Tuning
the chemical bonding characteristics and achieving high
band degeneracy by forming a superlattice structure could be an efficient
approach to improve thermoelectric performance. This study composes
two mechanisms: band convergence and localized vibration originating
from antibonding states between neighbouring atoms, responsible for
enhancing the thermoelectric figure of merit in a WSe2–WTe2 superlattice. Here, we achieve band convergence and high
band degeneracy, leading to a remarkably high Seebeck coefficient
of 2331 μV/K, considerably elevating that of the parent material
WSe2 (1695 μV/K). The presence of strong W–Te
antibonding near the Fermi level along with strong phonon softening
of particular out-of-plane ZA mode originating mostly from W–Te
bond vibration of the WTe2 sublayer plays a crucial role
in reducing lattice thermal conductivity. Additionally, the chemical
bonding inhomogeneity with mixed bonding and antibonding characteristics
present in the superlattice ignite significant lattice anharmonicity,
and the appearance of low energetic optical phonons generates more
three-phonon scattering events occurring in a superlattice with more
participation of low-lying phonon modes, strongly scatter heat-carrying
acoustics phonons. The improved electronic properties and ultralow
lattice thermal conductivity lead to a peak n-type ZT ∼ 2.71
at 900 K achieved in the superlattice compared to a WSe2 n-type ZT of 0.68, which is incredible among existing thermoelectric
materials.