Imaging current distribution in a topological insulator Bi2Se3 in the presence of competing surface and bulk contributions to conductivity

Abstract Two-dimensional (2D) topological surface states in a three-dimensional topological insulator (TI) should produce uniform 2D surface current distribution. However, our transport current imaging studies on Bi2Se3 thin film reveal non-uniform current sheet flow at 15 K with strong edge current...

Descripción completa

Guardado en:
Detalles Bibliográficos
Autores principales: Amit Jash, Ankit Kumar, Sayantan Ghosh, A. Bharathi, S. S. Banerjee
Formato: article
Lenguaje:EN
Publicado: Nature Portfolio 2021
Materias:
R
Q
Acceso en línea:https://doaj.org/article/2fe1dc8fee054417bf9fb73106b32c33
Etiquetas: Agregar Etiqueta
Sin Etiquetas, Sea el primero en etiquetar este registro!
id oai:doaj.org-article:2fe1dc8fee054417bf9fb73106b32c33
record_format dspace
spelling oai:doaj.org-article:2fe1dc8fee054417bf9fb73106b32c332021-12-02T13:27:08ZImaging current distribution in a topological insulator Bi2Se3 in the presence of competing surface and bulk contributions to conductivity10.1038/s41598-021-86706-02045-2322https://doaj.org/article/2fe1dc8fee054417bf9fb73106b32c332021-04-01T00:00:00Zhttps://doi.org/10.1038/s41598-021-86706-0https://doaj.org/toc/2045-2322Abstract Two-dimensional (2D) topological surface states in a three-dimensional topological insulator (TI) should produce uniform 2D surface current distribution. However, our transport current imaging studies on Bi2Se3 thin film reveal non-uniform current sheet flow at 15 K with strong edge current flow. This is consistent with other imaging studies on thin films of Bi2Se3. In contrast to strong edge current flow in thin films, in single crystal of Bi2Se3 at 15 K our current imaging studies show the presence of 3.6 nm thick uniform 2D sheet current flow. Above 70 K, this uniform 2D sheet current sheet begins to disintegrate into a spatially non-uniform flow. The flow becomes patchy with regions having high and low current density. The area fraction of the patches with high current density rapidly decreases at temperatures above 70 K, with a temperature dependence of the form $$1/\left| {T - 70} \right|^{0.35}$$ 1 / T - 70 0.35 . The temperature scale of 70 K coincides with the onset of bulk conductivity in the crystal due to electron doping by selenium vacancy clusters in Bi2Se3. Thus our results show a temperature dependent competition between surface and bulk conductivity produces a temperature dependent variation in uniformity of current flow in the topological insulator.Amit JashAnkit KumarSayantan GhoshA. BharathiS. S. BanerjeeNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 11, Iss 1, Pp 1-9 (2021)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Amit Jash
Ankit Kumar
Sayantan Ghosh
A. Bharathi
S. S. Banerjee
Imaging current distribution in a topological insulator Bi2Se3 in the presence of competing surface and bulk contributions to conductivity
description Abstract Two-dimensional (2D) topological surface states in a three-dimensional topological insulator (TI) should produce uniform 2D surface current distribution. However, our transport current imaging studies on Bi2Se3 thin film reveal non-uniform current sheet flow at 15 K with strong edge current flow. This is consistent with other imaging studies on thin films of Bi2Se3. In contrast to strong edge current flow in thin films, in single crystal of Bi2Se3 at 15 K our current imaging studies show the presence of 3.6 nm thick uniform 2D sheet current flow. Above 70 K, this uniform 2D sheet current sheet begins to disintegrate into a spatially non-uniform flow. The flow becomes patchy with regions having high and low current density. The area fraction of the patches with high current density rapidly decreases at temperatures above 70 K, with a temperature dependence of the form $$1/\left| {T - 70} \right|^{0.35}$$ 1 / T - 70 0.35 . The temperature scale of 70 K coincides with the onset of bulk conductivity in the crystal due to electron doping by selenium vacancy clusters in Bi2Se3. Thus our results show a temperature dependent competition between surface and bulk conductivity produces a temperature dependent variation in uniformity of current flow in the topological insulator.
format article
author Amit Jash
Ankit Kumar
Sayantan Ghosh
A. Bharathi
S. S. Banerjee
author_facet Amit Jash
Ankit Kumar
Sayantan Ghosh
A. Bharathi
S. S. Banerjee
author_sort Amit Jash
title Imaging current distribution in a topological insulator Bi2Se3 in the presence of competing surface and bulk contributions to conductivity
title_short Imaging current distribution in a topological insulator Bi2Se3 in the presence of competing surface and bulk contributions to conductivity
title_full Imaging current distribution in a topological insulator Bi2Se3 in the presence of competing surface and bulk contributions to conductivity
title_fullStr Imaging current distribution in a topological insulator Bi2Se3 in the presence of competing surface and bulk contributions to conductivity
title_full_unstemmed Imaging current distribution in a topological insulator Bi2Se3 in the presence of competing surface and bulk contributions to conductivity
title_sort imaging current distribution in a topological insulator bi2se3 in the presence of competing surface and bulk contributions to conductivity
publisher Nature Portfolio
publishDate 2021
url https://doaj.org/article/2fe1dc8fee054417bf9fb73106b32c33
work_keys_str_mv AT amitjash imagingcurrentdistributioninatopologicalinsulatorbi2se3inthepresenceofcompetingsurfaceandbulkcontributionstoconductivity
AT ankitkumar imagingcurrentdistributioninatopologicalinsulatorbi2se3inthepresenceofcompetingsurfaceandbulkcontributionstoconductivity
AT sayantanghosh imagingcurrentdistributioninatopologicalinsulatorbi2se3inthepresenceofcompetingsurfaceandbulkcontributionstoconductivity
AT abharathi imagingcurrentdistributioninatopologicalinsulatorbi2se3inthepresenceofcompetingsurfaceandbulkcontributionstoconductivity
AT ssbanerjee imagingcurrentdistributioninatopologicalinsulatorbi2se3inthepresenceofcompetingsurfaceandbulkcontributionstoconductivity
_version_ 1718393021049864192