Anharmonic Origin of the Giant Thermal Expansion of NaBr

Y. Shen, C. N. Saunders, C. M. Bernal, D. L. Abernathy, M. E. Manley, B. Fultz

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18 Scopus citations

Abstract

All phonons in a single crystal of NaBr are measured by inelastic neutron scattering at temperatures of 10, 300, and 700 K. Even at 300 K, the phonons, especially the longitudinal-optical phonons, show large shifts in frequencies and show large broadenings in energy owing to anharmonicity. Ab initio computations are first performed with the quasiharmonic approximation (QHA) in which the phonon frequencies depend only on V and on T only insofar as it alters V by thermal expansion. This QHA is an unqualified failure for predicting the temperature dependence of phonon frequencies, even 300 K, and the thermal expansion is in error by a factor of 4. Ab initio computations that include both anharmonicity and quasiharmonicity successfully predict both the temperature dependence of phonons and the large thermal expansion of NaBr. The frequencies of longitudinal-optical phonon modes decrease significantly with temperature owing to the real part of the phonon self-energy from explicit anharmonicity originating from the cubic anharmonicity of nearest-neighbor NaBr bonds. Anharmonicity is not a correction to the QHA predictions of thermal expansion and thermal phonon shifts but dominates the behavior.

Original languageEnglish
Article number085504
JournalPhysical Review Letters
Volume125
Issue number8
DOIs
StatePublished - Aug 21 2020

Funding

We thank D. Kim, O. Hellman, F. Yang, and J. Lin for helpful discussions. M. E. M. was supported by the U.S. Department of Energy (DOE), Office of Science, Office of Basic Energy Sciences, Materials Sciences, and Engineering Division under Award No. DE-AC05-00OR22725. Research with the Spallation Neutron Source at the Oak Ridge National Laboratory was sponsored by the Scientific User Facilities Division, Basic Energy Sciences, of the DOE. This work used resources from National Energy Research Scientific Computing Center, an Office of Science User Facility supported by the Office of Science of the US DOE under Award No. DE-AC02-05CH11231. This work was supported by the DOE Office of Science, Basic Energy Sciences, under Award No. DE-FG02-03ER46055.

FundersFunder number
DOE Office of ScienceDE-AC02-05CH11231
U.S. Department of Energy
Office of ScienceDE-FG02-03ER46055
Basic Energy Sciences
Division of Materials Sciences and EngineeringDE-AC05-00OR22725
National Energy Research Scientific Computing Center

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