1986
DOI: 10.1103/physrevlett.57.1699
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Observation of Quantum Jumps in a Single Atom

Abstract: Dehmelt had proposed this optical double-resonance scheme (terming it electron shelving) as an amplification mechanism to detect a weak transition in singleatom spectroscopy. 5 This technique has been used for several years in high-resolution spectroscopic studies of samples of many laser-cooled ions, achieving quantum amplifications of 10 and higher. In 1981, electron-shelving amplification was used to perform optical-optical double resonance in a single, lasercooled, trapped ion. While the signal-to-noise r… Show more

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Cited by 680 publications
(350 citation statements)
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“…Then, by monitoring fluorescence at 397 nm under laser excitation, we detect whether a transition to the non-fluorescing state D 5/2 occurred. The scheme allows one to discriminate between the internal states of the ion with an efficiency close to 100% [18][19][20]. In our experiment,the discrimination effiency is approximately 99.8%, limited by the lifetime of the metastable state [21].…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…Then, by monitoring fluorescence at 397 nm under laser excitation, we detect whether a transition to the non-fluorescing state D 5/2 occurred. The scheme allows one to discriminate between the internal states of the ion with an efficiency close to 100% [18][19][20]. In our experiment,the discrimination effiency is approximately 99.8%, limited by the lifetime of the metastable state [21].…”
Section: Methodsmentioning
confidence: 99%
“…Our calculations lead to quantitative statements of the precision of the operations, taking into account the complete Hamiltonian including all the vibrational states and the off-resonant coupling terms. These statements are given in equations (17), (18) for the Monroe et al "magic Lamb Dicke parameter" gate, and in equations (19), (20) for the Cirac-Zoller swap gate. If we set a limit of a fixed number of laser wavelengths for the spacing of the ions in a linear trap, then we arrive at a gate time per ion, for the swap gate, which depends only on the precision and the choice of ion and transition.…”
Section: B Sideband Excitationmentioning
confidence: 99%
“…In many modern experiments, an information is continuously extracted from the system's environment and its wave function follows a random trajectory exhibiting explicit quantum jumps [21,22,23]. The statistics of these jumps is reproduced by a Monte Carlo simulation involving an environment with as many states as the number of possible exclusive measurements outcomes.…”
Section: Monte Carlo Trajectoriesmentioning
confidence: 99%
“…The off-diagonal elements describe atomic coherences. The 10 -and ρ 20 -terms oscillate at the respective driving field frequency and the 21 oscillate with the frequency differences of the two light fields. So, we can define the slowly varying amplitudes of the off-diagonal density matrix elementsρ 1020 , andρ 21 through the relations…”
Section: Modelmentioning
confidence: 99%
“…Using this theoretical approximation, interesting phenomena have been predicted and then observed, such as the resonance fluorescence spectrum [3,4], photon antibunching [5][6][7], sub-Poissonian photon statistics [8,9], squeezing [10][11][12], photon echoes [13], and self-induced transparency [14][15][16]. With multilevel treatments of atoms, other phenomena are explained, such as quantum jumps [17][18][19][20] and laser cooling and trapping [21,22].…”
Section: Introductionmentioning
confidence: 99%