Poudeu Pierre F P, D'Angelo Jonathan, Kong Huijun, Downey Adam, Short Jarrod L, Pcionek Robert, Hogan Timothy P, Uher Ctirad, Kanatzidis Mercouri G
Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA.
J Am Chem Soc. 2006 Nov 8;128(44):14347-55. doi: 10.1021/ja0647811.
The series of Pb(9.6)Sb(0.2)Te(10)(-)(x)Se(x) compounds with different Se content (x) were prepared, and their structure was investigated at the atomic and nanosized regime level. Thermoelectric properties were measured in the temperature range from 300 to 700 K. The Pb(9.6)Sb(0.2)Te(10)(-)(x)Se(x) series was designed after the refinement of the single-crystal structure of Pb(3.82)Sb(0.12)Te(4) (Pb(9.6)Sb(0.3)Te(10); S.G. Pmm) by substituting isoelectronically in anion positions Te by Se. The Pb(9.6)Sb(0.2)Te(10)(-)(x)Se(x)() compounds show significantly lower lattice thermal conductivity (kappa(L)) compared to the well-known PbTe(1)(-)(x)Se(x) solid solutions. For Pb(9.6)Sb(0.2)Te(3)Se(7) (x = 7), a kappa(L) value as low as 0.40 W/m.K was determined at 700 K. High-resolution transmission electron microscopy of several Pb(9.6)Sb(0.2)Te(10)(-)(x)Se(x) samples showed widely distributed Sb-rich nanocrystals in the samples which is the key feature for the strong reduction of the lattice thermal conductivity. The reduction of kappa(L) results in a significantly enhanced thermoelectric figure of merit of Pb(9.6)Sb(0.2)Te(10)(-)(x)Se(x) compared to the corresponding PbTe(1)(-)(x)Se(x) solid solution alloys. For Pb(9.6)Sb(0.2)Te(3)Se(7) (x = 7), a maximum figure of merit of ZT approximately 1.2 was obtained at approximately 650 K. This value is about 50% higher than that of the state-of-the-art n-type PbTe. The work provides experimental validation of the theoretical concept that embedded nanocrystals can promote strong scattering of acoustic phonons.
制备了一系列具有不同硒含量(x)的Pb(9.6)Sb(0.2)Te(10)(-)Se(x)化合物,并在原子和纳米尺度水平上研究了它们的结构。在300至700 K的温度范围内测量了热电性能。Pb(9.6)Sb(0.2)Te(10)(-)Se(x)系列是在对Pb(3.82)Sb(0.12)Te(4)(Pb(9.6)Sb(0.3)Te(10);空间群Pmm)的单晶结构进行优化后设计的,通过在阴离子位置用硒等电子取代碲。与著名的PbTe(1)(-)Se(x)固溶体相比,Pb(9.6)Sb(0.2)Te(10)(-)Se(x)化合物的晶格热导率(κ(L))显著更低。对于Pb(9.6)Sb(0.2)Te(3)Se(7)(x = 7),在700 K时确定的κ(L)值低至0.40 W/m·K。对几个Pb(9.6)Sb(0.2)Te(10)(-)Se(x)样品进行的高分辨率透射电子显微镜观察表明,样品中存在分布广泛的富锑纳米晶体,这是晶格热导率大幅降低的关键特征。与相应的PbTe(1)(-)Se(x)固溶体合金相比,κ(L)的降低导致Pb(9.6)Sb(0.2)Te(10)(-)Se(x)的热电优值显著提高。对于Pb(9.6)Sb(0.2)Te(3)Se(7)(x = 7),在约650 K时获得了约1.2的最大优值ZT。该值比最先进的n型PbTe高约50%。这项工作为嵌入纳米晶体可促进声子强散射的理论概念提供了实验验证。