magnetic field dependence of  \(c_i\)

Next, we generate generated arrays of \(c_i\left(B\right)\) for each Chebyshev coefficient. In this case, we restrict ourselves to 6 coefficients — \(c_0\) through \(c_5\) — since higher order fits either did not converge for all field values and/or introduced artificial discontinuities in the higher order coefficients as a function of magnetic field. The results are shown below in Fig. \ref{742044}