The
synthesis of Sr<sub>2</sub>FeO<sub>3</sub> through a hydride reduction
of the Ruddlesden–Popper layered perovskite Sr<sub>2</sub>FeO<sub>4</sub> is reported. Rietveld refinements using synchrotron and neutron
powder diffraction data revealed that the structure contains corner-shared
FeO<sub>4</sub> square-planar chains running along the [010] axis,
being isostructural with Sr<sub>2</sub>CuO<sub>3</sub> (<i>Immm</i> space group). Fairly strong Fe–O–Fe and Fe–Fe
interactions along [010] and [100], respectively, make it an <i>S</i> = 2 quasi two-dimensional (2D) rectangular lattice antiferromagnet.
This compound represents the end-member (<i>n</i> = 1) of
the 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
previously 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> = ∞),
thus giving an opportunity to study the 2D-to-3D dimensional crossover.
Neutron diffraction and Mössbauer spectroscopy show the occurrence
of <i>G</i>-type antiferromagnetic order below 179 K, which
is, because of dimensional reduction, significantly lower than those
of 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
of magnetic moment shows a universal behavior.