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Spacetime Symmetries of the Quantum Hall Effect (1407.1252v2)

Published 4 Jul 2014 in cond-mat.mes-hall and hep-th

Abstract: We study the symmetries of non-relativistic systems with an emphasis on applications to the fractional quantum Hall effect. A source for the energy current of a Galilean system is introduced and the non-relativistic diffeomorphism invariance studied in previous work is enhanced to a full spacetime symmetry, allowing us to derive a number of Ward identities. These symmetries are smooth in the massless limit of the lowest Landau level. We develop a formalism for Newton-Cartan geometry with torsion to write these Ward identities in a covariant form. Previous results on the connection between Hall viscosity and Hall conductivity are reproduced.

Citations (169)

Summary

Overview of Spacetime Symmetries in the Quantum Hall Effect

The paper "EFI 14-21: Spacetime Symmetries of the Quantum Hall Effect" by Michael Geracie, Dam Thanh Son, Chaolun Wu, and Shao-Feng Wu introduces a novel approach to address complexities inherent in non-relativistic systems, particularly the fractional quantum Hall (FQH) effect, utilizing enhanced spacetime symmetries. This paper evolves previous insights on non-relativistic diffeomorphism invariance to a comprehensive spacetime symmetry model, producing numerous Ward identities relevant to understanding the quantum Hall phenomena in diverse geometrical contexts.

Key Contributions and Numerical Findings

Firstly, this paper proposes the enhancement of the symmetry framework for non-relativistic systems, transitioning from spatial diffeomorphism invariance to a full spacetime diffeomorphism invariant model. This advancement crucially incorporates a novel source for the energy current in Galilean systems, refining the theoretical representation of energy flow under non-relativistic conditions. In particular, the paper introduces the Newton-Cartan geometry with torsion, providing a covariant structure that encapsulates the symmetries of the lowest Landau level (LLL).

Importantly, the paper showcases that choosing specific parameters for spin (s = 1) and gyromagnetic ratio (g = 2) enables a regular massless limit in the LLL by enforcing constraints that eliminate kinetic energy contributions and streamline theoretical calculations. This methodological choice results in the derivation of Ward identities that substantiate existing relations between Hall viscosity and Hall conductivity, reproducing and extending previous findings in the context of FQH states.

Implications and Theoretical Developments

The implications of these theoretical advancements are substantial. By achieving a fully spacetime covariant treatment of quantum Hall systems, the paper enhances our ability to scrutinize the FQH effect under arbitrary geometrical conditions and electromagnetic backgrounds. This geometro-dynamical representation facilitates a deeper understanding of phenomena like momentum conservation and energy dissipation at quantum scales, offering a coherent framework that bridges classical fluid mechanics and quantum Hall physics.

The paper's novel approach encourages future explorations in non-relativistic holography and may significantly inform computational models that aim to simulate quantum Hall effects with higher accuracy and efficiency. Moreover, the constructed geometric formalism poses potential applications across condensed matter physics and beyond, paving the way for more generalized theories that accommodate spacetime torsion and quantum anomalies.

Speculation on Future Developments

Looking ahead, the insights gained from this paper may spark further developments in theoretical models where symmetry considerations are pivotal, such as low-dimensional quantum gravity theories or the modeling of non-relativistic scale-invariant systems. Additionally, integrating these advanced geometric frameworks with modern computational methods could enhance simulations, potentially driving innovations in quantum computing and materials science.

In summary, this paper's refined illustration of spacetime symmetries within the quantum Hall effect provides a robust theoretical foundation that may influence ongoing research across multiple domains of theoretical and applied physics. The formalism presented not only addresses intricacies within the FQH effect but also encourages exploring broader applications where spacetime geometry intersects with quantum mechanics.