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Deflection of atomic beams by resonance radiation using stimulated emission
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2.The frequency loss of the returning photon is very small. In principle it could be restored by pushing one mirror mechanically. This is a very interesting but impractical scheme of transmitting linear momentum at distance by a laser beam.
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4.Ashkin proposed a recirculation scheme for photons not scattered by the atoms. An atomic beam many absorption lengths deep, and a strong light beam which “burns through” it, could also be used. If the light is coherent, transient phenomena occur on a time scale shorter than the radiative lifetime. In particular, superradiance may become important in a pencil‐like geometry.
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6.Much of our discussion follows the notation of E. Courtens, in Laser Hand book, edited by F. F. Arecchi and E. O. Schultz‐DuBois (North Holland, Amsterdam, 1972), p. 1261.
7.In a more optimal and practical pulse, the amplitude has a Gaussian shape, while the frequency follows an error function.
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