Phase Selection in Self-catalyzed GaAs Nanowires
Author(s) -
Federico Panciera,
Zhaslan Baraissov,
G. Patriarche,
В. Г. Дубровский,
Frank Glas,
Laurent Travers,
Utkur Mirsaidov,
JeanChristophe Harmand
Publication year - 2020
Publication title -
nano letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 4.853
H-Index - 488
eISSN - 1530-6992
pISSN - 1530-6984
DOI - 10.1021/acs.nanolett.9b04808
Subject(s) - wurtzite crystal structure , nanowire , materials science , phase (matter) , heterojunction , molecular beam epitaxy , nanotechnology , chemical physics , crystal (programming language) , vapor–liquid–solid method , transmission electron microscopy , epitaxy , crystallography , optoelectronics , condensed matter physics , chemistry , physics , organic chemistry , layer (electronics) , zinc , computer science , metallurgy , programming language
Crystal phase switching between the zincblende and wurtzite structures in III-V nanowires is crucial from the fundamental viewpoint as well as for electronic and photonic applications of crystal phase heterostructures. Here, the results of in situ monitoring of self-catalyzed vapor-liquid-solid growth of GaAs nanowires by molecular beam epitaxy inside a transmission electron microscope are presented. It is demonstrated that the occurrence of the zincblende or wurtzite phase in self-catalyzed nanowires is determined by the sole parameter, the droplet contact angle, which can be finely tuned by changing the group III and V fluxes. The zincblende phase forms at small (<100°) and large (>125°) contact angles, whereas pure wurtzite phase is observed for intermediate contact angles. Wurtzite nanowires are restricted by vertical sidewalls, whereas zincblende nanowires taper or develop the truncated edge at their top. These findings are explained within a dedicated model for the surface energetics. These results give a clear route for the crystal phase control in Au-free III-V nanowires. On a more general note, in situ growth monitoring with atomic resolution and at the technological-relevant growth rates is shown to be a powerful tool for the fine-tuning of material properties at the nanoscale.
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