The model information is all encoded in the initial state nucleon distribution shown in Figure \[fig:SF\_2D\_distribution\]. Pauli blocking is implemented as a hard cut-off: final state nucleons with momenta less than the Fermi momentum ${\ensuremath{p_{\mathrm{F}}}\xspace}^{\mbox{\scriptsize{SF}}}$ are forbidden. There are two terms in the SF model: a short range correlation term, which extends to higher initial state nucleon momenta, and a mean field term, which contributes the main peak at lower momenta. These terms can be seen in Figure \[fig:SF\_dials\], where the two-dimensional SF in terms of the removal energy and initial state nucleon momentum has been projected on to the momentum axis. There are three parameters in [<span style="font-variant:small-caps;">NEUT</span>]{}which modify the SF as illustrated in Figure \[fig:SF\_dials\]. The default values for these parameters are given in Table \[tab:SF\_params\]. The mean field width and normalization of the correlation term are well-constrained by electron–scattering data [@andy_thesis] and have little effect on the shape or normalization of the cross section. Thus, they are not considered further in this work. Pauli blocking is modified by changing the Fermi momentum in the fits. It should be noted that in the RFG model, the Fermi momentum defines the Pauli blocking, but [*also*]{} modifies the width of 