2019
DOI: 10.1063/1.5091058
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Shape transition in InAs nanostructures formed by Stranski-Krastanow growth mode on InP (001) substrate

Abstract: The shape of InAs nanostructures formed by molecular beam epitaxy on a (001) InP substrate in the Stranski-Krastanow growth mode is studied. A transition from wires to round-shaped islands is observed as a function of the amount of InAs deposited. It is attributed to the non-equivalent energies of the A and B facets existing in zinc blende materials (facets along [1 10] and [110], respectively). This surface energy anisotropy is considered to determine the nanostructure equilibrium shape from the balance betwe… Show more

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Cited by 9 publications
(8 citation statements)
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“…In addition, the height of QNS is also limited, as the InSb adatoms do not have enough energy to migrate to the top of the QNSs due to the usage of low growth temperature. Observations of elongated nanostructures similar to InSb QNSs obtained in this work in other material systems have also been reported …”
Section: Resultssupporting
confidence: 83%
See 1 more Smart Citation
“…In addition, the height of QNS is also limited, as the InSb adatoms do not have enough energy to migrate to the top of the QNSs due to the usage of low growth temperature. Observations of elongated nanostructures similar to InSb QNSs obtained in this work in other material systems have also been reported …”
Section: Resultssupporting
confidence: 83%
“…The crystallographic planes of InSb that align parallel to [110] and [11¯0] directions possess different atomic arrangements. The facets along [110] and [11¯0] directions then have nonequivalent surface energies . This surface energy anisotropy is considered to determine the QNS equilibrium shape, in which, in this case, the facet of InSb QNS along [110] direction is postulated to have a lower surface energy than that of the facet along [11¯0] direction.…”
Section: Resultsmentioning
confidence: 99%
“…In this article, we aim at uncovering the mechanisms responsible for this important morphological evolution. As for some other nanostructures [8], the continuous approach adopted here provides a theoretical frame to explore the energy landscape as a function of the core and shell morphologies for NPs of any size, particularly in the typical experimental range (from 1 to 50 nm [7,[9][10][11]), and as such is a complementary approach to atomistic simulations.…”
Section: Introductionmentioning
confidence: 99%
“…Previously, we have also shown that small and large Qdashes have roughly the same aspect ratios [ 16 ]. This aspect ratio conservation points to the stability and energetic favorability of the {114} facet [ 30 ]. In InAs QDs on GaAs, the stable facet is {136}, which would appear as ~ 29° chevron tails on RHEED images [ 29 ].…”
Section: Resultsmentioning
confidence: 99%