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Ya. I. Jafarov S. Z. Imamalieva V. P. Zlomanov M. B. Babanly 《Inorganic Materials》2014,50(6):551-558
Phase equilibria in the reciprocal system 3Tl2S + Bi2Te3 ? 3Tl2Te + Bi2S3 (A) have been studied by differential thermal analysis, X-ray diffraction, microhardness tests, and emf measurements using thallium concentration cells, and a number of vertical sections, the 300-K isothermal section of its phase diagram, and the liquidus projection have been mapped out. The system is shown to be reversibly reciprocal, with broad solid solution regions in the Tl2S-Tl2Te-Tl9BiTe6 subsystem and along the TlBiS2-TlBiTe2 join. We have determined the homogeneity ranges and primary crystallization fields of the phases and identified the nature and coordinates of invariant equilibria in system A. 相似文献
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研究了用低温湿化学法和水热法制备纳米级的Bi2Te3和sb挪e3颗粒,并通过透射电镜观察其微观形貌。Bi2Te3粉末的微观形貌为直径在30-50n之间的片状小颗粒,而sb2Te3颗粒的微观形貌为薄带状,直径约为70nm,长度则为从150-300nm不等,并对其晶体的形核和长大机理进行了讨论。认为,纳米小颗粒状的Bi2Te3晶体可能是通过“表面形核和侧向生长”形成的产物,而薄带状的sb2Te3晶体可能是在Te块解体形成的条带状碎屑基础上形成的。用放电等离子烧结法(spark plasma sintering)制备不同比例的Bi2Te3/Sb2Te3块状复合材料,测量并比较了其热电性能。通过改变Bi2Te3的量,可以提高复合材料的电性能。成分不同的层片间的散射,能更有效地降低块体材料的热导率。在500K的温度下,Bi2Te3和sb2Te3以摩尔比为1:1复合烧结的试样的热导率低达0.7W/(m·K)。进一步优化Bi2Te3和sb2Te3的复合比例,其热电性能可能会有进一步的提高。 相似文献
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通过射频磁控溅射,在溅射气体为Ar,气压为1Pa,溅射功率为120W时分别在聚氨酯和玻璃基底上沉积了不同厚度的Bi2Te3薄膜。Bi2Te3薄膜主要是以(221)晶面平行于基底进行外延生长,先在基底形成大量微小晶粒,合并长大成典型的纤维状组织结构。在此条件下薄膜生长速率为26nm/min,通过控制溅射时间可沉积几纳米到几微米不同厚度的薄膜。得到的p-型半导体Bi2Te3薄膜,其电阻率随薄膜厚度的增大而减小。 相似文献
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L. E. Shelimova O. G. Karpinskii V. S. Zemskov P. P. Konstantinov 《Inorganic Materials》2000,36(3):235-242
Analysis of the available crystallographic data shows that the GeTe-Bi2Te3 and GeTe-Sb2Te3 pseudobinary systems contain a wide variety of many-layered, long-period compounds belonging to the nGeTe · mBi2Te3 and nGeTe · mSb2Te3 homologous series. The Hall coefficient, thermoelectric power, and electrical conductivity of some of these compounds were
measured over a wide temperature range. The temperature-dependent carrier mobility data suggest that both acoustic phonons
and point defects contribute to the scattering of charge carriers. The lattice thermal conductivity of the many-layered, long-period
compounds studied, κph = 6–8 mW/(cm K), is notably lower than that of the constituent tellurides 相似文献
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为结合一维纳米材料和纳米颗粒复合材料的优点,本文尝试进行了在氧化铝模板(AAO)中生长Bi2Te3-Si O2纳米颗粒复合纳米线阵列。通过在电化学溶液中添加Si O2纳米颗粒,制备包含纳米颗粒的Bi-Te纳米线阵列。应用XRD、SEM、TEM等方法对合成的样品进行了分析观察。研究发现Si O2纳米颗粒的加入对纳米线的形貌和结构都有明显的影响。在模板法沉积Bi2Te3纳米线阵列时,添加Si O2纳米颗粒将明显改变纳米线生长方式,Bi2Te3纳米线不再是等径的纳米棒,而是枝晶生长过程,最后形成Z字型的不断反复弯折纳米线,该枝晶状纳米线的直径远小于模板的孔径。这一新颖的现象为制备直径更小,并具备精细界面结构的纳米线热电材料提供了一种新的可能途径。 相似文献
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P. P. Konstantinov L. E. Shelimova E. S. Avilov M. A. Kretova V. S. Zemskov 《Inorganic Materials》2001,37(7):662-668
