Effects of Neighboring Transitions on Electromagnetically Induced Absorption and Transparency in 85rb Atoms ㅠBased on Linear Parallel Polarizations of Coupling and Probe Beams
SSRN Electronic Journal
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Example: if you select the 1-year option for an article published in 2019 and a metric category shows 90%, that means that the article or review is performing better than 90% of the other articles/reviews published in that journal in 2019. If you select the 3-year option for the same article published in 2019 and the metric category shows 90%, that means that the article or review is performing better than 90% of the other articles/reviews published in that journal in 2019, 2018 and 2017.
Citation Benchmarking is provided by Scopus and SciVal and is different from the metrics context provided by PlumX Metrics.
Article Description
The effects of neighboring transitions through Doppler broadening on the electromagnetically induced absorption (EIA) and electromagnetically induced transparency (EIT) of the degenerate two-level system (DTLS) in $^{85}$Rb atoms with respect to the linear parallel polarization configuration of coupling and probe lasers have been investigated. The calculated coherent absorption profiles with and without neighboring effects have been compared to elucidate the neighboring effects between the DTLS and nearby states for the conversion between EIA and EIT. Even in the case of the closed system, i.e., $F_g=3 \rightarrow F_e=4$ of $^{85}$Rb, for the first time, EIT instead of EIA has been observed owing to the neighboring effect of dominant $F_g=3 \rightarrow F_e=3$ on the linear parallel polarization configuration case of $^{85}$Rb in the low power regime. All the transitions ($F_g=3 \rightarrow F_e$=2 and 3 and $F_g=2 \rightarrow F_e$=1, 2, and 3) of linear parallel polarization cases exhibit EIT owing to dominant neighboring EIT in the DTLS. In each polarization scheme, the observed spectral trends of the transitions are similar owing to the neighboring effect. The EIT spectral trends with the neighboring effect of $F_g=2 \rightarrow F_e$=1, 2, and 3 are governed by the openness of pure DTLS calculation.
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