corner
corner

Phys. Rev. B 80, 184302 (2009) [9 pages]

Phonon density of states and heat capacity of La3−xTe4

Download: PDF (352 kB) Buy this article Export: BibTeX or EndNote (RIS)

O. Delaire1, A. F. May2, M. A. McGuire3, W. D. Porter3, M. S. Lucas1, M. B. Stone1, D. L. Abernathy1, V. A. Ravi4,5, S. A. Firdosy4, and G. J. Snyder2
1Neutron Scattering Science Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
2California Institute of Technology, Pasadena, California 91125, USA
3Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
4Jet Propulsion Laboratory, 4800 Oak Grove Drive, Pasadena, California 91109, USA
5Department of Chemical and Materials Engineering, California State Polytechnic University, Pomona, California 91768, USA

Received 25 August 2009; published 19 November 2009

The phonon density of states (DOS) of La3−xTe4 compounds (x=0.0,0.18,0.32) was measured at 300, 520, and 780 K, using inelastic neutron scattering. A significant stiffening of the phonon DOS and a large broadening of features were observed upon introduction of vacancies on La sites (increasing x). Heat-capacity measurements were performed at temperatures 1.85≤T≤1200 K and were analyzed to quantify the contributions of phonons and electrons. The Debye temperature and the electronic coefficient of heat capacity determined from these measurements are consistent with the neutron-scattering results, and with previously reported first-principles calculations. Our results indicate that La vacancies in La3−xTe4 strongly scatter phonons and this source of scattering appears to be independent of temperature. The stiffening of the phonon DOS induced by the introduction of vacancies is explained in terms of the electronic structure and the change in bonding character. The temperature dependence of the phonon DOS is captured satisfactorily by the quasiharmonic approximation.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.80.184302
DOI:
10.1103/PhysRevB.80.184302
PACS:
63.20.−e, 61.05.fg, 65.40.Ba, 72.20.Pa