cross section as a function of $(T_{\mu}, \cos\theta_{\mu})$, where $T_{\mu}$ is the kinetic energy of the outgoing muon and $\theta_{\mu}$ is the angle between the incoming neutrino and outgoing muon. Differential cross sections were also released as a function of [$Q^{2}_{\textrm{QE}}$]{}or ${\ensuremath{E_{\nu}}\xspace}^{\mathrm{QE \; RFG}}$, but the double-differential result was preferred as it is contains the most information and has minimal model dependence. The [MiniBooNE]{}data release included central values for each bin and the diagonal elements of the shape-only covariance matrix; correlations between bins were not released. Additionally, the overall normalization uncertainly was given as 10.7% for neutrino running.

The [MiniBooNE]{}CCQE cross sections are released as both CCQE-corrected, and CCQE-like measurements. The CCQE-like sample is obtained by selecting events in which a muon was detected with no pions, but no requirement was made on the proton. The CCQE-corrected measurement is produced by subtracting background events (where the primary interaction was not CCQE) based on the NUANCE [@nuanceMC] generator prediction. The dominant background is CC1$\pi^{+}$, and a dedicated sample was used to tune the NUANCE prediction which was used in the background subtraction. It should be noted that the NUANCE CC1$\pi^{+}$ simulation included $\pi$-less $\Delta$ decay. The published signal purity for the 