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. 2023 Mar 13;14(1):1366.
doi: 10.1038/s41467-023-37114-7.

High thermoelectric efficiency realized in SnSe crystals via structural modulation

Affiliations

High thermoelectric efficiency realized in SnSe crystals via structural modulation

Bingchao Qin et al. Nat Commun. .

Abstract

Crystalline thermoelectrics have been developed to be potential candidates for power generation and electronic cooling, among which SnSe crystals are becoming the most representative. Herein, we realize high-performance SnSe crystals with promising efficiency through a structural modulation strategy. By alloying strontium at Sn sites, we modify the crystal structure and facilitate the multiband synglisis in p-type SnSe, favoring the optimization of interactive parameters μ and m*. Resultantly, we obtain a significantly enhanced PF ~85 μW cm-1 K-2, with an ultrahigh ZT ~1.4 at 300 K and ZTave ~2.0 among 300-673 K. Moreover, the excellent properties lead to single-leg device efficiency of ~8.9% under a temperature difference ΔT ~300 K, showing superiority among the current low- to mid-temperature thermoelectrics, with an enhanced cooling ΔTmax of ~50.4 K in the 7-pair thermoelectric device. Our study further advances p-type SnSe crystals for practical waste heat recovery and electronic cooling.

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Conflict of interest statement

The authors declare no competing interests.

Figures

Fig. 1
Fig. 1. Theoretical simulations on the electrical parameters with dynamic carrier concentration n from Pnma phase to Cmcm phase at 300 K.
a Carrier mobility μ. b Electrical conductivity σ. c Seebeck coefficient S. d Power factor PF.
Fig. 2
Fig. 2. Temperature-dependent electrical performance for SnSe-9%Pb-x%Sr crystals.
a Electrical conductivity σ. b Seebeck coefficient S. c Power factor PF. and d Weighted mobility μW. Experimental data and multiband simulations with n on the e Seebeck coefficient S. And f Carrier mobility μ.
Fig. 3
Fig. 3. SR-XRD measurements and Rietveld refinements of p-type SnSe-9%Pb−1.2%Sr crystal.
a Diffraction patterns from 300 to 873 K. b Temperature-dependent lattice parameters for hole-doped SnSe, SnSe-9%Pb, and SnSe-9%Pb−1.2%Sr. The arrows show that Tpt declines from ~800 K in SnSe to ~748 K in SnSe-9%Pb and ~723 K for SnSe-9%Pb−1.2%Sr, indicating that Sr alloying further promotes the phase transition of SnSe.
Fig. 4
Fig. 4. Structural modulation by alloying Sr in SnSe.
a The crystal structure of Pnma- and Cmcm-SnSe, with the angle 1 marked, indicating the increased crystal symmetry. b The values of angle 1 in hole-doped SnSe, SnSe-9%Pb, and SnSe-9%Pb-1.2%Sr with temperature, showing that Sr alloying declines angle 1 and enhances the crystal symmetry over the whole temperature range. c The characteristic temperatures for p-type SnSe, SnSe-9%Pb, and SnSe-9%Pb-1.2%Sr crystals, including the bands merging temperature (Tm) from VBM 1 and 2 to VBM (1 + 2), bands alignment temperature (Ta) between VBM 3 and VBM (1 + 2), and completing phase transition temperature (Tpt). The reduction of the characteristic temperatures implies that Sr alloying further promotes the multiband synglisis in p-type SnSe.
Fig. 5
Fig. 5. Microstructure characterization on the p-type SnSe-9%Pb−1.2%Sr crystal.
a The ABF-STEM image exhibits the microstructure morphology of the sample. b The ADF-STEM image indicates the Sr-alloyed area. c1c4 Its corresponding elemental analysis. d The HAADF-STEM image of one Sr-alloyed area displays the expanded arrangement of atoms. e1e2 The corresponding GPA mappings along the horizontal (εxx) and vertical (εyy) axis. f Another Sr-alloyed region which reveals the contraction of atomic arrangements. g1g2 Its GPA maps. h The undoped area of zigzag structure with Pnma phase. i, j The enlarged atomic-resolved HAADF image demonstrates the high-symmetry phase around the Sr-alloyed area coming from d and f, respectively.
Fig. 6
Fig. 6. Thermal transports, ZT, and device efficiencies for SnSe-9%Pb-x%Sr crystals.
a Total thermal conductivity κtot and lattice thermal conductivity κlat. b ZT and ZTave at 300–673 K. c Comparisons on the experimental conversion efficiencies η between the devices in this study (fabricated by using the SnSe-9%Pb−1.2%Sr crystals) and the reported results among comparable temperature differences ΔT (SKD skutterudites, BST Bi2-xSbxTe3, HH half-Heusler, TAGS-85 (GeTe)85(AgSbTe2)15, S-L single-leg),,–. d Maximum cooling temperature difference ΔTmax for the fabricated seven-pair thermoelectric devices using the SnSe-9%Pb−1.2%Sr crystals, and the ΔTmax for the SnSe-9%Pb crystals was plotted for comparison.

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