2011
DOI: 10.1007/s00340-011-4502-7
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Resonance-enhanced isotope-selective photoionization of YbI for ion trap loading

Abstract: Neutral ytterbium (YbI) and singly ionized ytterbium (YbII) is widely used in experiments in quantum optics, metrology and quantum information science. We report on the investigation of isotope selective two-photon-ionization of YbI that allows for efficient loading of ion traps with YbII. Results are presented on two-colour (399 nm and 369 nm) and single-colour (399 nm) photoionization and their efficiency is compared to electron impact ionization. Nearly deterministic loading of a desired number of YbII ions… Show more

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Cited by 21 publications
(24 citation statements)
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“…These close transitions result in overlapping of the fluorescence spots and cannot be resolved by the spot method. The isotope-shift data presented in Table I for the Yb 1 S 0 ↔ 1 P 1 transitions are in very good agreement with previously published work [27,[29][30][31].…”
Section: Fluorescence Spot Techniquesupporting
confidence: 80%
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“…These close transitions result in overlapping of the fluorescence spots and cannot be resolved by the spot method. The isotope-shift data presented in Table I for the Yb 1 S 0 ↔ 1 P 1 transitions are in very good agreement with previously published work [27,[29][30][31].…”
Section: Fluorescence Spot Techniquesupporting
confidence: 80%
“…To ionize an Yb atom a 399-nm photon is required to drive the 1 S 0 ↔ 1 P 1 transition where a further 369-nm photon excites an electron past the continuum [22,27]. In the ion-trapping experiment the atomic oven and the 399-nm laser made an angle of 63…”
Section: Doppler-shifted Frequency Measurementsmentioning
confidence: 99%
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“…We create collimated beams of neutral ytterbium atoms by ohmic heating of a small sample of granular ytterbium in a miniature tube-shaped steel oven (for design, modeling, and operation, see [45,48]). Two identical ovens, mounted to the oven holder (see Fig.…”
Section: Loading and Trappingmentioning
confidence: 99%
“…Additional beneficial effects, like strongly reduced static charging of dielectrics [9], lower motional heating rates of the ions after loading due to the suppression of patch potentials [10] and easier loading of surface-electrode traps with a substantially reduced trap depth [11] is of great advantage in the laboratories. Loading of Paul traps by narrowband cw photoionization [12] has been achieved by several groups on a growing number of atomic species (Ba [13,14], Mg [15], Ca [9,16,17], Yb [18], Sr [19,20], In [21] etc.). Several of these schemes have been applied to photoionization loading techniques that substitute the resistively heated atomic oven as source of neutral atoms.…”
mentioning
confidence: 99%