We determine the phase diagram of a quasi-one-dimensional conductor (w
eakly coupled chains system with an open Fermi surface) in a magnetic
field. The usual Ginzburg-Landau regime is followed, when the field is
increased, by a cascade of superconducting phases separated by first
order transitions, which ends with a strong reentrance of the super-co
nducting phase. These new phases show a novel kind of symmetry of lami
nar type. The Zeeman splitting does not completely suppress the reentr
ance in very strongfield, the ground state being in this case a Larkin
-Ovchinnikov-Fulde-Ferrell state.