TY - JOUR
T1 - Crystallographic refinement of collective excitations using standing wave inelastic X-ray scattering
AU - Gan, Yu
AU - Kogar, Anshul
AU - Abbamonte, Peter
N1 - Funding Information:
We gratefully acknowledge Wei Ku, Thomas Gog, and Diego Casa for helpful discussions. This work was supported by U.S. Department of Energy grant DE-FG02-07ER46453 through the Frederick Seitz Materials Research Laboratory. Fig. 1 was generated from data taken at Sector 9 at the Advanced Photon Source, which is supported by DOE grant DE-AC02-06CH11357.
PY - 2013/3/12
Y1 - 2013/3/12
N2 - We propose a method for realizing true, real-space imaging of charge dynamics in a periodic system, with angstrom spatial resolution and attosecond time resolution. In this method, inelastic X-ray scattering (IXS) is carried out with a coherent, standing wave source, which provides the off-diagonal elements of the generalized dynamic structure factor, S(q1, q2,ω), allowing complete reconstruction of the inhomogeneous response function of the system, χ(x1,x2,t). The quantity χ has the physical meaning of a propagator for charge, so allows one to observe-in real time-the disturbance in the electron density created by a point source placed at a specified location, x1 (on an atom vs. between atoms, for example). This method may be thought of as a generalization of X-ray crystallography that allows refinement of the excited states of a periodic system, rather than just its ground state.
AB - We propose a method for realizing true, real-space imaging of charge dynamics in a periodic system, with angstrom spatial resolution and attosecond time resolution. In this method, inelastic X-ray scattering (IXS) is carried out with a coherent, standing wave source, which provides the off-diagonal elements of the generalized dynamic structure factor, S(q1, q2,ω), allowing complete reconstruction of the inhomogeneous response function of the system, χ(x1,x2,t). The quantity χ has the physical meaning of a propagator for charge, so allows one to observe-in real time-the disturbance in the electron density created by a point source placed at a specified location, x1 (on an atom vs. between atoms, for example). This method may be thought of as a generalization of X-ray crystallography that allows refinement of the excited states of a periodic system, rather than just its ground state.
KW - Attosecond
KW - Imaging
KW - Inelastic X-ray scattering
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U2 - 10.1016/j.chemphys.2012.06.018
DO - 10.1016/j.chemphys.2012.06.018
M3 - Article
AN - SCOPUS:84874935231
SN - 0301-0104
VL - 414
SP - 160
EP - 167
JO - Chemical Physics
JF - Chemical Physics
ER -