Expected exclusion limits at 95% CL on the lifetime and mass of the neutralino in electroweakino pair production models

Expected (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in electroweakino pair production models

Expected (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in electroweakino pair production models

Observed exclusion limits at 95% CL on the lifetime and mass of the neutralino in electroweakino pair production models

Observed (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in electroweakino pair production models

Observed (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in electroweakino pair production models

Expected exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.4 TeV

Expected (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.4 TeV

Expected (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.4 TeV

Observed exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.4 TeV

Observed (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.4 TeV

Observed (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.4 TeV

Exclusion limits at 95% CL on the production cross section in the electroweak pair production model.

Exclusion limits at 95% CL on the production cross section in the strong gluino pair production models and m(gluino)=2.4 TeV

Expected exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.0 TeV

Expected (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.0 TeV

Expected (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.0 TeV

Observed exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.0 TeV

Observed (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.0 TeV

Observed (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.0 TeV

Expected exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.2 TeV

Expected (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.2 TeV

Expected (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.2 TeV

Observed exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.2 TeV

Observed (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.2 TeV

Observed (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the neutralino in strong gluino pair production models and m(gluino)=2.2 TeV

Expected exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=50 GeV

Expected (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=50 GeV

Expected (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=50 GeV

Observed exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=50 GeV

Observed (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=50 GeV

Observed (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=50 GeV

Expected exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=450 GeV

Expected (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=450 GeV

Expected (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=450 GeV

Observed exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=450 GeV

Observed (+1 sigma) exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=450 GeV

Observed (-1 sigma) exclusion limits at 95% CL on the lifetime and mass of the gluino in strong gluino pair production models and m(chi0)=450 GeV

Expected exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.01 ns

Expected (+1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.01 ns

Expected (-1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.01 ns

Observed exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.01 ns

Observed (+1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.01 ns

Observed (-1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.01 ns

Expected exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.1 ns

Expected (+1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.1 ns

Expected (-1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.1 ns

Observed exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.1 ns

Observed (+1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.1 ns

Observed (-1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=0.1 ns

Expected exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=1 ns

Expected (+1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=1 ns

Expected (-1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=1 ns

Observed exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=1 ns

Observed (+1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=1 ns

Observed (-1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=1 ns

Expected exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=10 ns

Expected (+1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=10 ns

Expected (-1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=10 ns

Observed exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=10 ns

Observed (+1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=10 ns

Observed (-1 sigma) exclusion limits at 95% CL on the mass of the gluino and neutralino in strong gluino pair production models and tau(chi0)=10 ns

Exclusion limits at 95% CL on the production cross section in the strong gluino pair production models and m($ ilde{\chi}^0_1$)=1.25 TeV

Acceptance cutflow for the High-pT SR for representative points in the strong gluino pair production model. See additional resources for more information.

Acceptance cutflow for the Trackless SR for representative points in the electroweak pair production model. See additional resources for more information.

Acceptance cutflow for the Trackless SR for representative points in the electroweak pair production model with heavy-flavor quarks final state. See additional resources for more information.

Acceptance cutflow for the High-pT SR for representative points in the electroweak pair production model with heavy-flavor quarks final state. See additional resources for more information.

Reinterpretation Material: Vertex-level Efficiency for R < 22 mm

Reinterpretation Material: Vertex-level Efficiency for R [22, 25] mm

Cutflow (acceptance x efficiency) for the High-pT SR for representative points in the strong gluino pair production model. See additional resources for more information.

Cutflow (acceptance x efficiency) for the Trackless SR for representative points in the electroweak pair production model. See additional resources for more information.

Cutflow (acceptance x efficiency) for the Trackless SR for representative points in the electroweak pair production model with heavy-flavor quarks. See additional resources for more information.

Cutflow (acceptance x efficiency) for the High-pT SR for representative points in the electroweak pair production model with heavy-flavor quarks. See additional resources for more information.

