Nature, Volume 428Sir Norman Lockyer Macmillan Journals Limited, 2004 |
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Página 50
... probe laser blue detuned from the atomic resonance . For strong atom - cavity coupling , even one atom can significantly influence the optical path length between the cavity mirrors . Consequently , the intracavity intensity is strongly ...
... probe laser blue detuned from the atomic resonance . For strong atom - cavity coupling , even one atom can significantly influence the optical path length between the cavity mirrors . Consequently , the intracavity intensity is strongly ...
Página 51
... probe laser at 780.2 nm is used to observe and cool the atom . A strong , far - detuned dipole laser at 785.3 nm serves to trap the atom . The detunings of the probe laser with respect to the cavity , △ = 0 , and the atom , 4 / 2π = 35 ...
... probe laser at 780.2 nm is used to observe and cool the atom . A strong , far - detuned dipole laser at 785.3 nm serves to trap the atom . The detunings of the probe laser with respect to the cavity , △ = 0 , and the atom , 4 / 2π = 35 ...
Página 52
... probe powers below 0.1 pW more than 90 % of the atoms leave the cavity by hitting a mirror , whereas for higher probe powers 90 % of the atoms leave radially . We emphasize that , in contrast to Doppler cooling , cavity cooling extends ...
... probe powers below 0.1 pW more than 90 % of the atoms leave the cavity by hitting a mirror , whereas for higher probe powers 90 % of the atoms leave radially . We emphasize that , in contrast to Doppler cooling , cavity cooling extends ...
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of genetically modified grain | 8 |
Just | 14 |
Medical editors urged to accept ethical code | 17 |
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