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Springer eBooks

Inelastic Light Scattering and the Correlated Metal-Insulator Transition

James K. Freericks, T. P. Devereaux, R. Bulla

Published Jan 1, 2003• 0 citations
Publisher
DOI
10.1007/978-94-010-0213-4_11

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arXiv:cond-mat/0305140•Physical review. B, Condensed matter•Aug 8, 2003•10 citations
We use dynamical mean field theory to find an exact solution for inelastic light scattering in strongly correlated materials such as those near a quantum-critical metal-insulator transition. We evaluate the results for q=0 (Raman) scattering and find that resonant effects can be quite large, and yield a double resonance, a significant enhancement of nonresonant scattering peaks, a joint resonance of both peaks when the incident photon frequency is on the order of U, and the appearance of an isosbestic point in all symmetry channels for an intermediate range of incident photon frequencies.
Inelastic light scattering from electrons is a symmetry-selective probe of the charge dynamics within correlated materials. Many measurements have been made on correlated insulators, and recent exact solutions in large dimensions explain a number of anomalous features found in experiments. Here we focus on the correlated metal, as described by the Hubbard model away from half filling. We can determine the B1g{B}_{1\mathrm{g}}B1g​ Raman response and the inelastic x-ray scattering along the Brillouin-zone diagonal exactly in the large dimensional limit. We find a number of interesting features in the light-scattering response, which should be able to be seen in correlated metals such as the heavy fermions.
We construct an exact dynamical mean-field theory for nonresonant inelastic light scattering in the infinite-dimensional Falicov-Kimball model, which can be tuned through a quantum critical metal-insulator transition. Due to the projection of the polarization orientations onto different regions of the Brillouin zone and due to the transfer of energy and momentum from the weakly to the strongly correlated charge excitations, the nature of the dynamics can be naturally interpreted as strongly temperature-dependent low-energy particle-hole excitations and weakly temperature-dependent high-energy charge-transfer excitations which depend delicately on the electronic correlations. These results can be used to provide important information concerning the evolution of charge dynamics in different regions of the Brillouin zone.