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Photonic crystals in biology

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Poster Session, Tuesday, June 15<br />

Theme A1 - B702<br />

Thermodynamical Properties of Pd-Au and Pt-Au Core-Shell Nanoparticles:<br />

A Molecular Dynamics Study<br />

S. Kaya 1 , S.Ozdemir Kart 1* , T. Cag 2<br />

1 <br />

2<br />

Department of Chemical Eng<strong>in</strong>eer<strong>in</strong>g, Texas A&M University, Texas, TX 77843-3122, USA<br />

Abstract- The thermodynamical properties of Pt-Au and Pd-Au core-shell nanoparticles are studied at constant temperature and constant<br />

volume (TVN) molecular dynamics simulations with the use of quantum corrected Sutton-Chen potential energy function. The nanoparticles<br />

have the spherical core-shell structures with two different diameters of 5 nm and 10 nm. The spherical Pd or Pt is covered with the spherical<br />

Au shell with five different concentrations. The pure metals (Pd, Pt and Au) with the same particle sizes are also studied to compare with the<br />

results of core-shell nanoparticles. The melt<strong>in</strong>g temperature is determ<strong>in</strong>ed by exam<strong>in</strong><strong>in</strong>g the behaviour of the total energy as a function of the<br />

temperature. Simulation results such as k<strong>in</strong>etic energy, potential energy, heat capacity, and latent heat of the fusion are presented. The effects<br />

of the concentration of shell atoms on the physical properties for both core-shells <strong>in</strong>terested <strong>in</strong> this study are also <strong>in</strong>vestigated.<br />

In recent years, metallic nanoparticles attract grow<strong>in</strong>g<br />

<strong>in</strong>terest due to their unique properties -differ<strong>in</strong>g greatly<br />

fro m bulk- result<strong>in</strong>g fro m the large fraction of surface<br />

atoms. Furthermore, core-shell nanoparticles are of<br />

particular <strong>in</strong>terest <strong>in</strong> applications rang<strong>in</strong>g from catalysis to<br />

optical, magnetic and electronic applications because the<br />

properties of nanoparticles can change with not only size<br />

and but also chemical composition [1-4]. Core-shell<br />

nanoparticles are made up of core material coated with<br />

another material. The design of new nanoparticle<br />

functionalized with size, composition and atomic<br />

distribution necessitate the understand<strong>in</strong>g of the structure<br />

and properties of core-shell nanoparticles. In this study, we<br />

are particularly <strong>in</strong>terested <strong>in</strong> the thermodynamic and<br />

structural properties of both Pd-Au and Pt-Au core-shell<br />

nanoparticles. We have performed molecular dynamics<br />

simulations for five different core-shell concentrations by<br />

utiliz<strong>in</strong>g Quantum Sutton-Chen potential [5-6]. They are<br />

arranged as Pd(Pt) n-xAu x , where, n is the mu ltip lier of the<br />

lattice parameter to produce the radius of the<br />

nanoparticles. Here, n is taken as 6 and 12, respectively,<br />

for 5 nm and 10 nm core-shells while x is set as 0, 1, …6<br />

for the small size core-shell and 0, 2, 4, … 12 for the large<br />

size of the one. The total energy, melt<strong>in</strong>g temperature,<br />

specific heat and latent heat of the fusion are calculated as<br />

a function of temperature and concentrations. Atomic<br />

distribution of these core-shell nanoparticles at various<br />

temperatures are shown <strong>in</strong> Figure 1. Melt<strong>in</strong>g temperatures<br />

of the core-shell nanoparticles <strong>in</strong>crease with not only the<br />

size of the spherical nanoparticles, but also the number of<br />

the core atoms of Pd or Pt. Core atoms such as Pd coated<br />

by Au are redistributed among the Au shell atoms at high<br />

temperature as shown <strong>in</strong> Figure 1. c) and d).<br />

Figure 1. Typical snapshop of Pd 4 Au 2 core-shell paricles: halfdisplayed<br />

a)- 300K, b) 1200 K, c) 2000 K and d) full-structure<br />

displayed at 2000K<br />

*Correspond<strong>in</strong>g author: ozsev@pau.edu.tr<br />

[1] F. Delogu, Phys. Rev. B 76, 235421 (2007).<br />

[2] E. E. Zhurk<strong>in</strong>, T. V. Hoof, and M. Hou, Phys. Rev. B, 75,<br />

224102 (2007).<br />

[3] Y. H. Chui, G. Grochola, I. K. Snook, and S. P. Russo. Phys.<br />

Rev. B 75, 033404 (2007).<br />

[4] Z. Yang, X. Yang, and Zhijun Xu, J. Phys. Chem. C 112,<br />

4937 (2008).<br />

[5] Y. Qi, T. Cag<strong>in</strong>, W. L. Johnson, W. A. Goddard III, J. Chem.<br />

Phys. 115, 385 (2001).<br />

[6] H H Kart, G. Wang, I. Karaman an<br />

(2009).<br />

a) 300 K<br />

b) 1200 K<br />

c) 2000 K d) 2000 K<br />

6th Nanoscience and Nanotechnology Conference, zmir, 2010 256

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