Abstract
Based on a non-rigorous formalism called the “cavity method”, physicists have put forward intriguing predictions on phase transitions in diluted mean-field models, in which the geometry of interactions is induced by a sparse random graph or hypergraph. One example of such a model is the graph coloring problem on the Erdős–Renyi random graph G(n, d/n), which can be viewed as the zero temperature case of the Potts antiferromagnet. The cavity method predicts that in addition to the k-colorability phase transition studied intensively in combinatorics, there exists a second phase transition called the condensation phase transition (Krzakala et al. in Proc Natl Acad Sci 104:10318–10323, 2007). In fact, there is a conjecture as to the precise location of this phase transition in terms of a certain distributional fixed point problem. In this paper we prove this conjecture for k exceeding a certain constant k 0.
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Communicated by H.-T. Yau
The research leading to these results has received funding from the European Research Council under the European Union’s Seventh Framework Programme (FP/2007-2013)/ERC Grant Agreement No. 278857-PTCC.
An extended abstract version of this work appeared in the Proceedings of the 18th International Workshop on Randomization and Computation (‘RANDOM’) 2014.
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Bapst, V., Coja-Oghlan, A., Hetterich, S. et al. The Condensation Phase Transition in Random Graph Coloring. Commun. Math. Phys. 341, 543–606 (2016). https://doi.org/10.1007/s00220-015-2464-z
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DOI: https://doi.org/10.1007/s00220-015-2464-z