An extended universality hypothesis is proposed for critical phenomena in simple systems. The hypothesis implies the invariance of
VX=gXlXnXqXKCX, where
qX is the coordination number,
KCX is the dimensionless inverse critical temperature, and
nX,
gX, and
lX are the universality scale factors.
VX is an exact invariant for the two-dimensional
S=21 Ising model and invariant to high precision for several three-dimensional models. For the spherical model, however,
lXVX is an exact invariant.
In statistical physics, if we divide successively an equilibrium system into two parts, we will face a situation that, to a certain length ξ, the physics of a subsystem is no longer the same as the original one. The extensive property of the thermal entropy S (A ∪ B) = S (A) + S (B) is then violated. This observation motivates us to introduce a concept of correlation entropy between two points, as measured by the mutual information in information theory, to study the critical phenomena. A rigorous relation is established to display some drastic features of the non-vanishing correlation entropy of a subsystem formed by any two distant particles with long-range correlation. This relation actually indicates a universal role played by the correlation entropy for understanding the critical phenomena. We also verify these analytical studies in terms of two well-studied models for both the thermal and quantum phase transitions: the two-dimensional Ising model and the one-dimensional transverse-field Ising model. Therefore, the correlation entropy provides us with a new physical intuition of the critical phenomena from the point of view of information theory.