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Interferometry provides direct evidence for anyon statistics. In the fractional quantum Hall effect, interferometers are susceptible to dephasing by neutral modes. The latter support chargeless quasiparticles (neutralons) which propagate upstream along the edge and obey fractional statistics. Here we show that on a suitably engineered bilayer fractional quantum Hall edge, which is an experimentally available platform, the neutral modes can be gapped while leaving the desired charge modes gapless. The gapping mechanism is akin to a four-particle pairing superconductivity. Our considered bilayer structure can be shaped as an anyonic interferometer. We also discuss experimental charge transport signatures of the neutral mode gap.
We study proximity coupling between a superconductor and counter-propagating gapless modes arising on the edges of Abelian fractional quantum Hall liquids with filling fraction $ u=1/m$ (with $m$ an odd integer). This setup can be utilized to create
We show that edges of Quantum Spin Hall topological insulators represent a natural platform for realization of exotic supersolid phase. On one hand, fermionic edge modes are helical due to the nontrivial topology of the bulk. On the other hand, a dis
The structure of edge modes at the boundary of quantum Hall (QH) phases forms the basis for understanding low energy transport properties. In particular, the presence of ``upstream modes, moving against the direction of charge current flow, is critic
A two-dimensional (2D) topological insulator (TI) exhibits the quantum spin Hall (QSH) effect, in which topologically protected spin-polarized conducting channels exist at the sample edges. Experimental signatures of the QSH effect have recently been
Electrons living in a two-dimensional world under a strong magnetic field - the so-called fractional quantum Hall effect (FQHE) - often manifest themselves as fractionally charged quasiparticles (anyons). Moreover, being under special conditions they