Abstract:
A solution in quadratures of the doubly orbitally degenerate Hubbard chain with
strong correlations of the electrons in one orbital is obtained by means of the
spin-symmetrized Bethe–Gaudin–Yaug ansatz. The correlation gap in the
dielectric phase is due to both interorbital Coulomb repulsion of the electrons
and their Hund exchange interaction. The possibilities of a Mort transition are
investigated.
Citation:
A. V. Vedyaev, M. E. Zhuravlev, V. A. Ivanov, “Phase transitions in one-dimensional Hubbard model with degeneracy”, TMF, 67:3 (1986), 470–473; Theoret. and Math. Phys., 67:3 (1986), 627–629
This publication is cited in the following 4 articles:
Igor N. Karnaukhov, “Hybridized mechanism of pairing and the heavy fermion state: Exactly solvable two-band model with strong hybridized interactions”, Phys. Rev. B, 72:9 (2005)
Holger Frahm, Sascha Ledowski, “Boundary states and edge singularities in the degenerate Hubbard chain”, J. Phys.: Condens. Matter, 10:39 (1998), 8829
P. Schlottmann, “Spin and charge excitations of the degenerate Hubbard model in one dimension”, Phys. Rev. B, 43:4 (1991), 3101
A. V. Vedyaev, M. E. Zhuravlev, V. A. Ivanov, “Elementary excitations in the dimerized Hubbard model”, Theoret. and Math. Phys., 71:3 (1987), 660–665