Abstract
We discuss the Mott-Hubbard transition, the metal-insulator transition as a function of interaction strength U, for the half-filled Hubbard model in two numerically tractable cases: on a one-dimensional chain with nearest-neighbor hopping t’, and in the limit of infinite dimensions. In the one-dimensional model, we calculate the electric susceptibility using the Density Matrix Renormalization Group and show that the transition is infinite order, irrespective of t’ In infinite dimensions, we use the Random Dispersion Approximation to calculate the behavior of the quasiparticle weight and the single-particle gap for the transition from the paramagnetic metal to the paramagnetic insulator. Within the accuracy of our calculations, we find no evidence of the discontinuous behavior found in other approaches to the infinite-dimensional limit.
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Noack, R.M., Aebischer, C., Baeriswyl, D., Gebhard, F. (2001). Studies of the Mott-Hubbard Transition in one and Infinite Dimensions. In: Bonča, J., Prelovšek, P., Ramšak, A., Sarkar, S. (eds) Open Problems in Strongly Correlated Electron Systems. NATO Science Series, vol 15. Springer, Dordrecht. https://doi.org/10.1007/978-94-010-0771-9_36
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DOI: https://doi.org/10.1007/978-94-010-0771-9_36
Publisher Name: Springer, Dordrecht
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