In a ring-BEC cavity, atomic circulation splits the transparency windows and makes the transmitted-probe Goos-Hanchen shift grow with control power, with a maximum at the red sideband.
Exactly at the red sideband, ˜∆/Ωm = −1, these flanks are sym- metric and maximally steep, so the GHS rises from 0 to a much larger value, ≈ 1.0 × 10−4
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Goos-Hanchen Shift with a rotating atomic superfluid in a ring
In a ring-BEC cavity, atomic circulation splits the transparency windows and makes the transmitted-probe Goos-Hanchen shift grow with control power, with a maximum at the red sideband.