We consider a three-dimensional lattice Abelian Higgs gauge model for a charged N-component scalar field phi, which is invariant under SO(N) global transformations for generic values of the parameters. We focus on the strong-coupling regime, in which the kinetic Hamiltonian term for the gauge field is a small perturbation, which is irrelevant for the critical behavior. The Hamiltonian depends on a parameter v, which determines the global symmetry of the model and the symmetry of the low-temperature phases. We present renormalization-group predictions, based on a Landau-Ginzburg-Wilson effective description that relies on the identification of the appropriate order parameter and on the symmetry-breaking patterns that occur at the strong-coupling phase transitions. For v = 0, the global symmetry group of the model is SU(N); the corresponding model may undergo continuous transitions only for N = 2. For v not equal 0, i.e., in the SO(N) symmetric case, continuous transitions (in the Heisenberg universality class) are possible also for N = 3 and 4. We perform Monte Carlo simulations for N = 2, 3, 4, 6, to verify the renormalization-group predictions. Finite-size scaling analyses of the numerical data are in full agreement.

Strong-coupling critical behavior in three-dimensional lattice Abelian gauge models with charged N-component scalar fields and SO(N) symmetry

Bonati, Claudio;Vicari, Ettore
2024-01-01

Abstract

We consider a three-dimensional lattice Abelian Higgs gauge model for a charged N-component scalar field phi, which is invariant under SO(N) global transformations for generic values of the parameters. We focus on the strong-coupling regime, in which the kinetic Hamiltonian term for the gauge field is a small perturbation, which is irrelevant for the critical behavior. The Hamiltonian depends on a parameter v, which determines the global symmetry of the model and the symmetry of the low-temperature phases. We present renormalization-group predictions, based on a Landau-Ginzburg-Wilson effective description that relies on the identification of the appropriate order parameter and on the symmetry-breaking patterns that occur at the strong-coupling phase transitions. For v = 0, the global symmetry group of the model is SU(N); the corresponding model may undergo continuous transitions only for N = 2. For v not equal 0, i.e., in the SO(N) symmetric case, continuous transitions (in the Heisenberg universality class) are possible also for N = 3 and 4. We perform Monte Carlo simulations for N = 2, 3, 4, 6, to verify the renormalization-group predictions. Finite-size scaling analyses of the numerical data are in full agreement.
2024
Bonati, Claudio; Pelissetto, Andrea; Vicari, Ettore
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11568/1274338
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