2015
DOI: 10.1088/1367-2630/17/6/065001
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A high-flux BEC source for mobile atom interferometers

Abstract: Quantum sensors based on coherent matter-waves are precise measurement devices whose ultimate accuracy is achieved with Bose-Einstein condensates (BEC) in extended free fall. This is ideally realized in microgravity environments such as drop towers, ballistic rockets and space platforms. However, the transition from labbased BEC machines to robust and mobile sources with comparable performance is a challenging endeavor. Here we report on the realization of a miniaturized setup, generating a flux of 4 × 10 5 qu… Show more

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Cited by 103 publications
(120 citation statements)
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References 54 publications
(72 reference statements)
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“…Nonetheless, fast condensate production generally sacrifices total atom number for duty cycle. This is evident from the best integrated flux [32] achieved in fast devices, 2.5 × 10 5 atoms/s, when compared to the 4 × 10 5 atoms/s flux in this device. The application of techniques such as sideband cooling offer a path to improving flux on both atom chip and free-space based sensors [33] without sacrificing atom number.…”
Section: (B)mentioning
confidence: 64%
“…Nonetheless, fast condensate production generally sacrifices total atom number for duty cycle. This is evident from the best integrated flux [32] achieved in fast devices, 2.5 × 10 5 atoms/s, when compared to the 4 × 10 5 atoms/s flux in this device. The application of techniques such as sideband cooling offer a path to improving flux on both atom chip and free-space based sensors [33] without sacrificing atom number.…”
Section: (B)mentioning
confidence: 64%
“…Microwave fountain clocks, providing the realization of the SI second, are currently limited by the SQL. 22,[40][41][42] In combination with the recently developed sources of Bose-Einstein condensed atoms with small densities 43,44 and high repetition rates, 45 our results pave the way for the development of a new generation of atomic microwave clocks operating beyond the SQL.…”
Section: 39mentioning
confidence: 68%
“…This corresponds to a differential acceleration sensitivity of 1 × 10 −10 g per shot (5 × 10 −10 g= ffiffiffiffiffiffi Hz p given the 22 s cycle time) and is near the estimated shot noise limit of ∼1E per shot. Improvements in the atom source and imaging system would increase the atom number and contrast, allowing higher sensitivity, while a more advanced cold atom source [35] could reduce the cycle time to several seconds.…”
Section: Prl 118 183602 (2017) P H Y S I C a L R E V I E W L E T T Ementioning
confidence: 99%