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Speaker: Prof. Kanishka Biswas
New Chemistry Unit & International Centre for Materials
Science, Jawaharlal Nehru Centre for Advanced
Scientific Research (JNCASR), Jakkur P.O.,
Bangalore-560064 (India)
Title: "Phonon-Glass Electron-Crystal like High Performance Thermoelectrics".
Day and Date: Thursday, March 13, 2025
Time: 12.00 Noon.
Venue: Room no. 350, Chemistry Department Second floor, Annex
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Hosted by HOD
Abstract With about 2/3 of all utilized energy is being lost as heat. Thermoelectric materials can
convert waste heat to electrical energy, and it will have significant role in future energy
management. A careful balance between electrical and thermal transport is essential
for optimizing the thermoelectric performance. Achieving glass-like ultra-low thermal
conductivity in crystalline solids with high electrical conductivity, a crucial requirement
for high-performance thermoelectrics, continues to be a grand challenge. Despite this
inherent trade-off, the experimental realization of an ideal thermoelectric material with
a phonon-glass electron-crystal (PGEC) nature has rarely been achieved. We
demonstrated high thermoelectric performance with a near room-temperature figure
of merit, zT ~1.5 and a maximum zT ~2.6 at 573 K by optimizing atomic disorder in Cd
doped polycrystalline AgSbTe2.
1, 2 Cadmium doping in AgSbTe2 enhances cationic
ordering, which simultaneously improves electronic properties by tuning disorderinduced localization of electronic states and reduces lattice thermal conductivity via
spontaneous formation of nanoscale (~2-4 nm) superstructures. Recently, we showed
that isovalent Yb-doping induced enhanced atomic ordering decreases the overlap
between the hole and phonon mean free paths and consequently leads to a PGEClike transport in AgSbTe2.
3 A twofold increase in electrical mobility is observed while
keeping the position of the Fermi level nearly unchanged and corroborates the
enhanced crystalline nature of the AgSbTe2 lattice upon Yb doping for electrical
transport, which leads to zT ~2.4 at 573 K. These achievements highlight the potential
of our approach in enhancing the thermoelectric performance of the material by tuning
its inherent atomic disorder which can be applicable to other thermoelectric materials.4