2 research outputs found
Enhanced Thermoelectric Properties of Codoped Cr<sub>2</sub>Se<sub>3</sub>: The Distinct Roles of Transition Metals and S
Pristine
Cr<sub>2</sub>Se<sub>3</sub> is a narrow-band gap semiconductor but
with an inferior <i>ZT</i> value of 0.22 obtained at 623
K. In this paper, we improve the thermoelectric performance of the
Cr<sub>2</sub>Se<sub>3</sub> material by optimizing carrier concentration,
suppressing the bipolar thermal conductivity, and reducing the lattice
thermal conductivity simultaneously. First, the effect of different
dopants (Nb, Ni, and Mn) on the phase composition and thermoelectric
transport properties of M<sub>2<i>x</i></sub>Cr<sub>2β2<i>x</i></sub>Se<sub>3</sub> (M = Nb, Ni, and Mn; <i>x</i> = 0β0.02) compounds are systematically investigated. The
roles of those dopants are distinct. Mn-doped samples show superior
thermoelectric properties in comparison with those of other-element-doped
samples. Doping with Mn significantly increases the carrier concentration,
accompanied with a suppression of the intrinsic excitation and a reduction
of both the bipolar thermal conductivity and the lattice thermal conductivity
of Cr<sub>2</sub>Se<sub>3</sub>. To further reduce the thermal conductivity,
we have synthesized Mn and S codoped Mn<sub>0.04</sub>Cr<sub>1.96</sub>Se<sub>3β3<i>x</i></sub>S<sub>3<i>x</i></sub> (<i>x</i> = 0β0.1) samples. Alloying with
S significantly decreases the lattice thermal conductivity and enlarges
the band gap, boosting the Seebeck coefficient. The maximum <i>ZT</i> value of Mn<sub>0.04</sub>Cr<sub>1.96</sub>Se<sub>2.7</sub>S<sub>0.3</sub> reaches 0.33 at 823 K. Compared with the pristine
Cr<sub>2</sub>Se<sub>3</sub> sample, the maximum <i>ZT</i> value is increased by 50% and the temperature corresponding to the
peak value shifts toward higher temperatures by 200 K
Manipulating the Combustion Wave during Self-Propagating Synthesis for High Thermoelectric Performance of Layered Oxychalcogenide Bi<sub>1β<i>x</i></sub>Pb<sub><i>x</i></sub>CuSeO
Novel
time- and energy-efficient synthesis methods, especially
those adaptable to large-scale industrial processing, are of vital
importance for broader applications of thermoelectrics. We herein
reported a case study of layer-structured oxychalcogenides Bi<sub>1β<i>x</i></sub>Pb<sub><i>x</i></sub>CuSeO
(<i>x</i> = 0β10%) with emphases on the reaction
mechanism of self-propagating high-temperature synthesis (SHS) and
the impact of SHS conditions on the thermoelectric properties. The
combined results of X-ray powder diffraction, differential scanning
calorimetry, and quenching experiments corroborated that the SHS process
of BiCuSeO consisted two fast binary SHS reactions (2 Bi+3 Se β
Bi<sub>2</sub>Se<sub>3</sub> and 2 Cu+Se β Cu<sub>2</sub>Se)
intimately coupled with two relatively slow solid-state diffusion
reactions (2 Bi<sub>2</sub>Se<sub>3</sub>+B<sub>2</sub>O<sub>3</sub> β 3 Bi<sub>2</sub>SeO<sub>2</sub> and then Bi<sub>2</sub>SeO<sub>2</sub>+Cu<sub>2</sub>Se β 2 BiCuSeO). The formation
rate of the reaction intermediate Bi<sub>2</sub>SeO<sub>2</sub> was
the bottleneck in the SHS process of BiCuSeO. Importantly, we found
that adding PbO in the starting materials has (i) facilitated the
formation of Bi<sub>2</sub>SeO<sub>2</sub> and thus significantly
reduced the SHS reaction time; (ii) improved the phase purity and
sample homogeneity; (iii) increased the power factor via increasing
both carrier concentration and effective mass; and (iv) reduced the
lattice thermal conductivity via more point defect phonon scattering.
As a result, a state-of-the-art <i>ZT</i> value βΌ1.2
has been attained at 923 K for Bi<sub>0.94</sub>Pb<sub>0.06</sub>CuSeO.
These results not only open a new avenue for mass production of single
phased multinary thermoelectric materials but also inspire more investigation
into the SHS mechanisms of multinary materials in diverse fields of
material science and engineering