90% CL upper limit in axion-like particle coupling to SM fermions at UV scale Lambda=1TeV vs mass parameter space for di-lepton final states.

90% CL upper limit in axion-like particle coupling to SM gluons at UV scale Lambda=1TeV vs mass parameter space for hadronic final states.

Number of expected $a \to K^+K^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in B meson decays assuming production coupling $C_{bs}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\eta$ events for BR = 1 in the plane (mass, width) after full selection, for production in B meson decays assuming production coupling $C_{bs}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\gamma$ events for BR = 1 in the plane (mass, width) after full selection, for production in B meson decays assuming production coupling $C_{bs}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in B meson decays assuming production coupling $C_{bs}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in B meson decays assuming production coupling $C_{bs}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to e^+e^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\pi^0$ assuming production coupling $\theta_{\pi^0} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \mu^+\mu^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\pi^0$ assuming production coupling $\theta_{\pi^0} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to K^+K^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\pi^0$ assuming production coupling $\theta_{\pi^0} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\eta$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\pi^0$ assuming production coupling $\theta_{\pi^0} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\gamma$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\pi^0$ assuming production coupling $\theta_{\pi^0} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\pi^0$ assuming production coupling $\theta_{\pi^0} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\pi^0$ assuming production coupling $\theta_{\pi^0} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to e^+e^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta$ assuming production coupling $\theta_{\eta} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \mu^+\mu^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta$ assuming production coupling $\theta_{\eta} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to K^+K^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta$ assuming production coupling $\theta_{\eta} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\eta$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta$ assuming production coupling $\theta_{\eta} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\gamma$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta$ assuming production coupling $\theta_{\eta} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta$ assuming production coupling $\theta_{\eta} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta$ assuming production coupling $\theta_{\eta} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to e^+e^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta^\prime$ assuming production coupling $\theta_{\eta^\prime} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \mu^+\mu^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta^\prime$ assuming production coupling $\theta_{\eta^\prime} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to K^+K^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta^\prime$ assuming production coupling $\theta_{\eta^\prime} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\eta$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta^\prime$ assuming production coupling $\theta_{\eta^\prime} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\gamma$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta^\prime$ assuming production coupling $\theta_{\eta^\prime} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta^\prime$ assuming production coupling $\theta_{\eta^\prime} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in mixing with $\eta^\prime$ assuming production coupling $\theta_{\eta^\prime} = 1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to e^+e^-$ events for BR = 1 in the plane (mass, width) after full selection, for Primakoff production assuming production coupling $C_{\gamma\gamma}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \mu^+\mu^-$ events for BR = 1 in the plane (mass, width) after full selection, for Primakoff production assuming production coupling $C_{\gamma\gamma}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to K^+K^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for Primakoff production assuming production coupling $C_{\gamma\gamma}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\eta$ events for BR = 1 in the plane (mass, width) after full selection, for Primakoff production assuming production coupling $C_{\gamma\gamma}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\gamma$ events for BR = 1 in the plane (mass, width) after full selection, for Primakoff production assuming production coupling $C_{\gamma\gamma}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for Primakoff production assuming production coupling $C_{\gamma\gamma}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $a \to \pi^+\pi^-\pi^0\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for Primakoff production assuming production coupling $C_{\gamma\gamma}/\Lambda=1\,\mathrm{GeV}^{-1}$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to e^+e^-$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \mu^+\mu^-$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to K^+K^-$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to K^+K^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \pi^+\pi^-$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \pi^+\pi^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \pi^+\pi^-\pi^0\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to e^+e^-$ events for BR = 1 in the plane (mass, width) after full selection, for mixing production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \mu^+\mu^-$ events for BR = 1 in the plane (mass, width) after full selection, for mixing production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to K^+K^-$ events for BR = 1 in the plane (mass, width) after full selection, for mixing production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to K^+K^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for mixing production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \pi^+\pi^-$ events for BR = 1 in the plane (mass, width) after full selection, for mixing production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \pi^+\pi^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for mixing production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \pi^+\pi^-\pi^0\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for mixing production assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to e^+e^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in light meson decays assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \mu^+\mu^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in light meson decays assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \pi^+\pi^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in light meson decays assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \pi^+\pi^-\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in light meson decays assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $A^\prime \to \pi^+\pi^-\pi^0\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for production in light meson decays assuming production coupling $\varepsilon=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $S \to e^+e^-$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\mathrm{sin}^2\theta=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $S \to \mu^+\mu^-$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\mathrm{sin}^2\theta=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $S \to K^+K^-$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\mathrm{sin}^2\theta=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $S \to \pi^+\pi^-$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\mathrm{sin}^2\theta=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $S \to \pi^+\pi^-\pi^0\pi^0$ events for BR = 1 in the plane (mass, width) after full selection, for Bremsstrahlung production assuming production coupling $\mathrm{sin}^2\theta=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $S \to e^+e^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in B meson decays assuming production coupling $\mathrm{sin}^2\theta=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $S \to \mu^+\mu^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in B meson decays assuming production coupling $\mathrm{sin}^2\theta=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $S \to K^+K^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in B meson decays assuming production coupling $\mathrm{sin}^2\theta=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

