr; s&chi;&chi;) &times; B(s &rarr; W^&plusmn;W^&#8723;) for each of the dark Higgs signal points at m_Z′ ={2100, 2500, 2900, 3300} GeV, with g_q = 0.25, g<sub>&chi; = 1.0, sin&theta; = 0.01, m_Z′ = 1 TeV , and m_&chi; = 200 GeV. Also shown are experimentally excluded cross sections of &sigma;(pp &rarr; s&chi;&chi;) &times; B(s &rarr; W^&plusmn;W^&#8723;) (Obs.) together with the expectations (Exp.) varied up and down by one standard deviation (&plusmn;1&sigma;).

The unfolded differential charge asymmetry as a function of the transverse momentum of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.

The unfolded differential charge asymmetry as a function of the longitudinal boost of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.

The unfolded inclusive leptonic asymmetry. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the invariant mass of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the transverse momentum of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the longitudinal boost of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\bar{t}}$ inclusive measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.

Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ < 500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [500,750] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [750,1000] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [1000,1500] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ > 1500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ < 30 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ $\in$ [30,120] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ > 120 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ < 200 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ $\in$ [200,300] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ $\in$ [300,400] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ > 400 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ < 20 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ $\in$ [20, 70] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ > 70 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ inclusive measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ inclusive measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement.

Covariance matrix for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement.

Covariance matrix for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement.

Covariance matrix for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement.

Ratio of $p_{\mathrm{T,ch\ jet}}$-differential cross section of charm jets tagged with $\mathrm{D^{0}}$ mesons for different $R$: $\sigma(R=0.2)/\sigma(R=0.4)$ and $\sigma(R=0.2)/\sigma(R=0.6)$ in pp collisions at $\sqrt{s}=13$ TeV.

Ratio of $p_{\mathrm{T,ch\ jet}}$-differential cross section of charm jets tagged with $\mathrm{D^{0}}$ mesons for different $R$: $\sigma(R=0.2)/\sigma(R=0.4)$ and $\sigma(R=0.2)/\sigma(R=0.6)$ in pp collisions at $\sqrt{s}=5.02$ TeV.

The fraction of $\mathrm{D^{0}}$ jets over inclusive charged-particle jets in pp collisions at $\sqrt{s}=5.02$ TeV for $R=0.2$, $0.4$, and $0.6$.

Distributions of $z^{\mathrm{ch}}_{||}$-differential yield of charm jets tagged with $\mathrm{D^{0}}$ mesons normalised by the number of $\mathrm{D^{0}}$ jets within each distribution in pp collisions at $\sqrt{s}=13$ TeV in four jet-$p_{\mathrm{T}}$ intervals $5<p_{\mathrm{T,ch\ jet}}<7$ GeV/$c$, $7<p_{\mathrm{T,ch\ jet}}<10$ GeV/$c$, $10<p_{\mathrm{T,ch\ jet}}<15$ GeV/$c$, and $15<p_{\mathrm{T,ch\ jet}}<50$ GeV/$c$ for jet radii $R=0.2$, $0.4$, and $0.6$.

Distributions of $z^{\mathrm{ch}}_{||}$-differential yield of charm jets tagged with $\mathrm{D^{0}}$ mesons normalised by the number of $\mathrm{D^{0}}$ jets within each distribution in pp collisions at $\sqrt{s}=5.02$ TeV in four jet-$p_{\mathrm{T}}$ intervals $5<p_{\mathrm{T,ch\ jet}}<7$ GeV/$c$, $7<p_{\mathrm{T,ch\ jet}}<10$ GeV/$c$, $10<p_{\mathrm{T,ch\ jet}}<15$ GeV/$c$, and $15<p_{\mathrm{T,ch\ jet}}<50$ GeV/$c$ for jet radii $R=0.2$, $0.4$, and $0.6$.

$p_{\mathrm{T,ch\ jet}}$-differential cross section of charm jets tagged with $\mathrm{D^{0}}$ mesons for $R=0.3$ in pp collisions at $\sqrt{s}=5.02$ TeV.

The fraction of $\mathrm{D^{0}}$ jets over inclusive charged-particle jets in pp collisions at $\sqrt{s}=5.02$ TeV for $R=0.3$.

Distributions of $z^{\mathrm{ch}}_{||}$-differential yield of charm jets tagged with $\mathrm{D^{0}}$ mesons normalised by the number of $\mathrm{D^{0}}$ jets within each distribution in pp collisions at $\sqrt{s}=5.02$ TeV in four jet-$p_{\mathrm{T}}$ intervals $5<p_{\mathrm{T,ch\ jet}}<7$ GeV/$c$, $7<p_{\mathrm{T,ch\ jet}}<10$ GeV/$c$, $10<p_{\mathrm{T,ch\ jet}}<15$ GeV/$c$, and $15<p_{\mathrm{T,ch\ jet}}<50$ GeV/$c$ for jet radius $R=0.3$.

Ratio of measured PSI(2S) over J/PSI(1S) cross section in charged-particle multiplicity intervals and integrated in multiplicity.

Ratio of measured PSI(2S) over J/PSI(1S) cross section in charged-particle multiplicity intervals and integrated in multiplicity.

Ratio of measured PSI(2S) over J/PSI(1S) cross section in charged-particle multiplicity intervals and integrated in multiplicity.