By Benjamin Bederson
Proven in 1965, Advances in Atomic, Molecular, and Optical Physics keeps its culture of excellence with quantity 34. the newest quantity comprises 9 reports of subject matters concerning the functions of atomic and molecular physics to atmospheric physics and astrophysics.
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Extra resources for Advances In Atomic, Molecular, and Optical Physics, Vol. 34
E. Observable Effects of “Empty Waves” . . . . . VIII. The Single-Photon Tunneling Time . . . . . . A . An Application of EPR States: Dispersion Cancellation . B. Single-Photon Propagation Time Measurements . . C. Tunneling Time in a Multilayer Dielectric Mirror . . D . Interpretation of the Tunneling Time . . . . . 35 . . . . . . . 36 38 38 39 . . . . . . . . . . . 41 42 . . . . . . . 40 . . . . 42 43 45 46 . . . . . . . . . . . . . .
For typical atomic beam parameters, the Doppler dephasing term dominates, leading to a smearing out of the Ramsey fringes. For fringes to be observed the Doppler dephasing term where Au, is the transverse velocity spread of the beam. In a wave packet picture, this condition is equivalent to the requirement that the width of the wave packet Az h/rnAu, must be larger than the spatial splitting between the paths u,x1,2/u,. Hence, the fact that interference is only observed if there is spatial overlap of the split beams is identical to the requirement that all plane wave components experience approximately the same phase shift.
The potential for precision measurement of gravity and inertial effects has been demonstrated using an atomic fountain interferometer. In addition, it has been shown that atom interferometry has considerable potential for precision measurement of atomic properties and fundamental constants. These are just the first experiments in what is likely to be widespread application of atom interferometry in diverse areas of science. For a practical measuring device, miniaturization is an important consideration.
Advances In Atomic, Molecular, and Optical Physics, Vol. 34 by Benjamin Bederson