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Figure 2
Excitation on the [1\sigma_{\rm{g}}^{-1}3\sigma_{\rm{u}}] resonance in O2 reveals intriguing dynamics. First, coupling to the [1\sigma_{\rm{u}}^{-1}3s_{\rm{g}}] state is opening the channel to populate [3\sigma_{\rm{g}}^{-1}3s_{\rm{g}}] final states. Second, the angular anisotropy of the process demonstrates interference with the non-resonant inelastic scattering channel. [From Sun et al. (2013BB60); Copyright (2013) by the American Physical Society.]

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