NatureSir Norman Lockyer Macmillan Journals Limited, 2007 |
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Stran 889
... photon counting Christine Guerlin1 , Julien Bernu1 , Samuel Deléglise1 , Clément Sayrin1 , Sébastien Gleyzes1 , Stefan Kuhr1 † , Michel Brune1 , Jean - Michel Raimond1 & Serge Haroche 1,2 The irreversible evolution of a microscopic ...
... photon counting Christine Guerlin1 , Julien Bernu1 , Samuel Deléglise1 , Clément Sayrin1 , Sébastien Gleyzes1 , Stefan Kuhr1 † , Michel Brune1 , Jean - Michel Raimond1 & Serge Haroche 1,2 The irreversible evolution of a microscopic ...
Stran 890
... photon number distri- bution , Po ( n ) = | cn | 2 , is poissonian with an average photon number no = | x | 2 and a spread An = no . If we could determine the final atom state , the clock's delay - and hence n - would be read in a ...
... photon number distri- bution , Po ( n ) = | cn | 2 , is poissonian with an average photon number no = | x | 2 and a spread An = no . If we could determine the final atom state , the clock's delay - and hence n - would be read in a ...
Stran 891
... photon number distribution and average photon number , no = 3.82 ± 0.04 , are inferred from the experimental data ( see below ) . Our single - photon - sensitive spin- clocks are circular Rydberg atoms of rubidium . They cross C ...
... photon number distribution and average photon number , no = 3.82 ± 0.04 , are inferred from the experimental data ( see below ) . Our single - photon - sensitive spin- clocks are circular Rydberg atoms of rubidium . They cross C ...
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