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Rotational excitation of C(2)(X(1)Σ(g)(+)) by para- and ortho-H(2)

A new four dimensional (4D) potential energy surface for the C(2)(X(1)Σ(g)(+))–H(2) van der Waals system is generated. The potential was obtained from a multi-reference internally contracted configuration-interaction method including the Davidson correction (MRCI+Q). The four atoms were described us...

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Detalles Bibliográficos
Autores principales: Najar, Faouzi, Kalugina, Yulia
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9050006/
https://www.ncbi.nlm.nih.gov/pubmed/35497826
http://dx.doi.org/10.1039/c9ra10319h
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author Najar, Faouzi
Kalugina, Yulia
author_facet Najar, Faouzi
Kalugina, Yulia
author_sort Najar, Faouzi
collection PubMed
description A new four dimensional (4D) potential energy surface for the C(2)(X(1)Σ(g)(+))–H(2) van der Waals system is generated. The potential was obtained from a multi-reference internally contracted configuration-interaction method including the Davidson correction (MRCI+Q). The four atoms were described using the augmented correlation-consistent quadruple zeta (aug-cc-pVQZ) basis sets. Both molecules were treated as rigid rotors. Close-coupling calculations of the inelastic integral cross sections of C(2) in collisions with para-H(2)(j(H(2)) = 0) and ortho-H(2)(j(H(2)) = 1) were also carried out at low energies. After Boltzmann thermal averaging, rate coefficients were obtained for temperatures ranging from 5 to 100 K. The rate coefficients for collisions with ortho-H(2) are significantly larger than the rate coefficients for collisions with para-H(2).
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spelling pubmed-90500062022-04-29 Rotational excitation of C(2)(X(1)Σ(g)(+)) by para- and ortho-H(2) Najar, Faouzi Kalugina, Yulia RSC Adv Chemistry A new four dimensional (4D) potential energy surface for the C(2)(X(1)Σ(g)(+))–H(2) van der Waals system is generated. The potential was obtained from a multi-reference internally contracted configuration-interaction method including the Davidson correction (MRCI+Q). The four atoms were described using the augmented correlation-consistent quadruple zeta (aug-cc-pVQZ) basis sets. Both molecules were treated as rigid rotors. Close-coupling calculations of the inelastic integral cross sections of C(2) in collisions with para-H(2)(j(H(2)) = 0) and ortho-H(2)(j(H(2)) = 1) were also carried out at low energies. After Boltzmann thermal averaging, rate coefficients were obtained for temperatures ranging from 5 to 100 K. The rate coefficients for collisions with ortho-H(2) are significantly larger than the rate coefficients for collisions with para-H(2). The Royal Society of Chemistry 2020-02-27 /pmc/articles/PMC9050006/ /pubmed/35497826 http://dx.doi.org/10.1039/c9ra10319h Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/
spellingShingle Chemistry
Najar, Faouzi
Kalugina, Yulia
Rotational excitation of C(2)(X(1)Σ(g)(+)) by para- and ortho-H(2)
title Rotational excitation of C(2)(X(1)Σ(g)(+)) by para- and ortho-H(2)
title_full Rotational excitation of C(2)(X(1)Σ(g)(+)) by para- and ortho-H(2)
title_fullStr Rotational excitation of C(2)(X(1)Σ(g)(+)) by para- and ortho-H(2)
title_full_unstemmed Rotational excitation of C(2)(X(1)Σ(g)(+)) by para- and ortho-H(2)
title_short Rotational excitation of C(2)(X(1)Σ(g)(+)) by para- and ortho-H(2)
title_sort rotational excitation of c(2)(x(1)σ(g)(+)) by para- and ortho-h(2)
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9050006/
https://www.ncbi.nlm.nih.gov/pubmed/35497826
http://dx.doi.org/10.1039/c9ra10319h
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