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Electronic Transport Properties of Silicane Determined from First Principles

Silicane, a hydrogenated monolayer of hexagonal silicon, is a candidate material for future complementary metal-oxide-semiconductor technology. We determined the phonon-limited mobility and the velocity-field characteristics for electrons and holes in silicane from first principles, relying on densi...

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Autores principales: Khatami, Mohammad Mahdi, Gaddemane, Gautam, Van de Put, Maarten L., Fischetti, Massimo V., Moravvej-Farshi, Mohammad Kazem, Pourfath, Mahdi, Vandenberghe, William G.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6766188/
https://www.ncbi.nlm.nih.gov/pubmed/31514338
http://dx.doi.org/10.3390/ma12182935
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author Khatami, Mohammad Mahdi
Gaddemane, Gautam
Van de Put, Maarten L.
Fischetti, Massimo V.
Moravvej-Farshi, Mohammad Kazem
Pourfath, Mahdi
Vandenberghe, William G.
author_facet Khatami, Mohammad Mahdi
Gaddemane, Gautam
Van de Put, Maarten L.
Fischetti, Massimo V.
Moravvej-Farshi, Mohammad Kazem
Pourfath, Mahdi
Vandenberghe, William G.
author_sort Khatami, Mohammad Mahdi
collection PubMed
description Silicane, a hydrogenated monolayer of hexagonal silicon, is a candidate material for future complementary metal-oxide-semiconductor technology. We determined the phonon-limited mobility and the velocity-field characteristics for electrons and holes in silicane from first principles, relying on density functional theory. Transport calculations were performed using a full-band Monte Carlo scheme. Scattering rates were determined from interpolated electron–phonon matrix elements determined from density functional perturbation theory. We found that the main source of scattering for electrons and holes was the ZA phonons. Different cut-off wavelengths ranging from 0.58 nm to 16 nm were used to study the possible suppression of the out-of-plane acoustic (ZA) phonons. The low-field mobility of electrons (holes) was obtained as 5 (10) cm(2)/(Vs) with a long wavelength ZA phonon cut-off of 16 nm. We showed that higher electron (hole) mobilities of 24 (101) cm(2)/(Vs) can be achieved with a cut-off wavelength of 4 nm, while completely suppressing ZA phonons results in an even higher electron (hole) mobility of 53 (109) cm(2)/(Vs). Velocity-field characteristics showed velocity saturation at 3 × 10(5) V/cm, and negative differential mobility was observed at larger fields. The silicane mobility was competitive with other two-dimensional materials, such as transition-metal dichalcogenides or phosphorene, predicted using similar full-band Monte Carlo calculations. Therefore, silicon in its most extremely scaled form remains a competitive material for future nanoscale transistor technology, provided scattering with out-of-plane acoustic phonons could be suppressed.
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spelling pubmed-67661882019-09-30 Electronic Transport Properties of Silicane Determined from First Principles Khatami, Mohammad Mahdi Gaddemane, Gautam Van de Put, Maarten L. Fischetti, Massimo V. Moravvej-Farshi, Mohammad Kazem Pourfath, Mahdi Vandenberghe, William G. Materials (Basel) Article Silicane, a hydrogenated monolayer of hexagonal silicon, is a candidate material for future complementary metal-oxide-semiconductor technology. We determined the phonon-limited mobility and the velocity-field characteristics for electrons and holes in silicane from first principles, relying on density functional theory. Transport calculations were performed using a full-band Monte Carlo scheme. Scattering rates were determined from interpolated electron–phonon matrix elements determined from density functional perturbation theory. We found that the main source of scattering for electrons and holes was the ZA phonons. Different cut-off wavelengths ranging from 0.58 nm to 16 nm were used to study the possible suppression of the out-of-plane acoustic (ZA) phonons. The low-field mobility of electrons (holes) was obtained as 5 (10) cm(2)/(Vs) with a long wavelength ZA phonon cut-off of 16 nm. We showed that higher electron (hole) mobilities of 24 (101) cm(2)/(Vs) can be achieved with a cut-off wavelength of 4 nm, while completely suppressing ZA phonons results in an even higher electron (hole) mobility of 53 (109) cm(2)/(Vs). Velocity-field characteristics showed velocity saturation at 3 × 10(5) V/cm, and negative differential mobility was observed at larger fields. The silicane mobility was competitive with other two-dimensional materials, such as transition-metal dichalcogenides or phosphorene, predicted using similar full-band Monte Carlo calculations. Therefore, silicon in its most extremely scaled form remains a competitive material for future nanoscale transistor technology, provided scattering with out-of-plane acoustic phonons could be suppressed. MDPI 2019-09-11 /pmc/articles/PMC6766188/ /pubmed/31514338 http://dx.doi.org/10.3390/ma12182935 Text en © 2019 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Khatami, Mohammad Mahdi
Gaddemane, Gautam
Van de Put, Maarten L.
Fischetti, Massimo V.
Moravvej-Farshi, Mohammad Kazem
Pourfath, Mahdi
Vandenberghe, William G.
Electronic Transport Properties of Silicane Determined from First Principles
title Electronic Transport Properties of Silicane Determined from First Principles
title_full Electronic Transport Properties of Silicane Determined from First Principles
title_fullStr Electronic Transport Properties of Silicane Determined from First Principles
title_full_unstemmed Electronic Transport Properties of Silicane Determined from First Principles
title_short Electronic Transport Properties of Silicane Determined from First Principles
title_sort electronic transport properties of silicane determined from first principles
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6766188/
https://www.ncbi.nlm.nih.gov/pubmed/31514338
http://dx.doi.org/10.3390/ma12182935
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