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Harris, S.E.1
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71949117334
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note
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C is the driving field Rabi frequency, is the upper state lifetime.
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3
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71949130959
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note
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We note that no room-temperature, weakly driven (ultraslow-wave) EIT experiment using N 23 a or R 85 b can be found in literature. Even for R 87 b (about 800 MHz hyperfine splitting) the loss of the probe field using common EIT beam scheme is still significant at elevated temperature due to the presence of multiple channels.
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9
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0034287835
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High contrast ramsey fringes with coherent-population-Trapping pulses in a double lambda atomic system
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18344377748
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17444407520
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On the dynamic range of optical delay lines based on coherent atomic media
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Matsko, A.B.1
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17
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19644401075
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0031-9007,. 10.1103/PhysRevLett.93.160802
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39749098469
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g-1 atomic transitions
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R. Meshulam, T. Zigdon, A. D. Wilson-Gordon, and H. Friedmann, Opt. Lett. 0146-9592 32, 2318 (2007). 10.1364/OL.32.002318 (Pubitemid 351305749)
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Meshulam, R.1
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19
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71949113947
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note
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Indeed, state preparation schemes employed in these studies all result in the media being in a ground state where multiple -channels and near-by states contributions cannot be avoided.
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20
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71949104478
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note
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F =+3 is a "dark" state which does not contribute to the absorption.
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22
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71949106005
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note
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The beams have a crossing angle of ≈2.0 mrad in the atomic medium. The popular EIT scheme [Fig.] could not yield any detectable signal under our weak driving conditions even with zero crossing angle.
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23
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85037213080
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note
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By measuring delay time one obtains group velocity. Using group velocity expression one obtains density, see L. Deng, E. W. Hagley, M. Kozuma, and M. G. Payne, Phys. Rev. A 1050-2947 65, 051805 (R) (2002). 10.1103/PhysRevA.65.051805
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