$M_{\tau}$ distribution in signal region, (OS$\mu$, Belle II)

$M_{\tau}$ distribution in signal region, (SS$e$, Belle)

$M_{\tau}$ distribution in signal region, (SS$e$, Belle II)

$M_{\tau}$ distribution in signal region, (SS$\mu$, Belle)

$M_{\tau}$ distribution in signal region, (SS$\mu$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$ and $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (OS$e$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$ and $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (OS$e$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$ and $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (OS$\mu$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$ and $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (OS$\mu$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$ and $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (SS$e$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$ and $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (SS$e$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$ and $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (SS$\mu$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$ and $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (SS$\mu$, Belle II)

Efficiency as function the helicity angle of the kaon $\cos\theta_{K}$, and the helicity angle of the lepton $\cos\theta_{\ell}$ in bin e the four-momentum-transfer $q^{2}$, (OS$e$, Belle)

Efficiency as function the helicity angle of the kaon $\cos\theta_{K}$, and the helicity angle of the lepton $\cos\theta_{\ell}$ in bin e the four-momentum-transfer $q^{2}$, (OS$e$, Belle II)

Efficiency as function the helicity angle of the kaon $\cos\theta_{K}$, and the helicity angle of the lepton $\cos\theta_{\ell}$ in bin e the four-momentum-transfer $q^{2}$, (OS$\mu$, Belle)

Efficiency as function the helicity angle of the kaon $\cos\theta_{K}$, and the helicity angle of the lepton $\cos\theta_{\ell}$ in bin e the four-momentum-transfer $q^{2}$, (OS$\mu$, Belle II)

Efficiency as function the helicity angle of the kaon $\cos\theta_{K}$, and the helicity angle of the lepton $\cos\theta_{\ell}$ in bin e the four-momentum-transfer $q^{2}$, (SS$e$, Belle)

Efficiency as function the helicity angle of the kaon $\cos\theta_{K}$, and the helicity angle of the lepton $\cos\theta_{\ell}$ in bin e the four-momentum-transfer $q^{2}$, (SS$e$, Belle II)

Efficiency as function the helicity angle of the kaon $\cos\theta_{K}$, and the helicity angle of the lepton $\cos\theta_{\ell}$ in bin e the four-momentum-transfer $q^{2}$, (SS$\mu$, Belle)

Efficiency as function the helicity angle of the kaon $\cos\theta_{K}$, and the helicity angle of the lepton $\cos\theta_{\ell}$ in bin e the four-momentum-transfer $q^{2}$, (SS$\mu$, Belle II)

Efficiency as function of the helicity angle of the kaon $\cos\theta_{K}$, (OS$e$, Belle)

Efficiency as function of the helicity angle of the kaon $\cos\theta_{K}$, (OS$e$, Belle II)

Efficiency as function of the helicity angle of the kaon $\cos\theta_{K}$, (OS$\mu$, Belle)

Efficiency as function of the helicity angle of the kaon $\cos\theta_{K}$, (OS$\mu$, Belle II)

Efficiency as function of the helicity angle of the kaon $\cos\theta_{K}$, (SS$e$, Belle)

Efficiency as function of the helicity angle of the kaon $\cos\theta_{K}$, (SS$e$, Belle II)

Efficiency as function of the helicity angle of the kaon $\cos\theta_{K}$, (SS$\mu$, Belle)

Efficiency as function of the helicity angle of the kaon $\cos\theta_{K}$, (SS$\mu$, Belle II)

Efficiency as function of the helicity angle of the lepton $\cos\theta_{\ell}$, (OS$e$, Belle)

Efficiency as function of the helicity angle of the lepton $\cos\theta_{\ell}$, (OS$e$, Belle II)

Efficiency as function of the helicity angle of the lepton $\cos\theta_{\ell}$, (OS$\mu$, Belle)

Efficiency as function of the helicity angle of the lepton $\cos\theta_{\ell}$, (OS$\mu$, Belle II)

