Generalized exponential model: Difference between revisions
		
		
		
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| The '''Generalized exponential model''' (or '''GEM-m''' potential)  is given by (Eq. x in <ref></ref>): | The '''Generalized exponential model''' (or '''GEM-m''' potential)  is given by (Eq. x in <ref>xxx</ref>): | ||
| :<math> \Phi_{12}(r) = \epsilon \exp \left[ -\left( \frac{r}{\sigma} \right)^m \right]</math> | :<math> \Phi_{12}(r) = \epsilon \exp \left[ -\left( \frac{r}{\sigma} \right)^m \right]</math> | ||
| Line 8: | Line 8: | ||
| ==m=1== | ==m=1== | ||
| Also known as the EXP model | Also known as the EXP model <ref>[http://dx.doi.org/10.1038/ncomms6424 Andreas K. Bacher, Thomas B. Schrøder and Jeppe C. Dyre "Explaining why simple liquids are quasi-universal",     Nature Communications '''5''' Article number 5424 (2014)]</ref>. | ||
| ==m=4== | |||
| 2-dimensions <ref>[http://dx.doi.org/10.1063/1.4901302  Santi Prestipino and Franz Saija "Hexatic phase and cluster crystals of two-dimensional GEM4 spheres", Journal of Chemical Physics '''141''' 184502 (2014)]</ref>. | |||
| ==See also== | ==See also== | ||
Revision as of 14:04, 17 November 2014
The Generalized exponential model (or GEM-m potential) is given by (Eq. x in [1]):
where
- is the intermolecular pair potential between two particles or sites
m=1
Also known as the EXP model [2].
m=4
2-dimensions [3].
See also
References
- ↑ xxx
- ↑ Andreas K. Bacher, Thomas B. Schrøder and Jeppe C. Dyre "Explaining why simple liquids are quasi-universal", Nature Communications 5 Article number 5424 (2014)
- ↑ Santi Prestipino and Franz Saija "Hexatic phase and cluster crystals of two-dimensional GEM4 spheres", Journal of Chemical Physics 141 184502 (2014)
- Related reading