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Neutron powder diffraction experiments on the layered triangular-lattice antiferromagnets RbFe(MoO$$_4$$)$$_2$$ and CsFe(SO$$_4$$)$$_2$$

層状三角格子反強磁性体RbFe(MoO$$_4$$)$$_2$$とCsFe(SO$$_4$$)$$_2$$の中性子回折実験

稲見 俊哉

Inami, Toshiya

層状三角格子反強磁性体RbFe(MoO$$_4$$)$$_2$$とCsFe(SO$$_4$$)$$_2$$の粉末試料を作成し、粉末中性子回折実験を行って磁気構造を決めた。どちらの化合物も磁気構造は三角面内は、いわゆる120度構造で、面間は非整合構造であった。秩序モーメントはab面内にあった。RbFe(MoO$$_4$$)$$_2$$については190Kで$$Pbar{3}m1$$から$$Pbar{3}$$への結晶構造変化も見いだした。

Powder specimens of the layered triangular lattice antiferromagnets RbFe(MoO$$_4$$)$$_2$$ and CsFe(SO$$_4$$)$$_2$$ were prepared and neutron powder diffraction experiments were carried out in order to determine the magnetic structure. Magnetic structure of both compounds is so-called 120$$^circ$$ structure in the triangular plane and incommensurate between the plane. The ordered moments are confined in the basal $$ab$$-plane. It is also found that RbFe(MoO$$_4$$)$$_2$$ shows structural phase transition at around 190 K from $$Pbar{3}m1$$ to $$Pbar{3}$$.

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パーセンタイル:75.4

分野:Chemistry, Inorganic & Nuclear

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