Continuous Phase Transition
Near critical point, we expect scaling behavior: all physical quantities have power-law dependencies on the control parameter
No characteristic scales in observables
Critical exponents of power-laws are main quantities of interest
- t, Cluster size: ns(pc) _ s-t
- b, Order parameter: P _ (p-pc)b
- g, Divergence of s: _ |p-pc|-g
Hyper-scaling assumption 2-a = (t - 1) / s = 2b + g