“…In this section, we analyse a double-lambda configuration with a two-colour excitation of 87 Rb atoms within the D 1 line, i.e., 5s 2 S 1/2 − 5p 2 P 1/2 [2]. The bar states can be described in terms of the generic four states: |1〉 = |5 2 S 1/2 (F g = 1)〉; |2〉 = |5 2 S 1/2 (F g = 2)〉; |3〉 = |5 2 P 1/2 (F e = 1)〉; and |4〉 = |5 2 P 1/2 (F e = 1)〉, where F g (F e ) stands for the total angular momentum associated with ground and excited hyperfine states.…”