Review Article
Preferential Interface Nucleation: An Expansion of the VLS Growth Mechanism for Nanowires
Article first published online: 25 NOV 2008
DOI: 10.1002/adma.200800440
Copyright © 2009 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
Additional Information
How to Cite
Wacaser, B. A., Dick, K. A., Johansson, J., Borgström, M. T., Deppert, K. and Samuelson, L. (2009), Preferential Interface Nucleation: An Expansion of the VLS Growth Mechanism for Nanowires. Adv. Mater., 21: 153–165. doi: 10.1002/adma.200800440
Publication History
- Issue published online: 2 JAN 2009
- Article first published online: 25 NOV 2008
- Manuscript Revised: 30 MAY 2008
- Manuscript Received: 14 FEB 2008
Funded by
- Swedish Research Council (VR)
- Swedish Foundation for Strategic Research (SSF)
- Knut and Alice Wallenberg Foundation
- NoE SANDiE (EU). Grant Number: E500101-2
- IP NODE (EU). Grant Number: 015783 NODE
- Abstract
- References
- Cited By
Keywords:
- crystal growth;
- semiconductors;
- nanotubes;
- nanowires
Abstract
A review and expansion of the fundamental processes of the vapor–liquid–solid (VLS) growth mechanism for nanowires is presented. Although the focus is on nanowires, most of the concepts may be applicable to whiskers, nanotubes, and other unidirectional growth. Important concepts in the VLS mechanism such as preferred deposition, supersaturation, and nucleation are examined. Nanowire growth is feasible using a wide range of apparatuses, material systems, and growth conditions. For nanowire growth the unidirectional growth rate must be much higher than growth rates of other surfaces and interfaces. It is concluded that a general, system independent mechanism should describe why nanowires grow faster than the surrounding surfaces. This mechanism is based on preferential nucleation at the interface between a mediating material called the collector and a crystalline solid. The growth conditions used mean the probability of nucleation is low on most of the surfaces and interfaces. Nucleation at the collector-crystal interface is however different and of special significance is the edge of the collector-crystal interface where all three phases meet. Differences in nucleation due to different crystallographic interfaces can occur even in two phase systems. We briefly describe how these differences in nucleation may account for nanowire growth without a collector. Identifying the mechanism of nanowire growth by naming the three phases involved began with the naming of the VLS mechanism. Unfortunately this trend does not emphasize the important concepts of the mechanism and is only relevant to one three phase system. We therefore suggest the generally applicable term preferential interface nucleation as a replacement for these different names focusing on a unifying mechanism in nanowire growth.

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