Synthesis, Detailed Characterization, and Theoretical Understanding of Mononuclear Chromium(III)-Containing Polyoxotungstates [Cr<sup>III</sup>(HX<sup>V</sup>W<sub>7</sub>O<sub>28</sub>)<sub>2</sub>]<sup>13–</sup> (X = P, As) with Exceptionally Large Magnetic Anisotropy

Abstract

Two monochromium­(III)-containing heteropolytungstates, [Cr<sup>III</sup>(HP<sup>V</sup>­W<sub>7</sub>O<sub>28</sub>)<sub>2</sub>]<sup>13‑</sup> (<b>1a</b>) and [Cr<sup>III</sup>(HAs<sup>V</sup>­W<sub>7</sub>O<sub>28</sub>)<sub>2</sub>]<sup>13‑</sup> (<b>2a</b>), were prepared via simple, one-pot reactions in aqueous, basic medium, by reaction of the composing elements, and then isolated as hydrated sodium salts, Na<sub>13</sub>[Cr<sup>III</sup>(HP<sup>V</sup>­W<sub>7</sub>O<sub>28</sub>)<sub>2</sub>]·47H<sub>2</sub>O (<b>1</b>) and Na<sub>13</sub>[Cr<sup>III</sup>(HAs<sup>V</sup>­W<sub>7</sub>O<sub>28</sub>)<sub>2</sub>]·52H<sub>2</sub>O (<b>2</b>). Polyanions <b>1a</b> and <b>2a</b> comprise an octahedrally coordinated Cr<sup>III</sup> ion, sandwiched by two {PW<sub>7</sub>} or {AsW<sub>7</sub>} units. Both compounds <b>1</b> and <b>2</b> were fully characterized in the solid state by single-crystal XRD, IR spectroscopy, thermogravimetric and elemental analyses, magnetic susceptibility, and EPR measurements. Magnetic studies on <b>1</b> and <b>2</b> demonstrated that both compounds exhibit appreciable deviation from typical paramagnetic behavior, and have a ground state S = <sup>3</sup>/<sub>2</sub>, as expected for a Cr<sup>III</sup> ion, but with an exceptionally large zero-field uniaxial anisotropy parameter (<i>D</i>). EPR measurements on powder and single-crystal samples of <b>1</b> and <b>2</b> using 9.5, 34.5, and 239.2 GHz frequencies and over 4–295 K temperature fully support the magnetization results and show that <i>D</i> = +2.4 cm<sup>–1</sup>, the largest and sign-assigned <i>D</i>-value so far reported for an octahedral Cr<sup>III</sup>-containing, molecular compound. Ligand field analysis of results from CASSCF and NEVPT2-correlated electronic structure calculations on Cr­(OH)<sub>6</sub><sup>3–</sup> model complexes allowed to unravel the crucial role of the second coordination sphere of Cr<sup>III</sup> for the unusually large magnetic anisotropy reflected by the experimental value of <i>D</i>. The newly developed theoretical modeling, combined with the synthetic procedure for producing such unusual magnetic molecules in a well-defined and essentially magnetically isolated environment, appears to be a versatile new research area

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