Dynamic transition of nanosilicon from indirect to direct-like nature by strain-induced structural relaxation

Silicon nanoclusters exhibit light emission with direct-like ns–µs time dynamics; however, they show variable synthesis and structure, optical, and electronic characteristics. The widely adopted model is a core–shell in which the core is an indirect tetrahedral absorbing Si phase, while the shell is...

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Main Authors: Kevin Mantey, Huw Morgan, Jack Boparai, Zain Yamani, Ersin Bahceci, Munir Hasan Nayfeh
Format: Article
Language:English
Published: AIP Publishing LLC 2021-09-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/5.0050581
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author Kevin Mantey
Huw Morgan
Jack Boparai
Zain Yamani
Ersin Bahceci
Munir Hasan Nayfeh
author_facet Kevin Mantey
Huw Morgan
Jack Boparai
Zain Yamani
Ersin Bahceci
Munir Hasan Nayfeh
author_sort Kevin Mantey
collection DOAJ
description Silicon nanoclusters exhibit light emission with direct-like ns–µs time dynamics; however, they show variable synthesis and structure, optical, and electronic characteristics. The widely adopted model is a core–shell in which the core is an indirect tetrahedral absorbing Si phase, while the shell is a network of re-structured direct-like H–Si–Si–H molecular emitting phases, with the two connected via back Si–Si tetrahedral bonds, exhibiting a potential barrier, which significantly hinders emission. We carried out first-principles atomistic computations of a 1-nm Si nanoparticle to discern the variabilities. Enlarging the network reduces the potential barrier monotonically to a finite limit not sufficient for strong emission to proceed while inducing a path to quenching of emission via a conical crossing between the excited and ground states. However, enlarging the network is found to induce strain and structural instability, which causes structural relaxation that creates a direct path for emission without crossing the barrier. Following emission, the particle relaxes back to the indirect ground structure, which completes the cycle. The results also confirm the pivotal role of HF/H2O2 etching in synthesizing the core–shells and affording control over the molecular network. Measurements using synchrotron and laboratory UV excitation of thin films of 1-nm Si particles show good agreement with the simulation results. It is plausible that the relaxation is behind the stimulated emission, gain, or microscopic laser action, reported earlier in macroscopic distributions of 1- and 3-nm Si nanoparticles.
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spelling doaj.art-5551193a99e34e8a8c8639802f1a2fef2022-12-21T21:30:25ZengAIP Publishing LLCAIP Advances2158-32262021-09-01119095319095319-1610.1063/5.0050581Dynamic transition of nanosilicon from indirect to direct-like nature by strain-induced structural relaxationKevin Mantey0Huw Morgan1Jack Boparai2Zain Yamani3Ersin Bahceci4Munir Hasan Nayfeh5Department of Physics, University of Illinois at Urbana-Champaign, 1110 W. Green Street, Urbana, Illinois 61801, USADepartment of Physics, Aberystwyth University, Penglais, Aberystwyth, Ceredigion SY23 3BZ, United KingdomDepartment of Physics, University of Illinois at Urbana-Champaign, 1110 W. Green Street, Urbana, Illinois 61801, USADepartment of Physics, King Fahd University, Dhahran 34463, Saudi ArabiaDepartment of Metallurgical and Materials Engineering, Iskenderun Technical University, 31200 Hatay, TurkeyDepartment of Physics, University of Illinois at Urbana-Champaign, 1110 W. Green Street, Urbana, Illinois 61801, USASilicon nanoclusters exhibit light emission with direct-like ns–µs time dynamics; however, they show variable synthesis and structure, optical, and electronic characteristics. The widely adopted model is a core–shell in which the core is an indirect tetrahedral absorbing Si phase, while the shell is a network of re-structured direct-like H–Si–Si–H molecular emitting phases, with the two connected via back Si–Si tetrahedral bonds, exhibiting a potential barrier, which significantly hinders emission. We carried out first-principles atomistic computations of a 1-nm Si nanoparticle to discern the variabilities. Enlarging the network reduces the potential barrier monotonically to a finite limit not sufficient for strong emission to proceed while inducing a path to quenching of emission via a conical crossing between the excited and ground states. However, enlarging the network is found to induce strain and structural instability, which causes structural relaxation that creates a direct path for emission without crossing the barrier. Following emission, the particle relaxes back to the indirect ground structure, which completes the cycle. The results also confirm the pivotal role of HF/H2O2 etching in synthesizing the core–shells and affording control over the molecular network. Measurements using synchrotron and laboratory UV excitation of thin films of 1-nm Si particles show good agreement with the simulation results. It is plausible that the relaxation is behind the stimulated emission, gain, or microscopic laser action, reported earlier in macroscopic distributions of 1- and 3-nm Si nanoparticles.http://dx.doi.org/10.1063/5.0050581
spellingShingle Kevin Mantey
Huw Morgan
Jack Boparai
Zain Yamani
Ersin Bahceci
Munir Hasan Nayfeh
Dynamic transition of nanosilicon from indirect to direct-like nature by strain-induced structural relaxation
AIP Advances
title Dynamic transition of nanosilicon from indirect to direct-like nature by strain-induced structural relaxation
title_full Dynamic transition of nanosilicon from indirect to direct-like nature by strain-induced structural relaxation
title_fullStr Dynamic transition of nanosilicon from indirect to direct-like nature by strain-induced structural relaxation
title_full_unstemmed Dynamic transition of nanosilicon from indirect to direct-like nature by strain-induced structural relaxation
title_short Dynamic transition of nanosilicon from indirect to direct-like nature by strain-induced structural relaxation
title_sort dynamic transition of nanosilicon from indirect to direct like nature by strain induced structural relaxation
url http://dx.doi.org/10.1063/5.0050581
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