2012
DOI: 10.1021/nl303323t
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Evidence for Structural Phase Transitions Induced by the Triple Phase Line Shift in Self-Catalyzed GaAs Nanowires

Abstract: Self-catalyzed growth of GaAs nanowires are widely ascribed to the vapor-liquid-solid (VLS) mechanism due to the presence of Ga particles at the nanowire tips. Here we report synthesis of self-catalyzed GaAs nanowires by molecular-beam epitaxy covering a large growth parameter space. By carefully controlling the Ga flux and its ratio with the As flux, GaAs nanowires without Ga particles and exhibiting a flat growth front are produced. Using scanning electron microscopy and high-resolution transmission electron… Show more

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Cited by 83 publications
(122 citation statements)
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“…However, it is very uncertain under which material systems and growth conditions ideal regime I conditions applies. It is likely that it is only relevant under non-steady-state conditions where the liquid decreases significantly in size, such as immediately after closing the shutter of the group III source or upon during cool down where the nucleation barrier is lowered [27]. But as recent in-situ TEM experiments [40][41][42] strongly suggests and as shown in the modelling examples in section 3.5, regime II may be a dominant VLS steady-state growth mode.…”
Section: Nucleation Limited Growthmentioning
confidence: 98%
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“…However, it is very uncertain under which material systems and growth conditions ideal regime I conditions applies. It is likely that it is only relevant under non-steady-state conditions where the liquid decreases significantly in size, such as immediately after closing the shutter of the group III source or upon during cool down where the nucleation barrier is lowered [27]. But as recent in-situ TEM experiments [40][41][42] strongly suggests and as shown in the modelling examples in section 3.5, regime II may be a dominant VLS steady-state growth mode.…”
Section: Nucleation Limited Growthmentioning
confidence: 98%
“…If we assume a barrier free al transition, the exponentials vanish in equation (37) and the only dependence on δµ a j −ERS,III(V) is through the diffusion lengths. δµ a j −ERS,III(V) (ρ j,III , ρ j,V , T ) at z = L NW can now be solved numerically at every step time in a double iterative process for …”
Section: A2 Adatom Transition State Diffusion Calculations Using Anmentioning
confidence: 99%
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