Defect engineering is the core strategy for improving thermoelectric properties. Herein, cation doping along with modulation of cation vacancy has been developed in GeTebased materials as an effective method to induce vacancy-based defects to boost their thermoelectric performance. A series of ternary compounds of Ge 9 Sb 2 Te 12−x (x = 0, 0.03, 0.06, 0.09, 0.12, 0.15) was prepared by vacuum-melting and annealing combined with the spark plasma sintering (SPS) process. The role of Sb doping and cation vacancy on thermoelectric properties was systematically investigated. It is found that alloying Sb 2 Te 3 into GeTe increases the concentration of cation vacancies, which is corroborated by both positron annihilation measurements and theoretical calculations. The vacancies, stacking faults, and planar defect interactions determine the thermoelectric transport properties. Adjusting the deficiency of Te effectively tunes the concentration of cation vacancies and dopant defects in the structure. In turn, this tunes the carrier concentration close to its optimum. A high power factor of 32.6 μW cm −1 K −2 is realized for Ge 9 Sb 2 Te 11.91 at 725 K. Moreover, large strains induced by the defect structures, including Sb dopant, vacancy, staking faults, as well as planar defects intensify phonon scattering, leading to a significant decrease in the thermal conductivity from 7.6 W m −1 K −1 for pristine GeTe to 1.18 W m −1 K −1 for Ge 9 Sb 2 Te 11.85 at room temperature. All of the above contribute to a high ZT value of 2.1 achieved for the Ge 9 Sb 2 Te 11.91 sample at 775 K.
In
this paper, we report a series of x polycrystalline
AgCuTe1–x
Se samples with high thermoelectric
performance. X-ray photoelectron spectroscopy data suggest the observation
of Ag+, Cu+, Te2–, and Se2– states of Ag, Cu, Te, and Se. Meanwhile, the carrier
concentration of the obtained p-type samples changes from 9.12 ×
1018 to 0.86 × 1018 cm–3 as their carrier mobility varies from 698.55 to 410.12 cm2·V–1·s–1 at 300 K.
Compared with undoped AgCuTe, an ultralow thermal conductivity is
realized in AgCuTe1–x
Se
x
due to the enhanced phonon scattering. Ultimately,
a maximum figure of merit (ZT) of ∼1.45 at 573 K and a high
average ZT above 1.0 at temperatures ranging from room temperature
to 773 K can be achieved in AgCuTe0.9Se0.1,
which increases by 186% compared to that of the undoped AgCuTe (0.82
at 573 K). This work provides a viable insight toward understanding
the effect of the Se atom on the lattice structure and thermoelectric
properties of AgCuTe and other transition-metal dichalcogenides.
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