Widom line: Difference between revisions
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==References== | ==References== | ||
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;Related reading | |||
*[http://dx.doi.org/10.1038/nphys1683 G. G. Simeoni, T. Bryk, F. A. Gorelli, M. Krisch, G. Ruocco, M. Santoro, and T. Scopigno "The Widom line as the crossover between liquid-like and gas-like behaviour in supercritical fluids", Nature Physics '''6''' pp. 503-507 (2010)] | |||
[[category: statistical mechanics]] | [[category: statistical mechanics]] | ||
Revision as of 15:02, 2 November 2011
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The Widom line[1] (not to be confused with the Fisher-Widom line) is defined as the line in the pressure-temperature plane where the correlation length has its maximum [2] , and emanates from the hypothesized liquid–liquid critical point of water . It was named the Widom line by H. Eugene Stanley[3] in honour of Benjamin Widom.
References
- ↑ Limei Xu, Pradeep Kumar, S. V. Buldyrev, S.-H. Chen, P. H. Poole, F. Sciortino, and H. E. Stanley "Relation between the Widom line and the dynamic crossover in systems with a liquid–liquid phase transition", PNAS 102 pp. 16558-16562 (2005)
- ↑ H. E. Stanley, P. Kumar, G. Franzese, L. Xu, Z. Yan, M. G. Mazza, S. V. Buldyrev, S.-H. Chen and F. Mallamace "Liquid polyamorphism: Possible relation to the anomalous behaviour of water", European Physical Journal - Special Topics 161 pp. 1-17 (2008)
- ↑ Sergey V. Buldyrev "Water wisdom and Widom", Boston University Research Briefs December 6 (2005)
- Related reading