Experiments with Supersonic Beams as a Source of Cold Atoms
Experiments with Supersonic Beams as a Source of Cold Atoms
Experiments with Supersonic Beams as a Source of Cold Atoms
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Magnetic field (T)<br />
1.8<br />
1.75<br />
1.7<br />
1.65<br />
1.6<br />
1.55<br />
1.5<br />
1.45<br />
1.4<br />
1.35<br />
−4 −3 −2 −1 0 1 2 3 4<br />
x 10 −3<br />
1.3<br />
Radial position (m)<br />
(a)<br />
Magnetic field (T)<br />
0.7<br />
0.65<br />
0.6<br />
0.55<br />
0.5<br />
0.45<br />
−4 −3 −2 −1 0 1 2 3 4<br />
x 10 −3<br />
0.4<br />
Radial position (m)<br />
Figure 4.7: This figure illustrates the manner in which the magnitude <strong>of</strong> the magnetic<br />
field varies <strong>with</strong> radial position in a 1.05 cm diameter coil. The field at the center <strong>of</strong><br />
the coil (z = 0) is plotted in (a). The magnitude <strong>of</strong> the field is at a radial minimum<br />
on the axis <strong>of</strong> the coil at this axial position, which provides a focusing force to lowfield-seeking<br />
particles. The field, <strong>as</strong> a function <strong>of</strong> radial position well outside <strong>of</strong> the<br />
coil is plotted in (b). Here, the radial dependence <strong>of</strong> the field magnitude is at a<br />
maximum on the axis <strong>of</strong> the coil, providing a de-focusing effect for low-field-seekers.<br />
The interplay between the focusing effects inside the coil and the de-focusing outside<br />
the coil is complex, and depends on the velocity <strong>of</strong> the particles p<strong>as</strong>sing though the<br />
coil, <strong>as</strong> well <strong>as</strong> the switch-<strong>of</strong>f timing.<br />
large effect on the number <strong>of</strong> slowed atoms or molecules. Maxwell’s equations dictate<br />
that there can be no free space maximum in magnetic field. Though the magnitude<br />
<strong>of</strong> the magnetic field on the axis <strong>of</strong> a coil (z-axis) is at a maximum at center <strong>of</strong> the<br />
coil, this cannot be a true local maximum. Instead, this point at the center <strong>of</strong> a coil<br />
is a saddle point, and is at a minimum <strong>of</strong> the field radially. The magnitude <strong>of</strong> the<br />
field <strong>of</strong> a coil <strong>as</strong> a function <strong>of</strong> radial position at z = 0 is plotted in figure 4.7(a). The<br />
fact that the field is at a minimum on axis here means that low-field-seeking atoms<br />
feel a force pushing them towards the axis <strong>of</strong> the coil, producing a focusing effect on<br />
the beam <strong>of</strong> particles. This allows the coilgun to act <strong>as</strong> a waveguide, and can provide<br />
a degree <strong>of</strong> transverse stability to the slowed bunch <strong>of</strong> atoms in the coilgun.<br />
(b)<br />
Though the magnitude <strong>of</strong> the field is radially minimal on axis at the center<br />
<strong>of</strong> the coil, this is not true at all locations. Examining the radial dependence <strong>of</strong><br />
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