We present and study the infinite-dimensional limit of the Hubbard model on a class of non-nested bipartite lattices which generalize the two-dimensional honeycomb and three-dimensional diamond lattice, and are characterized by a semimetallic noninteracting density of states. The infinite-dimensional limit is studied by the well-known mapping onto a self-consistent one-impurity problem. This is solved using quantum Monte Carlo and second-order perturbation theory. The (U, T) phase diagram at half-filling shows a nonmagnetic semimetallic region and an antiferromagnetic insulating phase with a critical value of U for the transition at T = 0 which is strictly positive, U(c)/t almost-equal-to 2.3, in contrast with the hypercubic lattice, where antiferromagnetic order sets in at U(c) = 0.
Hubbard model on the infinite-dimensional diamond lattice / Santoro, Giuseppe Ernesto; Airoldi, M.; Sorella, Sandro; Tosatti, Erio. - In: PHYSICAL REVIEW. B, CONDENSED MATTER. - ISSN 0163-1829. - 47:24(1993), pp. 16216-16221. [10.1103/PhysRevB.47.16216]
Hubbard model on the infinite-dimensional diamond lattice
Santoro, Giuseppe Ernesto;Sorella, Sandro;Tosatti, Erio
1993-01-01
Abstract
We present and study the infinite-dimensional limit of the Hubbard model on a class of non-nested bipartite lattices which generalize the two-dimensional honeycomb and three-dimensional diamond lattice, and are characterized by a semimetallic noninteracting density of states. The infinite-dimensional limit is studied by the well-known mapping onto a self-consistent one-impurity problem. This is solved using quantum Monte Carlo and second-order perturbation theory. The (U, T) phase diagram at half-filling shows a nonmagnetic semimetallic region and an antiferromagnetic insulating phase with a critical value of U for the transition at T = 0 which is strictly positive, U(c)/t almost-equal-to 2.3, in contrast with the hypercubic lattice, where antiferromagnetic order sets in at U(c) = 0.File | Dimensione | Formato | |
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