2012
DOI: 10.1103/physreva.85.033420
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Vacuum-pressure measurement using a magneto-optical trap

Abstract: The loading dynamics of an alkali-metal-atom magneto-optical trap can be used as a reliable measure of vacuum pressure, with loading time τ indicating a pressure less than or equal to (2 × 10 −8 Torr s)/τ . This relation is accurate to approximately a factor of 2 over wide variations in trap parameters, background gas composition, or trapped alkali-metal species. The low-pressure limit of the method does depend on the trap parameters, but typically extends to below 1 × 10 −9 Torr.

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Cited by 78 publications
(105 citation statements)
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“…These results indicate that the main limitation of our measurements is the backgroundlimited lifetime of the atoms in the trap, which we estimate to correspond to a pressure of PՇ3 Â 10 À9 Torr. 28 The above results demonstrate that high fidelity state detection is achievable using sCMOS sensors despite the limited quantum efficiency compared to EMCCD cameras as summarised in Table I, meaning simply scattering more photons and thus slightly increased heating to achieve the same number of photon detection events but still providing excellent performance. For experiments requiring a fast repetition rate, readout time is also a consideration.…”
Section: Snrmentioning
confidence: 75%
“…These results indicate that the main limitation of our measurements is the backgroundlimited lifetime of the atoms in the trap, which we estimate to correspond to a pressure of PՇ3 Â 10 À9 Torr. 28 The above results demonstrate that high fidelity state detection is achievable using sCMOS sensors despite the limited quantum efficiency compared to EMCCD cameras as summarised in Table I, meaning simply scattering more photons and thus slightly increased heating to achieve the same number of photon detection events but still providing excellent performance. For experiments requiring a fast repetition rate, readout time is also a consideration.…”
Section: Snrmentioning
confidence: 75%
“…Since K and Rb are different species RCE is not possible, but nonresonant charge exchange (nRCE) is. However, careful experimental tests allow us to conclude that this channel is MOT [28].…”
Section: Doimentioning
confidence: 99%
“…The solid curve is a fit to Eq. (9) in which R capture = 1.12(3) × 10 8 atoms/s and τ trap = 2.20(3) seconds, corresponding to an upper limit on the pressure in the 3D chamber of ≈ 1 × 10 −8 Torr [30]. The steady state MOT number is 2.46(7) × 10 8 atoms.…”
Section: Fig 7 (Color Online)mentioning
confidence: 99%