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Poster Session, Tuesday, June 15<br />

Theme A1 - B702<br />

Melt<strong>in</strong>g evolution and diffusion behavior of bimetallic CuAu nanoparticles studied molecular<br />

dynamics simulations<br />

Serap Senturk Dalgic 1 * and Unal Domekeli 1<br />

1 Department of Physics, Trakya University, Edirne, 22030, Turkey<br />

Abstract-Molecular dynamics calculations have been performed to study the melt<strong>in</strong>g evolution and atomic diffusion behavior of bimetalic<br />

CuAu nanoparticles with the number of atoms rang<strong>in</strong>g from 1286 to 26066 (diameters around 3–9 nm) The <strong>in</strong>teractions between atoms are<br />

described us<strong>in</strong>g the quantum Sutton – Chen (Q-SC) many – body potential. The obta<strong>in</strong>ed results reveal that the melt<strong>in</strong>g temperatures of<br />

nanoparticles are <strong>in</strong>versely proportional to the reciprocal of the nanoparticle size, and are <strong>in</strong> good agreement with the predictions of the<br />

liquid-drop model. The melt<strong>in</strong>g process can be described as occurr<strong>in</strong>g <strong>in</strong> two stages, firstly the stepwise premelt<strong>in</strong>g of the surface region, and<br />

then the abrupt overall melt<strong>in</strong>g of the whole nanoparticles. The heat of fusion of nanoparticles are also <strong>in</strong>versely proportional to the<br />

reciprocal of the nanoparticle size. In addition, surface energies and entropies have been calculated for each sized CuAu nanoparticle at<br />

melt<strong>in</strong>g po<strong>in</strong>t. The diffusion is ma<strong>in</strong>ly localized to the surface region at low temperatures and <strong>in</strong>creases with the reduction of nanoparticle<br />

size, with the temperature be<strong>in</strong>g held constant.<br />

Bimetallic nanoparticles are of particular <strong>in</strong>terest <strong>in</strong><br />

applications because the nanoparticle properties can vary<br />

dramatically not only with size, as occurs <strong>in</strong> pure<br />

nanoparticles, but also with chemical composition. Cu-Au<br />

is a well-known model bimetallic alloys system, which is<br />

famous for the existence of a temperature-<strong>in</strong>duced orderdisorder<br />

transition and the capability of form<strong>in</strong>g<br />

thermodynamically stable long period superlattice structure<br />

[1]. On the other hand, size and shape effects on formation<br />

enthalpy and melt<strong>in</strong>g process of Cu-Au nanoparticles have<br />

been studied <strong>in</strong> recent years and results have been reported<br />

<strong>in</strong> literature [2-6].<br />

In this work, we have studied the melt<strong>in</strong>g evolution and<br />

diffusion behavior of bimetallic CuAu nanoparticles us<strong>in</strong>g<br />

molecular dynamics calculations with the quantum Sutton-<br />

Chen (Q-SC) potential. The whole melt<strong>in</strong>g process is traced<br />

from the chang<strong>in</strong>g of the local structure, atomic diffusion<br />

and thermodynamics properties such as the atomic energy,<br />

surface energy, heat of fusion and entropy. All spherical<br />

nanoparticles started with geometries constructed from a<br />

large cubic FCC (L1 0<br />

for CuAu) crystal structure us<strong>in</strong>g a<br />

series of spherical cutoff centered at a core of cubes. The<br />

stable structure at 0 K is obta<strong>in</strong>ed through the <strong>in</strong>itial<br />

configurations annealed fully at T=300 K and then cooled<br />

to T=0 K at a cool<strong>in</strong>g rate 0.5 K/ps. In order to get an<br />

energy-optimized structure dur<strong>in</strong>g heat<strong>in</strong>g at a given<br />

temperature for bulk systems it is performed molecular<br />

dynamics under constant temperature and constant pressure<br />

conditions (NPT) with a periodic boundary conditions. For<br />

the nanoparticles, we used the constant volume and<br />

constant temperature (NVT) molecular dynamics without<br />

the periodic boundary conditions. The temperature is<br />

controlled by Nose-Hoover thermostat. Newtonian<br />

equations of motion are <strong>in</strong>tegrated us<strong>in</strong>g the Leapfrog<br />

