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The First VanadateāCarbonate, K<sub>2</sub>Mn<sub>3</sub>(VO<sub>4</sub>)<sub>2</sub>(CO<sub>3</sub>): Crystal Structure and Physical Properties
Mixed potassiumāmanganese vanadateācarbonate,
K<sub>2</sub>Mn<sub>3</sub>(VO<sub>4</sub>)<sub>2</sub>(CO<sub>3</sub>),
represents a novel structure type; it has been synthesized hydrothermally
from the system MnCl<sub>2</sub>āK<sub>2</sub>CO<sub>3</sub>āV<sub>2</sub>O<sub>5</sub>āH<sub>2</sub>O. Its hexagonal
crystal structure was determined by single-crystal X-ray diffraction
with <i>a</i> = 5.201(1) Ć
, <i>c</i> = 22.406(3)
Ć
, space group <i>P</i>6<sub>3</sub>/<i>m</i>, <i>Z</i> = 2, Ļ<sub>c</sub> = 3.371 g/cm<sup>3</sup>, and <i>R</i> = 0.022. The layered structure of the compound
can be described as a combination of honeycomb-type modules of [MnO<sub>6</sub>] octahedra and [VO<sub>4</sub>] tetrahedra, alternating in
the [001] direction with layers of [MnCO<sub>3</sub>] built by [MnO<sub>5</sub>] trigonal bipyramids and [CO<sub>3</sub>] planar triangles,
sharing oxygen vertices. The K<sup>+</sup> ions are placed along channels
of the framework, elongated in the [100], [010], and [110] directions.
The title compound exhibits rich physical properties reflected in
a phase transition of presumably JahnāTeller origin at <i>T</i><sub>3</sub> = 80ā100 K as well as two successive
magnetic phase transitions at <i>T</i><sub>2</sub> = 3 K
and <i>T</i><sub>1</sub> = 2 K into a weakly ferromagnetic
ground state, as evidenced in magnetization, specific heat, and X-band
electron spin resonance measurements. A negative Weiss temperature
Ī = ā114 K and strongly reduced effective magnetic moment
Ī¼<sub>eff</sub><sup>2</sup> ā¼ 70 Ī¼<sub>B</sub><sup>2</sup> per formula unit suggest that antiferromagnetic exchange
interactions dominate in the system. Divalent manganese is present
in a high-spin state, <i>S</i> = <sup>5</sup>/<sub>2</sub>, in the octahedral environment and a low-spin state, <i>S</i> = <sup>1</sup>/<sub>2</sub>, in the trigonal-bipyramidal coordination