Ping Huang, Li You, Xing Liang, Ji-Ye Zhang, Jun Luo. Effects of Se substitution for Te on electrical and thermal transport properties of BiCuTeO [J]. Acta Physica Sinica, 2019, 68(7): 077201-1

Search by keywords or author
- Acta Physica Sinica
- Vol. 68, Issue 7, 077201-1 (2019)
![(a) XRD patterns of the hot-pressed BiCuTe1–xSexO (x = 0, 0.1, 0.2, 0.3, 0.4) samples; (b) cell volume V; (c) lattice parameter c; (d) lattice parameter a as a function of the Se content. The standard XRD pattern of BiCuTeO in (a) is calculated from the Rietveld refinement data given by literature[23]. The solid lines in (b)−(d) are the linear fitting results of the experiment data.BiCuTe1–xSexO (x = 0, 0.1, 0.2, 0.3和0.4) 热压样品的 (a) XRD图谱; (b)晶胞体积V; (c) 晶格常数c; (d) 晶格常数a. 图(a) 中提供的BiCuTeO标准图谱为文献精修数据计算所得[23]; 图(b)—图(d) 中实线为线性拟合结果](/Images/highlights-null.jpg)
Fig. 1. (a) XRD patterns of the hot-pressed BiCuTe1–x Sex O (x = 0, 0.1, 0.2, 0.3, 0.4) samples; (b) cell volume V ; (c) lattice parameter c ; (d) lattice parameter a as a function of the Se content. The standard XRD pattern of BiCuTeO in (a) is calculated from the Rietveld refinement data given by literature[23]. The solid lines in (b)−(d) are the linear fitting results of the experiment data.
BiCuTe1–x Sex O (x = 0, 0.1, 0.2, 0.3和0.4) 热压样品的 (a) XRD图谱; (b)晶胞体积V ; (c) 晶格常数c ; (d) 晶格常数a . 图(a) 中提供的BiCuTeO标准图谱为文献精修数据计算所得[23]; 图(b)—图(d) 中实线为线性拟合结果

Fig. 2. SEM images of polished samples (the insets are the EDS elemental mapping images) ((a)—(c)) and SEM images of fracture surfaces ((d)−(f))for BiCuTe1–x Sex O (x = 0, 0.2, 0.4) compounds.
BiCuTe1–x Sex O (x = 0, 0.2和0.4) 抛光样品的SEM图像(插图为相应的EDS面扫描元素分布图像)((a)—(c))以及断面SEM形貌图((d)—(f))
![Temperature dependent electrical transport properties of BiCuTe1-xSexO (x = 0, 0.1, 0.2, 0.3, 0.4) samples: (a) Electrical conductivity σ; (b) Seebeck coefficients S; (c) power factor S2σ. (d) Se cotent dependence of room temperature hole concentration n and mobility . The dashed and dotted lines in (a)−(c) represent the electrical transport properties of undoped BiCuSeO[14] and BiCuTeO[23], respectively.BiCuTe1-xSexO样品 (x = 0, 0.1, 0.2, 0.3和0.4) 的 (a) 电导率σ; (b) Seebeck系数S; (c) 功率因子S2σ随温度的变化曲线; (d) 样品的载流子浓度n和迁移率随Se含量的变化曲线. 图(a)—(c) 中短划线和点划线分别为文献中未掺杂的BiCuTeO[23]与BiCuSeO[14]的电输运性能](/Images/icon/loading.gif)
Fig. 3. Temperature dependent electrical transport properties of BiCuTe1-x Sex O (x = 0, 0.1, 0.2, 0.3, 0.4) samples: (a) Electrical conductivity σ ; (b) Seebeck coefficients S ; (c) power factor S 2σ . (d) Se cotent dependence of room temperature hole concentration n and mobility
. The dashed and dotted lines in (a)−(c) represent the electrical transport properties of undoped BiCuSeO[14] and BiCuTeO[23], respectively.
