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Improved Geometries and Frequencies with the PFD-3B DFT Method
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    A: New Tools and Methods in Experiment and Theory

    Improved Geometries and Frequencies with the PFD-3B DFT Method
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    • Jason M. Breslin
      Jason M. Breslin
      Institute for Computational Molecular Science, Temple University, 1925 North 12th Street, Philadelphia, Pennsylvania 19122, United States
    • Michael J. Frisch
      Michael J. Frisch
      Hall-Atwater Laboratories of Chemistry, Wesleyan University, Middletown, Connecticut 06459-0180, United States
      Gaussian, Inc., 340 Quinnipiac Street Bldg. 40, Wallingford, Connecticut 06492-4050, United States
    • George A. Petersson*
      George A. Petersson
      Institute for Computational Molecular Science, Temple University, 1925 North 12th Street, Philadelphia, Pennsylvania 19122, United States
      Department of Chemistry, Temple University, 1901 North 13th Street, Philadelphia, Pennsylvania 19122, United States
      *Email: [email protected]
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    The Journal of Physical Chemistry A

    Cite this: J. Phys. Chem. A 2022, 126, 34, 5814–5820
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    https://doi.org/10.1021/acs.jpca.2c03401
    Published August 23, 2022
    Copyright © 2022 American Chemical Society

    Abstract

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    Bond lengths have been calculated for a test set of 120 diatomic species, including all homonuclear diatomics, hydrides, fluorides, and oxides for elements H through Kr for which experimental data is available for comparison. The performance of the PFD-3B functional is significantly better than competitive DFT methods. The rms error in bond lengths is reduced to 0.01 Å using a moderate size 3Za1Pa + f triple-ζ basis set, with the rms error in harmonic vibrational constants, ωe, equal to 38 cm–1. A very small 2ZP0H basis set is sufficient to calculate anharmonic constants, ωeXe, within ±4 cm–1. The rotational constants, Be, agree with experiment to within ±2%, and the vibration–rotation coupling constants, αe, agree within 10%. The calculated vibrational zero-point energy, ZPE, agrees with experiment to within ±0.06 kcal mol–1 for the diatomic test set, and the error increases to just ±0.11 kcal mol–1 for a set of 12 small polyatomic species. Comparison of a detailed anharmonic analysis of the twisted ethylene cation to the PFI-ZEKE experimental data illustrates the reliability of the PFD-3B for atypical structures.

    Copyright © 2022 American Chemical Society

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    Supporting Information

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    The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.jpca.2c03401.

    • This gives the tables of the numerical calculated parameters from PFD-3B/3Za1Pa + f geometry and frequency calculations (PDF)

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    The Journal of Physical Chemistry A

    Cite this: J. Phys. Chem. A 2022, 126, 34, 5814–5820
    Click to copy citationCitation copied!
    https://doi.org/10.1021/acs.jpca.2c03401
    Published August 23, 2022
    Copyright © 2022 American Chemical Society

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