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Designer Optical Control of Two-body Interactions in Ultracold Gases.

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Figure

Figure 1.1 (a) The optical field arrangement for creating an interaction “sandwich." BothAtom transfer is suppressed in regions of resonant interactions-central region of the atomicThe outer regions of the atomic cloud illuminated ν1 andν2 beams illuminate
Figure 1.3 Magnetically tuning interactions near a Feshbach resonance. The hyperfine couplingbetween the triplet continuum |T,k〉 (open channel) and the singlet bound state |g1〉 cause mag-netic Feshbach resonance
Figure 1.5 Energy level scheme for optical Feshbach Resonance. Colliding atoms reside in thetriplet potential
Figure 1.6 Energy level scheme for two-field optical Feshbach Resonance. The triplet continuum|T,k〉 (open channel) is coupled with the triplet excited bound state |e 〉 (open channel) throughan optical beam of frequency ν1 and Rabi frequency Ω1
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