I have measured via MOKE the reduced remanence, Mr/Ms, of a Permalloy thin film with well-defined uniaxial anisotropy (induced by a field applied during deposition) as a function of applied field angle. The result is a pretty polar plot (https://www.dropbox.com/s/29x7w2gyhbvdd8v/UApolar.png) which fits well to abs(cos(theta)), with theta=0 being the easy axis.

I would like to know where to begin in deriving this functionality. I think I can start from the Stoner-Wohlfarth/coherent rotation model although I know my sample does not follow such a reversal mechanism for all field angles.

What I've done so far is write my free energy terms for uniaxial anisotropy and Zeeman energy. I see in a couple of my favorite resources (O'Handley's "Modern Magnetic Materials" pg. 319 and http://iopscience.iop.org/0143-0807/29/3/008) that the next step is to apply my equilibrium conditions (take derivatives wrt angle between H and M) to come up with some relations that allow you to analytically play with applied field as a function of magnetization.

It is here that I've hit a brick wall. Am I on the right track?

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