Large-N matrix Ising models with O(N1,Z) x O(N2,Z) symmetry reduce to spherically constrained bosonic matrix integrals that exhibit third-order topological transitions in the connectivity of the singular value distribution.
Large N matrices from a nonlocal spin system
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abstract
Large N matrices underpin the best understood models of emergent spacetime. We suggest that large N matrices can themselves be emergent from simple quantum mechanical spin models with finite dimensional Hilbert spaces. We exhibit the emergence of large N matrices in a nonlocal statistical physics model of order N^2 Ising spins. The spin partition function is shown to admit a large N saddle described by a matrix integral, which we solve. The matrix saddle is dominant at high temperatures, metastable at intermediate temperatures and ceases to exist below a critical order one temperature. The matrix saddle is disordered in a sense we make precise and competes with ordered low energy states. We verify our analytic results by Monte Carlo simulation of the spin system.
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Topological order in matrix Ising models
Large-N matrix Ising models with O(N1,Z) x O(N2,Z) symmetry reduce to spherically constrained bosonic matrix integrals that exhibit third-order topological transitions in the connectivity of the singular value distribution.