Summary of the impact of the systematic uncertainties on the $t\bar{t}\gamma$ fiducial inclusive cross-section in the single-lepton and dilepton channels and their combination grouped into different categories. The quoted relative uncertainties are obtained by repeating the fit, fixing a set of nuisance parameters of the sources corresponding to each category to their post-fit values, and subtracting in quadrature the resulting uncertainty from the total uncertainty of the nominal fit. The total uncertainty is different from the sum in quadrature of the components due to correlations among nuisance parameters.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(\gamma,b)_{min}$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(\gamma,b)_{min}$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(\gamma,l)$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(\gamma,l)$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(l,j)_{min}$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(l,j)_{min}$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,b)_{min}$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,b)_{min}$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,l)_{min}$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,l)_{min}$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(l,j)_{min}$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(l,j)_{min}$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in the combined fiducial phase space of the single-lepton and dilepton channels as a function of the photon $p_T$. The last bin of the distributions includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in the combined fiducial phase space of the single-lepton and dilepton channels as a function of the photon $p_T$. The last bin of the distributions includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in the combined fiducial phase space of the single-lepton and dilepton channels as a function of the photon $|\eta|$.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in the combined fiducial phase space of the single-lepton and dilepton channels as a function of the photon $|\eta|$.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $p_T(\gamma)$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $p_T(\gamma)$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $|\eta(\gamma)|$.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $|\eta(\gamma)|$.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $p_T(j_1)$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $p_T(j_1)$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(\gamma,b)_{min}$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(\gamma,b)_{min}$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(\gamma,l)$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(\gamma,l)$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(l,j)_{min}$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $\Delta R(l,j)_{min}$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $|\Delta \eta(l,l)|$ . The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $|\Delta \eta(l,l)|$ . The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta \phi(l,l)$ . The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta \phi(l,l)$ . The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $p_T(l,l)$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $p_T(l,l)$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,l_1)$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,l_1)$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,l_2)$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,l_2)$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $p_T(\gamma)$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $p_T(\gamma)$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $|\eta(\gamma)|$.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $|\eta(\gamma)|$.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $p_T(j_1)$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the single-lepton channel as a function of the $p_T(j_1)$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $p_T(\gamma)$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $p_T(\gamma)$. The last bin of the distribution includes the overflow events.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $|\eta(\gamma)|$.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $|\eta(\gamma)|$.

Absolute $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $p_T(j_1)$. The last bin of the distribution includes the overflow events.

Normalised $t\bar{t}\gamma$ production differential cross-sections measured in fiducial phase space in the dilepton channel as a function of the $p_T(j_1)$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $p_T(\gamma)$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $p_T(\gamma)$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $|\eta(\gamma)|$.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $|\eta(\gamma)|$.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $p_T(j_1)$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the single-lepton channel as a function of the $p_T(j_1)$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,b)_{min}$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,b)_{min}$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,l)_{min}$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(\gamma,l)_{min}$. The last bin of the distribution includes the overflow events.

Absolute differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(l,j)_{min}$. The last bin of the distribution includes the overflow events.

Normalised differential cross-section of the total $t\bar{t}\gamma$ production and decay measured in fiducial phase space in the dilepton channel as a function of the $\Delta R(l,j)_{min}$. The last bin of the distribution includes the overflow events.

Observed and expected 68% and 95% credible intervals on $C/\Lambda^2\ [\text{TeV}^{-2} ]$ for the $C_{tW}$ operators and $C_{tB}$ obtained from the $t\bar{t}\gamma$ measurement, comparing the results obtained from the marginalised quadratic fit (‘marg.’) and the independent quadratic fits (‘indep.’). Also shown are the best-fit values (global mode) for each operator.

Observed and expected 68% and 95% credible intervals on $C/\Lambda^2\ [\text{TeV}^{-2} ]$ for the $C_{tW}$ operators and $C_{tB}$ obtained from a combined $t\bar{t}Z$ and $t\bar{t}\gamma$ measurements comparing the results obtained from the marginalised global quadratic fit (‘marg.’) and the independent quadratic fits (‘indep.’). Also shown are the best-fit values (global mode) for each operator.

Contributions of the systematic uncertainties grouped in categories in each bin of the measurement of the absolute $t\bar{t}\gamma$ production differential cross-sections measured in the combined fiducial phase space of the single-lepton and dilepton channels as a function of the photon $p_T$. The relative uncertainties quoted are obtained by repeating the fit, fixing the set of nuisance parameters of the sources corresponding to each category to their post-fit values, and subtracting in quadrature the resulting uncertainty from the total uncertainty of the nominal fit.

