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锰取代合成黝铜矿的热电性质。

Thermoelectric properties of a Mn substituted synthetic tetrahedrite.

作者信息

Chetty Raju, D S Prem Kumar, Rogl Gerda, Rogl Peter, Bauer Ernst, Michor Herwig, Suwas Satyam, Puchegger Stephan, Giester Gerald, Mallik Ramesh Chandra

机构信息

Department of Physics, Indian Institute of Science, Bangalore 560012, India.

出版信息

Phys Chem Chem Phys. 2015 Jan 21;17(3):1716-27. doi: 10.1039/c4cp04039b. Epub 2014 Dec 2.

Abstract

Tetrahedrite compounds Cu(12-x)Mn(x)Sb4S13 (0 ≤x≤ 1.8) were prepared by solid state synthesis. A detailed crystal structure analysis of Cu10.6Mn1.4Sb4S13 was performed by single crystal X-ray diffraction (XRD) at 100, 200 and 300 K confirming the noncentrosymmetric structure (space group I4[combining macron]3m) of a tetrahedrite. The large atomic displacement parameter of the Cu2 atoms was described by splitting the 12e site into a partially and randomly occupied 24g site (Cu22) in addition to the regular 12e site (Cu21), suggesting a mix of dynamic and static off-plane Cu2 atom disorder. Rietveld powder XRD pattern and electron probe microanalysis revealed that all the Mn substituted samples showed a single tetrahedrite phase. The electrical resistivity increased with increasing Mn due to substitution of Mn(2+) at the Cu(1+) site. The positive Seebeck coefficient for all samples indicates that the dominant carriers are holes. Even though the thermal conductivity decreased as a function of increasing Mn, the thermoelectric figure of merit ZT decreased, because the decrease of the power factor is stronger than the decrease of the thermal conductivity. The maximum ZT = 0.76 at 623 K is obtained for Cu12Sb4S13. The coefficient of thermal expansion 13.5 ± 0.1 × 10(-6) K(-1) is obtained in the temperature range from 460 K to 670 K for Cu10.2Mn1.8Sb4S13. The Debye temperature, Θ(D) = 244 K for Cu10.2Mn1.8Sb4S13, was estimated from an evaluation of the elastic properties. The effective paramagnetic moment 7.45 μB/f.u. for Cu10.2Mn1.8Sb4S13 is fairly consistent with a high spin 3d(5) ground state of Mn.

摘要

通过固态合成法制备了黝铜矿化合物Cu(12 - x)Mn(x)Sb4S13(0≤x≤1.8)。通过在100、200和300 K下进行的单晶X射线衍射(XRD)对Cu10.6Mn1.4Sb4S13进行了详细的晶体结构分析,证实了黝铜矿的非中心对称结构(空间群I4[combining macron]3m)。除了规则的12e位(Cu21)外,通过将12e位分裂为部分且随机占据的24g位(Cu22)来描述Cu2原子的大原子位移参数,这表明存在动态和静态面外Cu2原子无序的混合。Rietveld粉末XRD图谱和电子探针微分析表明,所有Mn取代的样品均呈现单一的黝铜矿相。由于Mn(2+)在Cu(1+)位点的取代,电阻率随Mn含量的增加而升高。所有样品的正塞贝克系数表明主要载流子为空穴。尽管热导率随Mn含量的增加而降低,但热电优值ZT降低,因为功率因子的降低比热导率的降低更强。对于Cu12Sb4S13,在623 K时获得的最大ZT = 0.76。对于Cu10.2Mn1.8Sb4S13,在460 K至670 K的温度范围内获得的热膨胀系数为13.5±0.1×10(-6) K(-1)。通过对弹性性能的评估,估计Cu10.2Mn1.8Sb4S13的德拜温度Θ(D)= 244 K。Cu10.2Mn1.8Sb4S13的有效顺磁矩为7.45 μB/f.u.,与Mn的高自旋3d(5)基态相当一致。

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