Efficient implementation of the analytical second derivatives of hartree–fock and hybrid DFT energies within the framework of the conductor‐like polarizable continuum model

Calculation of vibrational frequencies for solvated systems is essential to study reactions in complex environments. In this paper, we report the implementation of the analytical self‐consistent field Hessian at the Hartree–Fock and density functional theory levels in the framework of the conductor‐...

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Published in:Journal of Computational Chemistry
Main Authors: Garcia-Ratés, M., Neese, F.
Format: Article in Journal/Newspaper
Language:English
Published: 2019
Subjects:
Online Access:http://hdl.handle.net/21.11116/0000-0004-4EDC-E
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spelling ftpubman:oai:pure.mpg.de:item_3145812 2023-08-27T04:11:26+02:00 Efficient implementation of the analytical second derivatives of hartree–fock and hybrid DFT energies within the framework of the conductor‐like polarizable continuum model Garcia-Ratés, M. Neese, F. 2019-07-30 http://hdl.handle.net/21.11116/0000-0004-4EDC-E eng eng info:eu-repo/semantics/altIdentifier/doi/10.1002/jcc.25833 http://hdl.handle.net/21.11116/0000-0004-4EDC-E Journal of Computational Chemistry info:eu-repo/semantics/article 2019 ftpubman https://doi.org/10.1002/jcc.25833 2023-08-02T00:01:38Z Calculation of vibrational frequencies for solvated systems is essential to study reactions in complex environments. In this paper, we report the implementation of the analytical self‐consistent field Hessian at the Hartree–Fock and density functional theory levels in the framework of the conductor‐like polarizable continuum model (C‐PCM) into the ORCA quantum chemistry suite. The calculated vibrational frequencies agree very well with those computed through numerical differentiation of the analytical gradients. The deviation between both sets of data is smaller than 3 cm −1 for frequencies larger than 200 cm −1 and smaller than 5 cm −1 for the low‐frequency regime (100 cm −1 < ω < 200 cm −1 ). The accuracy of the frequencies is not significantly affected by the size of the density functional theory (DFT) integration grid, with a deviation lower than 0.5 cm −1 between data computed with the smallest and that with the largest DFT grid size. The calculation of the analytical Hessian is between 3 and 12 times faster than its numerical counterpart. The C‐PCM terms only add an overhead of 10–30% relative to the gas phase calculations. Finally, for acetone, the (B3LYP) values for the frequency shifts obtained in going from the gas phase to liquid acetone are in agreement with experiment. Article in Journal/Newspaper Orca Max Planck Society: MPG.PuRe Hartree ENVELOPE(-44.716,-44.716,-60.783,-60.783) Journal of Computational Chemistry 40 20 1816 1828
institution Open Polar
collection Max Planck Society: MPG.PuRe
op_collection_id ftpubman
language English
description Calculation of vibrational frequencies for solvated systems is essential to study reactions in complex environments. In this paper, we report the implementation of the analytical self‐consistent field Hessian at the Hartree–Fock and density functional theory levels in the framework of the conductor‐like polarizable continuum model (C‐PCM) into the ORCA quantum chemistry suite. The calculated vibrational frequencies agree very well with those computed through numerical differentiation of the analytical gradients. The deviation between both sets of data is smaller than 3 cm −1 for frequencies larger than 200 cm −1 and smaller than 5 cm −1 for the low‐frequency regime (100 cm −1 < ω < 200 cm −1 ). The accuracy of the frequencies is not significantly affected by the size of the density functional theory (DFT) integration grid, with a deviation lower than 0.5 cm −1 between data computed with the smallest and that with the largest DFT grid size. The calculation of the analytical Hessian is between 3 and 12 times faster than its numerical counterpart. The C‐PCM terms only add an overhead of 10–30% relative to the gas phase calculations. Finally, for acetone, the (B3LYP) values for the frequency shifts obtained in going from the gas phase to liquid acetone are in agreement with experiment.
format Article in Journal/Newspaper
author Garcia-Ratés, M.
Neese, F.
spellingShingle Garcia-Ratés, M.
Neese, F.
Efficient implementation of the analytical second derivatives of hartree–fock and hybrid DFT energies within the framework of the conductor‐like polarizable continuum model
author_facet Garcia-Ratés, M.
Neese, F.
author_sort Garcia-Ratés, M.
title Efficient implementation of the analytical second derivatives of hartree–fock and hybrid DFT energies within the framework of the conductor‐like polarizable continuum model
title_short Efficient implementation of the analytical second derivatives of hartree–fock and hybrid DFT energies within the framework of the conductor‐like polarizable continuum model
title_full Efficient implementation of the analytical second derivatives of hartree–fock and hybrid DFT energies within the framework of the conductor‐like polarizable continuum model
title_fullStr Efficient implementation of the analytical second derivatives of hartree–fock and hybrid DFT energies within the framework of the conductor‐like polarizable continuum model
title_full_unstemmed Efficient implementation of the analytical second derivatives of hartree–fock and hybrid DFT energies within the framework of the conductor‐like polarizable continuum model
title_sort efficient implementation of the analytical second derivatives of hartree–fock and hybrid dft energies within the framework of the conductor‐like polarizable continuum model
publishDate 2019
url http://hdl.handle.net/21.11116/0000-0004-4EDC-E
long_lat ENVELOPE(-44.716,-44.716,-60.783,-60.783)
geographic Hartree
geographic_facet Hartree
genre Orca
genre_facet Orca
op_source Journal of Computational Chemistry
op_relation info:eu-repo/semantics/altIdentifier/doi/10.1002/jcc.25833
http://hdl.handle.net/21.11116/0000-0004-4EDC-E
op_doi https://doi.org/10.1002/jcc.25833
container_title Journal of Computational Chemistry
container_volume 40
container_issue 20
container_start_page 1816
op_container_end_page 1828
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