A theory of the magnetic grating free induction decay (MGFID) and the
magnetic grating echo (MGE) is presented. In the MGFID, a pulse of cou
nterpropagating waves creates a spatially modulated coherence between
magnetic sublevels of the same or different ground-state hyperfine lev
els. This coherence is probed at some later time by a traveling-wave p
ulse. In the MGE, a second pulse of counterpropaging fields is applied
at time T following the initial pulse. An echo or rephasing of the gr
ound-state coherence appears at a time T following the second pulse an
d can be probed by a traveling-wave pulse. The MGE can monitor ground-
state transients for time scales equal to some effective ground-state
lifetime; as such, it can be used effectively as an interferometric pr
obe of velocity changes in cold as well as thermal atoms. The calculat
ions are carried out in a perturbative limit in the amplitudes of the
applied fields, but fields of arbitrary polarization and atoms having
arbitrary manifolds of fine and hyperfine levels are considered. It is
assumed that the pulses vary slowly on a time scale compared with min
[atom-field detuning]-1, (excited-state decay rate)-1]; this allows fo
r spectral resolution of the scattered probe field on a frequency scal
e equal to the excited-state decay rate, independent of the Doppler wi
dths associated with the optical transitions.