Abstract

The two-liquids scenario for liquid water assumes the existence of two competing preferential local molecular structural states characterized by either low or high local density. While the former is expected to present good local order thus involving privileged structures, the latter is usually regarded as conforming a high-entropy unstructured state. A main difference in the local arrangement of such "classes" of water molecules can be inferred from the degree of translational order between the first and second molecular shells. This is so, since the low-local-density molecules present a clear gap between the first two shells while in the case of the high-local-density ones, one or more molecules from the second shell have collapsed toward the first one, thus populating the intershell region. Some structural indicators, like the widely employed local structure index and the recently introduced ζ index, have been devised precisely on the basis of this observation, being successful in detecting well-structured low-local-density molecules. However, the nature of the high-local-density state has been mainly disregarded over the years. In this work we employ molecular dynamics simulations for two water models (the extended simple point charge model and the five-site model) at the liquid and supercooled regimes combined with the inherent dynamics approach (energy minimizations of the instantaneous configurations) in order to both rationalize the detailed structural and topological information that these indicators provide and to advance in our understanding of the high-density state.

Highlights

  • A full comprehension of the behavior of liquid water both from a structural and a dynamical standpoint is mandatory in order to rationalize its central role in contexts ranging from biology to materials science [1,2,3,4,5,6,7,8,9,10,11,12,13,14]

  • It is expected that at any temperature liquid water consists of a mixture of two kinds “species”, low local density molecules and high local density ones, with the fraction of former increasing as temperature is lowered [15, 16, 18, 21,22,23,24,25,26,27,28,29,30,31,32]

  • As long ago introduced by the seminal works of Stillinger and Weber [64, 65] the potential energy surface (PES) of a many particle system can be partitioned into disjoint basins, where a basin is unambiguously defined as the set of points in configuration space connected to the same local minimum, called inherent structure (IS) via a minimization trajectory

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Summary

Introduction

A full comprehension of the behavior of liquid water both from a structural and a dynamical standpoint is mandatory in order to rationalize its central role in contexts ranging from biology to materials science [1,2,3,4,5,6,7,8,9,10,11,12,13,14]. The population of high local density water molecules dominates at the normal liquid regime (well above the melting temperature), while the fraction of low local density ones is expected to grow significantly within the supercooled regime Such regime is achieved when the liquid is cooled fast enough below the melting point to avoid crystallization and is characterized by a dramatic dynamical slowing down or glassy relaxation [17, 35, 36]. The existence of a definite link in such regard has not been firmly established yet [30, 54]

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