Kenji Ohoyama

Hole-concentration-induced transformation of the magnetic and orbital structures in Nd 1 − x Sr x MnO 3

We have peformed neutron diffraction measurements on melt-grown polycrystalline samples of

Relation between crystal and magnetic structures of layered manganite La2-2xSr1+2xMn2O7 (0.30 ≤ x ≤ 0.50)

{\mathrm{Nd}}_{1\ensuremath{-}x}{\mathrm{Sr}}_{x}{\mathrm{MnO}}_{3}

CaFeO2: a new type of layered structure with iron in a distorted square planar coordination.

(0.49l~xl~0.75).

Revised Crystal Structure Model of Li2NH by Neutron Powder Diffraction

A systematic transformation of the crystalline and magnetic structures of this system was observed. This can be consistently explained by the change of the character of the Mn

Relationship between Structure and Superconductivity in FeSe1-xTex

{e}_{g}

Ground State Properties of the A-site Ordered Manganites, RBaMn2O6 (R = La, Pr and Nd)

orbitals. When increasing X, the

Characteristic magnetic structure due to antiferroquadrupolar ordering in Ho11B2C2

{\mathrm{Nd}}_{1\ensuremath{-}x}{\mathrm{Sr}}_{x}{\mathrm{MnO}}_{3}

Emergence of Magnetic Long-range Order in Frustrated Pyrochlore Nd2Ir2O7 with Metal–Insulator Transition

system exhibits an evolution from a metallic ferromagnetic state, to a metallic A-type antiferromagnetic (AFM), and then to an insulating C-type AFM state. The CE-type charge-ordered AFM state was observed only in the vicinity of

Crystal and magnetic structure of conducting double perovskite Sr2FeMoO6

x=1/2