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Radial Potential Energy Functions of Linear Halogen-Bonded Complexes YX···ClF (YX = FB, OC, SC, N(2)) and the Effects of Substituting X by Second-Row Analogues: Mulliken Inner and Outer Complexes
[Image: see text] Energies of linear, halogen-bonded complexes in the isoelectronic series YX···ClF (YX = FB, OC, or N(2)) are calculated at several levels of theory as a function of the intermolecular distance r(X···Cl) to yield radial potential energy functions. When YX = OC, a secondary minimum i...
Autores principales: | , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2022
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9097511/ https://www.ncbi.nlm.nih.gov/pubmed/35426668 http://dx.doi.org/10.1021/acs.jpca.2c01205 |
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author | Hill, J. Grant Legon, Anthony C. |
author_facet | Hill, J. Grant Legon, Anthony C. |
author_sort | Hill, J. Grant |
collection | PubMed |
description | [Image: see text] Energies of linear, halogen-bonded complexes in the isoelectronic series YX···ClF (YX = FB, OC, or N(2)) are calculated at several levels of theory as a function of the intermolecular distance r(X···Cl) to yield radial potential energy functions. When YX = OC, a secondary minimum is observed corresponding to lengthened and shortened distances r(ClF) and r(CCl), respectively, relative to the primary minimum, suggesting a significant contribution from the Mulliken inner complex structure [O=C–Cl](+)···F(–). A conventional weak, halogen-bond complex OC···ClF occurs at the primary minimum. For YX = FB, the primary minimum corresponds to the inner complex [F=B–Cl](+)···F(–), while the outer complex FB···ClF is at the secondary minimum. The effects on the potential energy function of systematic substitution of Y and X by second-row congeners and of reversing the order of X and Y are also investigated. Symmetry-adapted perturbation theory and natural population analyses are applied to further understand the nature of the various halogen-bond interactions. |
format | Online Article Text |
id | pubmed-9097511 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-90975112022-05-13 Radial Potential Energy Functions of Linear Halogen-Bonded Complexes YX···ClF (YX = FB, OC, SC, N(2)) and the Effects of Substituting X by Second-Row Analogues: Mulliken Inner and Outer Complexes Hill, J. Grant Legon, Anthony C. J Phys Chem A [Image: see text] Energies of linear, halogen-bonded complexes in the isoelectronic series YX···ClF (YX = FB, OC, or N(2)) are calculated at several levels of theory as a function of the intermolecular distance r(X···Cl) to yield radial potential energy functions. When YX = OC, a secondary minimum is observed corresponding to lengthened and shortened distances r(ClF) and r(CCl), respectively, relative to the primary minimum, suggesting a significant contribution from the Mulliken inner complex structure [O=C–Cl](+)···F(–). A conventional weak, halogen-bond complex OC···ClF occurs at the primary minimum. For YX = FB, the primary minimum corresponds to the inner complex [F=B–Cl](+)···F(–), while the outer complex FB···ClF is at the secondary minimum. The effects on the potential energy function of systematic substitution of Y and X by second-row congeners and of reversing the order of X and Y are also investigated. Symmetry-adapted perturbation theory and natural population analyses are applied to further understand the nature of the various halogen-bond interactions. American Chemical Society 2022-04-15 2022-04-28 /pmc/articles/PMC9097511/ /pubmed/35426668 http://dx.doi.org/10.1021/acs.jpca.2c01205 Text en © 2022 American Chemical Society https://creativecommons.org/licenses/by/4.0/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/). |
spellingShingle | Hill, J. Grant Legon, Anthony C. Radial Potential Energy Functions of Linear Halogen-Bonded Complexes YX···ClF (YX = FB, OC, SC, N(2)) and the Effects of Substituting X by Second-Row Analogues: Mulliken Inner and Outer Complexes |
title | Radial Potential Energy Functions of Linear Halogen-Bonded
Complexes YX···ClF (YX = FB, OC, SC, N(2))
and the Effects of Substituting X by Second-Row Analogues: Mulliken
Inner and Outer Complexes |
title_full | Radial Potential Energy Functions of Linear Halogen-Bonded
Complexes YX···ClF (YX = FB, OC, SC, N(2))
and the Effects of Substituting X by Second-Row Analogues: Mulliken
Inner and Outer Complexes |
title_fullStr | Radial Potential Energy Functions of Linear Halogen-Bonded
Complexes YX···ClF (YX = FB, OC, SC, N(2))
and the Effects of Substituting X by Second-Row Analogues: Mulliken
Inner and Outer Complexes |
title_full_unstemmed | Radial Potential Energy Functions of Linear Halogen-Bonded
Complexes YX···ClF (YX = FB, OC, SC, N(2))
and the Effects of Substituting X by Second-Row Analogues: Mulliken
Inner and Outer Complexes |
title_short | Radial Potential Energy Functions of Linear Halogen-Bonded
Complexes YX···ClF (YX = FB, OC, SC, N(2))
and the Effects of Substituting X by Second-Row Analogues: Mulliken
Inner and Outer Complexes |
title_sort | radial potential energy functions of linear halogen-bonded
complexes yx···clf (yx = fb, oc, sc, n(2))
and the effects of substituting x by second-row analogues: mulliken
inner and outer complexes |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9097511/ https://www.ncbi.nlm.nih.gov/pubmed/35426668 http://dx.doi.org/10.1021/acs.jpca.2c01205 |
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