the neutrino mode sample.

[MINER$\nu$A]{}
---------------

The CCQE datasets from [MINER$\nu$A]{}are released as CCQE-corrected single-differential flux-averaged cross section as a function of [$Q^{2}_{\textrm{QE}}$]{}, where the flux has been averaged over the region $1.5 \leq {\ensuremath{E_{\nu}}\xspace}\leq 10$GeV. There is an additional requirement that $1.5 \leq {\ensuremath{E_{\nu}}\xspace}^{\mathrm{QE}} \leq 10$GeV, with ${\ensuremath{E_{\nu}}\xspace}^{\mathrm{QE}}$ as defined in Equation \[eq:ccqe-enuqe\]. Covariance matrices and central values have been released to perform fits to both shape-only and absolutely normalized neutrino and antineutrino datasets. In this work, the absolutely normalized distributions have been used in the fit.

The correction strategy for the [MINER$\nu$A]{}data is to fit the relative normalizations of simulated background distributions to the data in terms of the recoil energy, energy deposited outside a vertex region (the recoil region), and then subtract the predicted background from the CCQE-like sample. The published purity for the neutrino dataset ranges from 65% at low [$Q^{2}_{\textrm{QE}}$]{}to 40% at high [$Q^{2}_{\textrm{QE}}$]{}(with an overall purity of 49%). The purity for the antineutrino dataset is given as 77%. The purity is lower for the neutrino analysis because events with a proton from the initial interaction are more complicated to reconstruct than those with a neutron[^4].

In the [MINER$\nu$A]{}CCQE analyses, the efficiency for selecting events 