Arctic curves of the octahedron equation

PACS numbers: 64.60.De, 64.70.qd, 02.10.Ox International audience We study the octahedron relation (also known as the $A_{\infty}$ $T$-system), obeyed in particular by the partition function for dimer coverings of the Aztec Diamond graph. For a suitable class of doubly periodic initial conditions, w...

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Bibliographic Details
Published in:Journal of Physics A: Mathematical and Theoretical
Main Authors: Di Francesco, P., Soto-Garrido, R.
Other Authors: Department of Mathematics Urbana, University of Illinois at Urbana-Champaign Urbana (UIUC), University of Illinois System-University of Illinois System, Institut de Physique Théorique - UMR CNRS 3681 (IPHT), Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Direction de Recherche Fondamentale (CEA) (DRF (CEA)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Department of Physics Illinois at Urbana-Champaign, USA
Format: Article in Journal/Newspaper
Language:English
Published: HAL CCSD 2014
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Online Access:https://cea.hal.science/cea-01002519
https://doi.org/10.1088/1751-8113/47/28/285204
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Summary:PACS numbers: 64.60.De, 64.70.qd, 02.10.Ox International audience We study the octahedron relation (also known as the $A_{\infty}$ $T$-system), obeyed in particular by the partition function for dimer coverings of the Aztec Diamond graph. For a suitable class of doubly periodic initial conditions, we find exact solutions with a particularly simple factorized form. For these, we show that the density function that measures the average dimer occupation of a face of the Aztec graph, obeys a system of linear recursion relations with periodic coefficients. This allows us to explore the thermodynamic limit of the corresponding dimer models and to derive exact "arctic" curves separating the various phases of the system.