Knowledge of structure–property relationships
in solids
with intrinsic low thermal conductivity is crucial for fields such
as thermoelectrics, thermal barrier coatings, and refractories. Herein,
we propose a new “rigidness in softness” structural
scheme for intrinsic low lattice thermal conductivity (κL), which embeds rigid clusters into the soft matrix to induce
large lattice anharmonicity, and accordingly discover a new series
of chalcogenides Pt3Bi4Q9 (Q = S,
Se). Pt3Bi4S9–x
Se
x
(x = 3, 6)
achieved an intrinsic ultralow κL down to 0.39 W/(m
K) at 773 K, which is considerably low among the Bi chalcogenide thermoelectric
materials. Pt3Bi4Q9 contains the
rigid cubic [Pt6Q12]12– clusters
embedded in the soft Bi-Q sublattice, involving multiple bonding interactions
and vibration hierarchy. The hierarchical structure yields a large
lattice anharmonicity with high Grüneisen parameters (γ)
1.97 of Pt3Bi4Q9, as verified by
the effective scatter of low-lying optical phonons toward heat-carrying
acoustic phonons. Consequently, the rigid-soft coupling significantly
inhibits heat propagation, exhibiting low acoustic phonon frequencies
(∼25 cm–1) and Debye temperatures (ΘD = 170.4 K) in Pt3Bi4Se9.
Owing to the suppressed κL and considerable power
factor (PF), the ZT value of Pt3Bi4S6Se3 can reach 0.56 at 773 K without
heavy carrier doping, which is competitive among the pristine Bi chalcogenides.
Theoretical calculations predicted a large potential for performance
improvement via proper doping, indicating the great potential of this
structure type for promising thermoelectric materials.