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Volumn 77, Issue 24, 2008, Pages

Sum-rules for Raman scattering off strongly correlated electron systems

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Indexed keywords


EID: 45749130990     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.77.245128     Document Type: Article
Times cited : (10)

References (23)
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    • We are interested here in the Raman response of a bidimensional cubic lattice, so in the calculation of the response function we will make use of a form factor obtained by integrating functions of the cubic dispersion [Eq. 5] over the bidimensional Brillouin zone. Hence, DMFT here has to be thought as a local self-energy approximation of the finite dimensional lattice rather than the solution of the ∞-dimensional counterpart of the model under investigation. In this light the choice of a semicircular DOS (see the footnote on DMFT technical data) for the impurity model (which facilitates the numerical solution) is not a severe inconsistency with the cubic dispersion used in the response function.
    • We are interested here in the Raman response of a bidimensional cubic lattice, so in the calculation of the response function we will make use of a form factor obtained by integrating functions of the cubic dispersion [Eq. 5] over the bidimensional Brillouin zone. Hence, DMFT here has to be thought as a local self-energy approximation of the finite dimensional lattice rather than the solution of the ∞-dimensional counterpart of the model under investigation. In this light the choice of a semicircular DOS (see the footnote on DMFT technical data) for the impurity model (which facilitates the numerical solution) is not a severe inconsistency with the cubic dispersion used in the response function.
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    • The real-axis self-energies are calculated for ω=ω+i Γbr, with Γbr =0.1 in order to smoothen out the spikes due to the discretization of the bath.
    • The real-axis self-energies are calculated for ω=ω+i Γbr, with Γbr =0.1 in order to smoothen out the spikes due to the discretization of the bath.
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