Cédric Tassel (1466074)Liis Seinberg (1957501)Naoaki Hayashi (1406059)Subodh Ganesanpotti (1957498)Yoshitami Ajiro (1552075)Yoji Kobayashi (1466080)Hiroshi Kageyama (1466059)
The\nsynthesis of Sr<sub>2</sub>FeO<sub>3</sub> through a hydride reduction\nof the Ruddlesden–Popper layered perovskite Sr<sub>2</sub>FeO<sub>4</sub> is reported. Rietveld refinements using synchrotron and neutron\npowder diffraction data revealed that the structure contains corner-shared\nFeO<sub>4</sub> square-planar chains running along the [010] axis,\nbeing isostructural with Sr<sub>2</sub>CuO<sub>3</sub> (<i>Immm</i> space group). Fairly strong Fe–O–Fe and Fe–Fe\ninteractions along [010] and [100], respectively, make it an <i>S</i> = 2 quasi two-dimensional (2D) rectangular lattice antiferromagnet.\nThis compound represents the end-member (<i>n</i> = 1) of\nthe serial system Sr<sub><i>n</i>+1</sub>Fe<sub><i>n</i></sub>O<sub>2<i>n</i>+1</sub>, together with\npreviously reported Sr<sub>3</sub>Fe<sub>2</sub>O<sub>5</sub> (<i>n</i> = 2) and SrFeO<sub>2</sub> (<i>n</i> = ∞),\nthus giving an opportunity to study the 2D-to-3D dimensional crossover.\nNeutron diffraction and Mössbauer spectroscopy show the occurrence\nof <i>G</i>-type antiferromagnetic order below 179 K, which\nis, because of dimensional reduction, significantly lower than those\nof the other members, 296 K in Sr<sub>3</sub>Fe<sub>2</sub>O<sub>5</sub> and 468 K in SrFeO<sub>2</sub>. However, the temperature dependence\nof magnetic moment shows a universal behavior.
Jeongho Yeon (1406326)Sang-Hwan Kim (527119)Sau Doan Nguyen (1985821)Hana Lee (445860)P. Shiv Halasyamani (1261704)
Takamasa IshigakiShigeru YamauchiKazuo Fueki
Yong Dan ZhuCheng HuAn You Zuo
Junghwan Do (2102317)Ranko P. Bontchev (2425492)Allan J. Jacobson (1644922)