4.8 Article

Fourier-transform inelastic X-ray scattering from time- and momentum-dependent phonon-phonon correlations

Journal

NATURE PHYSICS
Volume 9, Issue 12, Pages 790-794

Publisher

NATURE PUBLISHING GROUP
DOI: 10.1038/NPHYS2788

Keywords

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Funding

  1. US Department of Energy (DOE), Office of Basic Energy Sciences (BES) through the Division of Materials Sciences and Engineering [DE-AC02-76SF00515]
  2. DOE Office of Science Graduate Fellowship Program
  3. AMOS program within the Chemical Sciences, Geosciences, and Biosciences Division, DOE, BES
  4. Volkswagen Foundation
  5. German Research Council (DFG) through the Collaborative Research Center 616 'Energy Dissipation at Surfaces'
  6. Swedish Science Council (VR)
  7. AWE
  8. UK EPSRC [EP/H035877/1]
  9. Engineering and Physical Sciences Research Council [EP/J017256/1] Funding Source: researchfish
  10. EPSRC [EP/J017256/1] Funding Source: UKRI

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The macroscopic characteristics of a material are determined by its elementary excitations, which dictate the response of the system to external stimuli. The spectrum of excitations is related to fluctuations in the density-density correlations and is typically measured through frequency-domain neutron(1) or X-ray(2-4) scattering. Time-domain measurements of these correlations could yield a more direct way to investigate the excitations of solids and their couplings both near to and far from equilibrium. Here we show that we can access large portions of the phonon dispersion of germanium by measuring the diffuse scattering from femtosecond X-ray free-electron laser pulses. A femtosecond optical laser pulse slightly quenches the vibrational frequencies, producing pairs of high-wavevector phonons with opposite momenta. These phonons manifest themselves as time-dependent coherences in the displacement correlations(5) probed by the X-ray scattering. As the coherences are preferentially created in regions of strong electron-phonon coupling, the time-resolved approach is a natural spectroscopic tool for probing low-energy collective excitations in solids, and their microscopic interactions.

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