2023
DOI: 10.1016/j.jallcom.2022.167756
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Thermoelectric performance in disordered Cu2ZnSnSe4 nanostructures driven by ultra-low thermal conductivity

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Cited by 9 publications
(15 citation statements)
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“…Regarding the CZTS/Se system, the difference between disordered cubic CZTS/Se ( F-43m ) and disordered tetragonal CZTS/Se ( I-42m ) are the superstructure reflections visible through the low-angle Bragg-peaks in XRD and the observed new rings in the SAED patterns [ 45 , 46 , 47 ]. These transitions were also observed in DSC measurements for CZTS/Se [ 20 , 52 ]. The SR-XRD for the monoclinic and cubic CTS at 350 °C is shown in Figure 1 .…”
Section: Structure and Nature Of Disordersupporting
confidence: 56%
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“…Regarding the CZTS/Se system, the difference between disordered cubic CZTS/Se ( F-43m ) and disordered tetragonal CZTS/Se ( I-42m ) are the superstructure reflections visible through the low-angle Bragg-peaks in XRD and the observed new rings in the SAED patterns [ 45 , 46 , 47 ]. These transitions were also observed in DSC measurements for CZTS/Se [ 20 , 52 ]. The SR-XRD for the monoclinic and cubic CTS at 350 °C is shown in Figure 1 .…”
Section: Structure and Nature Of Disordersupporting
confidence: 56%
“…As discussed, the tetragonal order–disorder transition in CZTS/CZTSe manifests in a variation of the Seebeck value, which sharply increases for CZTS, and moderately decreases for CZTSe at the transition temperatures of ~500 and ~450 K, respectively. This behavior is associated with two different mechanisms, as shown by first-principles calculations [ 20 , 51 ]. In both cases, the disorder contributes to a flattening of the bands (increasing the Seebeck coefficient) and suppression of the band gap (decreasing the resistivity).…”
Section: Electronic Propertiesmentioning
confidence: 98%
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