We studied mesoscopic Hubbard rings with impurities using the renormalization group (RG) technique and the exact diagonalizations. The exact diagonalization calculations showed that the charge stiffness normalized by the value of clean system has a peak as a function of electron-electron interactions. Previous RG analysis has succeeded to show the enhancement of the stiffness at weak interactions, but does not show the peak behavior. We derived RG equations with
4kF impurity scattering term, which was ignored in the previous studies, and reproduced the overall behavior of the exact diagonalization results.
We studied mesoscopic Hubbard rings with impurities using the renormalization group (RG) technique and the exact diagonalizations. The exact diagonalization calculations showed that the charge stiffness normalized by the value of a clean system has a peak as a function of electron-electron interactions. Previous RG analysis has succeeded in showing the enhancement of the stiffness at weak interactions, but does not reveal the peak behavior. We derived RG equations with a 4
kF impurity scattering term, which was ignored in the previous studies, and reproduced the overall behavior of the exact diagonalization results. \textcopyright{} 1996 The American Physical Society.
We investigate the energy spectrum of one‐dimensional ionic conductor described with Pauli statistics taking into account ion transfer as well as the short‐range non‐local correlation between particles. Both commutator and anticommutator Green’s functions constructed of Pauli creation and annihilation operators are calculated using exact diagonalization technique on the basis of finite ionic chains with periodic boundary conditions. The frequency dependencies of one‐particle spectral densities are calculated. In the limit of vanishing correlation strength the results are compared with the ones obtained by means of fermionization procedure while for different correlation strengths the results are compared to the ones obtained via exact diagonalization technique for similar systems described with Fermi statistics.