2011
DOI: 10.1103/physreva.84.053812
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Optimized coupling of cold atoms into a fiber using a blue-detuned hollow-beam funnel

Abstract: We theoretically investigate the process of coupling cold atoms into the core of a hollow-core photonic-crystal optical fiber using a blue-detuned Laguerre-Gaussian beam. In contrast to the use of a red-detuned Gaussian beam to couple the atoms, the blue-detuned hollow-beam can confine cold atoms to the darkest regions of the beam thereby minimizing shifts in the internal states and making the guide highly robust to heating effects. This single optical beam is used as both a funnel and guide to maximize the nu… Show more

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Cited by 14 publications
(6 citation statements)
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References 40 publications
(47 reference statements)
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“…These results show that the atomic number density distribution is also in our HCPBGF well-represented by Eq. ( 2), i.e., the density is highest on the fiber axis as observed in [27], in contrast to other predictions [14,49], which favored ring-shaped distributions.…”
Section: Light-shift Spectroscopycontrasting
confidence: 73%
“…These results show that the atomic number density distribution is also in our HCPBGF well-represented by Eq. ( 2), i.e., the density is highest on the fiber axis as observed in [27], in contrast to other predictions [14,49], which favored ring-shaped distributions.…”
Section: Light-shift Spectroscopycontrasting
confidence: 73%
“…The atomic coherence time will be limited by the faster of two effects: decoherence induced by interaction between trapped atoms and the optical guide field, or the loss of atoms. Photon scattering in the current experiment limits the atomic coherence time to around 200 µs, although this rate could be much reduced by replacing the attractive guide with a hollow repulsive guide mode [48]. This trap geometry would confine atoms predominantly within the low intensity region, vastly reducing the scattering rate.…”
Section: Performance and Limitationsmentioning
confidence: 92%
“…These techniques, however, do not extend the coherent interaction time with an optically excited state: in this case one requires no collisions with other atoms or the fiber wall. One solution to extend excited state coherence is to reduce the average motion of the atoms, pointing towards laser-cooled atoms as a route to create strong photon-photon interaction mediated by light-atom interactions in waveguide geometries [8,19,35,51,52].…”
Section: Discussionmentioning
confidence: 99%