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18544363800
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note
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To a first approximation the population of the excited and the bright state [the one that is orthogonal to |D(p)〉] can be neglected.
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14
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18544370787
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note
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2, one can simply treat the two cases separately and add the two inhomogeneous solutions afterward.
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15
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18544389581
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note
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s, have been neglected.
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16
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18544365577
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note
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Maxwell's equations impose boundary conditions on the electric and magnetic fields E and B at z=0 and z=a which result in a reflection of the fields at these boundaries. In the paraxial approximation, this reflection is negligible and the boundary conditions for the electric field reduce to Eq. (26).
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17
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84856130823
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D. A. Steck, http://steck.us/alkalidata/
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Steck, D.A.1
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19
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18544388587
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note
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1,2 has not been taken into account in the calculations for the density operator. This amounts to omitting the changed group velocity of the pulse within the gas.
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20
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84994613817
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Cambridge University Press, Cambridge, U.K.
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M. O. Scully and M. S. Zubairy, Quantum Optics (Cambridge University Press, Cambridge, U.K., 1995).
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18544384915
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F. Vewinger and F. Zimmer, e-print quant-ph/0501164
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F. Vewinger and F. Zimmer, e-print quant-ph/0501164.
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