Abstract
In this work we suggest a way of describing the Ramsey resonance for arbitrary saturation and arbitrary transverse laser field shape, which takes into account the first order term correction to resonance approximation (zero pulse width) of the order of a/ L ( a is the width of the laser beam, L is a distance between laser beams). It permits to take correctly into account the transverse velocity distribution and real (Gaussian) shape of laser fields. An additional rather interesting phenomenon consists in non-trivial performance of the recoil effect in case of the linear optical Ramsey resonance (in two standing waves separated by λ/2 grating), where we have a few (more than 2) recoil components of the same shape but with different intensities.
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