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Fine structure in the large n limit of the non-Hermitian Penner matrix model
In this paper we apply results on the asymptotic zero distribution of the Laguerre polynomials to discuss generalizations of the standard large n limit in the non-Hermitian Penner matrix model. In these generalizations gnn→t, but the product gnn is not necessarily fixed to the value of the ’t Hooft...
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Published in: | Annals of physics 2015-10, Vol.361, p.440-460 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | In this paper we apply results on the asymptotic zero distribution of the Laguerre polynomials to discuss generalizations of the standard large n limit in the non-Hermitian Penner matrix model. In these generalizations gnn→t, but the product gnn is not necessarily fixed to the value of the ’t Hooft coupling t. If t>1 and the limit l=limn→∞|sin(π/gn)|1/n exists, then the large n limit is well-defined but depends both on t and on l. This result implies that for t>1 the standard large n limit with gnn=t fixed is not well-defined. The parameter l determines a fine structure of the asymptotic eigenvalue support: for l≠0 the support consists of an interval on the real axis with charge fraction Q=1−1/t and an l-dependent oval around the origin with charge fraction 1/t. For l=1 these two components meet, and for l=0 the oval collapses to the origin. We also calculate the total electrostatic energy E, which turns out to be independent of l, and the free energy F=E−Qlnl, which does depend on the fine structure parameter l. The existence of large n asymptotic expansions of F beyond the planar limit as well as the double-scaling limit are also discussed. |
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ISSN: | 0003-4916 1096-035X |
DOI: | 10.1016/j.aop.2015.07.011 |