2020
DOI: 10.1063/5.0006026
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High-resolution imaging of Rydberg atoms in optical lattices using an aspheric-lens objective in vacuum

Abstract: We present a high-resolution, simple, and versatile system for imaging ultracold Rydberg atoms in optical lattices. The imaging objective is a single aspheric lens [with a working distance of 20.6 mm and a numerical aperture (NA) of 0.51] placed inside the vacuum chamber. Adopting a large-working-distance lens leaves room for electrodes and electrostatic shields to control electric fields around Rydberg atoms. With this setup, we achieve a Rayleigh resolution of 1.10 μm or 1.41λ (λ = 780 nm), limited by the NA… Show more

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Cited by 5 publications
(3 citation statements)
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“…The mixture is then loaded into an optical dipole trap (ODT) formed by a 1064-nm light beam and transferred to the desired initial states 85 Rb 5S 1/2 , F = 3, m F = −3 and 87 Rb 5S 1/2 , F = 2, m F = −2 via microwave driven adiabatic passages. Subsequently, the ultracold mixture is transported to a science chamber 21 cm away from the MOT chamber and loaded into a 1D optical lattice [37]. At this stage, we have typically 2.2 × 10 5 85 Rb atoms and 7.1 × 10 5 87 Rb atoms at a temperature of ∼10 µK.…”
Section: Methodsmentioning
confidence: 99%
“…The mixture is then loaded into an optical dipole trap (ODT) formed by a 1064-nm light beam and transferred to the desired initial states 85 Rb 5S 1/2 , F = 3, m F = −3 and 87 Rb 5S 1/2 , F = 2, m F = −2 via microwave driven adiabatic passages. Subsequently, the ultracold mixture is transported to a science chamber 21 cm away from the MOT chamber and loaded into a 1D optical lattice [37]. At this stage, we have typically 2.2 × 10 5 85 Rb atoms and 7.1 × 10 5 87 Rb atoms at a temperature of ∼10 µK.…”
Section: Methodsmentioning
confidence: 99%
“…A first lens inside vacuum can reduce the marginal ray angles and hence aberrations by the following window. Imaging systems of this type have been demonstrated with moderate NAs around 0.5 [87][88][89]. Their disadvantage is that the relative alignment of in-and ex-vacuum components is absolutely crucial and that great care must be taken to prevent mechanical vibrations or long-term drifts.…”
Section: Initial Options and Considerationsmentioning
confidence: 99%
“…32 1000 [23] 18.9 1000 [24] 21.4 1000 [25] 14.9 1000 [28] 摄物镜. 与之前的设计 [21][22][23][24][25][26][27][28] 相比, 该成像系统在保 持比较大的倍率和视场(field of view, FOV)的同 时, 缩短了原子与像平面之间的距离, 并可以在更 大的真空窗厚度范围内使用. 显微物镜的NA为 0.47, 工作距离(working distance, WD)为32 mm.…”
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