  We analyze the scattering rate for 2D fermions interacting via soft nematic
fluctuations. The ground state is an s-wave superconductor, but other pairing
channels are almost equally attractive. This strongly alters the scattering
rate: At energies beyond the pairing gap $\Delta$, it is renormalized by
contributions from all pairing channels. At energies of order $\Delta$, it is
determined by the competition between scattering into a gapped continuum and
dispersing nematic resonance. The outcome is a "peak-peak-dip-hump" spectrum,
similar, but not identical, to the "peak-dip-hump" structure in the cuprates.
