2010
DOI: 10.1103/physreva.82.053816
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Superradiance from a cylindrically shaped cloud ofNtwo-level atoms

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Cited by 6 publications
(10 citation statements)
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“…An interesting situation arises in the nearly inverted case when the two strongest modes have nearly the same Re (λ); then, the beats between them [16], observable on the fast time scale O (1/C), continue for a time much longer than λ D . A similar phenomenon occurs in the weakly excited case, when the two weakest dominant modes nearly are degenerate in Re (λ).…”
Section: Discussionmentioning
confidence: 99%
“…An interesting situation arises in the nearly inverted case when the two strongest modes have nearly the same Re (λ); then, the beats between them [16], observable on the fast time scale O (1/C), continue for a time much longer than λ D . A similar phenomenon occurs in the weakly excited case, when the two weakest dominant modes nearly are degenerate in Re (λ).…”
Section: Discussionmentioning
confidence: 99%
“…(4.3) and (4.5) that in the vector model cross polarization (P z from initialP x , orP x from initial P z ) does not occur in leading order in elapsed time t. At later times we expect this to remain true because of reflection symmetry in the y-z plane, even though individual eigenmodes no longer separate into TM and TE when k 2 > 0. Likewise, if the initial phase factor is not exp(ikz)but exp(ikx) as in [5,24,28], cross polarization should remain zero at all times by reflection symmetry in the x-z plane. But cross polarization may be expected at later times when the initial phase has both an x and a z dependence.…”
Section: Discussionmentioning
confidence: 99%
“…[We note that in [5,24,28] the phase factor is transverse, exp(ikx), rather than exp(ikz). Hence the only overlap between those and the present paper is in the case of k = 0.…”
Section: Initial Cooperative Decay Rate and Initial Cooperative Lmentioning
confidence: 99%
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