Sb and Se Substitution
in CsBi<sub>4</sub>Te<sub>6</sub>: The Semiconductors CsM<sub>4</sub>Q<sub>6</sub> (M = Bi, Sb; Q = Te, Se), Cs<sub>2</sub>Bi<sub>10</sub>Q<sub>15</sub>, and CsBi<sub>5</sub>Q<sub>8</sub>
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Abstract
The solid solutions of CsBi<sub>4</sub>Te<sub>6</sub>, a high ZT material at a low temperature region, with Sb and Se
were synthesized with general formulas CsBi<sub>4‑<i>x</i></sub>Sb<sub><i>x</i></sub>Te<sub>6</sub> and CsBi<sub>4</sub>Te<sub>6‑<i>y</i></sub>Se<sub><i>y</i></sub>. The introduction of Sb and Se in the lattice of CsBi<sub>4</sub>Te<sub>6</sub> is possible but only to a limited extent. The
Sb and Se atoms substituted are not uniformly distributed over all
crystallographic sites but display particular site preferences. The
structure of new Sb/Bi solid solutions retains the original framework
of CsBi<sub>4</sub>Te<sub>6</sub> composed of NaCl-type Bi/Te slabs
interconnected by characteristic Bi–Bi bonds and Cs atoms located
in the interlayer space. A structurally modified phase in Se/Te solid
solutions was found from the reactions targeted for 0.2 < <i>y</i> < 2.4 with the formula of CsBi<sub>5</sub>Te<sub>7.5‑<i>y</i></sub>Se<sub><i>y</i></sub> (or Cs<sub>2</sub>Bi<sub>10</sub>Q<sub>15</sub>, (Q = Se, Te)). The new structure is
constructed by the same structural motif with an extended Bi/Te slab
(29 Å) compared to that in CsBi<sub>4</sub>Te<sub>6</sub> (23
Å). The CsBi<sub>5</sub>Te<sub>7.5‑<i>y</i></sub>Se<sub><i>y</i></sub> possesses Bi/Te slabs that extend
by an additional “Bi<sub>2</sub>Te<sub>3</sub>” unit
compared to the structure of CsBi<sub>4</sub>Te<sub>6</sub>, which
implies the existence of a phase homology of compounds with the adjustable
parameter being the width of the Bi/Q slab. In the reactions targeted
for the compounds with higher <i>y</i>, a new phase CsBi<sub>5</sub>Te<sub>3.6</sub>Se<sub>4.4</sub> with a different type of
framework was found. The electrical conductivity and thermopower for
the selected samples show p-type conduction with metallic behavior.
The room temperature values measured are in the range of 300–1100
S/cm and 100–150 μV/K for Sb-substituted samples and
20–500 S/cm and 70–140 μV/K for Se-substituted
samples, respectively. Thermal conductivities of these samples are
in the range of 0.9–1.2 W/m·K at room temperature. Tailoring
the transport behavior of these materials for thermoelectric applications
may be achieved by doping, as is possible for the parent compound
CsBi<sub>4</sub>Te<sub>6</sub>