2026-05-12T15:00:35Zhttps://riubu.ubu.es/oai/request

oai:riubu.ubu.es:10259/105202025-06-06T00:05:17Zcom_10259.4_2527com_10259_5086com_10259_2604col_10259.4_2528

Alonso Martín, Julio Alfonso bf0711f1-a98f-4d89-bab3-82152985963f 600 Cordero Tejedor, Nicolás A. 128 600 0000-0002-3609-4163 2025-06-05T11:05:01Z 2025-06-05T11:05:01Z 2025-08 2027-05-24 2210-271X https://hdl.handle.net/10259/10520 10.1016/j.comptc.2025.115298 Accurate correlation energies Ecorr of neutral atoms with atomic number Z =1–18, calculated from a combination of experimental and theoretical information, are available in the literature. Those empirical correlation energies show a grossly linear behaviour with Z. However, in more detail Ecorr deviates from global linearity and reveals a piece-wise linear behaviour with different slopes as the different electronic shells are progressively filled. This behaviour can be explained by writing Ecorr as a sum of pairing-correlation contributions. The pairing- correlation energies have been obtained from the empirical total correlation energies of atoms. Those pairing- correlations are very weak for electrons in different main shells (K, L, M shells) and larger for electrons in the same main shell. In addition, the pairing-correlation energies depend on the angular momenta of the two electronic orbitals. Those features are due to the role of the quantum overlap between the wave functions of the electrons involved in the pairing. Pairs of electrons showing a very small orbital overlap lead to negligible pairing-correlation energies. Keeping a reasonable number of terms, the shell- and angular momentum- dependent pairing-correlation energies explain well the intricate piece-wise linear behaviour of Ecorr(Z) up to Z =18. Also, certain approximations applied to the pairing-correlation energies permit to justify the grossly linear trend of Ecorr with Z, and the more precise faster-than-linear behaviour of Ecorr(Z). This work was supported by grant PID2022-138340OB-I00 funded by MCIN/AEI/ 10.13039/501100011033 and FSE+, grant PID2023- 148373NB-I00 funded by MCIU/AEI/10.13039/501100011033/ FEDER UE, by the European Union Next Generation EU (PRTR C17.I1), and by Junta de Castilla y Le´ on (Apoyo a GIR, Project VA029G24). application/pdf eng Elsevier Computational and Theoretical Chemistry https://doi.org/10.1016/j.comptc.2025.115298 Attribution-NonCommercial-NoDerivatives 4.0 Internacional http://creativecommons.org/licenses/by-nc-nd/4.0/ info:eu-repo/semantics/embargoedAccess Atoms Correlation Pairing Química Chemistry Interpretation of the correlation energy of atoms, and its dependence with atomic number Z up to Z = 18 info:eu-repo/semantics/article info:eu-repo/semantics/acceptedVersion Computational and Theoretical Chemistry 1250 115298 THUMBNAIL Alonso-catc_2025.pdf.jpg Alonso-catc_2025.pdf.jpg IM Thumbnail image/jpeg 3876 https://riubu.ubu.es/bitstream/10259/10520/4/Alonso-catc_2025.pdf.jpg 6b3b7ddb5b31d2a539bcf1a420f52e6d MD5 4 LICENSE license.txt license.txt text/plain; charset=utf-8 1362 https://riubu.ubu.es/bitstream/10259/10520/3/license.txt 5d013bfa6e473ff0db22cd82a4d71a70 MD5 3 CC-LICENSE license_rdf license_rdf application/rdf+xml; charset=utf-8 805 https://riubu.ubu.es/bitstream/10259/10520/2/license_rdf 4460e5956bc1d1639be9ae6146a50347 MD5 2 ORIGINAL Alonso-catc_2025.pdf Alonso-catc_2025.pdf application/pdf 1635617 https://riubu.ubu.es/bitstream/10259/10520/1/Alonso-catc_2025.pdf 8f493c34f0970d7f85fc0abdc37fed1b MD5 1 10259/10520 oai:riubu.ubu.es:10259/10520 2025-06-06 02:05:17.103 Repositorio Institucional de la Universidad de Burgos bubrep@ubu.es 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