Efficiency as function of the helicity angle of the lepton $\cos\theta_{\ell}$, (SS$e$, Belle)

Efficiency as function of the helicity angle of the lepton $\cos\theta_{\ell}$, (SS$e$, Belle II)

Efficiency as function of the helicity angle of the lepton $\cos\theta_{\ell}$, (SS$\mu$, Belle)

Efficiency as function of the helicity angle of the lepton $\cos\theta_{\ell}$, (SS$\mu$, Belle II)

Efficiency as function of the acoplanarity angle $\phi$, (OS$e$, Belle)

Efficiency as function of the acoplanarity angle $\phi$, (OS$e$, Belle II)

Efficiency as function of the acoplanarity angle $\phi$, (OS$\mu$, Belle)

Efficiency as function of the acoplanarity angle $\phi$, (OS$\mu$, Belle II)

Efficiency as function of the acoplanarity angle $\phi$, (SS$e$, Belle)

Efficiency as function of the acoplanarity angle $\phi$, (SS$e$, Belle II)

Efficiency as function of the acoplanarity angle $\phi$, (SS$\mu$, Belle)

Efficiency as function of the acoplanarity angle $\phi$, (SS$\mu$, Belle II)

Efficiency as function of the four-momentum-transfer $q^{2}$, (OS$e$, Belle)

Efficiency as function of the four-momentum-transfer $q^{2}$, (OS$e$, Belle II)

Efficiency as function of the four-momentum-transfer $q^{2}$, (OS$\mu$, Belle)

Efficiency as function of the four-momentum-transfer $q^{2}$, (OS$\mu$, Belle II)

Efficiency as function of the four-momentum-transfer $q^{2}$, (SS$e$, Belle)

Efficiency as function of the four-momentum-transfer $q^{2}$, (SS$e$, Belle II)

Efficiency as function of the four-momentum-transfer $q^{2}$, (SS$\mu$, Belle)

Efficiency as function of the four-momentum-transfer $q^{2}$, (SS$\mu$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$, (OS$e$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$, (OS$e$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$, (OS$\mu$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$, (OS$\mu$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$, (SS$e$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$, (SS$e$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$, (SS$\mu$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}\ell)$, (SS$\mu$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (OS$e$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (OS$e$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (OS$\mu$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (OS$\mu$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (SS$e$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (SS$e$, Belle II)

Efficiency as function of the invariant mass squared $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (SS$\mu$, Belle)

Efficiency as function of the invariant mass squared $m^2(K^{*0}t_{\tau})$, where $t_{\tau}$ is the track from the $\tau$, (SS$\mu$, Belle II)

