Titlebook: Coherent Control of Four-Wave Mixing; Yanpeng Zhang,Zhiqiang Nie,Min Xiao Book 2011 The Editor(s) (if applicable) and The Author(s), under

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Michael A. Anikeeff,Glenn R. Mueller. The relative intensities and polarization characteristics of fourwave mixing (FWM) signals in different laser polarization configurations and different level systems are experimentally investigated and compared. Also the results are theoretically explained by different transition path combinations

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Henriette Herwig,Raimund Poussetweak probe and FWM beams with coupling/pumping beams, spatial optical switching and routing of one beam or multiple optical beams can be achieved. Such controllable spatial beam displacement and splitting effects are illustrated in two- and three-level atomic system.

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dura-mater

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Antecedent

Ultrafast Polarization Beats of Four-Wave Mixing Processes,ignals due to the unbalanced dispersion effects between two arms of interferometer and Doppler-width do not affect the overall accuracy in case using FLPB to measure the energy-level difference between two states, which are dipolar forbidden from the ground state. On the other hand, a Doppler-free p

Initial

Multi-Dressing Four-Wave Mixing Processes in Confined and Non-confined Atomic System,cal processes. Efficient and co-existing FWM and SWM signals are produced in the same EIT window via atomic coherence. On the other hand, we present the interplay between FWM, SWM, and eight-wave mixing (EWM) resulting from atomic coherence in multi-level atomic systems. FWM with three kinds of dual

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光亮

Multi-Wave Mixing Processes in Multi-level Atomic System,. The relative intensities and polarization characteristics of fourwave mixing (FWM) signals in different laser polarization configurations and different level systems are experimentally investigated and compared. Also the results are theoretically explained by different transition path combinations

Harridan

Controlling Spatial Shift and Spltting of Four-Wave Mixing,weak probe and FWM beams with coupling/pumping beams, spatial optical switching and routing of one beam or multiple optical beams can be achieved. Such controllable spatial beam displacement and splitting effects are illustrated in two- and three-level atomic system.