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Optics Communications

Electromagnetically induced absorption due to transfer of coherence and coherence population oscillation for the Fg=3→Fe=4 transition in 85Rb atoms

Hafeez Ur Rehman, Muhammad Qureshi Mohsin, Heung‐Ryoul Noh, Jin‐Tae Kim

Published Jul 14, 2016• 11 citations
Publisher
DOI
10.1016/j.optcom.2016.06.063

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Line Shapes in Electromagnetically Induced Absorption in 85 Rb atoms: Calculation and Experiment

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Abstract Optical Bloch equations with and without neighboring hyperfine states near the degenerate two-level system (DTLS) in the challenging case of 85Rb D2 transition that involves the Doppler broadening effect are solved herein. The calculated spectra agree well with the experimental results obtained using the coupling-probe scheme with orthogonal linear polarizations of the coupling and probe fields. The mechanisms of electromagnetically induced absorption (electromagnetically induced transparency) for the open Fg = 3 → Fe = 2 and 3 transitions (open Fg = 2 → Fe = 2 and 3 transitions) are clearly determined to be the effect of the strong closed Fg = 3 → Fe = 4 transition line (strong closed Fg = 2 → Fe = 1 transition line) based on the comparisons of the calculated absorption profiles of a DTLS without neighboring states and those of all levels with neighboring states depending on the coupling and probe power ratios. The crucial factors established based on comparisons of the calculated absorption profiles of DTLS with and without neighboring states, which enhance or reduce coherence effects and result in transformation between electromagnetically induced absorption and electromagnetically induced transparency, are the power ratios between coupling and probe beams, openness of the excited state, and effects of the neighboring states due to the Doppler broadening in a real atomic system.