Corrected Yield R=0.5 pi0+jet 15-20 pp at sqrt{s_{NN}}=200 GeV

Corrected Yield R=0.2 gamma+jet 10-15 pp at sqrt{s_{NN}}=200 GeV

Corrected Yield R=0.5 gamma+jet 10-15 pp at sqrt{s_{NN}}=200 GeV

Corrected Yield R=0.5 pi0+jet 10-15 AuAu 0-15% at sqrt{s_{NN}}=200 GeV

Corrected Yield R=0.2 pi0+jet 10-15 AuAu 0-15% at sqrt{s_{NN}}=200 GeV

Corrected Yield R=0.5 pi0+jet 15-20 AuAu 0-15% at sqrt{s_{NN}}=200 GeV

Corrected Yield R=0.2 pi0+jet 15-20 AuAu 0-15% at sqrt{s_{NN}}=200 GeV

Corrected Yield R=0.2 gamma+jet 10-15 AuAu 0-15% at sqrt{s_{NN}}=200 GeV

Corrected Yield R=0.5 gamma+jet 10-15 AuAu 0-15% at sqrt{s_{NN}}=200 GeV

IAA(Δφ) R=0.5 gamma+jet 10-15 GeV/c

IAA(Δφ) R=0.2 gamma+jet 10-15 GeV/c

IAA(Δφ) R=0.5 pi0+jet 10-15 GeV/c

IAA(Δφ) R=0.2 pi0+jet 10-15 GeV/c

IAA(Δφ) R=0.5 pi0+jet 15-20 GeV/c

IAA(Δφ) R=0.2 pi0+jet 15-20 GeV/c

Global polarization of $\Lambda$ and $\bar\Lambda$ and their difference in 20-50\% centrality in Ru+Ru collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Global polarization of $\Lambda$ and $\bar\Lambda$ and their difference in 20-50\% centrality in Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Global polarization of $\Lambda$ and $\bar\Lambda$ and their difference in 20-50\% centrality in Ru+Ru&Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Global polarization of $\Lambda$+$\bar\Lambda$ as a function of centrality in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV (left panel). The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.

Global polarization of $\Lambda$+$\bar\Lambda$ in 20-50\% centrality centrality in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV (right panel). The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.

Global polarization of $\Lambda$+$\bar\Lambda$ as a function of the average number of participants $\langle N_{\rm part} \rangle$ in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV. The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.

The transverse momentum dependence of $\Lambda$+$\bar\Lambda$ $P_{\rm H}$ for 20\%-60\% centrality in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV, together with the results for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.

The pseudorapidity dependence of $\Lambda$+$\bar\Lambda$ $P_{\rm H}$ for 20\%-60\% centrality in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV, together with the results for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.

The polarization coefficient $P_{y,c0}$ of $\Lambda\!+\!\bar\Lambda$ from method-1 and method-2 as a function of centrality (left panel) in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV. In this figure, $P_{H}$ is same data as in Figure 4.

The polarization coefficient $P_{y,c0}$ of $\Lambda\!+\!\bar\Lambda$ from method-1 and method-2 for 20-50\% centrality (right panel) in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV. In this figure, $P_{H}$ is same data as in Figure 4.

The polarization coefficient $P_{y,c2}$ of $\Lambda\!+\!\bar\Lambda$ from method-1 and method-2 as a function of centrality (left panel) in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.

The polarization coefficient $P_{y,c2}$ of $\Lambda\!+\!\bar\Lambda$ from method-1 and method-2 for 20-50\% centrality (right panel) in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Global polarization of $\Xi^{-}$+$\bar\Xi^{+}$ from polarization transfer method and direct measurement method as a function of centrality (left panel) in Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV. In this figure, $P_{H}$ of inclusive $\Lambda+\bar\Lambda$ is same data as in Figure 4.

Global polarization of $\Xi^{-}$+$\bar\Xi^{+}$ from polarization transfer method and direct measurement method for 20-50\% centrality (right panel) in Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV . In this figure, $P_{H}$ of inclusive $\Lambda+\bar\Lambda$ is same data as in Figure 4.

The 95% CL limits on the cross-section $\sigma(pp \rightarrow Z' \rightarrow \chi \chi$) times branching ratio B in fb with all statistical and systematic uncertainties, for the $R_{\text{inv}}=$0.6 signal points.

Data yield in the PFN signal region.

Yield of data in the ANTELOPE signal region in the binning used for BumpHunter fitting.

$R_{\rm p}$ vs. $m_{\rm T}$ for $0-10\%$ centrality for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs. $m_{\rm T}$ for $10-30\%$ centrality for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs. $m_{\rm T}$ for $30-50\%$ centrality for Pb-Pb collisions at 5020 GeV.

$R_{\rm N}$ vs. $m_{\rm T}$ for $0-10\%$ centrality for Pb-Pb collisions at 5020 GeV.

$R_{\rm N}$ vs. $m_{\rm T}$ for $10-30\%$ centrality for Pb-Pb collisions at 5020 GeV.

$R_{\rm N}$ vs. $m_{\rm T}$ for $30-50\%$ centrality for Pb-Pb collisions at 5020 GeV.

$R_{\rm d}$ vs. $m_{\rm T}$ for $0-10\%$ centrality for Pb-Pb collisions at 5020 GeV.

