Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirs
- Autores
- Aita, Hugo Alberto; arrechea, Liliana; Naón, Carlos María; Fradkin, Eduardo
- Año de publicación
- 2013
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- We study the heat transport along an edge state of a two-dimensional electron gas in the quantum Hall regime, in contact to two reservoirs at different temperatures. We consider two exactly solvable models for the edge state coupled to the reservoirs. The first one corresponds to filling ν=1 and tunneling coupling to the reservoirs. The second one corresponds to integer or fractional filling of the sequence ν = /m (with m odd), and capacitive coupling to the reservoirs. In both cases, we solve the problem by means of nonequilibrium Green function formalism. We show that heat propagates chirally along the edge in the two setups. We identify two temperature regimes, defined by Δ , the mean level spacing of the edge. At low temperatures, T < Δ , finite size effects play an important role in heat transport, for both types of contacts. The nature of the contacts manifests itself in different power laws for the thermal conductance as a function of the temperature. For capacitive couplings, a highly nonuniversal behavior takes place, through a prefactor that depends on the length of the edge as well as on the coupling strengths and the filling fraction. For larger temperatures, T >Δ , finite-size effects become irrelevant, but the heat transport strongly depends on the strength of the edge-reservoir interactions, in both cases. The thermal conductance for tunneling coupling grows linearly with T , whereas for the capacitive case, it saturates to a value that depends on the coupling strengths and the filling factors of the edge and the contacts.
Instituto de Física La Plata - Materia
-
Física
Coupling
Quantum tunnelling
Physics
Ballistic conduction
Quantum hall effect
Capacitive sensing
Condensed matter physics
Capacitive coupling
Fermi gas
Thermal conductivity - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- http://creativecommons.org/licenses/by-nc-sa/4.0/
- Repositorio
- Institución
- Universidad Nacional de La Plata
- OAI Identificador
- oai:sedici.unlp.edu.ar:10915/125905
Ver los metadatos del registro completo
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Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirsAita, Hugo Albertoarrechea, LilianaNaón, Carlos MaríaFradkin, EduardoFísicaCouplingQuantum tunnellingPhysicsBallistic conductionQuantum hall effectCapacitive sensingCondensed matter physicsCapacitive couplingFermi gasThermal conductivityWe study the heat transport along an edge state of a two-dimensional electron gas in the quantum Hall regime, in contact to two reservoirs at different temperatures. We consider two exactly solvable models for the edge state coupled to the reservoirs. The first one corresponds to filling ν=1 and tunneling coupling to the reservoirs. The second one corresponds to integer or fractional filling of the sequence ν = /m (with m odd), and capacitive coupling to the reservoirs. In both cases, we solve the problem by means of nonequilibrium Green function formalism. We show that heat propagates chirally along the edge in the two setups. We identify two temperature regimes, defined by Δ , the mean level spacing of the edge. At low temperatures, T < Δ , finite size effects play an important role in heat transport, for both types of contacts. The nature of the contacts manifests itself in different power laws for the thermal conductance as a function of the temperature. For capacitive couplings, a highly nonuniversal behavior takes place, through a prefactor that depends on the length of the edge as well as on the coupling strengths and the filling fraction. For larger temperatures, T >Δ , finite-size effects become irrelevant, but the heat transport strongly depends on the strength of the edge-reservoir interactions, in both cases. The thermal conductance for tunneling coupling grows linearly with T , whereas for the capacitive case, it saturates to a value that depends on the coupling strengths and the filling factors of the edge and the contacts.Instituto de Física La Plata2013-08-23info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfhttp://sedici.unlp.edu.ar/handle/10915/125905enginfo:eu-repo/semantics/altIdentifier/issn/1098-0121info:eu-repo/semantics/altIdentifier/issn/1550-235xinfo:eu-repo/semantics/altIdentifier/arxiv/1305.5833info:eu-repo/semantics/altIdentifier/doi/10.1103/physrevb.88.085122info:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-sa/4.0/Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-10-15T11:22:06Zoai:sedici.unlp.edu.ar:10915/125905Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-10-15 11:22:07.097SEDICI (UNLP) - Universidad Nacional de La Platafalse |
dc.title.none.fl_str_mv |
Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirs |
title |
Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirs |
spellingShingle |
Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirs Aita, Hugo Alberto Física Coupling Quantum tunnelling Physics Ballistic conduction Quantum hall effect Capacitive sensing Condensed matter physics Capacitive coupling Fermi gas Thermal conductivity |
