2013
DOI: 10.1080/00268976.2013.780107
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Ion-neutral chemistry at ultralow energies: dynamics of reactive collisions between laser-cooled Ca+ ions and Rb atoms in an ion-atom hybrid trap

Abstract: Cold chemical reactions between laser-cooled Ca+ ions and Rb atoms were studied in an ion-atom hybrid trap. Reaction rate constants were determined in the range of collision energies E coll /kB = 20 mK-20 K. The lowest energies were achieved in experiments using single localized Ca + ions. Product branching ratios were studied using resonant-excitation mass spectrometry. The dynamics of the reactive processes in this system (non-radiative and radiative charge transfer as well as radiative association leading t… Show more

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Cited by 70 publications
(165 citation statements)
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“…Other studies concern CaLi [41][42][43], LiBe [44,45]. More recently the electronic structure of the related molecular ions containing one alkali atom and Ca + [46], Sr + [47] or Ba + [48][49][50][51] with various high-level approaches have been published in relation with experiments aiming at creating cold molecular ions in merged cold ion and cold atom traps.…”
Section: Introductionmentioning
confidence: 99%
“…Other studies concern CaLi [41][42][43], LiBe [44,45]. More recently the electronic structure of the related molecular ions containing one alkali atom and Ca + [46], Sr + [47] or Ba + [48][49][50][51] with various high-level approaches have been published in relation with experiments aiming at creating cold molecular ions in merged cold ion and cold atom traps.…”
Section: Introductionmentioning
confidence: 99%
“…Instead, it is preferable to use strings of ions located on the central axis of the ion trap. In this configuration, the micromotion energies are minimised and the ions can be assumed to have negligible kinetic energies compared to the moving atoms [13,27]. However, due to the necessarily small number of ions in this case, collision events are rare and extensive averaging is required.…”
Section: Discussionmentioning
confidence: 99%
“…The first beam was sent through an AOM for shifting the frequency slightly to the red of the Rb (5s) 2 S 1/2 F = 2 → (5p) 2 P 3/2 F = 3 resonance to provide laser radiation for Doppler laser cooling and magneto-optical trapping. The firstorder diffracted output of the AOM was further passed through an electro-optic modulator (EOM) for generating sidebands repumping population on the Rb (5s) 2 S 1/2 F = 1 → (5p) 2 P 3/2 F = 2 transition [13]. The laser beam was subsequently coupled into a PM fibre, transported to the experiment table and split into two components propagating along the y and z axes of the trap, see Fig.…”
Section: Laser Systemmentioning
confidence: 99%
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