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Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE

Laser-induced dispersion optical filter at 532 nm

Yundong Zhang, Xutao Sun, Zhusong He

Published Mar 17, 2005• 0 citations
Publisher

Abstract

In this paper, the semi-classical theory was utilized to theoretically analyze K-532nm Laser-induced dispersion optical filter (LIDOF), and theoretical model was given. By solving the density matrix equations, the system induced polarizability was gained, and eventually the transmission spectra were gained by theoretical calculation.
DOI
10.1117/12.584250

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The potassium tunable excited state Stark anomalous dispersion optical filter (SADOF) at 532.33 nm was studied theoretically and experimentally. The theoretical model of SADOF was deduced and the transmission of SADOF was calculated. The transmission spectra of potassium SADOF in different electric fields were measured and the experimental frequency shifts of SADOF versus the strengths of the electric field were given. Furthermore, the comparison between the experimental results with the corresponding theoretically simulated results has been completed. The comparison shows that our experimental results agree with the theoretically simulated results in general.
A narrow-band, gate-able matched optical filter with large extinction ratio and high transmission is required for ocean lidar applications at wavelength of 532 nm. Two types of filters, the induced dichroism excited-state atomic line (IDEAL) and excited state anomalous Faraday dispersion optical filter (ESFADOF), are studied. They are operating on the 4P1/2 to 8S1/2 excited states transition line of potassium vapor and a narrow band at 532 nm. The measured critical features of the IDEAL filter are: 1.3 GHz (i.e..01A) narrow pass band, approximately 45% peak transmission, high extinction coefficient in the order of 10-5, very fast rise time (<3ns) and a 15 ns decay time determined by resonant enhanced two photon transition. The physical mechanism of the IDEAL filter operation is explained in terms of resonant enhanced two photon transition. Good agreement between experiment and the derived theoretical model is achieved. The pertinent features of the excited (ESFADOF) filter were measured to be: approximately 15% peak transmission, high extinction coefficient in the order of 10-5, very fast rise time (<3ns), and a decay time in the tens of microsecond range governed by resonant photon trapping. The physical processes contributing to the ESFADOF filter action are resonant photon trapping and Faraday anomalous dispersion. The experimental results confirmed theoretical predictions. The applications of these filters are discussed in terms of improving the lidar system performance. Specifically, the narrow bandwidth of these filters eliminates the background noise caused by stray solar radiation and thereby enhances the dynamic range of the lidar system. Furthermore the fast efficient gating of the filters minimizes reflection from the ocean surface, which is several orders of magnitude higher than the return signal from underwater targets.
In this paper the calculations for a K Faraday filter at 532.33 nm that can be used to detect the practical and important frequency-doubled Nd:YAG laser are presented and discussed. Our model predicts a peak transmission of 50% and an equivalent bandwidth of 4 GHz for the filter operating on the transition in potassium. The theoretical results show the transmission characteristics of the filter are relatively insensitive to the laser pump power and magnetic strength. The laser pump powers required range from 0.8 to .
We present a model of an atomic filter based on laser-induced optical anisotropy that is achieved by the combination of a double selective pump. Most of these kinds of atomic optical filters reported previously adopt only one pump to make the atoms populate on particular sublevels. In this paper, another pump is added to the filter system to make sure all the atoms are in the pump–probe cycle. The feasibility of the re-pump is analyzed by employing the rate equation, and the contribution of the re-pump to the filter is discussed under various conditions. Simulation results show that the re-pump can not only enhance the transmission of the filter, but also vary the transmission spectrum peak wavelength.