搜索

x
中国物理学会期刊

Mg2Si0.3Sn0.7掺杂Ag和Li的热电性能对比

Comparative study of thermoelectric properties of Mg2Si0.3Sn0.7 doped by Ag or Li

CSTR: 32037.14.aps.68.20190247
PDF
HTML
导出引用
  • 采用两步固相法合成了物相均匀的Mg2(1–x)Ag2xSi0.3Sn0.7 (x = 0, 0.01, 0.02, 0.03, 0.04, 0.05)和Mg2(1–y)Li2ySi0.3Sn0.7 (y = 0, 0.02, 0.04, 0.06, 0.08)热电材料, 测试了室温物理性能和室温至773 K的热电性能, 研究了不同掺杂剂的固溶度、微观结构、载流子浓度、电性能和热输运. X射线衍射图谱和扫描电子显微镜图像显示掺杂Ag和Li的固溶度分别为x = 0.03和y = 0.06. 根据单抛物线模型, p型的Mg2(1–x)Ag2xSi0.3Sn0.7和Mg2(1–y)Li2ySi0.3Sn0.7的有效质量为1.2m0. 对比结果表明: 掺杂Ag或Li的最大载流子浓度分别达到4.64 × 1019 cm–3和15.1 × 1019 cm–3; 掺杂Li元素的样品有较高的固溶度、较高的载流子浓度和较高的功率因子PF约为1.62 × 10–3 W·m–1·K–2; 掺杂Li元素样品中较高的载流子浓度能够有效抑制双极效应, 显著降低双极热导率; Mg1.92Li0.08Si0.3Sn0.7的最大ZT值0.54, 比Mg1.9Ag0.1Si0.3Sn0.7的最大ZT值0.34提高了大约58%. 根据Callaway理论, 由于质量场波动和应变场波动增强声子散射, 掺杂Ag和Li元素样品的晶格热导率比未掺杂样品明显降低.

     

    In recent decades, Mg2(Si, Sn) solid solutions have long been considered as one of the most important classes of eco-friendly thermoelectric materials. The thermoelectric performance of Mg2(Si, Sn) solid solutions with outstanding characteristics of low-price, non-toxicity, earth-abundant and low-density has been widely studied. The n-type Mg2(Si, Sn) solid solutions have achieved the dimensionless thermoelectric figure of merit ZT ~1.4 through Bi/Sb doping and convergence of conduction bands. However, the thermoelectric performances for p-type Mg2(Si, Sn) solid solutions are mainly improved by optimizing the carrier concentration. In this work, the thermoelectric properties for p-type Mg2Si0.3Sn0.7 are investigated and compared with those for different p-type dopant Ag or Li. The homogeneous Mg2Si0.3Sn0.7 with Ag or Li doping is synthesized by two-step solid-state reaction method at temperatures of 873 K and 973 K for 24 h, respectively. The transport parameters and the thermoelectric properties are measured at temperatures ranging from room temperature to 773 K for Mg2(1–x)Ag2xSi0.3Sn0.7 (x = 0, 0.01, 0.02, 0.03, 0.04, 0.05) and Mg2(1–y)Li2ySi0.3Sn0.7 (y = 0, 0.02, 0.04, 0.06, 0.08) samples. The influences of different dopants on solid solubility, microstructure, carrier concentration, electrical properties and thermal transport are also investigated. The X-ray diffraction (XRD) patterns and scanning electron microscopy (SEM) images show that the solid solubility for Ag and for Li are x = 0.03 and y = 0.06, respectively. Based on the assumption of single parabolic band model, the value of effective mass ~1.2m0 of p-type Mg2(1–x)Ag2xSi0.3Sn0.7 and Mg2(1–y)Li2ySi0.3Sn0.7 are similar to that reported in the literature. The comparative results demonstrate that the maximum carrier concentration for Ag doping and for Li doping are 4.64×1019 cm–3 for x = 0.01 and 15.1×1019 cm–3 for y = 0.08 at room temperature, respectively; the Li element has higher solid solubility in Mg2(Si, Sn), which leads to higher carrier concentration and power factor PF ~1.62×10–3 \rm W\cdot\rm m^–1\cdot\rm K^–2 in Li doped samples; the higher carrier concentration of Li doped samples effectively suppresses the bipolar effect; the maximum of ZT ~0.54 for Mg1.92Li0.08Si0.3Sn0.7 is 58% higher than that of Mg1.9Ag0.1Si0.3Sn0.7 samples. The lattice thermal conductivity of Li or Ag doped sample decreases obviously due to the stronger mass and strain field fluctuations in phonon transport.

     

    目录

    /

    返回文章
    返回
    Baidu
    map