Different Rise Times of Atomic Br M_4,5 3d_3/2,5/2 Core Level Absorptions during Br₂ C ¹Π_u 1_u State Dissociation via...

The reported "dissociation times" for the Br₂ C (¹Π_u 1_u) state by various measurement methods differ widely across the literature (30 to 340 fs). We consider this issue by leveraging attosecond extreme ultraviolet (XUV) transient absorption spectroscopy at the Br M_4,5 3d_3/2,5/2 edges (66 to 80 eV), tracking core-to-valence (3d → 4p) and core-to-Rydberg (3d → ns, np, n ≥ 5) transitions from the molecular to the atomic limit. The progress of dissociation can be ascertained by the buildup of the atomic absorption in time. Notably, the measured rise times of the 3d_5/2,3/2 → 4p transitions depend on the probed core level final state, 38 ± 1 and 20 ± 5 fs for ²D_5/2 and ²D_3/2 at 64.31 and 65.34 eV, respectively. Simulations by the nuclear time-dependent Schrödinger equation reproduce the rise-time difference of the 3d → 4p transitions, and the theory suggests several important factors. One is the transition dipole moments of each probe transition have different molecular and atomic values for ²D_5/2 versus ²D_3/2 that depend on the bond length. The other is the merger of multiple molecular absorptions into the same atomic absorption, creating multiple time scales even for a single probe transition. On the other hand, the core-to-Rydberg absorptions did not allow accurate atomic Br buildup times to be extracted due to spectral overlaps with ground state bleaching, otherwise an even more comprehensive picture of the role of the probe state transition would be possible. This work shows that the measured XUV probe signals accurately contain the dissociative wavepacket dynamics but also reveal how the specific core-to-valence transition affects the apparent progress toward dissociation with bond length. These results highlight the potential probe-transition-dependent effects that need to be considered when interpreting measured signals and their time scales.