Number of expected $S \to \pi^+\pi^-$ events for BR = 1 in the plane (mass, width) after full selection, for production in B meson decays assuming production coupling $\mathrm{sin}^2\theta=1$. Acceptance for particles that reach the FV and decay therein and mass resolution.

90% CL upper limit in dark photon coupling vs mass parameter space for the $A^\prime \rightarrow l^+l^-$ analysis.

90% CL upper limit in $BR(B \rightarrow K a, a \rightarrow e^+e^-)$ vs lifetime $\tau$ parameter space.

90% CL upper limit in $BR(B \rightarrow K a, a \rightarrow e^+e^-)$ vs lifetime $\tau$ parameter space.

Upper limits at 90% CL of $B(K^+\to\pi^+a)\times B(a\to\gamma\gamma)$ in the prompt ALP decay assumption.

See caption of Figure 9.

See caption of Figure 9.

See caption of Figure 9.

See caption of Figure 9.

See caption of Figure 9.

See caption of Figure 9.

Measurement of F2 at X = 0.125.

Measurement of F2 at X = 0.175.

Measurement of F2 at X = 0.225.

Measurement of F2 at X = 0.275.

Measurement of F2 at X = 0.350.

Measurement of F2 at X = 0.450.

Measurement of F2 at X = 0.550.

Measurement of F2 at X = 0.650.

Measurement of F2 at X = 0.750.

Measurement of XF3 at X = 0.015.

Measurement of XF3 at X = 0.045.

Measurement of XF3 at X = 0.080.

Measurement of XF3 at X = 0.125.

Measurement of XF3 at X = 0.175.

Measurement of XF3 at X = 0.225.

Measurement of XF3 at X = 0.275.

Measurement of XF3 at X = 0.350.

Measurement of XF3 at X = 0.450.

Measurement of XF3 at X = 0.550.

Measurement of XF3 at X = 0.650.

Measurement of XF3 at X = 0.750.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Measured values of the electron-proton elastic cross section for beam energy 3.114 GeV.

Measured values of the electron-proton elastic cross section for beam energy 4.104 GeV.

Measured values of the electron-proton elastic cross section for beam energy 4.413 GeV.

Measured values of the electron-proton elastic cross section for beam energy 5.494 GeV.

Measured inclusive jet differential cross section as a function of PT for the absolute rapidity range 1.1 to 1.6 with the jet resolution parameter D = 0.7.

Measured inclusive jet differential cross section as a function of PT for the absolute rapidity range 1.6 to 2.1 with the jet resolution parameter D = 0.7.

Measured inclusive jet differential cross section as a function of PT for the absolute rapidity range 0.1 TO 0.7 with the jet resolution parameter D = 0.5.

Measured inclusive jet differential cross section as a function of PT for the absolute rapidity range 0.1 TO 0.7 with the jet resolution parameter D = 1.0.

ET distribution for generic jets.

Pseudorapidity (YRAP) distribution for generic jets.

ET distribution for jets tagged as B-jets.

Pseudorapidity (YRAP) distribution for jets tagged as B-jets.