“…In this paper we present a re-assignment of the vibrational structure of both the Huggins and Hartley band systems which recognizes the considerable anharmonicity that is to be expected on the weakly bound upper surface͑s͒. In these new assignments, only progressions in 1 , the symmetric stretching vibration, and 2 , the bending vibration, are observed, as in the two earliest studies, 7,8 but now all hot bands originate from one quantum of 1 in the ground state rather than from one quantum of 3 . These re-assignments produce a rather different picture of motion on the excited surface in the asymmetric stretch coordinate.…”