Anomalous Seebeck effect and counter-propagating ballistic currents in graphene

Fuente: arXiv
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Main Authors: Kavokin, A. V., Kavokina, S. V., Varlamov, A. A., Yerin, Yuriy
Format: Preprint
Published: 2024
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author Kavokin, A. V.
Kavokina, S. V.
Varlamov, A. A.
Yerin, Yuriy
author_facet Kavokin, A. V.
Kavokina, S. V.
Varlamov, A. A.
Yerin, Yuriy
contents The Seebeck effect consists in the induction of a voltage drop due to the temperature difference in a conductor. In the middle of XIXth century, Lord Kelvin has proposed a relation between the Seebeck coefficient and the derivative of the chemical potential over temperature in the broken circuit regime. This relation appears to be nearly universal as it equally well applies to metals, semimetals and semiconductors. We show that it may fail, however, in graphene, due to the non-locality effects in the ballistic electronic transport regime. The correction to the Kelvin's formula emerges due to the coexistence of counter-propagating non-dissipative currents of cold and hot electrons. The external magnetic field normal to the graphene sample allows separating hot and cold currents in real space. The developed formalism may help interpreting the recent experimental data on ballistic edge currents in graphene bi-layers in the quantum Hall regime [1].
format Preprint
id arxiv_https___arxiv_org_abs_2405_10807
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Anomalous Seebeck effect and counter-propagating ballistic currents in graphene
Kavokin, A. V.
Kavokina, S. V.
Varlamov, A. A.
Yerin, Yuriy
Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
The Seebeck effect consists in the induction of a voltage drop due to the temperature difference in a conductor. In the middle of XIXth century, Lord Kelvin has proposed a relation between the Seebeck coefficient and the derivative of the chemical potential over temperature in the broken circuit regime. This relation appears to be nearly universal as it equally well applies to metals, semimetals and semiconductors. We show that it may fail, however, in graphene, due to the non-locality effects in the ballistic electronic transport regime. The correction to the Kelvin's formula emerges due to the coexistence of counter-propagating non-dissipative currents of cold and hot electrons. The external magnetic field normal to the graphene sample allows separating hot and cold currents in real space. The developed formalism may help interpreting the recent experimental data on ballistic edge currents in graphene bi-layers in the quantum Hall regime [1].
title Anomalous Seebeck effect and counter-propagating ballistic currents in graphene
topic Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
url https://arxiv.org/abs/2405.10807