Widom line: Difference between revisions

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*[http://dx.doi.org/10.1088/0953-8984/19/20/205126  Giancarlo Franzese and H. Eugene Stanley "The Widom line of supercooled water",  Journal of Physics: Condensed Matter '''19''' 205126 (2007)]
*[http://dx.doi.org/10.1088/0953-8984/19/20/205126  Giancarlo Franzese and H. Eugene Stanley "The Widom line of supercooled water",  Journal of Physics: Condensed Matter '''19''' 205126 (2007)]
*[http://dx.doi.org/10.1063/1.4930542  D. Corradini, M. Rovere and P. Gallo "The Widom line and dynamical crossover in supercritical water: Popular water models versus experiments", Journal of Chemical Physics 143, 114502 (2015)]
*[http://dx.doi.org/10.1063/1.4930542  D. Corradini, M. Rovere and P. Gallo "The Widom line and dynamical crossover in supercritical water: Popular water models versus experiments", Journal of Chemical Physics 143, 114502 (2015)]
*[https://doi.org/10.1038/s41467-024-47961-7 U. Ranieri, F. Formisano, F. A. Gorelli, M. Santoro, M. M. Koza, A. De Francesco, L. E. Bove "Crossover from gas-like to liquid-like molecular diffusion in a simple supercritical fluid", Nature Communications 15, 4142 (2024)]


[[category: statistical mechanics]]
[[category: statistical mechanics]]

Revision as of 22:58, 17 May 2024

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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. Recently the Widom line has been calculated for the Lennard-Jones model[4].

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References

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