9 Abstract Polycrystalline compounds of Ca 0.9 Y 0.1 Mn 12x 10 Fe x O 3 for 0 B x B 0.25 were prepared by solid-state 11 reaction, followed by spark plasma sintering process, and 12 their thermoelectric properties from 300 to 1200 K were 13 systematically investigated in terms of Y and Fe co-doping 14 at the Ca-and Mn-sites, respectively. Crystal structure 15 refinement revealed that all the investigated samples have 16 the O 0 -type orthorhombic structure, and the lattice param-17 eters slightly increased with increasing Fe concentration, 18 causing a crystal distortion. It was found that with 19 increasing the content of Fe doping, the Seebeck coefficient 20 of Ca 0.9 Y 0.1 Mn 12x Fe x O 3 tended to increase, while the 21 tendency toward the electrical conductivity was more 22 complicated. The highest power factor was found to be 23 2.1 9 10 -4 W/mK 2 at 1150 K for the sample with 24 x = 0.05 after annealing at 1523 K for 24 h in air. Thermal 25 conductivity of the Fe-doped samples showed a lower 26 value than that of the x = 0 sample, and the highest 27 dimensionless figure of merit, ZT was found to be 28 improved about 20 % for the sample with x = 0.05 as 29 compared to that of the x = 0 sample at 1150 K. 30 31 Introduction
32With increasing the global energy demand, thermoelectric 33 materials have recently gained much interest in both the 34 theoretical and technological aspects due to the potential 35 use of these materials in converting waste heat into elec-36 tricity [1,2]. In general, for a single thermoelectric mate-37 rial, the conversion efficiency can be evaluated by the 38 dimensionless figure of merit (ZT = rS 2 T/j, where r, S, T, 39 j are the electrical conductivity, the Seebeck coefficient, 40 the absolute temperature, and the thermal conductivity, 41 respectively). The requirements for practical application of 42 high thermal-to-electrical energy conversion place on 43 finding suitable thermoelectric materials, and are not easily 44 satisfied. They should not only possess good thermoelectric 45 performance, they must also be stable at high temperatures 46 and be composed of nontoxic and low-cost elements, but 47 also must be able to be processed and shaped cheaply. For 48 this purpose, metal oxide-based materials are considered as 49 good candidates. 50 CaMnO 3 , which is a perovskite oxide with orthorhombic 51 structure at room temperature, has also been considered as 52 a promising thermoelectric n-type material for high-53 temperature application [3][4][5][6][7][8][9]. Many attempts have been 54 made in order to improve the thermoelectric performance 55 of this type of material, mainly to enhance the electrical 56 conductivity, reduce further the thermal conductivity, 57 while avoiding degradation of the Seebeck coefficient. 58 Most of these studies have been focused on doping, for 59 example, Yb at Ca-site [4][5][6][7] or Nb at Mn-site [3,8], while 60 only few reports performed the research on dually doping, 61 e.g., Sr and Yb at Ca-site [9]. Previous reports have showed 62 that the subst...