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book of abstracts - IM2NP

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A B S T R A C T S MONDAY, JUNE 28 N A N O S E A 2 0 1 0<br />

Room Calendal<br />

10h30-11h10<br />

Nanoscale phase transitions and nanowire growth.<br />

J. Ters<strong>of</strong>f (IBM Watson Research Center Yorktown Heights NY 10598 USA)<br />

Semiconductor nanowires can be readily grown from tiny catalyst particles. These wires, with diameters as<br />

small as a few nanometers, have attracted intense interest due to their potential applications in nanoscale<br />

technologies. At the same time, they <strong>of</strong>fer a unique opportunity to deepen our understanding <strong>of</strong> crystal<br />

growth. It has long been realized that novel effects are expected for growth at the nanoscale. But only<br />

recently has it become possible to measure these effects directly, using in-situ microscopy.<br />

This talk will describe some recent progress in understanding growth at the nanoscale, by combining<br />

experimental observations, theoretical modeling, and direct computer simulation <strong>of</strong> nanowire growth [1-3].<br />

We studied the sequence <strong>of</strong> phase transformations as a Au seed particle is exposed to disilane to initiate<br />

nanowire growth. On an inert substrate and above the eutectic temperature, the system progresses from Au<br />

to a two-phase Au+AuSi eutectic system, to liquid AuSi, and finally to AuSi+Si, initiating nanowire growth<br />

[2,3]. By comparing the experimental measurements with a simple theoretical model, we determine the<br />

changes in the equilibrium phase diagram for nanoscale systems, and the effect <strong>of</strong> system size on the<br />

nucleation process. We also find dramatic deviations from equilibrium due to kinetic effects in nanowire<br />

growth. We have developed a theoretical model for the eutectic system evolution, allowing direct computer<br />

simulation <strong>of</strong> nanowire growth [3]. These simulations shed light on how material properties and growth<br />

conditions control the wire morphology and growth stability [3].<br />

* Work done in collaboration with K.W. Schwarz, B.J. Kim, S. Kodambaka, E.A. Stach, and F.M. Ross.<br />

[1] B. J. Kim, J. Ters<strong>of</strong>f, S. Kodambaka, M. C. Reuter, E. A. Stach, and F. M. Ross, Science 322, 1070 (2008).<br />

[2] K. W. Schwarz and J. Ters<strong>of</strong>f, Phys. Rev. Lett. 102, 206101 (2009).<br />

[3] B. J. Kim, J. Ters<strong>of</strong>f, C.-Y. Wen, M. C. Reuter, E. A. Stach, and F. M. Ross, Phys. Rev. Lett. 103, 155701 (2009)<br />

11h10-11h30<br />

Microstructure and compositional study <strong>of</strong> MBE grown ZnSe NWs with<br />

CdSe inclusions.<br />

S. Tatarenko (Nanophysics and Semiconductors Group, INAC and Institut NEEL, CEA/CNRS/University<br />

Joseph Fourier, France) serge.tatarenko@grenoble.cnrs.fr<br />

We have recently shown that a single CdSe quantum dot embedded in a ZnSe nanowire (NW) is an efficient<br />

single photon source operating at a temperature as high as 220K [1]. However, when grown on an oxidized<br />

Si (001) substrate in the VLS growth mode catalyzed by gold particles, the NWs present a random<br />

distribution <strong>of</strong> orientations and densities.<br />

In this contribution we report on the epitaxial growth <strong>of</strong> ZnSe/CdSe NWs on 2D epitaxial ZnSe (100) on<br />

GaAs (100) substrate. Scanning electron microscopy (SEM) and High Resolution Transmission Electron<br />

Microscopy (HRTEM) images (Fig 1) show ZnSe NWs with hexagonal wurtzite structure along the [0001]<br />

axis and also NWs with cubic zinc-blende structure along the [100] axis. The presence <strong>of</strong> different NW<br />

orientations is attributed in part to the formation <strong>of</strong> [110] oriented nanotrenches generated by Au dewetting<br />

at 530°C [2, 3]. The first steps <strong>of</strong> the growth for both growth directions will be presented in details as well<br />

as the influence <strong>of</strong> the growth parameters.<br />

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