The measured differential branching fractions as a function of the invariant hadronic mass squared of the $X_u$ system ($M_X^2$).

The measured differential branching fractions as a function of the light-cone momenta of the hadronic $X_u$ system [$P_+ = (E_X^B - |old{p}_X^B|)$].

The measured differential branching fractions as a function of the light-cone momenta of the hadronic $X_u$ system [$P_- = (E_X^B + |old{p}_X^B|)$].

The background-subtracted yields as a function of $E_\ell^B$.

The background-subtracted yields as a function of $q^2$.

The background-subtracted yields as a function of $M_X$.

The background-subtracted yields as a function of $M_X^2$.

The background-subtracted yields as a function of $P_+$. [$P_+ = (E_X^B - |P_X^B|)$]

The background-subtracted yields as a function of $P_-$. [$P_- = (E_X^B + |P_X^B|)$].

The full experimental correlation matrix for the background-subtracted spectrum of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The full experimental correlation matrix for the background-subtracted spectrum of $q^2$).

The full experimental correlation matrix for the background-subtracted spectrum of $M_X$.

The full experimental correlation matrix for the background-subtracted spectrum of $M_X^2$.

The full experimental correlation matrix for the background-subtracted spectrum of $P_+$.

The full experimental correlation matrix for the background-subtracted spectrum of $P_-$.

Migration matrix of $E_\ell^B$ [in %].

Migration matrix of $q^2$ [in %].

Migration matrix of $M_X$ [in %].

Migration matrix of $M_X^2$ [in %].

Migration matrix of $P_+$ [in %].

Migration matrix of $P_-$ [in %].

The total correction factors and phase space acceptance as a function of the invariant hadronic mass of the $X_u$ system ($M_X$).

The total correction factors and phase space acceptance as a function of the invariant hadronic mass squared of the $X_u$ system ($M_X^2$).

The total correction factors and phase space acceptance as a function of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The total correction factors and phase space acceptance as a function of the four-momentum-transfer squared of the $B$ to the $X_u$ system ($q^2$).

The total correction factors and phase space acceptance as a function of $P_+$.

The total correction factors and phase space acceptance as a function of $P_-$.

The statistical correlations of the differential branching fractions are shown. The matrix elements are ordered for $M_{X}$, $M_{X}^{2}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$.

The full experimental (statistical and systematical) correlations of the differential branching fractions are shown. The matrix elements are ordered for $M_{X}$, $M_{X}^{2}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$.

The total partial branching fraction with $E_{\ell}^{B} > 1$ GeV. The order of entries is: the 2D fit result of Phys. Rev. D 104, 012008 (2021), the results calcuated with the differential branching fractions of $M_{X}$, $M_{X}^{2}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$

The full experimental correlations between the total partial branching fractions from summing the individual bins are shown. The matrix elements are saved in the order of $M_{X}$, $M_{X}^{2}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$.

The first moment of the measured differential branching fraction of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The second moment of the measured differential branching fraction of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The third moment of the measured differential branching fraction of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The first moment of the measured differential branching fraction of $q^2$.

The second moment of the measured differential branching fraction of $q^2$.

The third moment of the measured differential branching fraction of $q^2$.

The first moment of the measured differential branching fraction of $M_{X}$.

The second moment of the measured differential branching fraction of $M_{X}$.

The third moment of the measured differential branching fraction of $M_{X}$.

The first moment of the measured differential branching fraction of $P_{+}$.

The second moment of the measured differential branching fraction of $P_{+}$.

The third moment of the measured differential branching fraction of $P_{+}$.

The first moment of the measured differential branching fraction of $P_{-}$.

The second moment of the measured differential branching fraction of $P_{-}$.

The third moment of the measured differential branching fraction of $P_{-}$.

The matrix elements are saved in the order of $M_{X}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$. For each variable, the entries is ordered for the first, second and third moments.

The predicted CC1$\pi^{-}$ background in units of fb/GeV $(10^{-39}~\mbox{cm}^2)/\mbox{GeV}$ . This background corresponds to an empirical adjustment of the Rein-Sehgal calculation based on the MiniBooNE CC1$\pi^{+}$ data.

