The physical properties of arbitrary half-integer spins
F=N−1/2 fermionic cold atoms loaded into a one-dimensional optical lattice are investigated by means of a
conformal field theory approach. We show that for attractive interactions two different superfluid phases emerge for
F
3/2: A BCS pairing phase, and a molecular superfluid phase which is formed from bound-states made of 2
N fermions. In the low-energy approach, the competition between these instabilities and charge-density waves is described in terms of
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parafermionic degrees of freedom. The quantum phase transition for
F=3/2,5/2 is universal and shown to belong to the Ising and three-state Potts universality classes respectively. In contrast, for
F
7/2, the transition is non-universal. For a filling of one atom per site, a Mott transition occurs and the nature of the possible Mott-insulating phases are determined.