The Hall coefficient, electrical conductivity, and thermoelectric power of Ge3Sb2Te6, Ge2Sb2Te5, GeSb2Te4, and GeSb4Te7were measured over a wide temperature range (R
Hand from 77 to 800 K and Sfrom 90 to 450 K). The carrier concentration was varied via compositional changes within the homogeneity regions of the compounds. All of the materials studied were found to be p-type. Some of the alloys have a low lattice thermal conductivity and are, therefore, candidate p-type thermoelectric materials. The temperature-dependent hole mobility data suggest that both acoustic phonons and point defects contribute to the scattering of charge carriers at low temperatures. 相似文献
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本文介绍了采用热塑形方法制备N型Bi2Te3温差电材料.并且给出了所获得样品的密度、抗弯强度、SEM以及温差电性能(包括电导率和塞贝克系数)的测试结果.实验结果表明,在最佳的热塑形工艺下制备的样品的功率因子与区熔材料相当,但其机械强度要明显优于区熔材料.热压塑形样品在垂直于塑形压力的方向上具有良好的取向,并且样品在此方向上的功率因子远远大于其在平行压力方向上的功率因子值. 相似文献
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电化学制备Bi2Te3纳米线用于微型温差发电器 总被引:1,自引:0,他引:1
借助于电化学沉积的方法,在氧化铝纳米孔内生长Bi2Te3材料,从而形成温差电纳米线阵列.利用SEM,XRD and TEM分析手段对制备的纳米线形貌和结构进行了分析,测量了纳米线的组成和温差电性能.p型和n型Bi2Te3纳米线材料的Seebeck系数经过测量分别为260μV/K和-188μV/K(307K),比同类的块状温差电材料性能高.同时研究了沉积电位对氧化铝模板中纳米孔的填充率的影响,并对纳米线阵列的电阻进行了测量.尝试了利用n型和P型Bi2Te3纳米线阵列制备一种新型的微型温差发电器. 相似文献
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T. I. Koneshova A. Yu. Vol'fkovich A. V. Filatov A. A. Kapichnikov V. M. Novotortsev 《Inorganic Materials》2000,36(12):1217-1218
InTe–Cr2Te3 alloys were prepared and characterized by temperature-dependent magnetic measurements. The results lend support to earlier phase-diagram data indicating the formation of compounds with the compositions In9Cr2Te12 and In2Cr6Te11. In9Cr2Te12 is shown to be a ferromagnet, while In2Cr6Te11 has a more complex magnetic structure. 相似文献
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Yin Yin Guanyong Wang Chen Liu Haili Huang Jiayi Chen Jiaying Liu Dandan Guan Shiyong Wang Yaoyii Li Canhua Liu Hao Zhenq Jinfeng Jia 《Nano Research》2022,(2):1115-1119
Moiré superlattice has recently been found in topological insulators,which can lead to periodic modulation on the electronic structure.In this work,we report th... 相似文献
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本工作研究了Bi-Fe-Se三元相在富Bi2Te3区的相图。测定了Bi2Te3和Bi2Se3从550℃到它们的熔点范围内的等浓度线,用移动加热器(THM)法生长Bi2(Te1-xSex)3(x=0.025和x=0.05)。用霍尔(Hall)效应测定这些化合物在富Te区的固线,研究表明,可再生法生长热力学定义的单晶是可能的。 相似文献
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在GeTe-Bi2Te3赝二元系统中, (GeTe)n(Bi2Te3)m化合物往往具有较低的晶格热导率, 但其中很多组分的热电性能尚未得到系统研究。本研究通过熔融、淬火、退火结合放电等离子烧结工艺制备了一系列(GeTe)nBi2Te3(n=10, 11, 12, 13, 14)单相多晶样品, 并对其相组成和热电性能进行表征和研究。掺杂Bi2Te3可以显著增强点缺陷声子散射, 大幅度降低材料的晶格热导率, 在723 K时, (GeTe)13Bi2Te3样品的总热导率低至1.63 W?m -1?K -1。此外, 掺杂Bi2Te3和调控GeTe的相对含量, 提高了材料的载流子有效质量, 即使在较高的载流子浓度下, 样品依然保持较高的塞贝克系数和功率因子, 在723 K, (GeTe)13Bi2Te3样品获得最大的功率因子为2.88×10 -3 W?m -1?K -2, 最终(GeTe)13Bi2Te3样品在723 K获得的最大ZT值达到1.27, 较未掺杂的GeTe样品提高了16%。 相似文献