Cargando…

Low-Lying Electronic States of the Nickel Dimer

The generalized Van Vleck second order multireference perturbation theory (GVVPT2) method was used to investigate the low-lying electronic states of Ni(2). Because the nickel atom has an excitation energy of only 0.025 eV to its first excited state (the least in the first row of transition elements)...

Descripción completa

Detalles Bibliográficos
Autores principales: Tamukong, Patrick K., Hoffmann, Mark R.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Frontiers Media S.A. 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8155684/
https://www.ncbi.nlm.nih.gov/pubmed/34055745
http://dx.doi.org/10.3389/fchem.2021.678930
_version_ 1783699262698160128
author Tamukong, Patrick K.
Hoffmann, Mark R.
author_facet Tamukong, Patrick K.
Hoffmann, Mark R.
author_sort Tamukong, Patrick K.
collection PubMed
description The generalized Van Vleck second order multireference perturbation theory (GVVPT2) method was used to investigate the low-lying electronic states of Ni(2). Because the nickel atom has an excitation energy of only 0.025 eV to its first excited state (the least in the first row of transition elements), Ni(2) has a particularly large number of low-lying states. Full potential energy curves (PECs) of more than a dozen low-lying electronic states of Ni(2), resulting from the atomic combinations (3)F(4) + (3)F(4) and (3)D(3) + (3)D(3), were computed. In agreement with previous theoretical studies, we found the lowest lying states of Ni(2) to correlate with the (3)D(3) + (3)D(3) dissociation limit, and the holes in the d-subshells were in the subspace of delta orbitals (i.e., the so-dubbed δδ-states). In particular, the ground state was determined as X (1)Γ(g) and had spectroscopic constants: bond length (R (e)) = 2.26 Å, harmonic frequency (ω(e)) = 276.0 cm(−1), and binding energy (D (e)) = 1.75 eV; whereas the 1 (1)Σ(g) (+) excited state (with spectroscopic constants: R (e) = 2.26 Å, ω(e) = 276.8 cm(−1), and D (e) = 1.75) of the (3)D(3) + (3)D(3) dissociation channel lay at only 16.4 cm(−1) (0.002 eV) above the ground state at the equilibrium geometry. Inclusion of scalar relativistic effects through the spin-free exact two component (sf-X2C) method reduced the bond lengths of both of these two states to 2.20 Å, and increased their binding energies to 1.95 eV and harmonic frequencies to 296.0 cm(−1) for X (1)Γ(g) and 297.0 cm(−1) for 1 (1)Σ(g) (+). These values are in good agreement with experimental values of R (e) = 2.1545 ± 0.0004 Å, ω(e) = 280 ± 20 cm(−1), and D (0) = 2.042 ± 0.002 eV for the ground state. All states considered within the (3)F(4) + (3)F(4) dissociation channel proved to be energetically high-lying and van der Waals-like in nature. In contrast to most previous theoretical studies of Ni(2), full PECs of all considered electronic states of the molecule were produced.
format Online
Article
Text
id pubmed-8155684
institution National Center for Biotechnology Information
language English
publishDate 2021
publisher Frontiers Media S.A.
record_format MEDLINE/PubMed
spelling pubmed-81556842021-05-28 Low-Lying Electronic States of the Nickel Dimer Tamukong, Patrick K. Hoffmann, Mark R. Front Chem Chemistry The generalized Van Vleck second order multireference perturbation theory (GVVPT2) method was used to investigate the low-lying electronic states of Ni(2). Because the nickel atom has an excitation energy of only 0.025 eV to its first excited state (the least in the first row of transition elements), Ni(2) has a particularly large number of low-lying states. Full potential energy curves (PECs) of more than a dozen low-lying electronic states of Ni(2), resulting from the atomic combinations (3)F(4) + (3)F(4) and (3)D(3) + (3)D(3), were computed. In agreement with previous theoretical studies, we found the lowest lying states of Ni(2) to correlate with the (3)D(3) + (3)D(3) dissociation limit, and the holes in the d-subshells were in the subspace of delta orbitals (i.e., the so-dubbed δδ-states). In particular, the ground state was determined as X (1)Γ(g) and had spectroscopic constants: bond length (R (e)) = 2.26 Å, harmonic frequency (ω(e)) = 276.0 cm(−1), and binding energy (D (e)) = 1.75 eV; whereas the 1 (1)Σ(g) (+) excited state (with spectroscopic constants: R (e) = 2.26 Å, ω(e) = 276.8 cm(−1), and D (e) = 1.75) of the (3)D(3) + (3)D(3) dissociation channel lay at only 16.4 cm(−1) (0.002 eV) above the ground state at the equilibrium geometry. Inclusion of scalar relativistic effects through the spin-free exact two component (sf-X2C) method reduced the bond lengths of both of these two states to 2.20 Å, and increased their binding energies to 1.95 eV and harmonic frequencies to 296.0 cm(−1) for X (1)Γ(g) and 297.0 cm(−1) for 1 (1)Σ(g) (+). These values are in good agreement with experimental values of R (e) = 2.1545 ± 0.0004 Å, ω(e) = 280 ± 20 cm(−1), and D (0) = 2.042 ± 0.002 eV for the ground state. All states considered within the (3)F(4) + (3)F(4) dissociation channel proved to be energetically high-lying and van der Waals-like in nature. In contrast to most previous theoretical studies of Ni(2), full PECs of all considered electronic states of the molecule were produced. Frontiers Media S.A. 2021-05-13 /pmc/articles/PMC8155684/ /pubmed/34055745 http://dx.doi.org/10.3389/fchem.2021.678930 Text en Copyright © 2021 Tamukong and Hoffmann. https://creativecommons.org/licenses/by/4.0/This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
spellingShingle Chemistry
Tamukong, Patrick K.
Hoffmann, Mark R.
Low-Lying Electronic States of the Nickel Dimer
title Low-Lying Electronic States of the Nickel Dimer
title_full Low-Lying Electronic States of the Nickel Dimer
title_fullStr Low-Lying Electronic States of the Nickel Dimer
title_full_unstemmed Low-Lying Electronic States of the Nickel Dimer
title_short Low-Lying Electronic States of the Nickel Dimer
title_sort low-lying electronic states of the nickel dimer
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8155684/
https://www.ncbi.nlm.nih.gov/pubmed/34055745
http://dx.doi.org/10.3389/fchem.2021.678930
work_keys_str_mv AT tamukongpatrickk lowlyingelectronicstatesofthenickeldimer
AT hoffmannmarkr lowlyingelectronicstatesofthenickeldimer