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Cu掺杂AgSbTe2化合物的相稳定、晶体结构及热电性能
引用本文:张贺,骆军,朱航天,刘泉林,梁敬魁,饶光辉.Cu掺杂AgSbTe2化合物的相稳定、晶体结构及热电性能[J].物理学报,2012,61(8):86101-086101.
作者姓名:张贺  骆军  朱航天  刘泉林  梁敬魁  饶光辉
作者单位:1. 北京科技大学材料科学与工程学院,新金属材料国家重点实验室,北京100083/中国科学院物理研究所,北京100190
2. 中国科学院物理研究所,北京,100190
3. 北京科技大学材料科学与工程学院,新金属材料国家重点实验室,北京100083
基金项目:国家自然科学基金 (批准号: 11144002)、国家重点基础研究发展计划 (批准号: 2007CB925003) 和教育部科学技术研究计划重大项目(批准号: 309006)资助的课题.
摘    要:利用熔融快淬结合放电等离子烧结(SPS), 制备了CuxAg1-xSbTe2(x= 0---0.3)样品. 粉末X射线衍射(XRD)分析结果显示, SPS处理以前, 含Cu样品形成NaCl型结构的固溶体, 而未加入Cu的样品析出Ag2Te第二相. 根据热分析和XRD测量结果, Cu的加入能够有效抑制Ag2Te的析出, 但同时会在快淬样品中产生少量非晶相. 在温度升高到540 K左右时, 非晶相发生晶化, 形成Sb7Te亚稳相, 并最终转变成Sb2Te3稳定相. 对快淬样品进行低温SPS快速处理后, x =0.1样品为面心立方结构的单相化合物, 但是x =0.2, 0.3的样品分别析出第二相Sb7Te和Sb2Te3. 由于析出第二相, x=0.2, 0.3样品的电导率增大, Seebeck系数减小, 热导率相应升高, 综合热电性能降低. x=0.1单相样品的功率因子与文献报道的AgSbTe2化合物相当. 元素替代的合金化效应 增强了Cu0.1Ag0.9SbTe2化合物的声子散射, 有效降低了样品的热导率. 因此, 单相样品Cu0.1Ag0.9SbTe2表现出较佳的热电性能, 在620 K时热电优值达到1.

关 键 词:AgSbTe2  相稳定  晶体结构  热电性能
收稿时间:2011-07-22

Phase stability, crystal structure and thermoelectric properties of Cu doped AgSbTe2
Zhang He,Luo Jun,Zhu Hang-Tian,Liu Quan-Lin,Liang Jing-Kui,Rao Guang-Hui.Phase stability, crystal structure and thermoelectric properties of Cu doped AgSbTe2[J].Acta Physica Sinica,2012,61(8):86101-086101.
Authors:Zhang He  Luo Jun  Zhu Hang-Tian  Liu Quan-Lin  Liang Jing-Kui  Rao Guang-Hui
Institution:1. State Key Laboratory for Advanced Metals and Materials, School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China; 2. Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
Abstract:CuxAg1-xSbTe2 samples with x = 0---0.3 are prepared by a combined process of melt-quenching and spark plasma sintering (SPS). X-ray powder diffraction (XRD) analysis indicates that single phase samples with the NaCl-type structure are obtained for the Cu-doped samples before SPS treatment, whereas a small quantity of Ag2Te impurities coexist with the main cubic phase for the sample without Cu. According to our thermoanalysis and XRD results, the substitution of Cu for Ag can effectively prevent the precipitation of Ag2Te, but this also leads to the presence of a minor amorphous phase in the melt-quenched sample. The amorphous phase crystallizes into Sb7Te metastable phase at about 540 K, which finally transforms into the stable Sb2Te3 compound. After the SPS treatment of the melt-quenched sample, the sample with x=0.1 remains a single phase with the face-centered-cubic crystal structure, while Sb7Te and Sb2Te3 are precipitated as the second phases for the samples with x = 0.2 and 0.3, respectively. The electrical conductivity increases and the Seebeck coefficient decreases with the addition of Cu due to the existence of the second phase in the samples with x = 0.2 and 0.3. Accordingly, thermal conductivities also increase with the addition of Cu, leading to the reduced thermoelectric performance of the x= 0.2 and 0.3 samples. For the sample with x = 0.1, its power factor is comparable to that of the literature reported AgSbTe2 compound. As a result of so-called alloying effect, the phonon scattering effect is enhanced due to the partial replacement of Ag by Cu, leading to the reduced thermal conductivity of the x = 0.1 sample. Therefore, the Cu0.1Ag0.9SbTe2 sample exhibits the promising thermoelectric performance and a dimensionless thermoelectric figure of merit (ZT) value of 1 is achieved at 620 K.
Keywords:AgSbTe2  phase stability  crystal structure  thermoelectric properties
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