Abnormal Seebeck Effect in Vertically Stacked 2D/2D PtSe2/PtSe2 Homostructure

Abstract When a thermoelectric (TE) material is deposited with a secondary TE material, the total Seebeck coefficient of the stacked layer is generally represented by a parallel conductor model. Accordingly, when TE material layers of the same thickness are stacked vertically, the total Seebeck coef...

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Main Authors: Won‐Yong Lee, Min‐Sung Kang, Jae Won Choi, Si‐Hoo Kim, No‐Won Park, Gil‐Sung Kim, Yun‐Ho Kim, Eiji Saitoh, Young‐Gui Yoon, Sang‐Kwon Lee
Format: Article
Language:English
Published: Wiley 2022-12-01
Series:Advanced Science
Subjects:
Online Access:https://doi.org/10.1002/advs.202203455
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author Won‐Yong Lee
Min‐Sung Kang
Jae Won Choi
Si‐Hoo Kim
No‐Won Park
Gil‐Sung Kim
Yun‐Ho Kim
Eiji Saitoh
Young‐Gui Yoon
Sang‐Kwon Lee
author_facet Won‐Yong Lee
Min‐Sung Kang
Jae Won Choi
Si‐Hoo Kim
No‐Won Park
Gil‐Sung Kim
Yun‐Ho Kim
Eiji Saitoh
Young‐Gui Yoon
Sang‐Kwon Lee
author_sort Won‐Yong Lee
collection DOAJ
description Abstract When a thermoelectric (TE) material is deposited with a secondary TE material, the total Seebeck coefficient of the stacked layer is generally represented by a parallel conductor model. Accordingly, when TE material layers of the same thickness are stacked vertically, the total Seebeck coefficient in the transverse direction may change in a single layer. Here, an abnormal Seebeck effect in a stacked two‐dimensional (2D) PtSe2/PtSe2 homostructure film, i.e., an extra in‐plane Seebeck voltage is produced by wet‐transfer stacking at the interface between the PtSe2 layers under a transverse temperature gradient is reported. This abnormal Seebeck effect is referred to as the interfacial Seebeck effect in stacked PtSe2/PtSe2 homostructures. This effect is attributed to the carrier‐interface interaction, and has independent characteristics in relation to carrier concentration. It is confirmed that the in‐plane Seebeck coefficient increases as the number of stacked PtSe2 layers increase and observed a high Seebeck coefficient exceeding ≈188 µV K−1 at 300 K in a four‐layer‐stacked PtSe2/PtSe2 homostructure.
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spelling doaj.art-f74eb2bffbde4b1998e3b5a6b9416ecc2022-12-29T14:19:16ZengWileyAdvanced Science2198-38442022-12-01936n/an/a10.1002/advs.202203455Abnormal Seebeck Effect in Vertically Stacked 2D/2D PtSe2/PtSe2 HomostructureWon‐Yong Lee0Min‐Sung Kang1Jae Won Choi2Si‐Hoo Kim3No‐Won Park4Gil‐Sung Kim5Yun‐Ho Kim6Eiji Saitoh7Young‐Gui Yoon8Sang‐Kwon Lee9Department of Physics Center for Berry Curvature based New Phenomena Chung‐Ang University Seoul 06974 Republic of KoreaDepartment of Physics Center for Berry Curvature based New Phenomena Chung‐Ang University Seoul 06974 Republic of KoreaDepartment of Physics Center for Berry Curvature based New Phenomena Chung‐Ang University Seoul 06974 Republic of KoreaDepartment of Physics Center for Berry Curvature based New Phenomena Chung‐Ang University Seoul 06974 Republic of KoreaDepartment of Physics Center for Berry Curvature based New Phenomena Chung‐Ang University Seoul 06974 Republic of KoreaDepartment of Physics Center for Berry Curvature based New Phenomena Chung‐Ang University Seoul 06974 Republic of KoreaDepartment of Physics Center for Berry Curvature based New Phenomena Chung‐Ang University Seoul 06974 Republic of KoreaDepartment of Applied Physics The University of Tokyo Tokyo 113–8656 JapanDepartment of Physics Center for Berry Curvature based New Phenomena Chung‐Ang University Seoul 06974 Republic of KoreaDepartment of Physics Center for Berry Curvature based New Phenomena Chung‐Ang University Seoul 06974 Republic of KoreaAbstract When a thermoelectric (TE) material is deposited with a secondary TE material, the total Seebeck coefficient of the stacked layer is generally represented by a parallel conductor model. Accordingly, when TE material layers of the same thickness are stacked vertically, the total Seebeck coefficient in the transverse direction may change in a single layer. Here, an abnormal Seebeck effect in a stacked two‐dimensional (2D) PtSe2/PtSe2 homostructure film, i.e., an extra in‐plane Seebeck voltage is produced by wet‐transfer stacking at the interface between the PtSe2 layers under a transverse temperature gradient is reported. This abnormal Seebeck effect is referred to as the interfacial Seebeck effect in stacked PtSe2/PtSe2 homostructures. This effect is attributed to the carrier‐interface interaction, and has independent characteristics in relation to carrier concentration. It is confirmed that the in‐plane Seebeck coefficient increases as the number of stacked PtSe2 layers increase and observed a high Seebeck coefficient exceeding ≈188 µV K−1 at 300 K in a four‐layer‐stacked PtSe2/PtSe2 homostructure.https://doi.org/10.1002/advs.202203455homostructurehot‐carrier injectionin‐plane Seebeck effectinterfacial Seebeck effectMott relationplatinum diselenide
spellingShingle Won‐Yong Lee
Min‐Sung Kang
Jae Won Choi
Si‐Hoo Kim
No‐Won Park
Gil‐Sung Kim
Yun‐Ho Kim
Eiji Saitoh
Young‐Gui Yoon
Sang‐Kwon Lee
Abnormal Seebeck Effect in Vertically Stacked 2D/2D PtSe2/PtSe2 Homostructure
Advanced Science
homostructure
hot‐carrier injection
in‐plane Seebeck effect
interfacial Seebeck effect
Mott relation
platinum diselenide
title Abnormal Seebeck Effect in Vertically Stacked 2D/2D PtSe2/PtSe2 Homostructure
title_full Abnormal Seebeck Effect in Vertically Stacked 2D/2D PtSe2/PtSe2 Homostructure
title_fullStr Abnormal Seebeck Effect in Vertically Stacked 2D/2D PtSe2/PtSe2 Homostructure
title_full_unstemmed Abnormal Seebeck Effect in Vertically Stacked 2D/2D PtSe2/PtSe2 Homostructure
title_short Abnormal Seebeck Effect in Vertically Stacked 2D/2D PtSe2/PtSe2 Homostructure
title_sort abnormal seebeck effect in vertically stacked 2d 2d ptse2 ptse2 homostructure
topic homostructure
hot‐carrier injection
in‐plane Seebeck effect
interfacial Seebeck effect
Mott relation
platinum diselenide
url https://doi.org/10.1002/advs.202203455
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