4 research outputs found
New Monoclinic Phase at the Composition Cu<sub>2</sub>SnSe<sub>3</sub> and Its Thermoelectric Properties
A new monoclinic phase (<i>m2</i>) of ternary diamond-like compound Cu<sub>2</sub>SnSe<sub>3</sub> was synthesized by reaction of the elements at 850 K. The crystal
structure of <i>m2</i>-Cu<sub>2</sub>SnSe<sub>3</sub> was
determined through electron diffraction tomography and refined by
full-profile techniques using synchrotron X-ray powder diffraction
data (space group <i>Cc</i>, <i>a</i> = 6.9714(2)
Å, <i>b</i> = 12.0787(5) Å, <i>c</i> = 13.3935(5) Å, β = 99.865(5)°, <i>Z</i> = 8). Thermal analysis and annealing experiments suggest that <i>m2</i>-Cu<sub>2</sub>SnSe<sub>3</sub> is a low-temperature phase,
while the high-temperature phase has a cubic crystal structure. According
to quantum chemical calculations, <i>m2</i>-Cu<sub>2</sub>SnSe<sub>3</sub> is a narrow-gap semiconductor. A study of the chemical
bonding, applying the electron localizability approach, reveals covalent
polar Cu–Se and Sn–Se interactions in the crystal structure.
Thermoelectric properties were measured on a specimen consolidated
using spark plasma sintering (SPS), confirming the semiconducting
character. The thermoelectric figure of merit <i>ZT</i> reaches
a maximum value of 0.33 at 650 K
BaGe<sub>6</sub> and BaGe<sub>6‑x</sub>: Incommensurately Ordered Vacancies as Electron Traps
We
report the high-pressure high-temperature synthesis of the germanium-based
framework compounds BaGe<sub>6</sub> (<i>P</i> = 15 GPa, <i>T</i> = 1073 K) and BaGe<sub>6–<i>x</i></sub> (<i>P</i> = 10 GPa, <i>T</i> = 1073 K) which
are metastable at ambient conditions. In BaGe<sub>6‑<i>x</i></sub>, partial fragmentation of the BaGe<sub>6</sub> network involves
incommensurate modulations of both atomic positions and site occupancy.
Bonding analysis in direct space reveals that the defect formation
in BaGe<sub>6–<i>x</i></sub> is associated with the
establishment of free electron pairs around the defects. In accordance
with the electron precise composition of BaGe<sub>6‑<i>x</i></sub> for <i>x</i> = 0.5, physical measurements evidence
semiconducting electron transport properties which are combined with
low thermal conductivity
BaGe<sub>6</sub> and BaGe<sub>6‑x</sub>: Incommensurately Ordered Vacancies as Electron Traps
We
report the high-pressure high-temperature synthesis of the germanium-based
framework compounds BaGe<sub>6</sub> (<i>P</i> = 15 GPa, <i>T</i> = 1073 K) and BaGe<sub>6–<i>x</i></sub> (<i>P</i> = 10 GPa, <i>T</i> = 1073 K) which
are metastable at ambient conditions. In BaGe<sub>6‑<i>x</i></sub>, partial fragmentation of the BaGe<sub>6</sub> network involves
incommensurate modulations of both atomic positions and site occupancy.
Bonding analysis in direct space reveals that the defect formation
in BaGe<sub>6–<i>x</i></sub> is associated with the
establishment of free electron pairs around the defects. In accordance
with the electron precise composition of BaGe<sub>6‑<i>x</i></sub> for <i>x</i> = 0.5, physical measurements evidence
semiconducting electron transport properties which are combined with
low thermal conductivity
Intermediate-Valence Ytterbium Compound Yb<sub>4</sub>Ga<sub>24</sub>Pt<sub>9</sub>: Synthesis, Crystal Structure, and Physical Properties
The
title compound was synthesized by a reaction of the elemental educts
in a corundum crucible at 1200 °C under an Ar atmosphere. The
excess of Ga used in the initial mixture served as a flux for the
subsequent crystal growth at 600 °C. The crystal structure of
Yb<sub>4</sub>Ga<sub>24</sub>Pt<sub>9</sub> was determined from single-crystal
X-ray diffraction data: new prototype of crystal structure, space
group <i>C</i>2<i>/m</i>, Pearson symbol <i>mS</i>74, <i>a</i> = 7.4809(1) Å, <i>b</i> = 12.9546(2) Å, <i>c</i> = 13.2479(2) Å, β
= 100.879(1)°, <i>V</i> = 1260.82(6) Å<sup>3</sup>, <i>R</i><sub><i>F</i></sub> = 0.039 for 1781
observed reflections and 107 variable parameters. The structure is
described as an <i>ABABB</i> stacking of two slabs with
trigonal symmetry and compositions Yb<sub>4</sub>Ga<sub>6</sub> (<i>A</i>) and Ga<sub>12</sub>Pt<sub>6</sub> (<i>B</i>). The hard X-ray photoelectron spectrum (HAXPES) of Yb<sub>4</sub>Ga<sub>24</sub>Pt<sub>9</sub> shows both Yb<sup>2+</sup> and Yb<sup>3+</sup> contributions as evidence of an intermediate valence state
of ytterbium. The evaluated Yb valence of ∼2.5 is in good agreement
with the results obtained from the magnetic susceptibility measurements.
The compound is a bad metallic conductor