Contributions of the systematic uncertainties grouped in categories in each bin of the measurement of the absolute $t\bar{t}\gamma$ production differential cross-sections measured in the combined fiducial phase space of the single-lepton and dilepton channels as a function of the photon $\eta$. The relative uncertainties quoted are obtained by repeating the fit, fixing the set of nuisance parameters of the sources corresponding to each category to their post-fit values, and subtracting in quadrature the resulting uncertainty from the total uncertainty of the nominal fit.

Observed excluded cross-section at 95% CL for the WZ-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production from Fig 8(aux).

Expected exclusion limits at 95% CL for the WZ-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production.

Observed exclusion limits at 95% CL for the Wh-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production from from Fig 13(a) and from Fig 7 and Fig 10(aux).

Observed excluded cross-section at 95% CL for the Wh-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production from Fig 7(aux) and Fig 10(aux).

positive one $\sigma$ observed exclusion limits at 95% CL for the Wh-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production from from Fig 13(a) and from Fig 7 and Fig 10(aux).

negative one $\sigma$ observed exclusion limits at 95% CL for the Wh-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production from from Fig 13(a) and from Fig 7 and Fig 10(aux).

Expected exclusion limits at 95% CL for the Wh-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production.

Expected exclusion limits at 95% CL for the Wh-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production.

Expected exclusion limits at 95% CL for the Wh-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production.

Signal acceptance for $SR^{Wh}_{high-m_{T2} }$ signal region from Fig 11(a)(aux) in a SUSY scenario where direct production of a lightest $\tilde{\chi}^{\pm} _{1} and \tilde{\chi}^{0} _{2}$ , decay with 100% branching ratio to a final state with a same sign light lepton (e or $\mu$) pair and two lightest neutralino1, via the on-shell emission of SM W and Higgs bosons,

Signal acceptance for $SR^{Wh}_{low-m_{T2} }$ signal region from Fig 11(b)(aux) in a SUSY scenario where direct production of a lightest $\tilde{\chi}^{\pm} _{1} and \tilde{\chi}^{0} _{2}$ , decay with 100% branching ratio to a final state with a same sign light lepton (e or $\mu$) pair and two lightest neutralino1, via the on-shell emission of SM W and Higgs bosons,

Signal efficiency for $SR^{Wh}_{high-m_{T2} }$ signal region from Fig 15(a)(aux) in a SUSY scenario where direct production of a lightest $\tilde{\chi}^{\pm} _{1} and \tilde{\chi}^{0} _{2}$ , decay with 100% branching ratio to a final state with a same sign light lepton (e or $\mu$) pair and two lightest neutralino1, via the on-shell emission of SM W and Higgs bosons,

Signal efficiency for $SR^{Wh}_{low-m_{T2} }$ signal region from Fig 15(b)(aux) in a SUSY scenario where direct production of a lightest $\tilde{\chi}^{\pm} _{1} and \tilde{\chi}^{0} _{2}$ , decay with 100% branching ratio to a final state with a same sign light lepton (e or $\mu$) pair and two lightest neutralino1, via the on-shell emission of SM W and Higgs bosons,

Observed 95% X-section upper limits as a function of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ mass in the WZ-mediated simplified model of wino $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ production from Fig 9(aux).

