2021
DOI: 10.1103/physreva.103.043306
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Aberrations in (3+1)-dimensional Bragg diffraction using pulsed Laguerre-Gaussian laser beams

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Cited by 5 publications
(10 citation statements)
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“…We again introduce a varying interference signal by adding a phase factor to the outer paths, but none to the central path. Hence, a superposition Ψ 𝑚 ( 𝑝) = e i𝜗 ext /2 𝜓 𝑚,−1,1 + 𝜓 𝑚,0,0 + e −i𝜗 ext /2 𝜓 𝑚,1,−1 (16) is detected and leads to the signal…”
Section: B Overlap Of Individual Pathsmentioning
confidence: 99%
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“…We again introduce a varying interference signal by adding a phase factor to the outer paths, but none to the central path. Hence, a superposition Ψ 𝑚 ( 𝑝) = e i𝜗 ext /2 𝜓 𝑚,−1,1 + 𝜓 𝑚,0,0 + e −i𝜗 ext /2 𝜓 𝑚,1,−1 (16) is detected and leads to the signal…”
Section: B Overlap Of Individual Pathsmentioning
confidence: 99%
“…In this context, atomic Bragg diffraction has become a versatile tool for enhancing the sensitivity of atom interferometers through techniques like sequential pulses [4][5][6] as well as double [7][8][9] and higher-order diffraction [10][11][12][13]. Because its efficiency crucially depends on the pulse duration, Bragg diffraction favors an intermediate regime where velocity selectivity does not dominate, but spurious diffraction orders may occur [14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
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“…In this context, atomic Bragg diffraction has become a versatile tool for enhancing the sensitivity of atom interferometers through techniques like sequential pulses [4][5][6] as well as double [7][8][9] and higher-order diffraction [10][11][12][13]. Because its efficiency crucially depends on the pulse duration, Bragg diffraction favors an intermediate regime where velocity selectivity does not dominate, but spurious diffraction orders may occur [14][15][16][17]. In this article, we study these effects in single and double Bragg interferometry.…”
Section: Introductionmentioning
confidence: 99%