Begin{eqnarray} G { text{Latt} ( boldsymbol{k}, omega n)= frac{1}{i omega n mu - epsilon(k) phantom{- Sigma text{AIM}( omega n)} end{eqnarray}. Begin{eqnarray} phantom{G { text{Latt} ( boldsymbol{k}, omega n)=} frac{ phantom{1} { phantom{i omega n mu - epsilon(k)} - color{blue}{ Sigma text{AIM}( omega n)} end{eqnarray}. Begin{eqnarray} G { text{Latt} end{eqnarray}. Begin{eqnarray} Sigma text{AIM} end{eqnarray}.
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Begin{eqnarray} G { text{Latt} ( boldsymbol{k}, omega n)= frac{1}{i omega n mu - epsilon(k) phantom{- Sigma text{AIM}( omega n)} end{eqnarray}. Begin{eqnarray} phantom{G { text{Latt} ( boldsymbol{k}, omega n)=} frac{ phantom{1} { phantom{i omega n mu - epsilon(k)} - color{blue}{ Sigma text{AIM}( omega n)} end{eqnarray}. Begin{eqnarray} G { text{Latt} end{eqnarray}. Begin{eqnarray} Sigma text{AIM} end{eqnarray}.
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General Discussion of Green Functions. Dynamical Mean Field Theory. W2Dynamics and Dynamical Mean Field Theory. Quantum Monte Carlo Technique. General Condensed Matter Theory. Quantum Field Theoretical Methods in Statistical Physics. Optical Properties of Solids. Conductor Insulator Transitions - RG Paper relevant. School of Physical and Mathematical Science. Division of Physics and Applied Physics. 21 Nanyang Link SPMS-PAP-04-21. Terahertz conductivity of tin oxide nanowire film.
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Pump Probe Electron Relaxation. Dynamic Mean Field Theory.
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Begin{eqnarray} G { text{Latt} ( boldsymbol{k}, omega n)= frac{1}{i omega n mu - epsilon(k) phantom{- Sigma text{AIM}( omega n)} end{eqnarray}. Begin{eqnarray} phantom{G { text{Latt} ( boldsymbol{k}, omega n)=} frac{ phantom{1} { phantom{i omega n mu - epsilon(k)} - color{blue}{ Sigma text{AIM}( omega n)} end{eqnarray}. Begin{eqnarray} G { text{Latt} end{eqnarray}. Begin{eqnarray} Sigma text{AIM} end{eqnarray}.
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