Two-photon absorption and stimulated emission in poly-crystalline Zinc Selenide with femtosecond laser excitation

The optical nonlinearity in polycrystalline zinc selenide (ZnSe), excited with 775 nm, 1 kHz femtosecond laser pulses was investigated via the nonlinear transmission with material thickness and the Z scan technique. The measured two photon absorption coefficient beta was intensity dependent, inferring that reverse saturated absorption (RSA) is also relevant during high intensity excitation in ZnSe. At low peak intensity I < 5 GW cm(-2), we find beta = 3.5 cm GW(-1) at 775 nm. The spectral properties of the broad blueish two-photon induced fluorescence (460 nm-500 nm) was studied, displaying self-absorption near the band edge while the upper state lifetime was measured to be tau(e) similar to 3.3 ns. Stimulated emission was observed when pumping a 0.5 mm thick polycrystalline ZnSe sample within an optical cavity, confirmed by significant line narrowing from Delta lambda = 11 nm (cavity blocked) to Delta lambda = 2.8 nm at peak wavelength lambda(p) = 475 nm while the upper state life-time also decreased. These results suggest that with more optimum pumping conditions and crystal cooling, polycrystalline ZnSe might reach lasing threshold via two-photon pumping at lambda = 775 nm.

Automated summary

By investigating the optical nonlinearity in polycrystalline zinc selenide (ZnSe) using femtosecond laser pulses, it was found that reverse saturated absorption (RSA) occurs during high intensity excitation in ZnSe. The two-photon absorption coefficient beta was found to be intensity dependent. Stimulated emission was observed when pumping a polycrystalline ZnSe sample within an optical cavity, indicating the possibility of reaching lasing threshold via two-photon pumping.