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• Fig. 1  Schematic diagram of first principles high-throughput (HT) study on materials
• Fig. 2  Relationship between calculation cost and accuracy
• Fig. 3  Electrical properties in MP with a constant relaxation time approximation^[35]
• Fig. 4  n- (a) and p-doped (b) average normalized power factor P/L and Seebeck coefficient^[15]
• Fig. 5  Power factor of chalcogenides with diamond-like structures (a) and vacancy-containing ternary chalcogenides (b)^[20]
• Fig. 6  Relationship between κ_L^AGLandκ_L^anh/κ_L^exp(Data from Ref.[13])
• Fig. 7  Relationship between calculated κ_L and experimental κ_L^[12]
• Fig. 8  Three prediction models of the κ_L in half-Heusler compounds^[16](a) Frequency densities of the estimators of thermal conductivity at 300 Kκ_transfand κ_forest;and (b) distribution of κ_anhover the 75 thermodynamically stable half-Heuslers
• Fig.1  A 128-member binary library^[15]
• Fig.2  Schematic diagram of combinatorial electrostatic atomization system “M-ist Combi”^[16]
• Fig. 3  Schematic illustration for the Czochralski crystal growth^[18]
• Fig.4  Schematic illustration for the vertical Bridgman crystal growth^[19]
• Fig.5  Variation of Seebeck coefficient values along n-type 0.01/0.055% PbI₂ doped (Pb_0.95Sn_0.05Te)_0.92(PbS)_0.08 functionally graded materials^[24]
• Fig.6  (a) Scheme of a rotor with capsules for sedimentation experiment and (b) mechanism of sedimentation of atoms in the strong acceleration field^[25]
• Fig.7  (a) Optical image of the annealed Ti-Ni-Sn thin film materials library; (b-d) color-coded results of the high-throughput EDX measurements of the material library^[27]
• Fig.8  EDX measurements of the concentration of (a)magnesium, (b)nickel and (c)aluminum of an Mg-Ni-Al ternary thin film library^[30]
• Fig.9  Layout of the nanocalorimeter cell^[34]
• Fig.10  Composition trends over the sample library, (a) Si:Cu ratio for the glass-forming component, (b) glass transition temperature and (c) the total enthalpy of this glass reaction^[35]
• Fig.11  (a) Schematic of the pump and probe laser measurement setup and (b)temperature increase as a function of time after a single-pulse^[33]
• Fig.12  Time-domain thermoreflectance experimental setup^[33]

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