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Phys. Rev. Lett. 97, 030403 (2006) [4 pages]

Unconventional Continuous Phase Transition in a Three-Dimensional Dimer Model

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Fabien Alet1,2, Grégoire Misguich2, Vincent Pasquier2, Roderich Moessner3, and Jesper Lykke Jacobsen4,2
1Laboratoire de Physique Théorique, UMR CNRS 5152, Université Paul Sabatier, 31062 Toulouse, France
2Service de Physique Théorique, URA CNRS 2306, CEA Saclay, 91191 Gif sur Yvette, France
3Laboratoire de Physique Théorique, UMR CNRS 8549, École Normale Supérieure, 75005 Paris, France
4LPTMS, UMR CNRS 8626, Université Paris Sud, 91405 Orsay, France

Received 21 March 2006; published 21 July 2006

Phase transitions occupy a central role in physics, due both to their experimental ubiquity and their fundamental conceptual importance. The explanation of universality at phase transitions was the great success of the theory formulated by Ginzburg and Landau, and extended through the renormalization group by Wilson. However, recent theoretical suggestions have challenged this point of view in certain situations. In this Letter we report the first large-scale simulations of a three-dimensional model proposed to be a candidate for requiring a description beyond the Landau-Ginzburg-Wilson framework: we study the phase transition from the dimer crystal to the Coulomb phase in the cubic dimer model. Our numerical results strongly indicate that the transition is continuous and is compatible with a tricritical universality class, at variance with previous proposals.

© 2006 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.97.030403
DOI:
10.1103/PhysRevLett.97.030403
PACS:
05.30.−d, 02.70.Ss, 64.60.−i, 75.10.−b