Abstract
Time and wavelength resolved fluorescence techniques are used to investigate C2 (B 2Σ) radiationless transitions following pulsed, tunable laser excitation. The purely radiative lifetimes in each host are Ne, ?64 nsec; Ar, ?40 nsec; Kr, ≃38 nsec; and Xe, ≃34 nsec. The principal B 2Σ vibrational relaxation mechanism is a sequential process: crossing into a 4Σ, vibrational relaxation within 4Σ, and reverse crossing into B 2Σ. The observed intermediate lifetimes strongly suggest that v=0 4Σ lies between v=0 and 1 of B 2Σ; this fact allows assignment of gas phase B 2Σ↔a 4Σ rotational perturbations reported by Herzberg and Lagerqvist. The unperturbed a 4Σ constants are Te=19 448.4 cm−1, ωe=1074.04 cm−1, Be=1.1348 cm−1, ωexe=24.68 cm−1, and αe=0.0035 cm−1. Vibrational relaxation within a 4Σ, and intersystem crossing, show a strong multiphonon relaxation energy gap law. The variation in behavior among the 12–12, 12–13, and 13–13 isotopes indicates that the photophysics is dominated by accidental near degeneracies with A 2Π (and probably X 2Σ) levels in addition to 4Σ levels.