$R_{\rm d}$ vs. $m_{\rm T}$ for $10-30\%$ centrality for Pb-Pb collisions at 5020 GeV.

$R_{\rm d}$ vs. $m_{\rm T}$ for $30-50\%$ centrality for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs. '<dN_{ch}/d \eta>^{1/3}' for mT bin 0 for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs. '<dN_{ch}/d \eta>^{1/3}' for mT bin 1 for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs. '<dN_{ch}/d \eta>^{1/3}' for mT bin 2 for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs. '<dN_{ch}/d \eta>^{1/3}' for mT bin 3 for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs. '<dN_{ch}/d \eta>^{1/3}' for mT bin 4 for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs. '<dN_{ch}/d \eta>^{1/3}' for mT bin 5 for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs. '<dN_{ch}/d \eta>^{1/3}' for mT bin 6 for Pb-Pb collisions at 5020 GeV.

$R_{\rm p}$ vs.'<dN_{ch}/d \eta>^{1/3}' for mT bin 7 for Pb-Pb collisions at 5020 GeV.

proton-deuteron (same charge) correlation function for centrality 0-10% from Pb-Pb collisions at 5020 GeV

proton-deuteron (same charge) correlation function for centrality 10-30% from Pb-Pb collisions at 5020 GeV

proton-deuteron (same charge) correlation function for centrality 30-50% from Pb-Pb collisions at 5020 GeV

Signal-selection efficiency as a function of the di-tau invariant mass squared $q^2$ for simulated events in the SR. The error bars indicate the statistical uncertainty.

Observed correlations between the production cross-sections multiplied by the $H \to WW^{\ast}$ branching ratio measured in data for each of the STXS categories.

Values of the negative log likelihood of 2-dimensional $\sigma_{VBF} \times B{H \to WW^{\ast}}$ versus $\sigma_{ggF} \times B_{H \to WW^{\ast}}$ scans.

Observed correlations between the production cross-sections multiplied by the $H \to WW^{\ast}$ branching ratio measured in data for each of the $\textrm{STXS}_\textrm{CP}$ categories.

Expected correlations between the production cross-sections multiplied by the $H \to WW^{\ast}$ branching ratio for each of the $\textrm{STXS}_\textrm{CP}$ categories.

Expected values and uncertainties for the signal strengths measured in each of the $\textrm{STXS}_\textrm{CP}$ categories, normalised to the corresponding SM predictions, for ggH and EW qqH production.

Best-fit values and uncertainties for the signal strengths measured in each of the $\textrm{STXS}_\textrm{CP}$ categories, normalised to the corresponding SM predictions, for ggH and EW qqH production.

The composition of the (orthonormal) eigenvectors defining the rotated basis in terms of operators in the Warsaw basis, labelled in terms of their corresponding Wilson coefficients.

Post-fit DNN distribution for the ggF different flavour 0-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 10\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 0-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 10\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 1-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 60\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 1-jet $60 \leq p_{T}^{\ell\ell, \textrm{miss}} < 120\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 1-jet $120 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 1-jet $200 \leq p_{T}^{\ell\ell, \textrm{miss}} < 300\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 1-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 300\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 2-jet $200 \leq p_{T}^{\ell\ell, \textrm{miss}} < 300\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 300\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF same flavour 2-jet $200 \leq p_{T}^{\ell\ell, \textrm{miss}} < 300\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 300\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 1-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 60\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 1-jet $60 \leq p_{T}^{\ell\ell, \textrm{miss}} < 120\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 1-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 120\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $700 \leq m_{jj} < 1000\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $1000 \leq m_{jj} < 1500\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 1500\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $700 \leq m_{jj} < 1000\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $1000 \leq m_{jj} < 1500\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 1500\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $350 \leq m_{jj} < 1000\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $1000 \leq m_{jj} < 1500\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 1500\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $350 \leq m_{jj} < 1000\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $1000 \leq m_{jj} < 1500\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the VBF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 1500\ \textrm{GeV}$ signal region; the post-fit results are obtained from the 15-POI fit.

