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MicroBooNE and T2K normalized $\nu_\mu$ fluxes.

T2K flux-integrated $\nu_\mu$ CC inclusive double differential cross section per nucleon of carbon as a function of the muon momentum $p_\mu$ calculated in average for different cosine intervals of muon scattering angle $\theta$. The experimental T2K polystyrene data are taken from Ref.~\cite{Abe:2018uhf}. The different contributions to the inclusive cross sections obtained in our approach are shown.

MicroBooNE flux-integrated $\nu_\mu$ CC inclusive double differential cross section on argon per nucleon as a function of the muon momentum $p_\mu$ calculated in average for different cosine intervals of muon scattering angle $\theta$. The experimental MicroBooNE data are taken from Ref.~\cite{Abratenko:2019jqo}. The different contributions to the inclusive cross sections obtained in our model are shown.

Charged current inclusive $\nu_\mu$ cross section on argon per nucleon as a function of the neutrino energy. The experimental MicroBooNE data are taken from Ref.~\cite{MicroBooNE:2021cue}. The genuine quasielastic, the np-nh contributions, the coherent and incoherent 1$\pi$ production as well as the sum of these channels calculated in our RPA model are shown. The genuine quasielastic and the total cross section are shown also when the RPA is switched off.

Charged current inclusive MicroBooNE $\nu_\mu$ flux-integrated single differential cross section on argon per nucleon as a function of the muon energy $E_\mu$. Left panel: the genuine quasielastic, the np-nh contributions, the coherent and incoherent 1$\pi$ production as well as the sum of these channels calculated in our RPA model are shown. Right panel: our total RPA predictions averaged on different bins calculated before (dotted line) and after (continuous line) the additional MicroBooNE smearing explained in the text. The experimental MicroBooNE data and the additional smearing matrix are taken from Ref.~\cite{MicroBooNE:2021cue}

Charged current inclusive MicroBooNE $\nu_\mu$ flux-integrated single differential cross section on argon per nucleon as a function of the muon energy $E_\mu$. Left panel: the genuine quasielastic, the np-nh contributions, the coherent and incoherent 1$\pi$ production as well as the sum of these channels calculated in our RPA model are shown. Right panel: our total RPA predictions averaged on different bins calculated before (dotted line) and after (continuous line) the additional MicroBooNE smearing explained in the text. The experimental MicroBooNE data and the additional smearing matrix are taken from Ref.~\cite{MicroBooNE:2021cue}

MicroBooNE flux-integrated single differential $\nu_\mu$ CC0$\pi$1p cross section on argon as a function of the cosine of the muon scattering angle. The experimental MicroBooNE data are taken from Ref.~\cite{Abratenko:2020acr}. The genuine quasielastic and the np-nh contributions as well as their sum calculated in our model are shown.

Charged current inclusive MicroBooNE $\nu_\mu$ flux-integrated single differential cross section on argon per nucleon as a function of the transferred energy $\omega$. The experimental MicroBooNE data are taken from Ref.~\cite{MicroBooNE:2021cue}. The genuine quasielastic, the np-nh contributions, the coherent and incoherent 1$\pi$ production as well as the sum of these channels calculated in our RPA model are shown. The genuine quasielastic and the total cross section are shown also when the RPA is switched off.

MicroBooNE flux-integrated single differential $\nu_\mu$ CC0$\pi$1p cross section on argon as a function of the muon momentum. Cross sections are shown for the full measured phase-space (left panel) and for events with $\cos \theta < 0.8$ (right panel) The experimental MicroBooNE data are taken from Ref.~\cite{Abratenko:2020acr}. The genuine quasielastic and the np-nh contributions as well as their sum calculated in our model are shown.

Charged current inclusive MicroBooNE $\nu_\mu$ flux-integrated single differential cross section on argon per nucleon as a function of the transferred energy $\omega$ calculated in our model with (left panel) and without (right panel) RPA effects before (dotted lines) and after (continuous lines) the additional MicroBooNE smearing. The experimental MicroBooNE data and the additional smearing matrix are taken from Ref.~\cite{MicroBooNE:2021cue}.

MicroBooNE flux-integrated single differential $\nu_\mu$ CC0$\pi$1p cross section on argon as a function of the muon momentum. Cross sections are shown for the full measured phase-space (left panel) and for events with $\cos \theta < 0.8$ (right panel) The experimental MicroBooNE data are taken from Ref.~\cite{Abratenko:2020acr}. The genuine quasielastic and the np-nh contributions as well as their sum calculated in our model are shown.

Charged current inclusive MicroBooNE $\nu_\mu$ flux-integrated single differential cross section on argon per nucleon as a function of the transferred energy $\omega$ calculated in our model with (left panel) and without (right panel) RPA effects before (dotted lines) and after (continuous lines) the additional MicroBooNE smearing. The experimental MicroBooNE data and the additional smearing matrix are taken from Ref.~\cite{MicroBooNE:2021cue}.

MicroBooNE flux-integrated single differential $\nu_\mu$ CC0$\pi$Np cross section on argon as a function of muon momentum. The experimental MicroBooNE data are taken from Ref.~\cite{Abratenko:2020sga}. The genuine quasielastic and the np-nh contributions as well as their sum calculated in our model are shown.

Charged current quasielastic, multinucleon, coherent and incoherent 1$\pi$ production contributions to the MicroBooNE $\nu_\mu$ flux-integrated single differential cross section on argon per nucleon as a function of the transferred energy $\omega$ calculated in our RPA model (dotted line) and by employing the additional MicroBooNE smearing (continuous line).

MicroBooNE flux-integrated single differential $\nu_\mu$ CC0$\pi$Np \cite{Abratenko:2020sga} and $\nu_\mu$ CC0$\pi$1p \cite{Abratenko:2020acr} cross sections on argon as a function of the muon momentum (left panel) and of the cosine of the muon scattering angle (right panel). The continuous line represents the $\nu_\mu$ CC0$\pi$Np measurement from which we have subtracted our theoretical evaluation of the multinucleon contribution.

MicroBooNE flux-integrated single differential $\nu_\mu$ CC0$\pi$Np \cite{Abratenko:2020sga} and $\nu_\mu$ CC0$\pi$1p \cite{Abratenko:2020acr} cross sections on argon as a function of the muon momentum (left panel) and of the cosine of the muon scattering angle (right panel). The continuous line represents the $\nu_\mu$ CC0$\pi$Np measurement from which we have subtracted our theoretical evaluation of the multinucleon contribution.