“…However, as explained below, since it is based upon two-photon XUV-IR transitions, it also changes the angular momentum of the final states and consequently the photoelectron angular distributions. 38 , 47 . For any ionization channel leading to the same final state, our experimental measurement involves three two-photon pathways: 3 p → λ →ℓ, with ( λ , ℓ ) = (0,1),(2,1),(2,3).…”