Z1 and Z2 potentials: Difference between revisions

Latest revision as of 15:13, 2 November 2010

The Z potentials (Z1 and Z2) are given by (Eq. 1 in ^[1])

\Phi _{12}(r)=a{\frac {e^{\alpha r}}{r^{3}}}\cos(2k_{F}r)+b\left({\frac {\sigma }{r}}\right)^{n}+V_{0}

The following parameters are taken from Table I

Related reading

Revision as of 14:59, 2 November 2010 (edit) Carl McBride (talk \| contribs) (Added table for the parameters of Z1 and Z2) ← Older edit		Latest revision as of 15:13, 2 November 2010 (edit) (undo) Carl McBride (talk \| contribs) mNo edit summary
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	The '''Z ~~potential~~''' is given by (Eq. 1 in <ref>[http://dx.doi.org/10.1063/1.1534831 Jonathan P. K. Doye, David J. Wales, Fredrik H. M. Zetterling, and Mikhail Dzugutov " The favored cluster structures of model glass formers", Journal of Chemical Physics '''118''' pp. 2792-2799 (2003)]</ref>)		The '''Z potentials''' ('''Z1''' and '''Z2''') are given by (Eq. 1 in <ref>[http://dx.doi.org/10.1063/1.1534831 Jonathan P. K. Doye, David J. Wales, Fredrik H. M. Zetterling, and Mikhail Dzugutov " The favored cluster structures of model glass formers", Journal of Chemical Physics '''118''' pp. 2792-2799 (2003)]</ref>)

	:<math>\Phi_{12}(r) = a \frac{e^{\alpha r}}{r^3} \cos (2k_Fr) + b \left( \frac{\sigma}{r} \right)^n + V_0 </math>		:<math>\Phi_{12}(r) = a \frac{e^{\alpha r}}{r^3} \cos (2k_Fr) + b \left( \frac{\sigma}{r} \right)^n + V_0 </math>