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Active Optical Metasurfaces Based on Defect-Engineered Phase-Transition Materials

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Figure

Figure 2. Defect engineering via ion beam irradiation. (a) Temper-cdamage formation model (mass, andcritical temperature is a result of lattice defects induced by ionirradiation and is not caused by impurity doping
Figure 3. Artithat cannot be trivially deduced by averaging the rebroadened phase transition
Figure 4. Switchable polarizer via tunable anisotropy. (a) Measured recrystal with form birefringence and dichroism
Figure 5. Limits of spatially selective defect engineering probed byLine scan of the AFM topography (blue) and near-scattering-type scanning near= 10.9amplitude is related to the local value of the dielectric function andthus yields a good contrast between

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