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, pp. 8138-8146
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Franczyk, T.S.1
Czerwinski, K.R.2
Raymond, K.N.3
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76
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33646576425
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note
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In their recent classical MD simulations based on a CASPT2-derived force field, Roos et al. do not observe hydrogen bonding between water and the uranyl oxygens, cf. ref 32g.
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78
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33646576753
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2 moieties are found in the CPMD simulations in water (cf. snapshots on the bottom of Figure 7).
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79
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33646540320
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note
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2O → 3c are -15.6 and -10.3 kcal/mol at the BSSE-corrected HF/LANL (ref 6b) and BLYP/ZORA levels, respectively.
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80
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0003838469
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Wiley-VCH: Weinheim
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This differential solvation effect for complexes involving neutral or anionic ligands arguably arises from a balance between cation-anion, ion-dipole, and dipole-dipole interactions in the dynamic ensemble. Even though the underlying electrostatics are usually modeled quite well with present-day density functionals (which also tend to afford reasonably accurate dipole moments and polarizabilities, cf. Koch, W.; Holthausen, M. C. A Chemist's Guide to Density Functional Theory; Wiley-VCH: Weinheim, 2000), such a delicate balance may be difficult to describe, and quantitative inaccuracies might add up to a qualitative change of the overall picture.
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(2000)
A Chemist's Guide to Density Functional Theory
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Koch, W.1
Holthausen, M.C.2
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81
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22944452112
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In context with the types of interactions studied here, however, we note that the solvent-induced bond contraction in metal-aquo complexes (cf. ref 33) is also found with DFT methods (e.g., ref 38b); likewise, the elongation of cation-anion distances in simple contact ion pairs such as alkali-metal or silver halides upon hydration (i.e., the onset of dissociation in water) is also well described with DFT (e.g., Godinho, S. S. M. C.; Cabral do Couto, P.; Costa Cabral, B. J. J. Chem. Phys. 2005, 122, 044316). Thus, we are confident that our results are qualitatively correct and are not artifacts of the adopted DFT approach.
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(2005)
J. Chem. Phys.
, vol.122
, pp. 044316
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Godinho, S.S.M.C.1
Cabral Do Couto, P.2
Costa Cabral, B.J.3
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33646549799
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note
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Effected via restart of the equilibrated 300 K simulation and instantaneous heatup.
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83
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33646571425
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note
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In the COSMO model, it is the screening term that dominates the changes with respect to the gas phase; the dispersion/cavitation term contributes less than 1.5 kcal/mol to the energy differences discussed.
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