“…In fact, all computations rely on the introduction of an additional parameter through a unitary transformation of the Hamiltonian. Then the Berry phase for a special class of loops in this extended parameter space is computed, leading to the results reported in references [1,2,3,4,5]. In this work, using the model proposed in [5], we intend to go a step further in the sense that, for each value of the external field (λ), we identify a space (isomorphic to the two-sphere) and a corresponding line bundle L λ over it, for which a topological invariant c 1 (λ) can be computed.…”