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Transfer learned potential energy surfaces: accurate anharmonic vibrational dynamics and dissociation energies for the formic acid monomer and dimer
The vibrational dynamics of the formic acid monomer (FAM) and dimer (FAD) is investigated from machine-learned potential energy surfaces at the MP2 (PES(MP2)) and transfer-learned (PES(TL)) to the CCSD(T) levels of theory. The normal mode (MAEs of 17.6 and 25.1 cm(−1)) and second order vibrational p...
Autores principales: | , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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The Royal Society of Chemistry
2021
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8890265/ https://www.ncbi.nlm.nih.gov/pubmed/34792523 http://dx.doi.org/10.1039/d1cp04393e |
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author | Käser, Silvan Meuwly, Markus |
author_facet | Käser, Silvan Meuwly, Markus |
author_sort | Käser, Silvan |
collection | PubMed |
description | The vibrational dynamics of the formic acid monomer (FAM) and dimer (FAD) is investigated from machine-learned potential energy surfaces at the MP2 (PES(MP2)) and transfer-learned (PES(TL)) to the CCSD(T) levels of theory. The normal mode (MAEs of 17.6 and 25.1 cm(−1)) and second order vibrational perturbation theory (VPT2, MAEs of 6.7 and 17.1 cm(−1)) frequencies from PES(TL) for all modes below 2000 cm(−1) for FAM and FAD agree favourably with experiment. For the OH stretch mode the experimental frequencies are overestimated by more than 150 cm(−1) for both FAM and FAD from normal mode calculations. Conversely, VPT2 calculations on PES(TL) for FAM reproduce the experimental OH frequency to within 22 cm(−1). For FAD the VPT2 calculations find the high-frequency OH stretch at 3011 cm(−1), compared with an experimentally reported, broad (∼100 cm(−1)) absorption band with center frequency estimated at ∼3050 cm(−1). In agreement with earlier reports, MD simulations at higher temperature shift the position of the OH-stretch in FAM to the red, consistent with improved sampling of the anharmonic regions of the PES. However, for FAD the OH-stretch shifts to the blue and for temperatures higher than 1000 K the dimer partly or fully dissociates using PES(TL). Including zero-point energy corrections from diffusion Monte Carlo simulations for FAM and FAD and corrections due to basis set superposition and completeness errors yields a dissociation energy of D(0) = −14.23 ± 0.08 kcal mol(−1) compared with an experimentally determined value of −14.22 ± 0.12 kcal mol(−1). |
format | Online Article Text |
id | pubmed-8890265 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | The Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
spelling | pubmed-88902652022-03-29 Transfer learned potential energy surfaces: accurate anharmonic vibrational dynamics and dissociation energies for the formic acid monomer and dimer Käser, Silvan Meuwly, Markus Phys Chem Chem Phys Chemistry The vibrational dynamics of the formic acid monomer (FAM) and dimer (FAD) is investigated from machine-learned potential energy surfaces at the MP2 (PES(MP2)) and transfer-learned (PES(TL)) to the CCSD(T) levels of theory. The normal mode (MAEs of 17.6 and 25.1 cm(−1)) and second order vibrational perturbation theory (VPT2, MAEs of 6.7 and 17.1 cm(−1)) frequencies from PES(TL) for all modes below 2000 cm(−1) for FAM and FAD agree favourably with experiment. For the OH stretch mode the experimental frequencies are overestimated by more than 150 cm(−1) for both FAM and FAD from normal mode calculations. Conversely, VPT2 calculations on PES(TL) for FAM reproduce the experimental OH frequency to within 22 cm(−1). For FAD the VPT2 calculations find the high-frequency OH stretch at 3011 cm(−1), compared with an experimentally reported, broad (∼100 cm(−1)) absorption band with center frequency estimated at ∼3050 cm(−1). In agreement with earlier reports, MD simulations at higher temperature shift the position of the OH-stretch in FAM to the red, consistent with improved sampling of the anharmonic regions of the PES. However, for FAD the OH-stretch shifts to the blue and for temperatures higher than 1000 K the dimer partly or fully dissociates using PES(TL). Including zero-point energy corrections from diffusion Monte Carlo simulations for FAM and FAD and corrections due to basis set superposition and completeness errors yields a dissociation energy of D(0) = −14.23 ± 0.08 kcal mol(−1) compared with an experimentally determined value of −14.22 ± 0.12 kcal mol(−1). The Royal Society of Chemistry 2021-10-26 /pmc/articles/PMC8890265/ /pubmed/34792523 http://dx.doi.org/10.1039/d1cp04393e Text en This journal is © the Owner Societies https://creativecommons.org/licenses/by-nc/3.0/ |
spellingShingle | Chemistry Käser, Silvan Meuwly, Markus Transfer learned potential energy surfaces: accurate anharmonic vibrational dynamics and dissociation energies for the formic acid monomer and dimer |
title | Transfer learned potential energy surfaces: accurate anharmonic vibrational dynamics and dissociation energies for the formic acid monomer and dimer |
title_full | Transfer learned potential energy surfaces: accurate anharmonic vibrational dynamics and dissociation energies for the formic acid monomer and dimer |
title_fullStr | Transfer learned potential energy surfaces: accurate anharmonic vibrational dynamics and dissociation energies for the formic acid monomer and dimer |
title_full_unstemmed | Transfer learned potential energy surfaces: accurate anharmonic vibrational dynamics and dissociation energies for the formic acid monomer and dimer |
title_short | Transfer learned potential energy surfaces: accurate anharmonic vibrational dynamics and dissociation energies for the formic acid monomer and dimer |
title_sort | transfer learned potential energy surfaces: accurate anharmonic vibrational dynamics and dissociation energies for the formic acid monomer and dimer |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8890265/ https://www.ncbi.nlm.nih.gov/pubmed/34792523 http://dx.doi.org/10.1039/d1cp04393e |
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