Evidence of electron interaction with an unidentified bosonic mode in superconductor CsCa₂Fe₄As₄F₂

The kink structure in band dispersion usually refers to a certain electron-boson interaction, which is crucial in understanding the pairing in unconventional superconductors. Here we report the evidence of the observation of a kink structure in Fe-based superconductor CsCa₂Fe₄As₄F₂ using angle-resolved photoemission spectroscopy. The kink shows an orbital selective and momentum dependent behavior, which is located at 15 meV below Fermi level along the \(\Gamma -{{\rm{{M}}}}\) $\mathrm{\Gamma }-\mathrm{M}$ direction at the band with d_xz orbital character and vanishes when approaching the \(\Gamma -{{\rm{{X}}}}\) $\mathrm{\Gamma }-\mathrm{X}$ direction, correlated with a slight decrease of the superconducting gap. Most importantly, this kink structure disappears when the superconducting gap closes, indicating that the corresponding bosonic mode (~ \(9\pm 1\) $9\pm 1$ meV) is closely related to superconductivity. However, the origin of this mode remains unidentified, since it cannot be related to phonons or the spin resonance mode (~15 meV) observed by inelastic neutron scattering. The behavior of this mode is rather unique and challenges our present understanding of the superconducting paring mechanism of the bilayer FeAs-based superconductors.