“…Performing experiments with rotational loops where the magnitude of M is kept constant by varying the applied field one can measure the corresponding angles which then allow to determine an analogous phase diagrams L 0 j ða; jMjÞ: From these diagrams, one can compute the phase diagram L 0 j ða; jMjÞ by using the relationship between L 0 j ða; jMjÞ and L j ða; jHjÞ (the complete mathematical formulation will be published elsewhere). In the isotropic case for a rotational loop the angle between the magnetization and the applied field depends only on the amplitude of the magnetization [6][7][8][9], so the phase diagram becomes a function of the magnetization only and it can be plot as a simple curve.…”