Fig. 3: Experimental setup and characterizations of the spectra, output power, pump threshold and parametric gain of the χ(2) micro-waveguide with birefringence PM based on a ZGP crystal. | Nature Communications

Fig. 3: Experimental setup and characterizations of the spectra, output power, pump threshold and parametric gain of the χ(2) micro-waveguide with birefringence PM based on a ZGP crystal.

From: Highly efficient octave-spanning long-wavelength infrared generation with a 74% quantum efficiency in a χ(2) waveguide

Fig. 3

a The schematic of the experimental setup for optical parametric generation (OPG) from the χ(2) waveguide. b The pump spectrum centered at 2.4 μm. c The measured OPG spectra from the χ(2) waveguide with different pump peak powers. The generated LWIR idler wave has an octave-spanning spectrum covering 5.4 to 10.3 μm at −20 dB, which is in good agreement with the simulated result in Fig. 1a. The noise floor is marked by a gray dotted line. d The measured OPG output power shown in a linear scale as a function of pump pulse energy and average power. The measured pump threshold energy is ~616 pJ, corresponding to a peak power of 1.9 kW. In addition, When the pump energy is 6.5 nJ corresponding to an average power of 3.25 mW, a LWIR power of 0.72 mW is detected from the χ(2) waveguide, corresponding to a power efficiency of 22% and a quantum efficiency of 74%. Meanwhile, further increasing the pump energy, the output power tends to saturate. Particularly, when the pump pulse energy is larger than 9 nJ, the LWIR output power decreases, due to parametric back conversion. e The OPG output intensity in a logarithm scale at different pump energy. A saturated parametric gain of >58.6 dB/cm calculated from the measured maximum idler power (0.83 mW) and minimum idler power (1.1 nW) is observed at a pump energy of 7.9 nJ, which indicates that a decent parametric gain could be provided by the χ(2) waveguide device. The inset shows the measured beam profile of LWIR OPG from the χ(2) waveguide, which agrees well with the simulated field profile shown in Fig. 1b.

Back to article page