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85037180399
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An analysis shows that after taking into account the first non-negligible correction to the Raman-Nath approximation, the atomic wave function just after the pulse has to be multiplied by a factor (Formula presented) Near the focal plane this factor can only lead to small changes of the atom wave function if (Formula presented)
-
An analysis shows that after taking into account the first non-negligible correction to the Raman-Nath approximation, the atomic wave function just after the pulse has to be multiplied by a factor (Formula presented) Near the focal plane this factor can only lead to small changes of the atom wave function if (Formula presented)
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37
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0003498504
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85037180005
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The analysis of Ref
-
The analysis of Ref. 28 can be generalized to an open system, where the excited state decays to many ground-state sublevels including (Formula presented)
-
-
-
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39
-
-
85037230591
-
-
Note that by fixing (Formula presented) we are not actually using the time (Formula presented) where the function (Formula presented) is a maximum when evaluating (Formula presented) The correction is small even for the largest value of (Formula presented) plotted
-
Note that by fixing (Formula presented) we are not actually using the time (Formula presented) where the function (Formula presented) is a maximum when evaluating (Formula presented) The correction is small even for the largest value of (Formula presented) plotted.
-
-
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40
-
-
85037243033
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See, for example, J. Schmiedmayer, M.S. Chapman, C.R. Ekstrom, T.D. Hammond, D.A. Kokorowski, A. Lenef, R.A. Rubinstein, E.T. Smith, and D.E. Pritchard, in Atom Interferometry (Ref. 17).
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Atom Interferometry
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Hammond, T.D.4
Kokorowski, D.A.5
Lenef, A.6
Rubinstein, R.A.7
Smith, E.T.8
Pritchard, D.E.9
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