2002
DOI: 10.1016/s0921-4526(02)01196-1
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Magnetic anisotropy and ferro-antiferromagnetic phase transition in LaMn2Si2

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Cited by 28 publications
(21 citation statements)
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“…In contrast to the soft magnetic bulk material with neglectable coercivity (o10 Oe), magnetic hardening is observed for the nanocrystalline LaMn 2 Si 2, reflected in the coercivity field strength of 6 kOe at 10 K. The coercivity decreases with increasing temperature and vanishes at the Curie temperature. The Mn sublattice exhibits a large uniaxial magnetic anisotropy with the easy magnetization direction lying along the tetragonal c-axis below T inter C , and the anisotropy field of this compound reaches 60 kOe at the cryogenic temperatures [25]. This may leads to observed magnetic hardness of LaMn 2 Si 2, in a nanocrystalline state.…”
Section: Article In Pressmentioning
confidence: 96%
“…In contrast to the soft magnetic bulk material with neglectable coercivity (o10 Oe), magnetic hardening is observed for the nanocrystalline LaMn 2 Si 2, reflected in the coercivity field strength of 6 kOe at 10 K. The coercivity decreases with increasing temperature and vanishes at the Curie temperature. The Mn sublattice exhibits a large uniaxial magnetic anisotropy with the easy magnetization direction lying along the tetragonal c-axis below T inter C , and the anisotropy field of this compound reaches 60 kOe at the cryogenic temperatures [25]. This may leads to observed magnetic hardness of LaMn 2 Si 2, in a nanocrystalline state.…”
Section: Article In Pressmentioning
confidence: 96%
“…1. It can be seen that substitution of Cu for Mn results in a linear decrease in [14][15][16][17]. In the LaMn 2−x Cu x Si 2 series, the lattice parameter a is always longer than 4.06 Å, and ferromagnetic coupling at room temperature would be expected accordingly.…”
Section: Resultsmentioning
confidence: 96%
“…The RMn 2 Ge 2 compounds (where R is La, Ce, Pr and Nd) and LaMn 2 Si 2 are simple ferromagnets with Curie temperatures around room temperature and their easy direction of magnetization has been found to be along the c-axis [1,4]. According to recent neutron diffraction studies on LaMn 2 Si 2 , it has a canted ferromagnetic structure (F mc ) from T C down to around 45 K, where the canted structure and a conical magnetic structure (F mi ) coexist below T h ≈ 45 K. An antiferromagnetic structure (AF mc ) occurs at T > T C up to the Néel temperature T N = 470 K [15][16][17]. In our previous study [18], it was found that LaMn 2 Si 2 exhibits a mixed magnetic phase composed of F mc and AF mc structure just below the Curie temperature between T 1 and T 2 .…”
Section: Introductionmentioning
confidence: 99%
“…По данным магнитных измерений LaMn 2 Si 2 при низ-ких температурах является одноосным ферромагнети-ком (F) с полем анизотропии 60 kOe [13,14]. Однако данные нейтронографии показывают, что помимо фер-ромагнитно упорядоченной z -компоненты присутствуют антиферромагнитно связанные компоненты магнитного момента марганца в базисной плоскости.…”
Section: экспериментальные результаты и их обсуждениеunclassified
“…В соединении LaMn 2 Si 2 с немагнитным La и ферро-магнитным межслоевым упорядочением магнитных мо-ментов Mn наблюдается большая одноосная магнитная анизотропия в марганцевой подрешетке с легким направ-лением вдоль тетрагональной c-оси [12,13], вследствие чего суммарный отличный от нуля магнитный момент атомов Mn в слое практически всегда направлен перпен-дикулярно плоскости слоя вдоль c-оси. Дополнительную анизотропию при низкой температуре вносят редкозе-мельные атомы с частично заполненной 4 f -электронной оболочкой, что может приводить к индуцированным магнитным полем фазовым переходам.…”
unclassified