We investigate spin-(1/2) electrons with local Hubbard interaction and
variable-range hopping amplitudes which decay like sinh(kappa)/sinh(k
appa r). Assuming integrability, the asymptotic-Bethe-ansatz approach
allows us to derive the generalized Lieb-Wu integral equations from th
e two-particle phase shift. Due to the nesting property there is a met
al-to-insulator transition at U-c (kappa > 0) = 0(+). The charge gap i
n the singular limit kappa = 0 opens when the interaction strength equ
als the bandwidth, U-c (kappa = 0) = W > 0.