1989
DOI: 10.1016/0370-1573(89)90018-5
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Inversion produced and reversed by adiabatic passage

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Cited by 89 publications
(47 citation statements)
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“…With proper focusing and sufficient infrared power, complete population transfer is achieved by rapid adiabatic passage between the initial and final ro-vibrational levels that are connected by the IR field. 26 Without focusing, the population of the initial and final state connected by the coherent IR field will undergo Rabi-cycling while molecules are traversing the IR beam. The final population in the vibrationally excited state will be a sensitive function of the laser intensity, the transit time, and the transition dipole moment of the ro-vibrational transition.…”
mentioning
confidence: 99%
“…With proper focusing and sufficient infrared power, complete population transfer is achieved by rapid adiabatic passage between the initial and final ro-vibrational levels that are connected by the IR field. 26 Without focusing, the population of the initial and final state connected by the coherent IR field will undergo Rabi-cycling while molecules are traversing the IR beam. The final population in the vibrationally excited state will be a sensitive function of the laser intensity, the transit time, and the transition dipole moment of the ro-vibrational transition.…”
mentioning
confidence: 99%
“…By sweeping the frequency of the excitation field across the molecular resonance it is possible to achieve a level crossing for a two level system in the presence of a resonant electromagnetic field. 12 If the frequency sweep is sufficiently slow, adiabatic following occurs resulting in complete population transfer from the ground to the excited state. [10][11][12] The creation of this population inversion is relatively insensitive to precise experimental conditions including the velocity of the molecules, changes in laser intensity and the different transition strengths corresponding to degenerate m sublevels in a given J level, making this a widely applicable method for obtaining complete population transfer.…”
Section: Rapid Adiabatic Passagementioning
confidence: 99%
“…12,14 First, the frequency sweep rate has to be sufficiently slow to ensure an adiabatic following to transfer the population from the ground state to the excited state. At the same time, the total sweep amplitude given by the product of the sweep rate and transit time must be larger than the Rabi frequency to ensure that the molecules experience a frequency sweep while passing through the laser beam that starts and ends out of resonance.…”
Section: Rapid Adiabatic Passagementioning
confidence: 99%
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