Abstract
Parity quantum numbers for dipole-excited states of the nuclei $^{92}\mathrm{Zr}$ and $^{96}\mathrm{Mo}$ have been determined from azimuthal asymmetries of nuclear resonance fluorescence intensities induced with the linearly polarized photon beam of the $\mathrm{HI}\ensuremath{\gamma}\mathrm{S}$ facility at Duke University. This parity information is crucial for an interpretation of the investigated $J=1$ states as two-phonon excitations originating from inhomogeneous phonon coupling.
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