&& + [|u]{}\^i\_[R]{} Y\^[  j]{}\_[U i]{} Q\_[L j]{} S + [|d]{}\^i\_[R]{} Y\^[  j]{}\_[D i]{} Q\_[L j]{} S\^+[h.c.]{} where flavour indicies $i,j$ are shown and color and $ SU(2)_L$ indices have been suppressed. [MFV]{} asserts that any [NP]{} also has the quark flavour symmetry group only broken by insertions proportional to Yukawa matrices so that $Y^{~~j}_{U~i}, Y^{~~j}_{D~i}$ are proportional to $g^{~~j}_{U~i}, g^{~~j}_{D~i}$. One can construct allowed NP terms by treating the Yukawa matrices as spurion fields that transform under flavour rotations as, $$g_U \rightarrow V_U \, g_U \, V_Q^{\dagger},~~~~~~~~~~g_D \rightarrow V_D \, g_D \, V_Q^{\dagger},$$ where $V_U$ is an element of $ SU(3)_{U_R}$, $V_D$ is an element of $ SU(3)_{D_R}$, and $V_Q$ is an element of $ SU(3)_{Q_L}$, i.e., the Yukawa matrices transform as $g_U \sim ({\bf 3},{\bf 1}, {\bf {\bar{3}}})$ and $g_D \sim ({\bf 1},{\bf 3},{\bf {\bar{3}}})$ under the flavour group. MFV can be formulated up to linear order in top Yukawa insertions, or extended to a nonlinear representation of the symmetry [@Feldmann:2008ja; @Kagan:2009bn]. For enhanced CP violation in $B_q$ mixing we are interested in a nonlinear realization of MFV. It is sufficient to only expand to next order in insertions of $g_U$ so that \[yuk\] Y\^[  j]{}\_[U i]{} &=& 