1997
DOI: 10.1080/095003497152636
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Autler-Townes microscopy on a single atom

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Cited by 31 publications
(41 citation statements)
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“…These examples involve laser cooling [1], Bose-Einstein condensation [2], and atom lithography [3], and measurement of the center-of-mass wave function of moving atoms [4]. Earlier schemes for the localization include the measurement of the phase shift of either the standing wave [5][6][7] or of the atomic dipole [8] due to the interaction of the atom with the standing wave field, the entanglement between the atom's position and its internal states [9], and resonance imaging methods [10,11].More recently, Zubairy and co-workers proposed a scheme based on Autler-Townes spontaneous spectrum [12,13]. In this scheme a three-level atom is used, in which either of two levels that are involved in spontaneous emission is coupled to the auxiliary level by a classical standing field.…”
mentioning
confidence: 99%
“…These examples involve laser cooling [1], Bose-Einstein condensation [2], and atom lithography [3], and measurement of the center-of-mass wave function of moving atoms [4]. Earlier schemes for the localization include the measurement of the phase shift of either the standing wave [5][6][7] or of the atomic dipole [8] due to the interaction of the atom with the standing wave field, the entanglement between the atom's position and its internal states [9], and resonance imaging methods [10,11].More recently, Zubairy and co-workers proposed a scheme based on Autler-Townes spontaneous spectrum [12,13]. In this scheme a three-level atom is used, in which either of two levels that are involved in spontaneous emission is coupled to the auxiliary level by a classical standing field.…”
mentioning
confidence: 99%
“…Zubairy and coworkers have discussed atom localization using resonance fluorescence and phase and amplitude control of the absorption spectrum [14][15][16], and Agarwal and Kapale presented a scheme [17] based on coherent population trapping (CPT). Also, one-dimensional (1D) atom localization can be realized via dual measurement of the field and the atomic internal state [18], double-dark resonance effects [19], phase and amplitude control of the driving field [20,21], coherent manipulation of the Raman gain process [22], or spontaneous emission [23,24]. Recently, atom localization has been demonstrated in a proof-of-principle experiment using the technique of electromagnetically induced transparency (EIT) [25].…”
Section: Introductionmentioning
confidence: 99%
“…Several simple localization schemes have been proposed using such as the resonance fluorescence in a two-level system, the measurement of Autler-Townes split spontaneous emission in a three-level system, and a three-level -type atom interacting with a classical standing-wave field and a weak probe field [4][5][6]. Furthermore, one-dimensional (1D) atom localization can be achieved in Raman gain atoms [7], and coherent population trapping [8][9][10].…”
Section: Introductionmentioning
confidence: 99%