  We calculate $pp \to \ell^{+}\nu, \ell^-\bar \nu$ to ${\cal{O}}(1/\Lambda^4)$
within the Standard Model Effective Field Theory (SMEFT) framework. In
particular, we calculate the four-fermion contribution from dimension six and
eight operators, which dominates at large center of mass energy. We explore the
relative size of the $\mathcal O(1/\Lambda^4)$ and $\mathcal O(1/\Lambda^2)$
results for various kinematic regimes and assumptions about the Wilson
coefficients. Results for Drell-Yan production $pp \to \ell^+\ell^-$ at
${\cal{O}}(1/\Lambda^4)$ are also provided. Additionally, we develop the form
for four fermion contact term contributions to $pp \to \ell^{+}\nu, \ell^-\bar
\nu, pp \to \ell^+\ell^-$ of arbitrary mass dimension. This allows us to
estimate the effects from even higher dimensional (dimension $> 8$) terms in
the SMEFT framework.
