The behavior of systems near critical points is a long‐standing puzzle in statistical mechanics and solid‐state physics. Experimentally this behavior is characterized by divergences in a variety of thermodynamic quantities as powers of the deviation from criticality. These divergences are described by critical indices, which are the exponents in power laws; for example, the susceptibility of a ferromagnet diverges like (T−Tc)γ as T approaches Tc.

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