2017
DOI: 10.1063/1.4976972
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Laser controlled charge-transfer reaction at low temperatures

Abstract: We study the low-temperature charge transfer reaction between a neutral atom and an ion under the influence of near-resonant laser light. By setting up a multi-channel model with field-dressed states, we demonstrate that the reaction rate coefficient can be enhanced by several orders of magnitude with laser intensities of 10 W/cm or larger. In addition, depending on laser frequency, one can induce a significant enhancement or suppression of the charge-exchange rate coefficient. For our intensities, multi-photo… Show more

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Cited by 9 publications
(8 citation statements)
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“…where a laser field can be employed to directly stimulate the transition to the ground electronic state [34,37] or to excite the ion-atom system to higher excited states [36].…”
Section: Vibrational Levelsmentioning
confidence: 99%
See 1 more Smart Citation
“…where a laser field can be employed to directly stimulate the transition to the ground electronic state [34,37] or to excite the ion-atom system to higher excited states [36].…”
Section: Vibrational Levelsmentioning
confidence: 99%
“…In cold ion-atom mixtures, diatomic molecular ions can be produced via collision-induced charge-transfer radiative association or light-induced photoassociation [10,[33][34][35][36][37]. The radiative association is predicted to dominate charge-transfer processes in most of the mixtures of alkaline-earth-metal ions and alkali-metal atoms.…”
Section: Introductionmentioning
confidence: 99%
“…Crucially, for our system both contributions to the long-range potential are diagonal in this body-fixed basis [31]. The matrix elements of C 3 , expressed in two equivalent ways, are…”
Section: Discussionmentioning
confidence: 99%
“…The MOT and catalyst lasers couple the initial photondressed Ca(4s 2 1 S 0 ) + Yb + (6s 2 S 1/2 ) + ω MOT,C and excited Ca(4s4p 1 P 1 ) + Yb + (6s 2 S 1/2 ) channels. Using a dressed-state approach [31] and in the IOSA we find coupling matrix element −(1/ √ 3) d I/(2c 0 ) in SI units between the initial Ω = ±1/2 channel and the attractive Ω = ±1/2 excited channel with the same J. Here, I is the MOT or catalyst laser intensity, 0 is the electric constant, dipole moment d = S/3 = 2.85ea 0 , using line strength S of the 4s 2 1 S 0 to 4s4p 1 P 1 transition of Ca [32], and e is the electron charge.…”
Section: Laser-induced Couplingmentioning
confidence: 99%
“…The average values can be calculated analytically using an operator method [13,14]. If the axis displacement is zero (  = 0), then we have:…”
mentioning
confidence: 99%