REVIEW 2 cited by
Ensemble inequivalence and phase transitions in unlabeled networks
Not yet reviewed by Pith; the record is open.
This paper has not been read by Pith yet. Machine review is queued; the pith claim, tier, and objections will appear here once it completes.
SPECIMEN: schema-true, not a live event
T0 review · schema-true
One-sentence machine reading of the paper's core claim.
pith:XXXXXXXX · record.json · timestamp
Signed reviews
read the original abstract
We discover a first-order phase transition in the canonical ensemble of random unlabeled networks with a prescribed average number of links. The transition is caused by the nonconcavity of microcanonical entropy. Above the critical point coinciding with the graph symmetry phase transition, the canonical and microcanonical ensembles are equivalent and have a well-behaved thermodynamic limit. Below the critical point, the ensemble equivalence is broken, and the canonical ensemble is a mixture of phases: empty networks and networks with average degrees diverging logarithmically with the network size. As a consequence, networks with bounded average degrees do not survive in the thermodynamic limit, decaying into the empty phase. The celebrated percolation transition in labeled networks is thus absent in unlabeled networks. In view of these differences between labeled and unlabeled ensembles, the question of which one should be used as a null model of different real-world networks cannot be ignored.
Forward citations
Cited by 2 Pith papers
-
Negative heat capacities in spherically symmetric sectors of $d$-matrix quantum mechanics
SO(d) and O(d) invariant sectors of d-matrix QM show negative microcanonical heat capacity that becomes positive at k_crit ~ N^2/4, forming a caloric fold similar to AdS black holes.
-
Gauged permutation invariant tensor quantum mechanics, least common multiples and the inclusion-exclusion principle
Canonical partition functions for gauged permutation-invariant s-index tensor oscillators are expressed exactly as products of (1 - x^{LCM(...)})^{-...} factors, with a large-N critical Boltzmann factor x_c ~ log N/(s...
Discussion (0). Continue with ORCID to comment.