Breaking of Ensemble Equivalence in Networks.

It is generally believed that, in the thermodynamic limit, the microcanonical description as a function of energy coincides with the canonical description as a function of temperature. However, various examples of systems for which the microcanonical and canonical ensembles are not equivalent have been identified. A complete theory of this intriguing phenomenon is still missing. Here we show that ensemble nonequivalence can manifest itself also in random graphs with topological constraints. We find that, while graphs with a given number of links are ensemble equivalent, graphs with a given degree sequence are not. This result holds irrespective of whether the energy is nonadditive (as in unipartite graphs) or additive (as in bipartite graphs). In contrast with previous expectations, our results show that (1) physically, nonequivalence can be induced by an extensive number of local constraints, and not necessarily by long-range interactions or nonadditivity, (2) mathematically, nonequivalence is determined by a different large-deviation behavior of microcanonical and canonical probabilities for a single microstate, and not necessarily for almost all microstates. The latter criterion, which is entirely local, is not restricted to networks and holds in general.

[1]  S. Ruffo,et al.  Inequivalence of ensembles in a system with long-range interactions. , 2001, Physical review letters.

[2]  V. J. Emery,et al.  Ising Model for the ? Transition and Phase Separation in He^{3}-He^{4} Mixtures , 1971 .

[3]  Brendan D. McKay,et al.  Asymptotic enumeration by degree sequence of graphs with degreeso(n1/2) , 1991, Comb..

[4]  公庄 庸三 Discrete math = 離散数学 , 2004 .

[5]  Diego Garlaschelli,et al.  Analytical maximum-likelihood method to detect patterns in real networks , 2011, 1103.0701.

[6]  H. Touchette,et al.  Thermodynamic versus statistical nonequivalence of ensembles for the mean-field Blume–Emery–Griffiths model , 2003, cond-mat/0307007.

[7]  R. Ellis,et al.  Nonequivalent statistical equilibrium ensembles and refined stability theorems for most probable flows , 2000, math-ph/0012022.

[8]  Negative heat capacity in the critical region of nuclear fragmentation: an experimental evidence of the liquid-gas phase transition , 1999, nucl-ex/9906004.

[9]  P. Chavanis Gravitational instability of isothermal and polytropic spheres , 2002, astro-ph/0207080.

[10]  Large Deviation Principles and Complete Equivalence and Nonequivalence Results for Pure and Mixed Ensembles , 2000, math/0012081.

[11]  J. Gibbs Elementary Principles in Statistical Mechanics , 1902 .

[12]  Hugo Touchette,et al.  Equivalence and Nonequivalence of Ensembles: Thermodynamic, Macrostate, and Measure Levels , 2014, 1403.6608.

[13]  D. Lynden-Bell NEGATIVE SPECIFIC HEAT IN ASTRONOMY, PHYSICS AND CHEMISTRY , 1999 .

[14]  H. Touchette The large deviation approach to statistical mechanics , 2008, 0804.0327.

[15]  Hugo Touchette,et al.  An introduction to the thermodynamic and macrostate levels of nonequivalent ensembles , 2004 .

[16]  Edward A. Bender,et al.  The Asymptotic Number of Labeled Graphs with Given Degree Sequences , 1978, J. Comb. Theory A.