The MiniBooNE numub single differential cross section $\frac{d\sigma}{dQ^2_{QE}}$ on mineral oil, shape error, and the predicted CCQE-like and CC1$\pi^{-}$ backgrounds in units of fb $(10^{-39} \mbox{cm}^2)$. Not included in the table is the total normalization error of 13.0$\%$.

The MiniBooNE $\bar{\nu}_\mu$ CCQE total cross section on mineral oil, total and shape errors, and predicted CCQE-like and CC1$\pi^{-}$ backgrounds in bins of $E_\nu^{\textrm{QE,RFG}}$ and units of fb $(10^{-39} \mbox{cm}^2)$. The total error includes both the shape and normalization uncertainties. Note that the total error is incorrectly quoted as a power of 10 too low in the paper and the preprint. It is corrected in the resource file from which these data here are taken.

The MiniBooNE $\bar{\nu}_\mu$ CCQE double-differential cross section, with the shape uncertainty, on carbon. The units are fb/GeV $(10^{-39} \mbox{cm}^2/\mbox{GeV})$. Not included in the table is the total normalization uncertainty of 17.4%.

The QE-like $\bar{\nu}_\mu$ background subtracted from the double-differential cross section on carbon. The $\bar{\nu}_\mu$ CCQE interactions with hydrogen are treated as background in this calculation, and so their contribution is included here. The units are fb/GeV $(10^{-39} \mbox{cm}^2/\mbox{GeV})$ .

The MiniBooNE $\bar{\nu}_\mu$ CCQE single differential cross section $\frac{d\sigma}{dQ^2_{QE}}$ on carbon, shape error, and CCQE-like background in units of fb/GeV$^2$ $(10^{-39} \mbox{cm}^2/\mbox{GeV}^2)$ . The $\bar{\nu}_\mu$ CCQE content is treated as background. Not included in the table is the total normalization error of 17.4%.

The MiniBooNE $\bar{\nu}_\mu$ CCQE total cross section on carbon, total and shape errors, and predicted CCQE-like background in bins of $E_\nu^{\textrm{QE,RFG}}$ and units of fb $(10^{-39} \mbox{cm}^2)$. The total error includes both the shape and normalization uncertainties.

Production cross section for two-photon data as a function of W.

Production cross section for two-photon data as a function of W.

Measured production cross section for the E+ E- process as a function of W for Q**2 from 1.2 to 8.5 GeV**2 for the Z-pole data.

Measured production cross section for the E+ E- process as a function of W for Q**2 from 8.8 to 30 GeV**2 for the high energy data.

Measured production cross section cross section for the two photon process as a function of W for Q**2 from 1.2 to 8.5 GeV**2 for the Z-pole data.

Measured production cross section cross section for the two photon process as a function of W for Q**2 from 8.8 to 30 GeV**2 for the high energy data.

Measured production cross section for the two-photon process as a function of W for Q**2 from 1.2 to 8.5 GeV**2 for the Z-pole data.

Measured production cross section for the two-photon process as a function of W for Q**2 from 8.8 to 30 GeV**2 for the high energy data.

Cross sections as a function of W for the lower Q**2, Z pole, data.

Cross sections as a function of W for the high Q**2 data.

Cross sections for the two photon RHO0 RHO0 and non-resonance data for the lower Q**2, Z pole, data.

Cross sections for the two photon RHO0 RHO0 and non-resonance data for the higher Q**2 data.

The two-photon cross section as a function of the photon virtualities Qi**2. H ere Q1 is the virtuality w.r.t the electron vertex, and Q2 w.r.t the positron vertex. Data are given both before and after radiative corrections.

The two-photon cross section as a function of W, the invariant mas of the vir tual GAMMA*GAMMA* system. Data are given both before and after radiative corrections.

The two-photon cross section as a function of LN(W**2/Q1*Q2). Data are given both before and after radiative corrections.