The solid solutions of with the “114” hexagonal symmetry could be synthesized for . The dc magnetization study of these oxides shows that they are ferrimagnetic (FiM). The FiM to paramagnetic transition temperature, , decreases from 265.6 K for to 97.5 K for in agreement with the introduction of the diamagnetic cation at the Fe sublattice. No magnetic saturation is observed and the coercive field is very large, ranging from 0.7 to 0.9 T at 5 K. Importantly, the ac magnetic susceptibility, , indicates a frequency-dependent freezing temperature, , increasing with frequency and satisfying the conventional power law, . For the undoped (CBFO) , the best fitting parameters are characteristic of a spin glass with a transition temperature , spin-relaxation time , and critical exponent of 6.4. In contrast, for series the increases from to as is increased; the values of are in the range of 12–13, which lies much closer to that of cluster glasses (; ). The resistivity behavior is consistent with small polaronic hopping which changes to variable range hopping at low temperatures. The measurements under show that only CBFO (undoped) exhibits magnetoresistance, with a maximum value of 4.3% at 264 K.
8 December 2020 in Journal of Materials Chemistry C
Derivatives of the natural mineral colusite with general formula Cu26A2E6S32 (A = V, Nb, Ta, Cr, Mo, W; E = Ge, Sn, As, Sb) are an emerging class of excellent thermoelectric materials. Within just a few years, they have been promoted as serious candidates for cost-efficient, environmentally-friendly thermoelectric power generation, reaching performances comparable to tetrahedrites and other advanced thermoelectric sulphides. From ultralow thermal conductivity to the record-high power factor, this review gives an extensive description of the current state of the art regarding the crystal chemistry and electrical and thermal transport properties of colusites.
1 May 2024 in Journal of the American Chemical Society
The discovery of the monoclinic Cu5Sn2S7phase adds a high mobility member to the Cu–Sn–S diagram and demonstrates how the crystal structure can be advantageously manipulated to design novel compositions for energy-oriented applications.
15 October 2024 in Journal of the American Chemical Society