“…Similar to the case of SPPs, there exists a momentum mismatch between the incident photons and the SPhP modes (illustrated for the 4H-SiC/ air interface in Figure 2B along with the well-known bulk phonon polariton branches). This mismatch can be overcome using the coupling of the incident field to surface modes through a diffraction grating [92], high index prism [58,93,94], scattering from a nearby sub-wavelength particle such as an SNOM tip [20,36,38,64] or via nanostructuring of the SPhP material into sub-wavelength particles [23,53,91]. By doing so, an overlap between the light line, k = ω/c and the SPhP dispersion curve, can be realized.…”