Figure 6
From: The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary
Fluctuation function \({F}_{q}(n)\) for different values of \(q\in [\,-\,10,10]\) for the whole signal for the 2D sample of size \(L=512\) (left panel), and 3D sample in the HLC (right, upper panel) and the initial segment of the loop (right, lower panel). Insets: corresponding generalised Hurst exponents H(q) against the amplification parameter q, see text.
