2017
DOI: 10.1080/09500340.2017.1328749
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Velocity selection in a Doppler-broadened ensemble of atoms interacting with a monochromatic laser beam

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Cited by 8 publications
(13 citation statements)
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“…The distribution of velocities within our atom cloud, measured by Raman velocimetry (2.5 mW per Raman beam for 100 µs), is shown in Figure 4, and fits well a Gaussian distribution with a temperature of 21 µK superimposed upon a broad background that we have previously attributed to inhomogeneous sub-Doppler cooling [4 , 24 ]. This velocimetry method is itself subject to inaccuracies, and at longer exposure times yields higher temperatures, perhaps for the reasons discussed in [19 ]. Figure 5 shows the in-phase and quadrature interferometer traces, C(T ) and S(T ), for our atom cloud.…”
Section: Resultsmentioning
confidence: 99%
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“…The distribution of velocities within our atom cloud, measured by Raman velocimetry (2.5 mW per Raman beam for 100 µs), is shown in Figure 4, and fits well a Gaussian distribution with a temperature of 21 µK superimposed upon a broad background that we have previously attributed to inhomogeneous sub-Doppler cooling [4 , 24 ]. This velocimetry method is itself subject to inaccuracies, and at longer exposure times yields higher temperatures, perhaps for the reasons discussed in [19 ]. Figure 5 shows the in-phase and quadrature interferometer traces, C(T ) and S(T ), for our atom cloud.…”
Section: Resultsmentioning
confidence: 99%
“…Unlike conventional c.w. spectroscopy, however, measurements of velocities in the wings of the distribution are not distorted by weak interactions with more numerous atoms [19 ].…”
Section: Interferometric Velocimetrymentioning
confidence: 99%
“…The astute reader will notice that the Fourier transform of the signal defined in Equation (5) can only be measured experimentally for positive pulse separations τ , and that the signal is thus effectively multiplied by a Heaviside step function. With ideal interferometer pulses that perform perfect, instantaneous operations upon all atoms ( Figure 1a) this would introduce an orthogonal component to the Fourier transform that could be separated from the velocity information, but in practice deconvolution becomes intractable because pulses of finite duration ( Figure 1b) themselves exhibit Doppler sensitivity, introducing a velocity-dependent amplitude and phase shift that we have explored in more detail in [27].…”
Section: A Mach-zehnder Interferometer For Atom Velocimetrymentioning
confidence: 99%
“…Popular methods of measuring velocity distributions, such as time-of-flight imaging [3], Raman [4,5] and Bragg [6,7] Doppler spectroscopy, rely upon separate interactions with small slices of the velocity distribution to build up a complete measurement. Each involves the signal from only a small number of atoms, and there are artefacts from the initial cloud size and measurement-induced perturbation of the velocity distribution.…”
Section: Introductionmentioning
confidence: 99%
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