Research paperTheoreticalComputational Kinetic ModelThermal conductance and noise of Majorana modes along interfaced ν = 5/2 fractional quantum Hall statesMichael Hein, Christian SpånslättarXiv·2023·10.48550/arXiv.2208.07908·arXiv:2211.08000AbstractIdentifying the topological order of the fractional quantum Hall state at filling ν = 5/2 is an important step towards realizing non-Abelian Majorana modes in condensed matter physics. This work uses an incoherent edge-transport model to compute thermal conductances, voltage-biased charge current noise, and delta-T noise for interfaced ν = 5/2 candidate states (Pfaffian, anti-Pfaffian, and particle-hole-Pfaffian) matched to integer quantum Hall edges. The results are used to interpret recent experiments and estimate thermal and charge equilibration lengths in real devices.Read more
Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.4 propertiesSimulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.4 propertiesSimulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−3 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Research paperTheoreticalComputational Kinetic ModelThermal conductance and noise of Majorana modes along interfaced ν = 5/2 fractional quantum Hall statesMichael Hein, Christian SpånslättarXiv·2023·10.48550/arXiv.2208.07908·arXiv:2211.08000AbstractIdentifying the topological order of the fractional quantum Hall state at filling ν = 5/2 is an important step towards realizing non-Abelian Majorana modes in condensed matter physics. This work uses an incoherent edge-transport model to compute thermal conductances, voltage-biased charge current noise, and delta-T noise for interfaced ν = 5/2 candidate states (Pfaffian, anti-Pfaffian, and particle-hole-Pfaffian) matched to integer quantum Hall edges. The results are used to interpret recent experiments and estimate thermal and charge equilibration lengths in real devices.Read more
Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.4 propertiesSimulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.4 propertiesSimulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−3 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Research paperTheoreticalComputational Kinetic ModelThermal conductance and noise of Majorana modes along interfaced ν = 5/2 fractional quantum Hall statesMichael Hein, Christian SpånslättarXiv·2023·10.48550/arXiv.2208.07908·arXiv:2211.08000AbstractIdentifying the topological order of the fractional quantum Hall state at filling ν = 5/2 is an important step towards realizing non-Abelian Majorana modes in condensed matter physics. This work uses an incoherent edge-transport model to compute thermal conductances, voltage-biased charge current noise, and delta-T noise for interfaced ν = 5/2 candidate states (Pfaffian, anti-Pfaffian, and particle-hole-Pfaffian) matched to integer quantum Hall edges. The results are used to interpret recent experiments and estimate thermal and charge equilibration lengths in real devices.Read more
Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.4 propertiesSimulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.4 propertiesSimulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−3 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Research paperTheoreticalComputational Kinetic ModelThermal conductance and noise of Majorana modes along interfaced ν = 5/2 fractional quantum Hall statesMichael Hein, Christian SpånslättarXiv·2023·10.48550/arXiv.2208.07908·arXiv:2211.08000AbstractIdentifying the topological order of the fractional quantum Hall state at filling ν = 5/2 is an important step towards realizing non-Abelian Majorana modes in condensed matter physics. This work uses an incoherent edge-transport model to compute thermal conductances, voltage-biased charge current noise, and delta-T noise for interfaced ν = 5/2 candidate states (Pfaffian, anti-Pfaffian, and particle-hole-Pfaffian) matched to integer quantum Hall edges. The results are used to interpret recent experiments and estimate thermal and charge equilibration lengths in real devices.Read more
Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.4 propertiesSimulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.4 propertiesSimulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−3 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
Interfaced ν = 5/2−2 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.2 propertiesSimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference MaterialExpand
