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Abstracts Book - IMRC 2018

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• SD1-O019<br />

CONFIGURATIONAL ENERGY LANDSCAPE OF ALLOYS<br />

Juan Miguel Sanchez 1<br />

1 University of Texas at Austin, Institute for Computationa Science and Engineering, United<br />

States.<br />

A widely used approach to describe the configurational energy of alloys consists of<br />

fitting the energies of a set of compounds, typically calculated using some<br />

implementation of the Kohn-Sham equations in Density Functional Theory (DFT), to<br />

a generalized Ising-like energy model. The Ising-like model itself is characterized by<br />

a set of constant Effective Cluster Interactions (ECI). The approach is known as the<br />

Connolly-Williams (CW) method and its implementation to real alloy systems is<br />

usually justified by invoking the Cluster Expansion (CE) formalism introduced by<br />

Sanchez et al. 1 , and by the assumption that the ECIs decay sufficiently fast so that<br />

the CE can be truncated for clusters larger than a judiciously chosen maximum<br />

cluster. In this talk, we show that truncation of the CE and/or structural relaxations<br />

in the alloy invalidate the commonly used Ising-like representation of the<br />

configurational energy of alloys. In particular, we show that truncating the cluster<br />

expansion of the energy of alloys gives rise to renormalized effective cluster<br />

interactions that are explicit functions of the configurational variables that<br />

characterize the state of short- and long-range order of the system. The<br />

dependence of the renormalized cluster interactions on the configurational<br />

variables is in addition to their dependence on the alloys volume and on other<br />

structural parameters. A new physical picture emerges in which the sum of the<br />

interactions, which are projections of the energy onto the basis functions in<br />

configurational space, contribute over long distances but the expected “near -<br />

sightedness of the energy is preserved by the renormalized interactions. The latter<br />

are configuration dependent and decay rapidly with both cluster size and distances.<br />

In order to illustrate our results and observations, we revisit the cluster expansion<br />

of the energy of the Cu-Au system.<br />

1<br />

J.M. Sanchez, F. Ducastelle, and D. Gratias, Physica A 128, 334 (1984).<br />

Acknowledgment: The author acknowledges the computational support<br />

provided by the Texas Advanced Computing Center (TACC) at the University of<br />

Texas at Austin<br />

Keywords: Cluster Expansion, Configurational Energy, Alloys<br />

Presenting authors email: jsanchez@austin.utexas.edu

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