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Название: Corrigendum to “Theoretical study of frustrated magnetic ordering in La1/3Ca2/3MnO3: The role of charge-orbital ordering” [J. Magn. Magn. Mater. 513 (2020) 167248] (Journal of Magnetism and Magnetic Materials (2020) 513, (S0304885320303437), (10.1016/j.jmmm.2020.167248))
Авторы: Gonchar, L. E.
Дата публикации: 2023
Издатель: Elsevier B.V.
Библиографическое описание: Gonchar, LE 2023, 'Corrigendum to “Theoretical study of frustrated magnetic ordering in La1/3Ca2/3MnO3: The role of charge-orbital ordering” [J. Magn. Magn. Mater. 513 (2020) 167248] (Journal of Magnetism and Magnetic Materials (2020) 513, (S0304885320303437), (10.1016/j.jmmm.2020.167248))', Journal of Magnetism and Magnetic Materials, Том. 575, 170749. https://doi.org/10.1016/j.jmmm.2023.170749
Gonchar, L. E. (2023). Corrigendum to “Theoretical study of frustrated magnetic ordering in La1/3Ca2/3MnO3: The role of charge-orbital ordering” [J. Magn. Magn. Mater. 513 (2020) 167248] (Journal of Magnetism and Magnetic Materials (2020) 513, (S0304885320303437), (10.1016/j.jmmm.2020.167248)). Journal of Magnetism and Magnetic Materials, 575, [170749]. https://doi.org/10.1016/j.jmmm.2023.170749
Аннотация: The author regrets an unintentional mistake in “Effect of external magnetic field” subsection of a recently published article. This mistake is concerned Fig. 6 horizontal axis labels and further discussion about it. Notwithstanding these corrections, all the other equations and results of the paper are correct as originally presented. The corrections are as follows: The estimation of the spin-flop field is Hsf = 27 T. The inflection point of the curve corresponds to a partial (for one kind of stripe) spin-flop transition at H = 27 T. The determinant contribution to the dependence of Fig. 6(c) gives the magnetization component, which is parallel to the field direction at H = 0 T. The spin-flop field is mainly dependent upon SIA and AFM SE interactions, and less dependent upon FM SE parameter. It is supposed to be stronger than the same field in half-doped manganites (Hsf ∼ 5 T [2]) and in pure manganite (Hsf ∼ 19 T [1])1. That can be explained by increase in the number of AFM pairs of manganese ions in crystal, despite decrease of the mean AFM-type SE interaction value in the pair and mean SIA value per magnetic ion with the increase of doping level comparing with pure and half-doped CO manganites. The author would like to apologise for any inconvenience caused. © 2023 Elsevier B.V.
URI: http://elar.urfu.ru/handle/10995/130405
Условия доступа: info:eu-repo/semantics/openAccess
Идентификатор SCOPUS: 85153188747
Идентификатор WOS: 000988637500001
Идентификатор PURE: 37832589
ISSN: 0304-8853
DOI: 10.1016/j.jmmm.2023.170749
Располагается в коллекциях:Научные публикации ученых УрФУ, проиндексированные в SCOPUS и WoS CC

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