Structural characterization of Bi2Te3 and Sb2Te3 as a function of temperature using neutron powder diffraction and extended X-ray absorption fine structure techniques

  • A. N. Mansour
    Naval Surface Warfare Center, Carderock Division, West Bethesda 1 , Maryland 20817, USA
  • W. Wong-Ng
    National Institute of Standards and Technology 2 Materials Measurement Science Division , Gaithersburg, Maryland 20899, USA
  • Q. Huang
    Center for Neutron Research National Institute of Standards and Technology 3 , Gaithersburg, Maryland 20899, USA
  • W. Tang
    Zhejiang Sci-Tech University 4 , Hangzhou, Zhejiang 310018, China
  • A. Thompson
    Marlow Industries, Inc 5 Dallas, Texas 75238, USA
  • J. Sharp
    Marlow Industries, Inc 5 Dallas, Texas 75238, USA

抄録

<jats:p>The structure of Bi2Te3 (Seebeck coefficient Standard Reference Material (SRM™ 3451)) and the related phase Sb2Te3 have been characterized as a function of temperature using the neutron powder diffraction (NPD) and the extended X-ray absorption fine structure (EXAFS) techniques. The neutron structural studies were carried out from 20 K to 300 K for Bi2Te3 and from 10 K to 298 K for Sb2Te3. The EXAFS technique for studying the local structure of the two compounds was conducted from 19 K to 298 K. Bi2Te3 and Sb2Te3 are isostructural, with a space group of R3¯m. The structure consists of repeated quintuple layers of atoms, Te2-M-Te1-M-Te2 (where M = Bi or Sb) stacking along the c-axis of the unit cell. EXAFS was used to examine the bond distances and static and thermal disorders for the first three shells of Bi2Te3 and Sb2Te3 as a function of temperature. The temperature dependencies of thermal disorders were analyzed using the Debye and Einstein models for lattice vibrations. The Debye and Einstein temperatures for the first two shells of Bi2Te3 are similar to those of Sb2Te3 within the uncertainty in the data. However, the Debye and Einstein temperatures for the third shell of Bi-Bi are significantly lower than those of the third shell of Sb-Sb. The Einstein temperature for the third shell is consistent with a soft phonon mode in both Bi2Te3 and Sb2Te3. The lower Einstein temperature of Bi-Bi relative to Sb-Sb is consistent with the lower value of thermal conductivity of Bi2Te3 relative to Sb2Te3.</jats:p>

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