Thermal conductance and noise of Majorana modes along interfaced ν = 5/2 fractional quantum Hall states

Michael Hein; Christian Spånslätt

doi:10.48550/arXiv.2208.07908

Paper details

Research paper

TheoreticalComputational Kinetic Model

Thermal conductance and noise of Majorana modes along interfaced ν = 5/2 fractional quantum Hall states

Michael Hein, Christian Spånslätt

arXiv·2023·10.48550/arXiv.2208.07908·arXiv:2211.08000

Samples

Each sample groups how it was prepared, characterized, and measured. Click a card to expand.

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 properties

Simulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference Material

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 properties

Simulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference Material

Interfaced ν = 5/2−3 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.

2 properties

SimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 3Reference Material

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 properties

Simulatedparticle-hole-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference Material

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 properties

Simulatedanti-Pfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference Material

Interfaced ν = 5/2−2 edge based on the Pfaffian candidate state and an integer quantum Hall state exposing the second Landau level.

2 properties

SimulatedPfaffian ν = 5/2 edge stateStudied Materialinteger quantum Hall state ν = 2Reference Material

Materials

Pfaffian ν = 5/2 edge state

Studied Material

Also known as

PfPfaffian

Variables

topological_order= Pf

studied material

anti-Pfaffian ν = 5/2 edge state

Studied Material

Why these are connected

Related documents with shared materials, methods, properties, or citations.

Thermal conductance and noise of Majorana modes along interfaced ν = 5/2 fractional quantum Hall states | Matter42 Literature

Properties

Type	Label	Value	Material	Sample	Source
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the Pfaffian candidate st	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the Pfaffian candidate st	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffia	—
Thermal Conductance	GQ₂T	3/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candida	—
Thermal Conductance	GQ₂T	3/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the Pfaffian candidate st	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffia	—
Thermal Hall Conductance	GQ_H	3/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candida	—
Thermal Hall Conductance	GQ_H	3/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the Pfaffian candidate st	—
Charge Current Noise	voltage biased charge current noise	0.113[ΔV e³/h]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Charge Current Noise	voltage biased charge current noise	0.152[ΔV e³/h]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Delta T Noise	downstream excess delta-T noise	0.865[2G₂T kB ΔT]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Delta T Noise	downstream excess delta-T noise	1.361[2G₂T kB ΔT]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—

Properties

Type	Label	Value	Material	Sample	Source
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the Pfaffian candidate st	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the Pfaffian candidate st	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffia	—
Thermal Conductance	GQ₂T	3/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candida	—
Thermal Conductance	GQ₂T	3/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the Pfaffian candidate st	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffia	—
Thermal Hall Conductance	GQ_H	3/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candida	—
Thermal Hall Conductance	GQ_H	3/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the Pfaffian candidate st	—
Charge Current Noise	voltage biased charge current noise	0.113[ΔV e³/h]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Charge Current Noise	voltage biased charge current noise	0.152[ΔV e³/h]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Delta T Noise	downstream excess delta-T noise	0.865[2G₂T kB ΔT]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Delta T Noise	downstream excess delta-T noise	1.361[2G₂T kB ΔT]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—

Properties

Type	Label	Value	Material	Sample	Source
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the Pfaffian candidate st	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the Pfaffian candidate st	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffia	—
Thermal Conductance	GQ₂T	3/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candida	—
Thermal Conductance	GQ₂T	3/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the Pfaffian candidate st	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffia	—
Thermal Hall Conductance	GQ_H	3/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candida	—
Thermal Hall Conductance	GQ_H	3/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the Pfaffian candidate st	—
Charge Current Noise	voltage biased charge current noise	0.113[ΔV e³/h]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Charge Current Noise	voltage biased charge current noise	0.152[ΔV e³/h]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Delta T Noise	downstream excess delta-T noise	0.865[2G₂T kB ΔT]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Delta T Noise	downstream excess delta-T noise	1.361[2G₂T kB ΔT]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—

Properties

Type	Label	Value	Material	Sample	Source
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the Pfaffian candidate st	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the Pfaffian candidate st	—
Thermal Conductance	GQ₂T	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffia	—
Thermal Conductance	GQ₂T	3/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candida	—
Thermal Conductance	GQ₂T	3/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the Pfaffian candidate st	—
Thermal Hall Conductance	GQ_H	1/2[κ0 T̄]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the particle-hole-Pfaffia	—
Thermal Hall Conductance	GQ_H	3/2[κ0 T̄]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the anti-Pfaffian candida	—
Thermal Hall Conductance	GQ_H	3/2[κ0 T̄]	Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−2 edge based on the Pfaffian candidate st	—
Charge Current Noise	voltage biased charge current noise	0.113[ΔV e³/h]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Charge Current Noise	voltage biased charge current noise	0.152[ΔV e³/h]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—
Delta T Noise	downstream excess delta-T noise	0.865[2G₂T kB ΔT]	particle-hole-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the particle-hole-Pfaffia	—
Delta T Noise	downstream excess delta-T noise	1.361[2G₂T kB ΔT]	anti-Pfaffian ν = 5/2 edge state	Interfaced ν = 5/2−3 edge based on the anti-Pfaffian candida	—