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Nuclear Physics B - Proceedings Supplements

Critical dynamics: Finite size effects and supersymmetry

J. C. Niel

Published Apr 1, 1988• 0 citations
Publisher
DOI
10.1016/0920-5632(88)90172-7

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A detailed study of a model for strongly-interacting fermions with exclusion rules and lattice N=2\mathcal N=2N=2 supersymmetry is presented. A submanifold in the space of parameters of the model where it is Bethe-ansatz solvable is identified. The relation between this manifold and the existence of additional, so-called dynamic, supersymmetries is discussed. The ground states are analysed with the help of cohomology techniques, and their exact finite-size Bethe roots are found. Moreover, through analytical and numerical studies it is argued that the model provides a lattice version of the N=1\mathcal N=1N=1 super-sine-Gordon model at a particular coupling where an additional N=(2,2)\mathcal N=(2,2)N=(2,2) supersymmetry is present. The dynamic supersymmetry is shown to allow an exact determination of the gap scaling function of the model.
We obtain exact, nonperturbative results for the zero- and finite-temperature dynamical responses at the semimetal-superconductor quantum critical point (QCP) of two-dimensional Dirac fermions, which can occur on the surface of a topological insulator. This strongly interacting QCP is described by a conformal field theory with emergent N=2\mathcal{N}=2N=2 supersymmetry, which imposes strong constraints. At zero temperature, we obtain closed-form results for the optical conductivity, dynamical shear viscosity, and corner entanglement entropy. We also make exact statements for the optical conductivity at finite temperature regarding large-frequency asymptotics and sum rules. Finally, we discuss experimental considerations for the observation of these signatures in topological insulators.
Abstract This work is dedicated to the study of a supersymmetric quantum spherical spin system with short-range interactions. We examine the critical properties both a zero and finite temperature. The model undergoes a quantum phase transition at zero temperature without breaking supersymmetry. At finite temperature the supersymmetry is broken and the system exhibits a thermal phase transition. We determine the critical dimensions and compute critical exponents. In particular, we find that the model is characterized by a dynamical critical exponent z = 2. We also investigate properties of correlations in the one-dimensional lattice. Finally, we explore the connection with a nonrelativistic version of the supersymmetric nonlinear sigma model and show that it is equivalent to the system of spherical spins in the large N limit.