2009
DOI: 10.1103/physreva.79.021605
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Technique for measuring atomic recoil frequency using coherence functions

Abstract: We have developed a technique for measuring the atomic recoil frequency using a single-state echo-type atom interferometer that manipulates laser-cooled atoms in the ground state. The interferometer relies on momentum-state interference due to two standing-wave pulses that produce density gratings. The interference is modified by applying a third standing-wave pulse during the interferometer pulse sequence. As a result, the grating contrast exhibits periodic revivals at the atomic recoil frequency r as a funct… Show more

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Cited by 13 publications
(22 citation statements)
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“…Specifically, the only momentum states contributing to the signal are those that differ byhq after SW3 and after SW2. 4 The non-uniform magnetic field produced by a stainless-steel vacuum chamber, and the gravity-induced Doppler shift limited previous experiments to T 10 ms [76,100,101]. diameter of d ∼ 1.7 cm and are circularly polarized in the same sense by a pair of λ/4 wave plates.…”
Section: Methodsmentioning
confidence: 99%
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“…Specifically, the only momentum states contributing to the signal are those that differ byhq after SW3 and after SW2. 4 The non-uniform magnetic field produced by a stainless-steel vacuum chamber, and the gravity-induced Doppler shift limited previous experiments to T 10 ms [76,100,101]. diameter of d ∼ 1.7 cm and are circularly polarized in the same sense by a pair of λ/4 wave plates.…”
Section: Methodsmentioning
confidence: 99%
“…τ 3 (Ω eff ω q ) −1/2 ) the full-width at half-maximum (FWHM) of the fringe scales as 1/u 3 , as illustrated in Fig. 2(c) [54,56,101].…”
Section: Description Of the Modified Three-pulse Aimentioning
confidence: 99%
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“…This allows for precise determination of the period of a signal like that in Fig. 2(a), and thereby of the recoil frequency ω r = π/2T T [26] (which in turn can be used to determine the fine structure constant α [27]). The increase in precision yielded by the steep edges results from the enhancement of high-order diffraction due to the phase modulation provided by the off-resonance standing wave.…”
Section: B Effect Of Microlensingmentioning
confidence: 99%