“…The differences amount ∼ 1.5% (∼ 5.7%) for ν µ (ν µ ) that is (especially in antineutrino case) above the statistical error of the fit and is caused mainly by uncertainties in the energy spectra of ν µ and ν µ and, in lesser extent, in the nuclear effects. Figures 2 and 3 show a compilation of the available data on the total QES cross sections for the following nuclear targets: hydrogen [24], deuterium [15-18, 25, 35, 60], carbon [64], aluminium [66,68,70,71], argon [63], iron [40], steel [13], propane [46], freon [43,48,51,53,65,73,74,111], and also propane-freon [55,58,59] and neonhydrogen [36,37,39] mixtures. The recent MiniBooNE 2007 datapoint [5] (carbon target) estimated from the reported value of M A is also shown in Fig.…”