2019
DOI: 10.1021/acs.nanolett.9b01345
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Strong Hot Carrier Effects in Single Nanowire Heterostructures

Abstract: We use transient Rayleigh scattering to study the thermalization of hot photoexcited carriers in single GaAs 0.7 Sb 0.3 / InP nanowire heterostructures. By comparing the energy loss rate in single core-only GaAs 0.7 Sb 0.3 nanowires which do not show substantial hot carrier effects with the coreshell nanowires, we show that the presence of an InP shell substantially suppresses the longitudinal optical phonon emission rate at low temperatures which then leads to strong hot carrier effects.

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Cited by 14 publications
(20 citation statements)
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References 50 publications
(118 reference statements)
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“…3(c). 18 The energy loss rate due to optical phonons was found to decrease by an order of magnitude at 300 K for nanowires with the InP shell (and more than two orders at 10 K). While this is indeed a noticeable change, it remains unclear if this increase is due to extra functionality enabled by the shell itself, or due to hot-carrier lifetimes being typically longer in InP than in GaAs, assuming the GaAsSb properties are close to those for GaAs.…”
Section: Iva Ultra-fast Probing Of Carrier Relaxationmentioning
confidence: 97%
See 3 more Smart Citations
“…3(c). 18 The energy loss rate due to optical phonons was found to decrease by an order of magnitude at 300 K for nanowires with the InP shell (and more than two orders at 10 K). While this is indeed a noticeable change, it remains unclear if this increase is due to extra functionality enabled by the shell itself, or due to hot-carrier lifetimes being typically longer in InP than in GaAs, assuming the GaAsSb properties are close to those for GaAs.…”
Section: Iva Ultra-fast Probing Of Carrier Relaxationmentioning
confidence: 97%
“…ref. 18 Copyright © 2019, American Chemical Society. This is the author's peer reviewed, accepted manuscript.…”
Section: Iva Ultra-fast Probing Of Carrier Relaxationmentioning
confidence: 99%
See 2 more Smart Citations
“…Despite the extensive work on the topic, most studies involved only a macroscopic description of the problem, while the fewer existing state-of-the-art modelling of the NESS have several limitations. First, the tenet that the photo-excited HCs ultimately achieve the lattice temperature in the steady-state [31] has been challenged in a recent experiment on group III-V semiconductors; it unveils that in the NESS carrier temperatures can be much higher than lattice temperature [32][33][34][35]. A theoretical understanding of the existence of such a high carrier-temperature in NESS is still lacking [32][33][34][35], especially in light of the different techniques available for measuring the various temperatures.…”
Section: Introductionmentioning
confidence: 99%