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  • Thermal and chemical vapor deposition of Si nanowires: Shapecontrol, dispersion, and electrical propertiesA. Colli, A. Fasoli, P. Beecher, P. Servati, S. Pisana et al. Citation: J. Appl. Phys. 102, 034302 (2007); doi: 10.1063/1.2764050 View online: http://dx.doi.org/10.1063/1.2764050 View Table of Contents: http://jap.aip.org/resource/1/JAPIAU/v102/i3 Published by the American Institute of Physics. Related ArticlesTwo-dimensional electron gas related emissions in ZnMgO/ZnO heterostructures Appl. Phys. Lett. 99, 211906 (2011) Strain dependent resistance in chemical vapor deposition grown graphene Appl. Phys. Lett. 99, 213107 (2011) Manipulating InAs nanowires with submicrometer precision Rev. Sci. Instrum. 82, 113705 (2011) Elimination of the weak inversion hump in Si3N4/InGaAs (001) gate stacks using an in situ NH3 pre-treatment Appl. Phys. Lett. 99, 203504 (2011) Influence of the interface on growth rates in AlN/GaN short period superlattices via metal organic vapor phaseepitaxy Appl. Phys. Lett. 99, 201903 (2011) Additional information on J. Appl. Phys.Journal Homepage: http://jap.aip.org/ Journal Information: http://jap.aip.org/about/about_the_journal Top downloads: http://jap.aip.org/features/most_downloaded Information for Authors: http://jap.aip.org/authors

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  • Thermal and chemical vapor deposition of Si nanowires:Shape control, dispersion, and electrical properties

    A. Colli,a A. Fasoli, P. Beecher, P. Servati,b S. Pisana, Y. Fu, A. J. Flewitt, W. I. Milne,and J. RobertsonDepartment of Engineering, University of Cambridge, Cambridge CB3 0FA, United Kingdom

    C. DucatiDepartment of Materials Science and Metallurgy, University of Cambridge, Cambridge CB3 6GF,United Kingdom

    S. De FranceschiLaboratoire de Transport Electronique Quantique et Supraconductivit, CEA-Grenoble,38054 Grenoble cedex 9, France

    S. Hofmann and A. C. Ferraric

    Department of Engineering, University of Cambridge, Cambridge CB3 0FA, United Kingdom

    Received 21 March 2007; accepted 14 June 2007; published online 6 August 2007

    We investigate and compare complementary approaches to SiNW production in terms of yield,morphology control, and electrical properties. Vapor-phase techniques are considered, includingchemical vapor deposition with or without the assistance of a plasma and thermal evaporation. Wereport Au-catalyzed nucleation of SiNWs at temperatures as low as 300 C using SiH4 as precursor.We get yields up to several milligrams by metal-free condensation of SiO powders. For allprocesses, we control the final nanostructure morphology. We then report concentrated and stabledispersions of SiNWs in solvents compatible with semiconducting organic polymers. Finally, weinvestigate the electrical response of intrinsic SiNWs grown by different methods. All our SiNWsexhibit p-type behavior and comparable performance, though in some cases ambipolar devices areobserved. Thus, processing and morphology, rather than the growth technique, are key to achieveoptimal samples for applications. 2007 American Institute of Physics. DOI: 10.1063/1.2764050

    I. INTRODUCTION

    The bottom-up synthesis of one-dimensional 1D semi-conducting nanostructures has attracted increasing interest inrecent years both for fundamental physics and for potentialdevice applications.18 On the one hand, the capability tosynthesize nanoscale building blocks without the need of ex-pensive and time-consuming lithography techniques offerskey opportunities for high-integration nanoelectronics. Re-search is therefore heading towards the realization of single-nanowire NW or crossed-NW devices with the aim of in-tegrating a large number of active components into a rationalgeometry.35,9,10 On the other hand, applications are envis-aged where nanostructured materials do not require indi-vidual manipulation but are assembled as bulk, while indi-vidually retaining their nanoscale properties such as quantumconfinement or large surface-to-volume ratio.68,11,12 As aconsequence, several synthesis approaches are being devel-oped to match the specific requirements of different possibleapplications. Bulk production of nanocrystals both insolution13,14 or from the vapor phase15,16 for post-growthmanipulation has received as much attention as the selectiveand oriented growth of NWs directly into devices.17,18

