# Conformality loss and quantum criticality in topological Higgs   electrodynamics in 2+1 dimensions

**Authors:** Flavio S. Nogueira, Jeroen van den Brink, Asle Sudbo

arXiv: 1907.00613 · 2019-10-17

## TL;DR

This paper explores the quantum critical behavior and conformality loss in a 2+1 dimensional topological Higgs electrodynamics model with a Chern-Simons term, revealing exotic universality classes and variable critical exponents.

## Contribution

It uncovers a new universality class for the massless theory and analyzes the transition between conformal and non-conformal phases driven by the Chern-Simons coupling.

## Key findings

- Massless theory exhibits exotic critical behavior beyond Landau-Ginzburg-Wilson paradigm.
- Finite Chern-Simons coupling leads to a quantum critical phase with variable exponents.
- Transition at critical coupling $ppa_c$ results in loss of conformality and modified scaling.

## Abstract

The electromagnetic response of topological insulators and superconductors is governed by a modified set of Maxwell equations that derive from a topological Chern-Simons (CS) term in the effective Lagrangian with coupling constant $\kappa$. Here we consider a topological superconductor or, equivalently, an Abelian Higgs model in $2+1$ dimensions with a global $O(2N)$ symmetry in the presence of a CS term, but without a Maxwell term. At large $\kappa$, the gauge field decouples from the complex scalar field, leading to a quantum critical behavior in the $O(2N)$ universality class. When the Higgs field is massive, the universality class is still governed by the $O(2N)$ fixed point. However, we show that the massless theory belongs to a completely different universality class, exhibiting an exotic critical behavior beyond the Landau-Ginzburg-Wilson paradigm. For finite $\kappa$ above a certain critical value $\kappa_c$, a quantum critical behavior with continuously varying critical exponents arises. However, as a function $\kappa$ a transition takes place for $|\kappa| < \kappa_c$ where conformality is lost. Strongly modified scaling relations ensue. For instance, in the case where $\kappa^2>\kappa_c^2$, leading to the existence of a conformal fixed point, critical exponents are a function of $\kappa$.

## Full text

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## Figures

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## References

59 references — full list in the complete paper: https://tomesphere.com/paper/1907.00613/full.md

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Source: https://tomesphere.com/paper/1907.00613