\relax 
\@writefile{toc}{\contentsline {section}{\numberline {1}Abstract}{1}}
\@writefile{toc}{\contentsline {section}{\numberline {2}Introduction}{1}}
\@writefile{toc}{\contentsline {section}{\numberline {3}Genetic Algorithm}{1}}
\@writefile{toc}{\contentsline {section}{\numberline {4}Functional Form}{1}}
\@writefile{toc}{\contentsline {section}{\numberline {5}Results}{2}}
\@writefile{toc}{\contentsline {section}{\numberline {6}Computational Issues}{2}}
\@writefile{toc}{\contentsline {section}{\numberline {7}Discussion}{2}}
\@writefile{toc}{\contentsline {section}{\numberline {8}References}{3}}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Comparison of energies calculated for $\@mathrm {Si_{33}}$ clusters using tight-binding vs. evolved and published SW parameters. Each cross represents a cluster. Crosses on the diagonal line are a perfect fit. Evolved parameters were generated using a fitness function with $\@mathrm {Si_{2-6}}$ cluster energies calculated by the tight-binding method. In (a) the vertical axis is the energy calculated using evolved parameters in the same units as [Stillinger, Weber (1985)]. In (b) the vertical axis is the energy calculated using the published parameters. Horizontal axes are the energies calculated by the tight-binding method. The figures clearly show that the evolved parameters match the tight-binding energies much more closely than the published parameters. All energies are kcal/mol.}}{4}}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Comparison of energies calculated for $\@mathrm {Ge_{2-6}}$ clusters of tight-binding vs. evolved. Each cross represents a cluster. Crosses on the diagonal line are a perfect fit. Evolved parameters were generated using a fitness function with $\@mathrm {Si_{2-6}}$ cluster energies calculated by the tight-binding method. The vertical axis is the energy calculated using evolved parameters in eV/angstrom. The horizontal axis are the energies calculated by the tight-binding method. All energies are eV.}}{4}}