Fig. 4: The nonlinear emissions from the Si metasurface and power dependence between input power and nonlinear emissions. | Light: Science & Applications

Fig. 4: The nonlinear emissions from the Si metasurface and power dependence between input power and nonlinear emissions.

From: Broadband infrared imaging governed by guided-mode resonance in dielectric metasurfaces

Fig. 4: The nonlinear emissions from the Si metasurface and power dependence between input power and nonlinear emissions.

ac The measured FWM and THG emission spectra from Si metasurface while tuning the signal wavelength (λs) when fixing the pump wavelength λp = 1130 nm. The tuning ranges of the signal wavelength are (a) from 1350 to 1500 nm, (b) from 1500 to 1900 nm, and (c) from 2300 to 4700 nm. d The measured FWM emission spectra from Si metasurface while tuning the pump wavelength (λp) from 1080 nm to 1140 nm. The signal beam wavelength is fixed at λs = 2250 nm. The relation between the frequencies of FWM emissions, signal frequency, and pump frequency can be expressed as: ωFWMp = 2ωpump + ωsignal, ωFWMs = ωpump + 2ωsignal, and ω’FWMp = 2ωpump − ωsignal. The THG emission is generated by the signal beam (ωTHG = 3ωsignal). The color indicates the perceived color of human eye for the wavelength range 380 − 780 nm. e, f The quadratic and linear power dependence of pump beam (a) and signal beam (b) on the two FWM processes (ωFWMp = 2ωpump + ωsignal and ωFWMs = ωpump + 2ωsignal) with experimental data and fitting curves

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