2016
DOI: 10.1063/1.4960997
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Design and experimental validation of a compact collimated Knudsen source

Abstract: In this paper, the design and performance of a collimated Knudsen source, which has the benefit of a simple design over recirculating sources, is discussed. Measurements of the flux, transverse velocity distribution, and brightness of the resulting rubidium beam at different source temperatures were conducted to evaluate the performance. The scaling of the flux and brightness with the source temperature follows the theoretical predictions. The transverse velocity distribution in the transparent operation regim… Show more

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Cited by 6 publications
(8 citation statements)
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“…Figure 8 shows the beam density as a function of source temperature in two cases: with the magnetic field gradient set to the optimal value of 1.1 T/m and without any magnetic field. The figure also shows a scaling law that scales the first data point of both measurements with the flux coming from the Knudsen source [27]. Although the beam density does increase with increasing source temperature, figure 8 shows that the scaling law only holds for the lowest temperatures and in the case of no magnetic field gradient.…”
Section: E Beam Density Vs Source Temperaturementioning
confidence: 88%
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“…Figure 8 shows the beam density as a function of source temperature in two cases: with the magnetic field gradient set to the optimal value of 1.1 T/m and without any magnetic field. The figure also shows a scaling law that scales the first data point of both measurements with the flux coming from the Knudsen source [27]. Although the beam density does increase with increasing source temperature, figure 8 shows that the scaling law only holds for the lowest temperatures and in the case of no magnetic field gradient.…”
Section: E Beam Density Vs Source Temperaturementioning
confidence: 88%
“…Note that in the actual experiment the beam travels in the vertical direction since this will also be the orientation of the source when mounted on a FIB system. As shown, an atomic rubidium beam from a collimated Knudsen source [27] with temperature T s effuses into a two-dimensional magneto-optical trap (2D MOT) [30]. After the 2D MOT the atoms can be cooled to sub-Doppler temperature with a second set of counter propagating laser beams, forming an optical molasses.…”
Section: Methodsmentioning
confidence: 99%
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“…Looking forward, combining Monte Carlo and master equation simulations allows the tracking of atom trajectories and their internal states simultaneously, which is indispensable for customizing the laser manipulation of atoms close to or within a chip-scale source itself [37]. The simple recipe phrased in linear algebra for reconstructing the speed/angular distribution of the atomic beams is important for precision spectroscopy [38] or atom scattering experiments [39], and useful for guiding collimator and oven designs [40][41][42]. where we've dropped all constants as coefficients and A(v, r, θ, φ, δ) represents A(v, r, θ, φ, δ, s 0 ) = sin θ • R sc (r, θ, φ, s 0 , δ, v) • v 2 e −(v/α) 2 .…”
Section: Discussionmentioning
confidence: 99%
“…In this article the ionization strategy that is applied in the atomic beam laser cooled ion source (ABLIS) [7] is introduced. In the ABLIS setup a thermal beam of Rb atoms effuses from a collimated Knudsen source [8] and is laser cooled and compressed in the transverse direction. Subsequently the atoms are ionized in a two-step * e.j.d.vredenbregt@tue.nl photoionization process.…”
Section: Introductionmentioning
confidence: 99%