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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the coil can instead be switched before it arrives at this position. This is illustrated<br />
in figure 4.6(b). In this c<strong>as</strong>e, the particles that are ahead <strong>of</strong> the synchronous atom in<br />
the bunch are slowed more, and thus will be pushed back towards the center <strong>of</strong> the<br />
bunch. Similarly, particles which are behind the center <strong>of</strong> the bunch are slowed less<br />
than the synchronous particle and catch up. This creates a region <strong>of</strong> ph<strong>as</strong>e stability,<br />
where the bunch remains in ph<strong>as</strong>e <strong>with</strong> the coil pulses for the entire coil sequence.<br />
This also reduces the necessary accuracy <strong>of</strong> the timing sequence for the coil pulses,<br />
<strong>as</strong> slight deviations in coil timing are sel-correcting. A slight error in coil timing may<br />
mean that the bunch is slowed slightly more(less) than predicted by a particular coil,<br />
but because the bunch w<strong>as</strong> slowed more(less), the next coil in the coilgun slows it<br />
less(more) because the bunch is farther(closer) from(to) the peak field when the coil<br />
is switched. This makes the coilgun quite robust against small timing errors.<br />
A brief comment on notation is useful at this point. When producing the<br />
timing sequence, the numerical simulation <strong>of</strong> the synchronous atom switches each coil<br />
at a pre-defined position in that coil. This position can also be referred to <strong>as</strong> a ph<strong>as</strong>e<br />
angle using the following conversion. The midpoint between two coils is considered<br />
to be a ph<strong>as</strong>e angle <strong>of</strong> 0 ◦ and switching when the synchronous atom or molecule is in<br />
the center <strong>of</strong> a coil is labeled 90 ◦ , <strong>with</strong> intermediate positions linearly converted to<br />
an angle. This convention comes from previous work <strong>with</strong> particle accelerators, and<br />
the concept <strong>of</strong> ph<strong>as</strong>e stability is similar to that found in colliders [76, 77], and the<br />
pulsed electric field decelerator [15, 78]. The concept <strong>of</strong> ph<strong>as</strong>e stability in the coilgun<br />
is discussed in [21, 25, 69–71].<br />
4.3.2 Electromagnetic Coils <strong>as</strong> a Waveguide<br />
While the longitudinal stability <strong>of</strong> the slowed bunch <strong>of</strong> particles is addressed<br />
in the previous section, the transverse behavior <strong>of</strong> particles in the coilgun also h<strong>as</strong> a<br />
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