Post-fit DNN distribution for the ggF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $-\pi \leq \Delta \phi_{jj}^\pm < - \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $- \frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < 0$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $0 \leq \Delta \phi_{jj}^\pm < \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $\frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < \pi$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $-\pi \leq \Delta \phi_{jj}^\pm < - \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $- \frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < 0$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $0 \leq \Delta \phi_{jj}^\pm < \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $\frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < \pi$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $-\pi \leq \Delta \phi_{jj}^\pm < - \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $- \frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < 0$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $0 \leq \Delta \phi_{jj}^\pm < \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the ggF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $\frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < \pi$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$, $-\pi \leq \Delta \phi_{jj}^\pm < - \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$, $- \frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < 0$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$, $0 \leq \Delta \phi_{jj}^\pm < \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$, $\frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < \pi$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$, $-\pi \leq \Delta \phi_{jj}^\pm < - \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$, $- \frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < 0$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$, $0 \leq \Delta \phi_{jj}^\pm < \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $350 \leq m_{jj} < 700\ \textrm{GeV}$, $\frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < \pi$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 700\ \textrm{GeV}$, $-\pi \leq \Delta \phi_{jj}^\pm < - \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 700\ \textrm{GeV}$, $- \frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < 0$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 700\ \textrm{GeV}$, $0 \leq \Delta \phi_{jj}^\pm < \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 700\ \textrm{GeV}$, $\frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < \pi$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 700\ \textrm{GeV}$, $-\pi \leq \Delta \phi_{jj}^\pm < - \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 700\ \textrm{GeV}$, $- \frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < 0$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 700\ \textrm{GeV}$, $0 \leq \Delta \phi_{jj}^\pm < \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $0 \leq p_{T}^{\ell\ell, \textrm{miss}} < 200\ \textrm{GeV}$, $m_{jj} \geq 700\ \textrm{GeV}$, $\frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < \pi$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 350\ \textrm{GeV}$, $-\pi \leq \Delta \phi_{jj}^\pm < - \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 350\ \textrm{GeV}$, $- \frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < 0$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 350\ \textrm{GeV}$, $0 \leq \Delta \phi_{jj}^\pm < \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF different flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 350\ \textrm{GeV}$, $\frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < \pi$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 350\ \textrm{GeV}$, $-\pi \leq \Delta \phi_{jj}^\pm < - \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 350\ \textrm{GeV}$, $- \frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < 0$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 350\ \textrm{GeV}$, $0 \leq \Delta \phi_{jj}^\pm < \frac{\pi}{2}$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

Post-fit DNN distribution for the VBF same flavour 2-jet $p_{T}^{\ell\ell, \textrm{miss}} \geq 200\ \textrm{GeV}$, $m_{jj} \geq 350\ \textrm{GeV}$, $\frac{\pi}{2} \leq \Delta \phi_{jj}^\pm < \pi$ signal region used in the $\textrm{STXS}_\textrm{CP}$ measurement.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})/v_{0}$ for inclusive charged particles is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 10$–$20% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})/v_{0}$ for inclusive charged particles is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 30$–$40% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})/v_{0}$ for inclusive charged particles is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 60$–$70% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for pions is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 10$–$20% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for kaons is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 10$–$20% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for protons is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 10$–$20% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for pions is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 30$–$40% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for kaons is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 30$–$40% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for protons is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 30$–$40% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for pions is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 60$–$70% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for kaons is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 60$–$70% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for protons is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 60$–$70% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.

The extracted kinetic decoupling temperature is derived from $\pi^{-}$–d correlation functions.

This is the mixed event distribution for $\pi^{+}$–d, required for the fitting

This is the mixed event distribution for $\pi^{-}$–d, required for the fitting

The momentum smearing matrix, required for the fitting, used both for $\pi^{-}$–d and $\pi^{+}$–d