TY - JOUR

T1 - 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))

AU - Gonchar, L. E.

PY - 2023

Y1 - 2023

N2 - 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.

AB - 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.

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U2 - 10.1016/j.jmmm.2023.170749

DO - 10.1016/j.jmmm.2023.170749

M3 - Comment/debate

VL - 575

JO - Journal of Magnetism and Magnetic Materials

JF - Journal of Magnetism and Magnetic Materials

SN - 0304-8853

M1 - 170749

ER -