1999/12/31 by Luiz C. de Albuquerque, Nelson A. Alves, D. Dalmazi · 1 citation
Mathematics · Physics and Astronomy · #Markov Chains and Monte Carlo Methods #Random Matrices and Applications #Theoretical and Computational Physics #cond-mat.stat-mech #hep-th
paper · pdf · doi:10.1016/s0550-3213(00)00290-x
published as Nucl.Phys. B580 (2000) 739-756 · 19 pages, 7 figures ,1 reference and a note added ,To Appear in Nucl.Phys B
arxiv created 2000/05/03 · openalex publication_date 2000/08/01 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28
We obtain in a closed form the 1/N2 contribution to the free energy of the two Hermitian N× N random matrix model with non symmetric quartic potential. From this result, we calculate numerically the Yang-Lee zeros of the 2D Ising model on dynamical random graphs with the topology of a torus up to n=16 vertices. They are found to be located on the unit circle on the complex fugacity plane. In order to include contributions of even higher topologies we calculated analytically the nonperturbative (sum over all genus) partition function of the model Zn = ∑h=0∞ \fracZn(h)N2h for the special cases of N=1,2 and graphs with n≤ 20 vertices. Once again the Yang-Lee zeros are shown numerically to lie on the unit circle on the complex fugacity plane. Our results thus generalize previous numerical results on random graphs by going beyond the planar approximation and strongly indicate that there might be a generalization of the Lee-Yang circle theorem for dynamical random graphs.