BiCuTe1-x Sex O样品 (x = 0, 0.1, 0.2, 0.3和0.4) 的 (a) 电导率σ ; (b) Seebeck系数S ; (c) 功率因子S 2σ 随温度的变化曲线; (d) 样品的载流子浓度n 和迁移率
随Se含量的变化曲线. 图(a)—(c) 中短划线和点划线分别为文献中未掺杂的BiCuTeO[23]与BiCuSeO[14]的电输运性能
![Hole concentration n dependent effective mass m* of (a) Heavily doped BiCuSeO[14,16,28] and BiCuTeO[24,25]; (b) Se doped BiCuTeO (this work) and Te doped BiCuSeO[28].(a) 重掺杂BiCuSeO[14,16,28]和BiCuTeO[24,25]的载流子有效质量m*随载流子浓度n的变化曲线; (b) Se掺杂BiCuTeO(本工作)和Te掺杂BiCuSeO[28]的载流子有效质量m*随载流子浓度n的变化曲线](/Images/icon/loading.gif)
Fig. 4. Hole concentration n dependent effective mass m * of (a) Heavily doped BiCuSeO[14,16,28] and BiCuTeO[24,25]; (b) Se doped BiCuTeO (this work) and Te doped BiCuSeO[28].
(a) 重掺杂BiCuSeO[14,16,28]和BiCuTeO[24,25]的载流子有效质量m *随载流子浓度n 的变化曲线; (b) Se掺杂BiCuTeO(本工作)和Te掺杂BiCuSeO[28]的载流子有效质量m *随载流子浓度n 的变化曲线
![Temperature dependent thermal transport properties of BiCuTe1–xSexO (x = 0, 0.1, 0.2, 0.3, 0.4) samples: (a) Total thermal conductivity; (b) the combination of lattice and bipolar thermal conductivity, and the electronic thermal conductivity. The dashed and dotted lines in (a) represent the total thermal conductivities of undoped BiCuTeO[23] and BiCuSeO[14], respectively.BiCuTe1–xSexO (x = 0, 0.1, 0.2, 0.3和0.4) 样品的(a) 总热导率和(b) 电子热导率、晶格热导率与双极扩散热导率之和随温度的变化曲线. 图(a)中短划线和点划线分别为未掺杂的BiCuTeO[23]与BiCuSeO[14]的热输运性能](/Images/icon/loading.gif)
Fig. 5. Temperature dependent thermal transport properties of BiCuTe1–x Sex O (x = 0, 0.1, 0.2, 0.3, 0.4) samples: (a) Total thermal conductivity; (b) the combination of lattice and bipolar thermal conductivity, and the electronic thermal conductivity. The dashed and dotted lines in (a) represent the total thermal conductivities of undoped BiCuTeO[23] and BiCuSeO[14], respectively.
BiCuTe1–x Sex O (x = 0, 0.1, 0.2, 0.3和0.4) 样品的(a) 总热导率和(b) 电子热导率、晶格热导率与双极扩散热导率之和随温度的变化曲线. 图(a)中短划线和点划线分别为未掺杂的BiCuTeO[23]与BiCuSeO[14]的热输运性能
![Temperature dependent zT values of BiCuTe1–xSexO (x = 0, 0.1, 0.2, 0.3, 0.4) samples. The dashed and dotted lines represent the zT values of undoped BiCuTeO[23] and BiCuSeO[14], respectively.BiCuTe1–xSexO (x = 0, 0.1, 0.2, 0.3和0.4)样品的zT值随温度的变化曲线. 短划线和点划线分别为未掺杂的BiCuTeO[23]与BiCuSeO[14]的zT值](/Images/icon/loading.gif)
Fig. 6. Temperature dependent zT values of BiCuTe1–x Sex O (x = 0, 0.1, 0.2, 0.3, 0.4) samples. The dashed and dotted lines represent the zT values of undoped BiCuTeO[23] and BiCuSeO[14], respectively.
BiCuTe1–x Sex O (x = 0, 0.1, 0.2, 0.3和0.4)样品的zT 值随温度的变化曲线. 短划线和点划线分别为未掺杂的BiCuTeO[23]与BiCuSeO[14]的zT值
|
Table 1. Room temperature carrier concentrations (n ), Hall mobilities (
), electrical conductivities (σ ) and effective masses of BiCuTe1–x Sex O (x = 0, 0.1, 0.2, 0.3, 0.4) samples.
室温下BiCuTe1–x Sex O (x = 0, 0.1, 0.2, 0.3和0.4) 样品的载流子浓度 (n )、迁移率 (
)、电导率 (σ ) 以及载流子有效质量 (m *)
Set citation alerts for the article
Please enter your email address