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Matrix Quantum Mechanics from Qubits
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We introduce a transverse field Ising model with order N^2 spins interacting via a nonlocal quartic interaction. The model has an O(N,Z), hyperoctahedral, symmetry. We show that the large N partition function admits a saddle point in which the symmetry is enhanced to O(N). We further demonstrate that this `matrix saddle' correctly computes large N observables at weak and strong coupling. The matrix saddle undergoes a continuous quantum phase transition at intermediate couplings. At the transition the matrix eigenvalue distribution becomes disconnected. The critical excitations are described by large N matrix quantum mechanics. At the critical point, the low energy excitations are waves propagating in an emergent 1+1 dimensional spacetime.
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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.
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