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.65-1.66 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.66-1.67 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.67-1.68 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.68-1.69 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.69-1.7 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.7-1.71 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.71-1.72 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.72-1.73 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.73-1.74 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.74-1.75 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.75-1.76 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.76-1.77 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.77-1.78 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.78-1.79 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.79-1.8 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.8-1.81 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.81-1.82 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.82-1.83 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.83-1.84 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.84-1.85 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.85-1.86 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.86-1.87 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.87-1.88 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.88-1.89 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.89-1.9 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.9-1.91 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.91-1.92 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.92-1.93 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.93-1.94 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.94-1.95 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.96-1.97 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.97-1.98 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.98-1.99 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 1.99-2 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2-2.01 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.01-2.02 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.02-2.03 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.03-2.04 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.04-2.05 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.05-2.06 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.06-2.07 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.07-2.08 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.08-2.09 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.09-2.1 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.1-2.11 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.11-2.12 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.12-2.13 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.13-2.14 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.14-2.15 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.15-2.16 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.16-2.17 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.17-2.18 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.18-2.19 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.19-2.2 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.2-2.21 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.21-2.22 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.22-2.23 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.23-2.24 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.24-2.25 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.25-2.26 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.26-2.27 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.27-2.28 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.28-2.29 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.29-2.3 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.3-2.31 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.31-2.32 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.32-2.33 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.33-2.34 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.34-2.35 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.35-2.36 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.36-2.37 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.37-2.38 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.38-2.39 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.39-2.4 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.4-2.41 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.41-2.42 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.42-2.43 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.43-2.44 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.44-2.45 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.45-2.46 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.46-2.47 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.47-2.48 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.48-2.49 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.49-2.5 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.5-2.51 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.51-2.52 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.52-2.53 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.53-2.54 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.54-2.55 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.55-2.56 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.56-2.57 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.57-2.58 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.58-2.59 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.59-2.6 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.6-2.61 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.61-2.62 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.62-2.63 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.63-2.64 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.64-2.65 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.65-2.66 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.66-2.67 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.67-2.68 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.68-2.69 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.69-2.7 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.7-2.71 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.71-2.72 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.72-2.73 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.75-2.76 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.76-2.77 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.77-2.78 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.78-2.79 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.79-2.8 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.8-2.81 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.81-2.82 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.82-2.83 GeV.

Differential cross section as a function of COS(THETA(K)) for the centre-of-mass range 2.83-2.84 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.62-1.63 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.63-1.64 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.64-1.65 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.65-1.66 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.66-1.67 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.67-1.68 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.68-1.69 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.69-1.7 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.7-1.71 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.71-1.72 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.72-1.73 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.73-1.74 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.74-1.75 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.75-1.76 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.76-1.77 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.77-1.78 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.78-1.79 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.79-1.8 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.8-1.81 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.81-1.82 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.82-1.83 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.83-1.84 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.84-1.85 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.85-1.86 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.86-1.87 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.87-1.88 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.88-1.89 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.89-1.9 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.9-1.91 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.91-1.92 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.92-1.93 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.93-1.94 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.94-1.95 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.95-1.96 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.96-1.97 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.97-1.98 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.98-1.99 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 1.99-2 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2-2.01 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.01-2.02 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.02-2.03 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.03-2.04 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.04-2.05 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.05-2.06 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.06-2.07 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.07-2.08 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.08-2.09 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.09-2.1 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.1-2.11 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.11-2.12 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.12-2.13 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.13-2.14 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.14-2.15 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.15-2.16 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.16-2.17 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.17-2.18 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.18-2.19 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.19-2.2 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.2-2.21 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.21-2.22 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.22-2.23 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.23-2.24 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.24-2.25 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.25-2.26 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.26-2.27 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.27-2.28 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.28-2.29 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.29-2.3 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.3-2.31 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.31-2.32 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.32-2.33 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.33-2.34 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.34-2.35 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.35-2.36 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.36-2.37 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.37-2.38 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.38-2.39 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.39-2.4 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.4-2.41 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.41-2.42 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.42-2.43 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.43-2.44 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.44-2.45 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.45-2.46 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.46-2.47 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.47-2.48 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.48-2.49 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.49-2.5 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.5-2.51 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.51-2.52 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.52-2.53 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.53-2.54 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.54-2.55 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.55-2.56 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.56-2.57 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.57-2.58 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.58-2.59 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.59-2.6 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.6-2.61 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.61-2.62 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.62-2.63 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.63-2.64 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.64-2.65 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.65-2.66 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.66-2.67 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.67-2.68 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.68-2.69 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.69-2.7 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.7-2.71 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.71-2.72 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.72-2.73 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.73-2.74 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.74-2.75 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.75-2.76 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.76-2.77 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.77-2.78 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.78-2.79 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.79-2.8 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.8-2.81 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.81-2.82 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.82-2.83 GeV.

Polarization(LAMBDA) as a function of COS(THETA(K)) for the centre-of-mass range 2.83-2.84 GeV.

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