2015
DOI: 10.1063/1.4905333
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Isobaric first-principles molecular dynamics of liquid water with nonlocal van der Waals interactions

Abstract: We investigate the structural properties of liquid water at near ambient conditions using first-principles molecular dynamics simulations based on a semilocal density functional augmented with nonlocal van der Waals interactions. The adopted scheme offers the advantage of simulating liquid water at essentially the same computational cost of standard semilocal functionals. Applied to the water dimer and to ice I h , we find that the hydrogen-bond energy is only slightly enhanced compared to a standard semilocal… Show more

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Cited by 74 publications
(140 citation statements)
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“…These results are in agreement with previous NVT simulations, 42 and a recent NPT simulation performed with the rVV10 functional in Ref. 74, where a reparameterization of the functional was proposed to cure this deficiency. Even though at the limit of statistical accuracy, both the inclusion of the D3 correction and the use of hybrid functionals reduce the height of the first peak of the g OO (r) for PBE, while the ADMM approximation influences the equilibrium density by ∼2% and leads to slightly more TABLE I.…”
Section: Structural Propertiessupporting
confidence: 82%
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“…These results are in agreement with previous NVT simulations, 42 and a recent NPT simulation performed with the rVV10 functional in Ref. 74, where a reparameterization of the functional was proposed to cure this deficiency. Even though at the limit of statistical accuracy, both the inclusion of the D3 correction and the use of hybrid functionals reduce the height of the first peak of the g OO (r) for PBE, while the ADMM approximation influences the equilibrium density by ∼2% and leads to slightly more TABLE I.…”
Section: Structural Propertiessupporting
confidence: 82%
“…The introduction of dispersion forces, either in a semi-empirical way, such as the Grimme's D3 correction, or by including an explicit non-local term in the functional, such as in the van der Waals density functionals, 69,70 improves the liquid description, but in general gives too dense water (5%-10%). 38,40,42,74,135,136 An illustration of the change induced by van der Waals interactions is provided in Figure 2(a), where BLYP and PBE0-D3 RDF's are shown. In particular, the distributions of the 4th and 5th neighboring waters show a clear separation between the first and second coordination shells in the BLYP case, whereas these peaks move closer at the PBE0-D3.…”
Section: Structural Propertiesmentioning
confidence: 99%
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“…Björkman et al further proposed b ¼ 9.15 for VV10 by fitting to the binding energies of 26 layered materials [18], and we obtained the same number for rVV10. Reference [39] found b ¼ 9.3 for the structural properties of water. These results highlight the flexibility of the VV10 and rVV10 methods but also point out the need for a new approach with a single set of vdW empirical parameters for all materials.…”
Section: Theory: Parameters In Scanþrvv10mentioning
confidence: 99%
“…Norm-conserving pseudopotentials with a plane-wave cutoff of 85 Ry are used in the DFT calculations. To account for the nonlocal van der Waals dispersion, which is critical for the hydrogen-bond network [50,51,[60][61][62][63], the revised Vydrov and Van Voorhis (rVV10) van der Waals density functional [52,53] is used in the MD simulations. The short-range behavior is controlled by an empirical parameter b in the rVV10 density functional [52,53].…”
mentioning
confidence: 99%