The $\nu = 2/3$ filling is the simplest paradigmatic example of a fractional quantum Hall state, which contains counter-propagating edge modes. These modes can be either in the unequilibrated regime or equilibrated to different extents, on top of the possible edge reconstruction. In the unequilibrated regime, two distinct renormalization group fixed points have been previously proposed, namely Kane-Fischer-Polchinski and Wang-Meir-Gefen. In the equilibration regime, different degree of thermal equilibration can exist, while charge is fully equilibrated. Here, we show that these rich variety of models can give rise to three possible conductance plateaus at $e^2/2h$ (recently observed in experiments), $5e^2/9h$ (predicted here), and $e^2/3h$ ...
AC transformer action of a quantum point contact separating quantum Hall states with distinct fillin...
The interplay of high magnetic fields and many-body interactions in a two-dimensional electron gas ...
Reznikov et al. [Phys. Rev. Lett. 75, 3340 (1995)] have presented definitive observations of nonequi...
Bulk-boundary correspondence allows one to probe the bulk topological order by studying the transpor...
Understanding topological matter in the fractional quantum Hall (FQH) effect requires identifying th...
The fractional charge of quasiparticles is a fundamental feature of quantum Hall effect (QHE) States...
Quantum Hall edge channels can be combined with metallic regions to fractionalize electrons and form...
Hole-conjugate states of the fractional quantum Hall effect host counter-propagating edge channels w...
To determine the topological quantum numbers of fractional quantum Hall (FQH) states hosting counter...
Chiral gapless boundary modes are characteristic of quantum Hall (QH) states. For hole-conjugate fra...
Two-dimensional topological insulators, and in particular quantum Hall states, are characterized by ...
Abstract A comprehensive understanding of quantum Hall edge transmission, especially a hole-conjugat...
We propose a method to extract the mutual exchange statistics of the anyonic excitations of a genera...
Transport through edge channels is responsible for conduction in quantum Hall (QH) phases. Robust qu...
To determine the topological quantum numbers of fractional quantum Hall (FQH) states hosting counter...
AC transformer action of a quantum point contact separating quantum Hall states with distinct fillin...
The interplay of high magnetic fields and many-body interactions in a two-dimensional electron gas ...
Reznikov et al. [Phys. Rev. Lett. 75, 3340 (1995)] have presented definitive observations of nonequi...
Bulk-boundary correspondence allows one to probe the bulk topological order by studying the transpor...
Understanding topological matter in the fractional quantum Hall (FQH) effect requires identifying th...
The fractional charge of quasiparticles is a fundamental feature of quantum Hall effect (QHE) States...
Quantum Hall edge channels can be combined with metallic regions to fractionalize electrons and form...
Hole-conjugate states of the fractional quantum Hall effect host counter-propagating edge channels w...
To determine the topological quantum numbers of fractional quantum Hall (FQH) states hosting counter...
Chiral gapless boundary modes are characteristic of quantum Hall (QH) states. For hole-conjugate fra...
Two-dimensional topological insulators, and in particular quantum Hall states, are characterized by ...
Abstract A comprehensive understanding of quantum Hall edge transmission, especially a hole-conjugat...
We propose a method to extract the mutual exchange statistics of the anyonic excitations of a genera...
Transport through edge channels is responsible for conduction in quantum Hall (QH) phases. Robust qu...
To determine the topological quantum numbers of fractional quantum Hall (FQH) states hosting counter...
AC transformer action of a quantum point contact separating quantum Hall states with distinct fillin...
The interplay of high magnetic fields and many-body interactions in a two-dimensional electron gas ...
Reznikov et al. [Phys. Rev. Lett. 75, 3340 (1995)] have presented definitive observations of nonequi...