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Exploiting the Close-to-Dirac Point Shift of the Fermi Level in the Sb(2)Te(3)/Bi(2)Te(3) Topological Insulator Heterostructure for Spin-Charge Conversion

[Image: see text] Properly tuning the Fermi level position in topological insulators is of vital importance to tailor their spin-polarized electronic transport and to improve the efficiency of any functional device based on them. Here, we report the full in situ metal organic chemical vapor depositi...

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Autores principales: Longo, Emanuele, Locatelli, Lorenzo, Tsipas, Polychronis, Lintzeris, Akylas, Dimoulas, Athanasios, Fanciulli, Marco, Longo, Massimo, Mantovan, Roberto
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10623560/
https://www.ncbi.nlm.nih.gov/pubmed/37862590
http://dx.doi.org/10.1021/acsami.3c08830
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author Longo, Emanuele
Locatelli, Lorenzo
Tsipas, Polychronis
Lintzeris, Akylas
Dimoulas, Athanasios
Fanciulli, Marco
Longo, Massimo
Mantovan, Roberto
author_facet Longo, Emanuele
Locatelli, Lorenzo
Tsipas, Polychronis
Lintzeris, Akylas
Dimoulas, Athanasios
Fanciulli, Marco
Longo, Massimo
Mantovan, Roberto
author_sort Longo, Emanuele
collection PubMed
description [Image: see text] Properly tuning the Fermi level position in topological insulators is of vital importance to tailor their spin-polarized electronic transport and to improve the efficiency of any functional device based on them. Here, we report the full in situ metal organic chemical vapor deposition (MOCVD) and study of a highly crystalline Bi(2)Te(3)/Sb(2)Te(3) topological insulator heterostructure on top of large area (4″) Si(111) substrates. The bottom Sb(2)Te(3) layer serves as an ideal seed layer for the growth of highly crystalline Bi(2)Te(3) on top, also inducing a remarkable shift of the Fermi level to place it very close to the Dirac point, as visualized by angle-resolved photoemission spectroscopy. To exploit such ideal topologically protected surface states, we fabricate the simple spin-charge converter Si(111)/Sb(2)Te(3)/Bi(2)Te(3)/Au/Co/Au and probe the spin-charge conversion (SCC) by spin pumping ferromagnetic resonance. A large SCC is measured at room temperature and is interpreted within the inverse Edelstein effect, thus resulting in a conversion efficiency of λ(IEEE) ∼ 0.44 nm. Our results demonstrate the successful tuning of the surface Fermi level of Bi(2)Te(3) when grown on top of Sb(2)Te(3) with a full in situ MOCVD process, which is highly interesting in view of its future technology transfer.
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spelling pubmed-106235602023-11-04 Exploiting the Close-to-Dirac Point Shift of the Fermi Level in the Sb(2)Te(3)/Bi(2)Te(3) Topological Insulator Heterostructure for Spin-Charge Conversion Longo, Emanuele Locatelli, Lorenzo Tsipas, Polychronis Lintzeris, Akylas Dimoulas, Athanasios Fanciulli, Marco Longo, Massimo Mantovan, Roberto ACS Appl Mater Interfaces [Image: see text] Properly tuning the Fermi level position in topological insulators is of vital importance to tailor their spin-polarized electronic transport and to improve the efficiency of any functional device based on them. Here, we report the full in situ metal organic chemical vapor deposition (MOCVD) and study of a highly crystalline Bi(2)Te(3)/Sb(2)Te(3) topological insulator heterostructure on top of large area (4″) Si(111) substrates. The bottom Sb(2)Te(3) layer serves as an ideal seed layer for the growth of highly crystalline Bi(2)Te(3) on top, also inducing a remarkable shift of the Fermi level to place it very close to the Dirac point, as visualized by angle-resolved photoemission spectroscopy. To exploit such ideal topologically protected surface states, we fabricate the simple spin-charge converter Si(111)/Sb(2)Te(3)/Bi(2)Te(3)/Au/Co/Au and probe the spin-charge conversion (SCC) by spin pumping ferromagnetic resonance. A large SCC is measured at room temperature and is interpreted within the inverse Edelstein effect, thus resulting in a conversion efficiency of λ(IEEE) ∼ 0.44 nm. Our results demonstrate the successful tuning of the surface Fermi level of Bi(2)Te(3) when grown on top of Sb(2)Te(3) with a full in situ MOCVD process, which is highly interesting in view of its future technology transfer. American Chemical Society 2023-10-20 /pmc/articles/PMC10623560/ /pubmed/37862590 http://dx.doi.org/10.1021/acsami.3c08830 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Longo, Emanuele
Locatelli, Lorenzo
Tsipas, Polychronis
Lintzeris, Akylas
Dimoulas, Athanasios
Fanciulli, Marco
Longo, Massimo
Mantovan, Roberto
Exploiting the Close-to-Dirac Point Shift of the Fermi Level in the Sb(2)Te(3)/Bi(2)Te(3) Topological Insulator Heterostructure for Spin-Charge Conversion
title Exploiting the Close-to-Dirac Point Shift of the Fermi Level in the Sb(2)Te(3)/Bi(2)Te(3) Topological Insulator Heterostructure for Spin-Charge Conversion
title_full Exploiting the Close-to-Dirac Point Shift of the Fermi Level in the Sb(2)Te(3)/Bi(2)Te(3) Topological Insulator Heterostructure for Spin-Charge Conversion
title_fullStr Exploiting the Close-to-Dirac Point Shift of the Fermi Level in the Sb(2)Te(3)/Bi(2)Te(3) Topological Insulator Heterostructure for Spin-Charge Conversion
title_full_unstemmed Exploiting the Close-to-Dirac Point Shift of the Fermi Level in the Sb(2)Te(3)/Bi(2)Te(3) Topological Insulator Heterostructure for Spin-Charge Conversion
title_short Exploiting the Close-to-Dirac Point Shift of the Fermi Level in the Sb(2)Te(3)/Bi(2)Te(3) Topological Insulator Heterostructure for Spin-Charge Conversion
title_sort exploiting the close-to-dirac point shift of the fermi level in the sb(2)te(3)/bi(2)te(3) topological insulator heterostructure for spin-charge conversion
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10623560/
https://www.ncbi.nlm.nih.gov/pubmed/37862590
http://dx.doi.org/10.1021/acsami.3c08830
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