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Evidence of a liquid–liquid phase transition in H[Formula: see text] O and D[Formula: see text] O from path-integral molecular dynamics simulations

We perform path-integral molecular dynamics (PIMD), ring-polymer MD (RPMD), and classical MD simulations of H[Formula: see text] O and D[Formula: see text] O using the q-TIP4P/F water model over a wide range of temperatures and pressures. The density [Formula: see text] , isothermal compressibility...

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Autores principales: Eltareb, Ali, Lopez, Gustavo E., Giovambattista, Nicolas
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8994788/
https://www.ncbi.nlm.nih.gov/pubmed/35397618
http://dx.doi.org/10.1038/s41598-022-09525-x
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author Eltareb, Ali
Lopez, Gustavo E.
Giovambattista, Nicolas
author_facet Eltareb, Ali
Lopez, Gustavo E.
Giovambattista, Nicolas
author_sort Eltareb, Ali
collection PubMed
description We perform path-integral molecular dynamics (PIMD), ring-polymer MD (RPMD), and classical MD simulations of H[Formula: see text] O and D[Formula: see text] O using the q-TIP4P/F water model over a wide range of temperatures and pressures. The density [Formula: see text] , isothermal compressibility [Formula: see text] , and self-diffusion coefficients D(T) of H[Formula: see text] O and D[Formula: see text] O are in excellent agreement with available experimental data; the isobaric heat capacity [Formula: see text] obtained from PIMD and MD simulations agree qualitatively well with the experiments. Some of these thermodynamic properties exhibit anomalous maxima upon isobaric cooling, consistent with recent experiments and with the possibility that H[Formula: see text] O and D[Formula: see text] O exhibit a liquid-liquid critical point (LLCP) at low temperatures and positive pressures. The data from PIMD/MD for H[Formula: see text] O and D[Formula: see text] O can be fitted remarkably well using the Two-State-Equation-of-State (TSEOS). Using the TSEOS, we estimate that the LLCP for q-TIP4P/F H[Formula: see text] O, from PIMD simulations, is located at [Formula: see text]  MPa, [Formula: see text]  K, and [Formula: see text]  g/cm[Formula: see text] . Isotope substitution effects are important; the LLCP location in q-TIP4P/F D[Formula: see text] O is estimated to be [Formula: see text]  MPa, [Formula: see text]  K, and [Formula: see text]  g/cm[Formula: see text] . Interestingly, for the water model studied, differences in the LLCP location from PIMD and MD simulations suggest that nuclear quantum effects (i.e., atoms delocalization) play an important role in the thermodynamics of water around the LLCP (from the MD simulations of q-TIP4P/F water, [Formula: see text]  MPa, [Formula: see text]  K, and [Formula: see text]  g/cm[Formula: see text] ). Overall, our results strongly support the LLPT scenario to explain water anomalous behavior, independently of the fundamental differences between classical MD and PIMD techniques. The reported values of [Formula: see text] for D[Formula: see text] O and, particularly, H[Formula: see text] O suggest that improved water models are needed for the study of supercooled water.
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spelling pubmed-89947882022-04-13 Evidence of a liquid–liquid phase transition in H[Formula: see text] O and D[Formula: see text] O from path-integral molecular dynamics simulations Eltareb, Ali Lopez, Gustavo E. Giovambattista, Nicolas Sci Rep Article We perform path-integral molecular dynamics (PIMD), ring-polymer MD (RPMD), and classical MD simulations of H[Formula: see text] O and D[Formula: see text] O using the q-TIP4P/F water model over a wide range of temperatures and pressures. The density [Formula: see text] , isothermal compressibility [Formula: see text] , and self-diffusion coefficients D(T) of H[Formula: see text] O and D[Formula: see text] O are in excellent agreement with available experimental data; the isobaric heat capacity [Formula: see text] obtained from PIMD and MD simulations agree qualitatively well with the experiments. Some of these thermodynamic properties exhibit anomalous maxima upon isobaric cooling, consistent with recent experiments and with the possibility that H[Formula: see text] O and D[Formula: see text] O exhibit a liquid-liquid critical point (LLCP) at low temperatures and positive pressures. The data from PIMD/MD for H[Formula: see text] O and D[Formula: see text] O can be fitted remarkably well using the Two-State-Equation-of-State (TSEOS). Using the TSEOS, we estimate that the LLCP for q-TIP4P/F H[Formula: see text] O, from PIMD simulations, is located at [Formula: see text]  MPa, [Formula: see text]  K, and [Formula: see text]  g/cm[Formula: see text] . Isotope substitution effects are important; the LLCP location in q-TIP4P/F D[Formula: see text] O is estimated to be [Formula: see text]  MPa, [Formula: see text]  K, and [Formula: see text]  g/cm[Formula: see text] . Interestingly, for the water model studied, differences in the LLCP location from PIMD and MD simulations suggest that nuclear quantum effects (i.e., atoms delocalization) play an important role in the thermodynamics of water around the LLCP (from the MD simulations of q-TIP4P/F water, [Formula: see text]  MPa, [Formula: see text]  K, and [Formula: see text]  g/cm[Formula: see text] ). Overall, our results strongly support the LLPT scenario to explain water anomalous behavior, independently of the fundamental differences between classical MD and PIMD techniques. The reported values of [Formula: see text] for D[Formula: see text] O and, particularly, H[Formula: see text] O suggest that improved water models are needed for the study of supercooled water. Nature Publishing Group UK 2022-04-09 /pmc/articles/PMC8994788/ /pubmed/35397618 http://dx.doi.org/10.1038/s41598-022-09525-x Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/Open AccessThis article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) .
spellingShingle Article
Eltareb, Ali
Lopez, Gustavo E.
Giovambattista, Nicolas
Evidence of a liquid–liquid phase transition in H[Formula: see text] O and D[Formula: see text] O from path-integral molecular dynamics simulations
title Evidence of a liquid–liquid phase transition in H[Formula: see text] O and D[Formula: see text] O from path-integral molecular dynamics simulations
title_full Evidence of a liquid–liquid phase transition in H[Formula: see text] O and D[Formula: see text] O from path-integral molecular dynamics simulations
title_fullStr Evidence of a liquid–liquid phase transition in H[Formula: see text] O and D[Formula: see text] O from path-integral molecular dynamics simulations
title_full_unstemmed Evidence of a liquid–liquid phase transition in H[Formula: see text] O and D[Formula: see text] O from path-integral molecular dynamics simulations
title_short Evidence of a liquid–liquid phase transition in H[Formula: see text] O and D[Formula: see text] O from path-integral molecular dynamics simulations
title_sort evidence of a liquid–liquid phase transition in h[formula: see text] o and d[formula: see text] o from path-integral molecular dynamics simulations
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8994788/
https://www.ncbi.nlm.nih.gov/pubmed/35397618
http://dx.doi.org/10.1038/s41598-022-09525-x
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