Emergence of spin-active channels at a quantum Hall interface
arXiv:2009.10539 · doi:10.1103/PhysRevB.103.L081401
Abstract
We study the ground state of a system with an interface between and in the quantum Hall regime. Far from the interface, for a range of interaction strengths, the region is fully polarized but region is locally a singlet. Upon varying the strength of the interactions and the width of the interface, the system chooses one of two distinct edge/interface phases. In phase A, stabilized for wide interfaces, spin is a good quantum number, and there are no gapless long-wavelength spin fluctuations. In phase B, stabilized for narrow interfaces, spin symmetry is spontaneously broken at the Hartree-Fock level. Going beyond Hartree-Fock, we argue that phase B is distinguished by the emergence of gapless long-wavelength spin excitations bound to the interface, which can, in principle, be detected by a measurement of the relaxation time in nuclear magnetic resonance.
arXiv comment9 pages 10 figures including supplemental material
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- Edge Reconstruction and Emergent Neutral Modes in Integer and Fractional Quantum Hall Phases
- Magnon transmission across mono-layer graphene junction as a probe of electronic structure
- Dc Electrical Current Generated by Upstream Neutral Modes
- Edge Reconstruction in a Quantum Spin Hall Insulator