Diffuse intensity from phonon noise in inelastic neutron scattering

Atomic vibrational dynamics in cuprite ${\mathrm{Cu}}_{2}\mathrm{O}$ was studied by inelastic neutron scattering and molecular-dynamics (MD) simulations from 10 K to 900 K. At 300 K, a diffuse inelastic intensity (DII) appeared in the phonon dispersions, and dominated the spectral intensity at higher temperatures. Classical MD simulations with a machine-learning interatomic potential reproduced general features of the DII. Better agreement with experiment was obtained with the addition of a stiffer potential at close approaches of the Cu and O-atoms. The DII originates from random phase shifts of vibrating O atoms that have brief ($\ensuremath{\sim}10\phantom{\rule{0.28em}{0ex}}\mathrm{fs}$) anharmonic interactions with neighboring Cu atoms. The spectrum of DII gives information about the interaction time of anharmonic interactions between atoms, and its intensity gives a strength of coupling between vibrating atoms and a thermal bath.

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Publication Details

Journal
Physical Review Materials
Published
2025-02-13
DOI
https://doi.org/10.1103/physrevmaterials.9.024602
Primary Topic
Nuclear Physics and Applications
Type
article
Field-Weighted Citation Impact
0.00

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article

Diffuse intensity from phonon noise in inelastic neutron scattering

Dennis Kim, Vladimir Ladygin, S. H. Lohaus, C. M. Bernal-Choban et al.
Physical Review Materials
Nuclear Physics and Applications
article

Diffuse intensity from phonon noise in inelastic neutron scattering

Dennis Kim, Vladimir Ladygin, S. H. Lohaus, C. M. Bernal-Choban, C. N. Saunders, G. E. Granroth, Brent T. Fultz, D. L. Abernathy
article en

Abstract

Atomic vibrational dynamics in cuprite ${\mathrm{Cu}}_{2}\mathrm{O}$ was studied by inelastic neutron scattering and molecular-dynamics (MD) simulations from 10 K to 900 K. At 300 K, a diffuse inelastic intensity (DII) appeared in the phonon dispersions, and dominated the spectral intensity at higher temperatures. Classical MD simulations with a machine-learning interatomic potential reproduced general features of the DII. Better agreement with experiment was obtained with the addition of a stiffer potential at close approaches of the Cu and O-atoms. The DII originates from random phase shifts of vibrating O atoms that have brief ($\ensuremath{\sim}10\phantom{\rule{0.28em}{0ex}}\mathrm{fs}$) anharmonic interactions with neighboring Cu atoms. The spectrum of DII gives information about the interaction time of anharmonic interactions between atoms, and its intensity gives a strength of coupling between vibrating atoms and a thermal bath.

Physical Review MaterialsVol. 9(2)
California Institute of Technology (US), Oak Ridge National Laboratory (US), University of California, Los Angeles (US)
U.S. Department of Energy, Office of Science
Affordable and clean energy
Openalex Percentile: Top 96%
Nuclear Physics and Applications
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