strain, it depicts a very interesting trend: it has a value of 229.68 × 10 −6 V K −1 at 100 K, and it slightly reduces to 205.47 at 200 K and then sharply rises to the highest value of 334.32 × 10 −6 V K −1 at 500 K and further follows a decreasing trend down to 286.73 × 10 −6 V K −1 at 800 K (see Fig. 12(b) ).
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Ultra low thermal conductivity, giant figure of merit of 1.61, and high absorption in CsKTiCl<sub>6</sub>: a potential material from a transport and optoelectronic perspective.
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