Effects of praseodymium doping on thermoelectric transport properties of CaMnO_3 compound system

来源 :Journal of Rare Earths | 被引量 : 0次 | 上传用户:leefenbo
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The rare earth Pr doped Ca1-x Prx MnO3(x=0,0.06,0.08,0.1,0.12,and 0.14) compound bulk samples were prepared to study the effect of Pr doping on thermoelectric transport properties of CaMnO3 compound system.The doped samples exhibited single phase composition within the experimental doping range,with condensed bulk microstructure and small porosities.The electrical resistivity was remarkably reduced for doped samples,on account of the enhanced carrier concentration;the absolute value of Seebeck coefficient was deteriorated mainly due to enhanced electron carrier concentration.The electrical performances of the doped samples reflected by resistivity and Seebeck coefficient fluctuations were optimistically tuned,with an optimized power factor value of 0.342 mW/(m·K2) at 873 K for x=0.08 sample,which was very much higher comparing with that of the un-doped sample.The lattice thermal conduction was really confined,leading to distinctly repressed total thermal conductivity.The thermoelectric performance was noticeably improved by Pr doping and the dimensionless figure of merit ZT for the Ca0.92 Pr0.08 MnO3 compound was favorably optimized with the maximum value 0.16 at 873 K. The rare earth Pr doped Ca1-x Prx MnO3 (x = 0,0.06,0.08,0.1,0.12, and 0.14) compound bulk samples were prepared to study the effect of Pr doping on thermoelectric transport properties of CaMnO3 compound system.The doped samples show single phase composition within the experimental doping range, with condensed bulk microstructure and small porosities. The electrical resistivity was remarkably reduced for doped samples, on account of the enhanced carrier concentration; the absolute value of Seebeck coefficient was deteriorated due due to enhanced electron carrier concentration. The electrical performances of the doped samples are shown by resistivity and Seebeck coefficient fluctuations were significantly tuned, with an optimized power factor value of 0.342 mW / (m · K2) at 873 K for x = 0.08 sample, which was very much more with that of the un-doped sample. The lattice thermal conduction was really confined, leading to distinctly repressed total thermal conductivity. the thermoelectri c performance was noticeably improved by Pr doping and the dimensionless figure of merit ZT for the Ca 0.92 Pr 0.08 MnO 3 compound was favorably optimized with the maximum value 0.16 at 873 K.
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