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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.
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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.
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