title_short |
Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirs |
title_full |
Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirs |
title_fullStr |
Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirs |
title_full_unstemmed |
Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirs |
title_sort |
Heat transport through quantum Hall edge states: tunneling versus capacitive coupling to reservoirs |
dc.creator.none.fl_str_mv |
Aita, Hugo Alberto arrechea, Liliana Naón, Carlos María Fradkin, Eduardo |
author |
Aita, Hugo Alberto |
author_facet |
Aita, Hugo Alberto arrechea, Liliana Naón, Carlos María Fradkin, Eduardo |
author_role |
author |
author2 |
arrechea, Liliana Naón, Carlos María Fradkin, Eduardo |
author2_role |
author author author |
dc.subject.none.fl_str_mv |
Física Coupling Quantum tunnelling Physics Ballistic conduction Quantum hall effect Capacitive sensing Condensed matter physics Capacitive coupling Fermi gas Thermal conductivity |
topic |
Física Coupling Quantum tunnelling Physics Ballistic conduction Quantum hall effect Capacitive sensing Condensed matter physics Capacitive coupling Fermi gas Thermal conductivity |
dc.description.none.fl_txt_mv |
We study the heat transport along an edge state of a two-dimensional electron gas in the quantum Hall regime, in contact to two reservoirs at different temperatures. We consider two exactly solvable models for the edge state coupled to the reservoirs. The first one corresponds to filling ν=1 and tunneling coupling to the reservoirs. The second one corresponds to integer or fractional filling of the sequence ν = /m (with m odd), and capacitive coupling to the reservoirs. In both cases, we solve the problem by means of nonequilibrium Green function formalism. We show that heat propagates chirally along the edge in the two setups. We identify two temperature regimes, defined by Δ , the mean level spacing of the edge. At low temperatures, T < Δ , finite size effects play an important role in heat transport, for both types of contacts. The nature of the contacts manifests itself in different power laws for the thermal conductance as a function of the temperature. For capacitive couplings, a highly nonuniversal behavior takes place, through a prefactor that depends on the length of the edge as well as on the coupling strengths and the filling fraction. For larger temperatures, T >Δ , finite-size effects become irrelevant, but the heat transport strongly depends on the strength of the edge-reservoir interactions, in both cases. The thermal conductance for tunneling coupling grows linearly with T , whereas for the capacitive case, it saturates to a value that depends on the coupling strengths and the filling factors of the edge and the contacts. Instituto de Física La Plata |
description |
We study the heat transport along an edge state of a two-dimensional electron gas in the quantum Hall regime, in contact to two reservoirs at different temperatures. We consider two exactly solvable models for the edge state coupled to the reservoirs. The first one corresponds to filling ν=1 and tunneling coupling to the reservoirs. The second one corresponds to integer or fractional filling of the sequence ν = /m (with m odd), and capacitive coupling to the reservoirs. In both cases, we solve the problem by means of nonequilibrium Green function formalism. We show that heat propagates chirally along the edge in the two setups. We identify two temperature regimes, defined by Δ , the mean level spacing of the edge. At low temperatures, T < Δ , finite size effects play an important role in heat transport, for both types of contacts. The nature of the contacts manifests itself in different power laws for the thermal conductance as a function of the temperature. For capacitive couplings, a highly nonuniversal behavior takes place, through a prefactor that depends on the length of the edge as well as on the coupling strengths and the filling fraction. For larger temperatures, T >Δ , finite-size effects become irrelevant, but the heat transport strongly depends on the strength of the edge-reservoir interactions, in both cases. The thermal conductance for tunneling coupling grows linearly with T , whereas for the capacitive case, it saturates to a value that depends on the coupling strengths and the filling factors of the edge and the contacts. |
publishDate |
2013 |
dc.date.none.fl_str_mv |
2013-08-23 |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion Articulo http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
format |
article |
status_str |
publishedVersion |
dc.identifier.none.fl_str_mv |
http://sedici.unlp.edu.ar/handle/10915/125905 |
url |
http://sedici.unlp.edu.ar/handle/10915/125905 |
dc.language.none.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
info:eu-repo/semantics/altIdentifier/issn/1098-0121 info:eu-repo/semantics/altIdentifier/issn/1550-235x info:eu-repo/semantics/altIdentifier/arxiv/1305.5833 info:eu-repo/semantics/altIdentifier/doi/10.1103/physrevb.88.085122 |
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http://creativecommons.org/licenses/by-nc-sa/4.0/ Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0) |
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