4 research outputs found
Exceptional Layered Ordering of Cobalt and Iron in Perovskites
Exceptional
Layered Ordering of Cobalt and Iron in
Perovskite
Copper Hyper-Stoichiometry: The Key for the Optimization of Thermoelectric Properties in Stannoidite Cu<sub>8+<i>x</i></sub>Fe<sub>3–<i>x</i></sub>Sn<sub>2</sub>S<sub>12</sub>
A univalent
copper hyper-stoichiometric stannoidite Cu<sub>8+<i>x</i></sub>Fe<sub>3–<i>x</i></sub>Sn<sub>2</sub>S<sub>12</sub> with 0 ≤ <i>x</i> ≤ 0.5 has
been synthesized using mechanical alloying followed by spark plasma
sintering. The X-ray diffraction analysis combined with <sup>57</sup>Fe and <sup>119</sup>Sn Mössbauer investigations has allowed
the charge distribution of the cationic species on the various sites
to be established and suggests the possibility of a small tin deficiency.
The transport properties show a remarkable crossover from a semiconducting
to a metal-like behavior as the copper content increases from <i>x</i> = 0 to <i>x</i> = 0.5, whereas correlatively
the Seebeck coefficient decreases moderately, with <i>S</i> values ranging from 310 to 100 μV/K. The thermal conductivity
decreases as the temperature increases showing low values at high
temperature, far below those reported in related stannite materials.
The investigation of the thermoelectric properties shows that the <i>ZT</i> figure of merit is dramatically enhanced by the copper
hyper-stoichiometry by a factor of 5 going from 0.07 for <i>x</i> = 0 to 0.35 for <i>x</i> = 0.5 at 630 K. This thermoelectric
behavior is interpreted on the basis of a model involving the Cu–S
framework as the conducting electronic network where the Fe<sup>2+</sup>/Fe<sup>3+</sup> species play the role of hole reservoir
Lone-Pair-Driven Structure Dimensionality: the Way to Ultralow Thermal Conductivity in Pb<sub><i>m</i></sub>Bi<sub>2</sub>S<sub>3+<i>m</i></sub> Sulfides
Understanding the mechanisms that connect heat transport
with crystal
structures is fundamental to develop materials with optimized electrical
and thermal properties for thermoelectric applications. In this work,
we synthesized a series of bulk Cl-doped PbBi2S4 by mechanical alloying combined with spark plasma sintering. A detailed
structural analysis of PbBi2S4 (m = 1 member of the series PbmBi2S3+m) and of the compounds Bi2S3 (m = 0) and Pb3Bi2S6 (m = 3) shows that the low dimensionality
of their frameworks is induced by the stereochemical activity of Bi3+ and Pb2+ 6s2 lone pairs (L) and is
mainly governed by the presence of BiS3L chains of tetrahedrons.
By combining experiments with the ab initio band structure and phonon
calculations, we discuss the structure-thermoelectric property relationships
and clarify the interesting crystal chemistry in this system. We demonstrate
that the ultralow thermal conductivity of these sulfides originates
from the prominent 1D character induced by the bismuth chains in these
frameworks, leading to weak interchain interactions compared to their
strong intrachain bonds
Designing a Thermoelectric Copper-Rich Sulfide from a Natural Mineral: Synthetic Germanite Cu<sub>22</sub>Fe<sub>8</sub>Ge<sub>4</sub>S<sub>32</sub>
This
study shows that the design of copper-rich sulfides by mimicking natural
minerals allows a new germanite-type sulfide Cu<sub>22</sub>Fe<sub>8</sub>Ge<sub>4</sub>S<sub>32</sub> with promising thermoelectric
properties to be synthesized. The Mössbauer spectroscopy and
X-ray diffraction analyses provide evidence that the structure of
our synthetic compound differs from that of the natural germanite
mineral Cu<sub>26</sub>Fe<sub>4</sub>Ge<sub>4</sub>S<sub>32</sub> by
its much higher Cu<sup>+</sup>/Cu<sup>2+</sup> ratio and different
cationic occupancies. The coupled substitution Cu/Fe in the Cu<sub>26–<i>x</i></sub>Fe<sub>4+<i>x</i></sub>Ge<sub>4</sub>S<sub>32</sub> series also appears as a promising
approach to optimize the thermoelectric properties. The electrical
resistivity, which decreases slightly as the temperature increases,
shows that these materials exhibit a semiconducting behavior, but
are at the border of a metallic state. The magnitudes of the electrical
resistivity and Seebeck coefficient increase with <i>x</i>, which suggests that Fe for Cu substitution decreases the hole concentration.
The thermal conductivity decreases as the temperature increases leading
to a moderately low value of 1.2 W m<sup>–1</sup> K<sup>–1</sup> and a maximum ZT value of 0.17 at 575 K