Verlet method with a time step 2 fs. For the simulation of<br />

the bulk system and nanoparticles the heat<strong>in</strong>g process<br />

consists of a series of MD simulations with temperature<br />

<strong>in</strong>crements T=50 K and relax<strong>in</strong>g time 100ps. However,<br />

for a temperature near the melt<strong>in</strong>g region, we used smaller<br />

temperature <strong>in</strong>crement, T=10 K, and the relaxation time<br />

still keeps 100 ps.<br />

The experimental observation of the melt<strong>in</strong>g phenomena<br />

on a particle is just the surface liquid sk<strong>in</strong> resulted by<br />

surface premelt<strong>in</strong>g. Us<strong>in</strong>g molecular dynamic simulation,<br />

the melt<strong>in</strong>g process and melt<strong>in</strong>g mechanism of<br />

nanoparticles can be analyzed size. In Figure 1, we show<br />

snapshot views of the MD sample with 2708 (D=4nm) at<br />

different temperature. It is observed that CuAu particle with<br />

D=4nm diameter melts at approximately 800 K.<br />

T=300K T =500K T=800K<br />

Figure 1. Snapshot views of the MD sample with N=2708<br />

(D= 4 nm) at a series of temperatures dur<strong>in</strong>g heat<strong>in</strong>g.<br />

To conclude, the melt<strong>in</strong>g evolution of bimetallic CuAu<br />

nanoparticles with the number of atoms rang<strong>in</strong>g from 1286<br />

to 26066 under heat<strong>in</strong>g condition is <strong>in</strong>vestigated by the<br />

molecular dynamics simulations us<strong>in</strong>g Q-SC potentials. It<br />

has been found that the melt<strong>in</strong>g po<strong>in</strong>t is <strong>in</strong>versely<br />

proportional to the reciprocal of the nanoparticle size and<br />

the results are <strong>in</strong> good agreement with the theoretical<br />

analysis from the liquid drop model [7]. The evolution of<br />

atomic configuration and energy with temperature reveals<br />

that the melt<strong>in</strong>g process of CuAu nanoparticles can be<br />

described <strong>in</strong> two stages, the stepwise premelt<strong>in</strong>g from the<br />

surface region and the sudden melt<strong>in</strong>g <strong>in</strong> the <strong>in</strong>terior region.<br />

Ow<strong>in</strong>g to the two stages melt<strong>in</strong>g, the heat of melt<strong>in</strong>g for<br />

nanoparticles should <strong>in</strong>volve two parts. As the particle size<br />

decreases, the heat of fusion, surface energy and entropy<br />

decreases correspond<strong>in</strong>gly. We have also studied the<br />

structural evolution of CuAu nanoparticles with different<br />

temperature. Radial distribution functions are adopted to<br />

explore structural transition. The atomic diffusion <strong>in</strong><br />

nanoparticles is ma<strong>in</strong>ly localized to the surface regions<br />

before the melt<strong>in</strong>g temperature and <strong>in</strong>creases with the<br />

reduction of particle size at the same temperature.<br />

*Correspond<strong>in</strong>g author: dserap@yahoo.com<br />

<br />

13 657 (2005).<br />

[2] W.H.Qi, B.Y. Huang, M.P. Wang, Physica B 404 1761<br />

(2009).<br />

[3] S. Darby, T. V. Mortimer-Jones, R.L.Johnston and C.<br />

Roberts, J. Chem. Phys. 116, 1536 (2002).<br />

[4] J. L. Rodriguez-Lopez, J. M. Montejono-Carrizales, M. Jose-<br />

Yacaman, Appl. Surf. Sci. 219, 56 (2003).<br />

[5] F. Delogu, Nanotechnology 18 (2007) 235706.<br />

[6] Y.J. Li, W.H.Qi, B.Y.Huang, M.P.Wang, S.Y.Xiong, J. Phys.<br />

and Chem. Sol. Article <strong>in</strong> press.<br />

[7] K.K. Nanda, S.N. Sahu, S.N. Behera, Phys. Rev. A 66,<br />

013208 (2002).<br />

6th Nanoscience and Nanotechnology Conference, zmir, 2010 341

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