Since  the \(\gamma_{0,2}B^2\) term in the denominator of Eq. \ref{eq:expand_y_32} does not significantly differ from zero, we should try dropping that term. 
Running the fit again for the modified Padé expansion specified by Eq.\ref{eq:expand_y_31} below (omitting the \(\gamma_{0,2}B^2\) term from Eq. \ref{eq:expand_y_32})