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\contentsline {table}{\numberline {1.1}{\ignorespaces DEVIATION FROM PAIRWISE BEHAVIOR IN FCC METALS COMPARED WITH NON-METALLIC SYSTEMS. REPRODUCED FROM REFERENCE \cite {DAW:1993p1640} TABLE 1.}}{11} |
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\contentsline {table}{\numberline {1.2}{\ignorespaces {\sc SC} and {\sc Q-SC } PARAMETERS\cite {kimura-quantum,Chen90} TABLE 1.}}{19} |
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\contentsline {table}{\numberline {1.1}{\ignorespaces DEVIATION FROM PAIRWISE BEHAVIOR IN FCC METALS COMPARED WITH NON-METALLIC SYSTEMS}}{13}{table.1.1} |
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\contentsline {table}{\numberline {1.2}{\ignorespaces {\sc SC} AND {\sc Q-SC } PARAMETERS}}{23}{table.1.2} |
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\contentsline {table}{\numberline {5.1}{\ignorespaces Values of bond orientational order parameters for simple structures cooresponding to $l=4$ and $l=6$ spherical harmonic functions.\cite {wolde:9932} $Q_4$ and $\mathaccentV {hat}05E{W}_4$ have values for {\it individual} icosahedral clusters, but these values are not invariant under rotations of the reference coordinate systems. Similar behavior is observed in the bond-orientational order parameters for individual liquid-like structures.}}{74} |
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\contentsline {table}{\numberline {5.2}{\ignorespaces Estimates of the glass transition temperatures $T_g$ for three different sizes of bimetallic Ag$_6$Cu$_4$ nanoparticles cooled under two different values of the interfacial conductance, $G$.}}{85} |
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\contentsline {table}{\numberline {5.1}{\ignorespaces VALUES OF BOND ORIENTATIONAL ORDER PARAMETERS FOR SIMPLE STRUCTURES}}{101}{table.5.1} |
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\contentsline {table}{\numberline {5.2}{\ignorespaces ESTIMATES OF THE GLASS TRANSITION TEMPERATURES $T_G$}}{114}{table.5.2} |
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