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Resonance Parameters, Autoionisation of 2S+1Lo Doubly Excited N5+ Ion States Associated with n=3 and 4, N6+ Threshold

Received: 8 August 2020    Accepted: 26 August 2020    Published: 3 September 2020
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Abstract

The motivation of the diagonalization method is to take into consideration the coupling between closed and opened channels in term of perturbation theory and to neglect the indirect coupling as well but also the autoionisation states through the opened channels. This procedure leads to a relatively simple mathematical problem consisting of solving a system of linear algebraic equations instead of a system of coupled differential equations or integro-differential equations. Diagonalization method under LS coupling scheme for the states 1,3Po; 1,3Do; 1,3Fo; 1,3Go; 1,3Ho was performed. The partial widths for multi-channel autoionizing levels to sublevels of N6+ were carried out by neglecting the direct coupling between opened channels. The calculations of total and partial widths of the (nln'l') 1,3Lo (L=1, 2, 3, 4 and 5) multiple-decay-channel system N5+ were performed. From L=1 to 2, the (4l4l') 1,3Lo states located under n=3 and the (3lnl') 1,3Lo states follow the same rules. All the (4l4l') 1,3Go and (4l4l') 1,3Ho states located under n=3 observe the rule 1.

Published in Nuclear Science (Volume 5, Issue 3)
DOI 10.11648/j.ns.20200503.11
Page(s) 27-35
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This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2024. Published by Science Publishing Group

Keywords

Autoionisation, Electron Correlation, Partial Width

References
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    Oumar Tidiane Ba, Cheikh Amadou Bamba Dath, Alassane Traore, Ababacar Sadikhe Ndao. (2020). Resonance Parameters, Autoionisation of 2S+1Lo Doubly Excited N5+ Ion States Associated with n=3 and 4, N6+ Threshold. Nuclear Science, 5(3), 27-35. https://doi.org/10.11648/j.ns.20200503.11

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    Oumar Tidiane Ba; Cheikh Amadou Bamba Dath; Alassane Traore; Ababacar Sadikhe Ndao. Resonance Parameters, Autoionisation of 2S+1Lo Doubly Excited N5+ Ion States Associated with n=3 and 4, N6+ Threshold. Nucl. Sci. 2020, 5(3), 27-35. doi: 10.11648/j.ns.20200503.11

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    AMA Style

    Oumar Tidiane Ba, Cheikh Amadou Bamba Dath, Alassane Traore, Ababacar Sadikhe Ndao. Resonance Parameters, Autoionisation of 2S+1Lo Doubly Excited N5+ Ion States Associated with n=3 and 4, N6+ Threshold. Nucl Sci. 2020;5(3):27-35. doi: 10.11648/j.ns.20200503.11

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  • @article{10.11648/j.ns.20200503.11,
      author = {Oumar Tidiane Ba and Cheikh Amadou Bamba Dath and Alassane Traore and Ababacar Sadikhe Ndao},
      title = {Resonance Parameters, Autoionisation of 2S+1Lo Doubly Excited N5+ Ion States Associated with n=3 and 4, N6+ Threshold},
      journal = {Nuclear Science},
      volume = {5},
      number = {3},
      pages = {27-35},
      doi = {10.11648/j.ns.20200503.11},
      url = {https://doi.org/10.11648/j.ns.20200503.11},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ns.20200503.11},
      abstract = {The motivation of the diagonalization method is to take into consideration the coupling between closed and opened channels in term of perturbation theory and to neglect the indirect coupling as well but also the autoionisation states through the opened channels. This procedure leads to a relatively simple mathematical problem consisting of solving a system of linear algebraic equations instead of a system of coupled differential equations or integro-differential equations. Diagonalization method under LS coupling scheme for the states 1,3Po; 1,3Do; 1,3Fo; 1,3Go; 1,3Ho was performed. The partial widths for multi-channel autoionizing levels to sublevels of N6+ were carried out by neglecting the direct coupling between opened channels. The calculations of total and partial widths of the (nln'l') 1,3Lo (L=1, 2, 3, 4 and 5) multiple-decay-channel system N5+ were performed. From L=1 to 2, the (4l4l') 1,3Lo states located under n=3 and the (3lnl') 1,3Lo states follow the same rules. All the (4l4l') 1,3Go and (4l4l') 1,3Ho states located under n=3 observe the rule 1.},
     year = {2020}
    }
    

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  • TY  - JOUR
    T1  - Resonance Parameters, Autoionisation of 2S+1Lo Doubly Excited N5+ Ion States Associated with n=3 and 4, N6+ Threshold
    AU  - Oumar Tidiane Ba
    AU  - Cheikh Amadou Bamba Dath
    AU  - Alassane Traore
    AU  - Ababacar Sadikhe Ndao
    Y1  - 2020/09/03
    PY  - 2020
    N1  - https://doi.org/10.11648/j.ns.20200503.11
    DO  - 10.11648/j.ns.20200503.11
    T2  - Nuclear Science
    JF  - Nuclear Science
    JO  - Nuclear Science
    SP  - 27
    EP  - 35
    PB  - Science Publishing Group
    SN  - 2640-4346
    UR  - https://doi.org/10.11648/j.ns.20200503.11
    AB  - The motivation of the diagonalization method is to take into consideration the coupling between closed and opened channels in term of perturbation theory and to neglect the indirect coupling as well but also the autoionisation states through the opened channels. This procedure leads to a relatively simple mathematical problem consisting of solving a system of linear algebraic equations instead of a system of coupled differential equations or integro-differential equations. Diagonalization method under LS coupling scheme for the states 1,3Po; 1,3Do; 1,3Fo; 1,3Go; 1,3Ho was performed. The partial widths for multi-channel autoionizing levels to sublevels of N6+ were carried out by neglecting the direct coupling between opened channels. The calculations of total and partial widths of the (nln'l') 1,3Lo (L=1, 2, 3, 4 and 5) multiple-decay-channel system N5+ were performed. From L=1 to 2, the (4l4l') 1,3Lo states located under n=3 and the (3lnl') 1,3Lo states follow the same rules. All the (4l4l') 1,3Go and (4l4l') 1,3Ho states located under n=3 observe the rule 1.
    VL  - 5
    IS  - 3
    ER  - 

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Author Information
  • Department of Physics, Sciences and Technologies Faculty, University Cheikh Anta Diop, Dakar, Senegal

  • Department of Physics, Sciences and Technologies Faculty, University Cheikh Anta Diop, Dakar, Senegal

  • Department of Physics, Sciences and Technologies Faculty, University Cheikh Anta Diop, Dakar, Senegal

  • Department of Physics, Sciences and Technologies Faculty, University Cheikh Anta Diop, Dakar, Senegal

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