Time-dependent mean-field theory for x-ray near-edge spectroscopy

G. F. Bertsch and A. J. Lee
Phys. Rev. B 89, 075135 – Published 27 February 2014
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Abstract

We derive equations of motion for calculating the near-edge x-ray absorption spectrum in molecules and condensed matter, based on a two-determinant approximation and Dirac's variational principle. The theory provides an exact solution for the linear response when the Hamiltonian or energy functional has only diagonal interactions in some basis. We numerically solve the equations to compare with the Mahan–Nozières–De Dominicis theory of the edge singularity in metallic conductors. Our extracted power-law exponents are similar to those of the analytic theory, but are not in quantitative agreement. The calculational method can be readily generalized to treat Kohn-Sham Hamiltonians with electron-electron interactions derived from correlation-exchange potentials.

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  • Received 27 June 2013
  • Revised 31 January 2014

DOI:https://doi.org/10.1103/PhysRevB.89.075135

©2014 American Physical Society

Authors & Affiliations

G. F. Bertsch1 and A. J. Lee2

  • 1Institute for Nuclear Theory and Department of Physics, University of Washington, Seattle, Washington, USA
  • 2Department of Physics, University of Washington, Seattle, Washington, USA

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Issue

Vol. 89, Iss. 7 — 15 February 2014

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