Mobile bipolarons in the adiabatic Holstein-Hubbard model in one and two dimensions

The bound states of two electrons in the adiabatic Holstein-Hubbard model are studied numerically in one and two dimensions from the anticontinuous limit. This model involves a competition between a local electron-phonon coupling (with a classical lattice) which tends to form pairs of electrons and the repulsive Hubbard interaction U greater than or equal to 0 which tends to break them. In one-dimensional (1D), the ground-state always consists of a pair of localized polarons in a singlet state. They are located at the same site for U = 0. Increasing Ii, there is a first-order transition at which the bipolaron becomes a spin singlet pair of two polarons bounded by a magnetic interaction. The pinning mode of the bipolaron soften in the vicinity of this transition leading to a higher mobility of the bipolaron which is tested numerically. In 2D, and for any U, the electron-phonon coupling needs to be large enough in order to form small polarons or bipolarons instead of extended electrons. We calculate the phase diagram of the bipolaron involving first-order transition lines with a triple point. A pair of polarons can form three types of bipolarons: (a) on a single site at small U, (b) a spin singlet state on two nearest neighbor sites for larger U as in 1D, and (c) a new intermediate state obtained as the resonant combination of four 2-site singlet states sharing a central site, called quadrisinglet. The breathing and pinning internal modes of bipolarons in 2D generally only weakly soften and thus, they are practically not mobile. On the contrary, in the vicinity of the triple point involving the quadrisinglet, both modes exhibit a significant softening. However, it was not sufficient for allowing he existence of a classical mobile bipolaron (at least in that model). Copyright (C) 1998 Elsevier Science B.V.