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Ultralow thermal conductivity in all-inorganic halide perovskites.


ABSTRACT: Controlling the flow of thermal energy is crucial to numerous applications ranging from microelectronic devices to energy storage and energy conversion devices. Here, we report ultralow lattice thermal conductivities of solution-synthesized, single-crystalline all-inorganic halide perovskite nanowires composed of CsPbI3 (0.45 ± 0.05 W·m-1·K-1), CsPbBr3 (0.42 ± 0.04 W·m-1·K-1), and CsSnI3 (0.38 ± 0.04 W·m-1·K-1). We attribute this ultralow thermal conductivity to the cluster rattling mechanism, wherein strong optical-acoustic phonon scatterings are driven by a mixture of 0D/1D/2D collective motions. Remarkably, CsSnI3 possesses a rare combination of ultralow thermal conductivity, high electrical conductivity (282 S·cm-1), and high hole mobility (394 cm2·V-1·s-1). The unique thermal transport properties in all-inorganic halide perovskites hold promise for diverse applications such as phononic and thermoelectric devices. Furthermore, the insights obtained from this work suggest an opportunity to discover low thermal conductivity materials among unexplored inorganic crystals beyond caged and layered structures.

SUBMITTER: Lee W 

PROVIDER: S-EPMC5565476 | biostudies-literature | 2017 Aug

REPOSITORIES: biostudies-literature

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Ultralow thermal conductivity in all-inorganic halide perovskites.

Lee Woochul W   Li Huashan H   Wong Andrew B AB   Zhang Dandan D   Lai Minliang M   Yu Yi Y   Kong Qiao Q   Lin Elbert E   Urban Jeffrey J JJ   Grossman Jeffrey C JC   Yang Peidong P  

Proceedings of the National Academy of Sciences of the United States of America 20170731 33


Controlling the flow of thermal energy is crucial to numerous applications ranging from microelectronic devices to energy storage and energy conversion devices. Here, we report ultralow lattice thermal conductivities of solution-synthesized, single-crystalline all-inorganic halide perovskite nanowires composed of CsPbI<sub>3</sub> (0.45 ± 0.05 W·m<sup>-1</sup>·K<sup>-1</sup>), CsPbBr<sub>3</sub> (0.42 ± 0.04 W·m<sup>-1</sup>·K<sup>-1</sup>), and CsSnI<sub>3</sub> (0.38 ± 0.04 W·m<sup>-1</sup>·K<  ...[more]

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