Abstract

The crystal structure of KRuO<sub>4</sub> is refined at both 280 and 3.5 K from neutron powder data, and magnetic properties are reported for the first time. The scheelite structure, <i>I</i>4<sub>1</sub>/<i>a</i>, is confirmed at both temperatures. Atomic positions of greater accuracy than the original 1954 X-ray study are reported. The rare Ru<sup>7+</sup> ion resides in a site of distorted tetrahedral symmetry with nominal electronic configuration 4d<sup>1</sup>(e<sup>1</sup>). Curie–Weiss parameters are near free ion values for the effective moment and θ = −77 K, indicating dominant antiferromagnetic (AF) correlations. A broad susceptibility maximum occurs near 34 K, but long-range AF order sets in only below 22.4 K as determined by magnetization and heat capacity data. The entropy loss below 50 K is only 44% of the expected <i>R</i> ln 2, indicating the presence of short-range spin correlations over a wide temperature range. The Ru sublattice consists of centered, corner-sharing tetrahedra which can lead to geometric frustration if both the nearest-neighbor, <i>J</i><sub>1</sub>, and the next-nearest-neighbor, <i>J</i><sub>2</sub>, exchange constants are AF and of similar magnitude. A spin dimer analysis finds <i>J</i><sub>1</sub>/<i>J</i><sub>2</sub> ≈ 25, indicating weak frustration, and a (d<sub><i>z</i></sub><sup>2</sup>)<sup>1</sup> ground state. A single, weak magnetic reflection was indexed as (110). The absence of the (002) magnetic reflection places the Ru moments parallel to the <i>c</i> axis. The Ru<sup>7+</sup> moment is estimated to be 0.57(7) μ<sub>B</sub>, reduced from an expected value near 1 μ<sub>B</sub>. A recent computational study of isostructural, isoelectronic KOsO<sub>4</sub> predicts a surprisingly large orbital moment due to spin–orbit coupling (SOC). However, the free ion SOC constant for Ru<sup>7+</sup> is only ∼30% that of Os<sup>7+</sup>, so it is unclear that this effect can be implicated in the low ordered moment for KRuO<sub>4</sub>. The origin of the short-range spin correlations is also not understood

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