2016
DOI: 10.1364/ol.41.004795
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Non-destructive shadowgraph imaging of ultra-cold atoms

Abstract: An imaging system is presented that is capable of far-detuned non-destructive imaging of a Bose-Einstein condensate with the signal proportional to the second spatial derivative of the density. Whilst demonstrated with application to Rb85, the technique generalizes to other atomic species and is shown to be capable of a signal-to-noise of ∼25 at 1 GHz detuning with 100 in-trap images showing no observable heating or atom loss. The technique is also applied to the observation of individual trajectories of stoch… Show more

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Cited by 33 publications
(37 citation statements)
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“…Firstly, a horizontal absorption beam allows the cloud to be imaged after 20ms of ballistic expansion (a s = 0) in free space to calibrate absolute atom number. A second vertical, far-detuned imaging beam utilizes nondestructive shadowgraph imaging to take in situ images of the condensate [12]. Up to 100 images can be taken in a single run as little as 0.4ms apart with no measurable change in atom number.…”
mentioning
confidence: 99%
“…Firstly, a horizontal absorption beam allows the cloud to be imaged after 20ms of ballistic expansion (a s = 0) in free space to calibrate absolute atom number. A second vertical, far-detuned imaging beam utilizes nondestructive shadowgraph imaging to take in situ images of the condensate [12]. Up to 100 images can be taken in a single run as little as 0.4ms apart with no measurable change in atom number.…”
mentioning
confidence: 99%
“…However, during the process the atoms are released from the confining potential and undergo a strong resonant interaction with the probe laser light, which heats up and destroys the sample. This allows for acquisition of just one data point per experimental run, and has motivated the development of probing methods using off-resonant light to reduce the spontaneous scattering of photons away from the probe beam, such as dispersive dark-ground imaging [5], phase contrast imaging [6,7], and Faraday imaging [8][9][10].…”
Section: Introductionmentioning
confidence: 99%
“…The theoretical system is modelled according to experimentally-realizable parameters [30][31][32], briefly described below. A BEC of 10 5 85 Rb atoms is initially prepared in a cylindrically-symmetric harmonic trapping potential with radial and axial trapping frequencies ω ⊥ = 2π × 70 Hz and ω z = 2π × 10 Hz, respectively.…”
Section: Model System and Parametersmentioning
confidence: 99%