There are three additional pairs of Helmholtz coils put in across the system to compensate for the ambient magnetic field. The distributing frame is made by Plexiglas, and 4 mirrors are attached on angled mounts to direct the beams. The AHCs are mounted on the rails to align the middle of the quadrupole field to the middle of the intersection region of optical beams. The coil present of four.4 A produces a 16 G/cm magnetic area gradient, which is fascinating for the operation of the rubidium (Rb) MOT. The primary vacuum chamber is an anti-reflection coated glass cell, whose dimensions are 35 mm by 24 mm by 60 mm, and is pumped by a 2 liter/s ion pump.
(A) Schematic of the spatial distribution of the transmitted laser beams after the metasurface optical chip. The laser beams are labeled depending on the location on the projection display by east (E), west (W), central (C), north (N), and south (S), respectively. (B) Intensity profile of the laser beams captured by a cost-coupled gadget digital camera after the metasurface optical chip. All the laser intensity profiles are plotted with the identical scale as the colour bar. The laser depth integral along the x and y axis is plotted because the green and yellow curves in every picture.
Excimer optics presents a tighter course of digital digicam decision depends upon finishing a robotic. The MOT apparatus (fig. S5) contains a light distribution frame and anti-Helmholtz coils (AHCs) producing the quadrupole magnetic subject and a vacuum chamber containing the rubidium atoms.
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The rubidium atoms are produced by heating a rubidium dispenser with an electrical current flowing by way of. The background pressure is about 2 × 10−9 mbar as the dispenser is cool and raised to 2 × 10−8 mbar when the experiment is running.