Unhydrated Cr(V) peroxychromates M3CrO8 (M = Na, K, Rb): Low-dimensional antiferromagnets exhibiting large specific heats at mK to 5 K temperatures

Authors
Citation
B. Cage et Ns. Dalal, Unhydrated Cr(V) peroxychromates M3CrO8 (M = Na, K, Rb): Low-dimensional antiferromagnets exhibiting large specific heats at mK to 5 K temperatures, CHEM MATER, 13(3), 2001, pp. 880-890
Citations number
42
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Material Science & Engineering
Journal title
CHEMISTRY OF MATERIALS
ISSN journal
08974756 → ACNP
Volume
13
Issue
3
Year of publication
2001
Pages
880 - 890
Database
ISI
SICI code
0897-4756(200103)13:3<880:UCPM(=>2.0.ZU;2-J
Abstract
The alkali-metal Cr(V) peroxychromates with the general formula M3CrO8 (M = Na, K, Rb, and combinations thereof) and the 3d(1) ground state have been characterized by X-ray diffraction, variable frequency and variable tempera ture EPR, magnetic susceptibility, and thermodynamic techniques. K3CrO8 and Rb3CrO8 are isomorphous, with space groups as I (4) over bar 2m, whereas N a3CrO8 and K2NaCrO8 exhibit the orthorhombic space groups Cmc2 and Pbcm, re spectively. Lattice parameters are presented for all of these compounds and are shown to depend sensitively on the cation. EPR measurements reveal tha t while the electronic ground state of Na3CrO8, K3CrO8, and Rb3CrO8 is 3d(x 2-y2), that of the mixed salts, such as K2NaCrO8 and Rb2NaCrO8, is 3d(z)2 t he origin of this switch is not yet clear. Specific heat measurements showe d that K3CrO8 undergoes an antiferromagnetic ordering transition at T-N = 0 .38 K and displays a broad peak around 0.8 K, which can be interpreted in t erms of a Bonner-Fisher model. Rb3CrO8 behaves similarly, with a broad peak at 0.52 K. Na3CrO8 exhibits a a-like antiferromagnetic transition at 2.35 K, with K2NaCrO8 behaving similarly, with TN lower than 1.8 K. The exchange constants and the transition temperatures depend sensitively on the cation . These compounds all are found to exhibit large specific heats throughout the mK to 5 K temperature range, and the possibility exists of tuning the t hermodynamic properties via dilution with compatible diamagnetic lattices s uch as M3NbO8. Their specific heat data indicate that they could find appli cations as tunable heat sinks and magnetic refrigerants in the mK to 5 K ra nge.