The 1D system of correlated electrons characterized in addition to the
usual on-site (U) and nearest-neighbour (V) repulsion by a correlated
-hopping term (t) is considered. The ground state phase diagram is st
udied within the framework of the weak-coupling continuum-limit approa
ch. At filling nu the effective interaction originating from the corre
lated-hopping term which appears in the continuum-limit theory is give
n by tcos(pinu). Being repulsive for nu < 1/2 and attractive for nu >
1/2, this interaction leads to a characteristic band-filling dependen
ce of the phase diagram of the system. For nu not-equal 1/2, depending
on the relation between the bare values of the coupling constants (U,
V, tcos(pinu)) and, hence, on the band-filling, the system shows thr
ee different phases in the infrared limit: a Luttinger metal, a nonmag
netic metal and a singlet superconducting phase. For nu = 1/2, the cor
related-hopping interaction is dynamically trivial, leading only to a
renormalization of the one-electron hopping amplitude and the phase di
agram of the model coincides with that of the extended Hubbard model.