    Si nanowires SiNWs are particularly relevant due to

    the central role of Si in the semiconductor industry. Deposi-tion techniques for SiNWs include laser ablation16,19 hightemperature thermal evaporation,2022 molecular beam epi-taxy MBE,23 chemical vapor deposition CVD,2426 andplasma-enhanced CVD PECVD.27

    CVD is probably the most investigated synthesis tech-nique for SiNWs.2426 Generally, a metal nanoparticle is re-quired to favor selective decomposition of the precursor gasand the consequent nucleation of substrate-bound 1Dnanostructures.28,29 By patterning the catalyst on orientedcrystalline substrates, defined and oriented arrays of SiNWshave been fabricated.26 This highlights the potential of theCVD approach for the realization of bottom-up nanoscaledevices, where active components are no longer manufac-tured but grown from point to point in a controlled fashion.In this framework, however, the fabrication step involvingNW synthesis must be compatible with the whole processflow. This implies, for example, that the NW growth tem-perature must be low enough to ensure compatibility with thefinal device substrate. Efforts are therefore addressed to fullyunderstand the physics and chemistry behind the growth ofsemiconductor NWs and to explore the lowest growth tem-perature achievable by the metal-assisted mechanism.3034

    Bulk production is emerging as an alternative approachfor the fabrication and assembly of NWs in large quantities.Several growth strategies have been proposed to achievelarge-scale SiNW growth, most of them still requiring thepresence of a metal catalyst to promote 1D nucleation.16,1922

    aElectronic mail: [email protected] address: University of British Columbia, 2332 Main Mall, Vancou-

    ver, BC V6T 1Z4, Canada.cElectronic mail: [email protected]

    JOURNAL OF APPLIED PHYSICS 102, 034302 2007

    0021-8979/2007/1023/034302/13/$23.00 2007 American Institute of Physics102, 034302-1

    Downloaded 27 Nov 2011 to 131.111.129.170. Redistribution subject to AIP license or copyright; see http://jap.aip.org/about/rights_and_permissions

    http://dx.doi.org/10.1063/1.2764050http://dx.doi.org/10.1063/1.2764050http://dx.doi.org/10.1063/1.2764050

  • With process temperatures usually exceeding 1000 C, Au,Fe, Ga, and Sn are mixed to the Si precursor vapor either bythermal evaporation or laser ablation. NWs are collectedfrom the furnace reactor in form of woolenlike bundles.19,20

    There is a need, however, to avoid the metal contamina-tion potentially arising from the residual catalyst particles.Removing the catalyst postgrowth may require complex andexpensive purification treatments.35 The so-called oxide-assisted growth OAG method provides a viable alternativefor metal-free bulk production of SiNWs.15,36 Reference 37reported the production of milligrams of SiNWs by thermalevaporation of SiO. It was suggested that SiO triggers theself-assembly of SiNWs, based on the observation that pureSi or pure SiO2 as precursor materials gave negligibleyield.38 Indeed, a SiOx x1 thin film 1.3 nm was alsofound to promote the metal-free nucleation of InAs NWs,39,40

    although it was not clear in this case if this process could beexplained by the oxide-assisted growth model of Ref. 15. Todate, evaporation of SiO or mixtures of Si and SiO2 stillremains the most flexible and reliable approach to metal-freeSiNW synthesis.37,38,41 This method, however, has limita-tions for the shape control and uniformity of the resultingnanostructures. Thin and crystalline SiNWs are oftencoupled with partially or fully oxidized structures, resultingin crystalline S