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      Infrared Spectroscopy of Li + Solvation in Diglyme: Ab Initio Molecular Dynamics and Experiment

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          Abstract

          Infrared (IR) spectra of solutions of the lithium salt LiBF 4 in diglyme, CH 3O(CH 2CH 2O) 2CH 3, are studied via IR spectroscopy and ab initio molecular dynamics (AIMD) simulations. Experiments show that the major effects of LiBF 4, compared to neat diglyme, are the appearance of a new broad band in the 250–500 cm –1 frequency region and a broadening and intensity enhancement of the diglyme band in the 900–1150 cm –1 region accompanied by a red-shift. Computational analysis indicates that hindered translational motions of Li + in its solvation cage are mainly responsible for the new far-IR band, while the changes in the mid-IR are due to Li +-coordination-dependent B–F stretching vibrations of BF 4 anions coupled with diglyme vibrations. Molecular motions in these and lower frequency regions are generally correlated, revealing the collective nature of the vibrational dynamics, which involve multiple ions/molecules. Herein, a detailed analysis of these features via AIMD simulations of the spectrum and its components, combined with analysis of the generalized normal modes of the solution components, is presented. Other minor spectral changes as well as diglyme conformational changes induced by the lithium salt are also discussed.

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          A consistent and accurate ab initio parametrization of density functional dispersion correction (DFT-D) for the 94 elements H-Pu.

          The method of dispersion correction as an add-on to standard Kohn-Sham density functional theory (DFT-D) has been refined regarding higher accuracy, broader range of applicability, and less empiricism. The main new ingredients are atom-pairwise specific dispersion coefficients and cutoff radii that are both computed from first principles. The coefficients for new eighth-order dispersion terms are computed using established recursion relations. System (geometry) dependent information is used for the first time in a DFT-D type approach by employing the new concept of fractional coordination numbers (CN). They are used to interpolate between dispersion coefficients of atoms in different chemical environments. The method only requires adjustment of two global parameters for each density functional, is asymptotically exact for a gas of weakly interacting neutral atoms, and easily allows the computation of atomic forces. Three-body nonadditivity terms are considered. The method has been assessed on standard benchmark sets for inter- and intramolecular noncovalent interactions with a particular emphasis on a consistent description of light and heavy element systems. The mean absolute deviations for the S22 benchmark set of noncovalent interactions for 11 standard density functionals decrease by 15%-40% compared to the previous (already accurate) DFT-D version. Spectacular improvements are found for a tripeptide-folding model and all tested metallic systems. The rectification of the long-range behavior and the use of more accurate C(6) coefficients also lead to a much better description of large (infinite) systems as shown for graphene sheets and the adsorption of benzene on an Ag(111) surface. For graphene it is found that the inclusion of three-body terms substantially (by about 10%) weakens the interlayer binding. We propose the revised DFT-D method as a general tool for the computation of the dispersion energy in molecules and solids of any kind with DFT and related (low-cost) electronic structure methods for large systems.
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              Development of the Colle-Salvetti correlation-energy formula into a functional of the electron density

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                Author and article information

                Journal
                J Phys Chem B
                J Phys Chem B
                jp
                jpcbfk
                The Journal of Physical Chemistry. B
                American Chemical Society
                1520-6106
                1520-5207
                11 October 2023
                26 October 2023
                : 127
                : 42
                : 9191-9203
                Affiliations
                []Department of Chemistry, Carnegie Mellon University , Pittsburgh, Pennsylvania 15213, United States
                []Department of Chemistry, The Pennsylvania State University , University Park, Pennsylvania 16802, United States
                Author notes
                Author information
                https://orcid.org/0000-0002-2822-9160
                https://orcid.org/0000-0003-2467-5056
                https://orcid.org/0000-0003-1633-1472
                https://orcid.org/0000-0003-4334-1879
                Article
                10.1021/acs.jpcb.3c05612
                10614183
                37820068
                75ee17da-7724-4cca-af0e-881d314557e5
                © 2023 The Authors. Published by American Chemical Society

                Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained ( https://creativecommons.org/licenses/by/4.0/).

                History
                : 19 August 2023
                : 24 September 2023
                Funding
                Funded by: Basic Energy Sciences, doi 10.13039/100006151;
                Award ID: DE-SC0019200
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                Custom metadata
                jp3c05612
                jp3c05612

                Physical chemistry
                Physical chemistry

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