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Single-Photon Atomic Cooling - Raizen Lab - The University of ...

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produces a quadrupole magnetic field.<br />

<strong>The</strong> form <strong>of</strong> the magnetic field produced in this configuration can be<br />

arrived at by first considering the form <strong>of</strong> the magnetic field produced by a<br />

single circular loop carrying a current I in a region <strong>of</strong> permittivity µ which is<br />

given by [56]<br />

where<br />

Bz = µI<br />

2π<br />

<br />

1<br />

K(k<br />

(R + ρ) 2 + (z) 2<br />

2 ) + R2 − ρ2 − z2 Bρ = µI z<br />

<br />

2πρ (R + ρ) 2 + (z) 2<br />

k 2 =<br />

(R − ρ) 2 + z2E(k2 <br />

)<br />

<br />

−K(k 2 ) + R2 + ρ2 − z2 (R − ρ) 2 + z2E(k2 )<br />

4Rρ<br />

(R + ρ) 2 + z 2<br />

<br />

(2.36a)<br />

(2.36b)<br />

(2.37)<br />

and K(k 2 ) and E(k 2 ) are the complete elliptic integrals <strong>of</strong> the first and second<br />

kind, respectively [57]. <strong>The</strong> terms in this expression are clarified in Fig. 2.4.<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

Figure 2.4: Geometry <strong>of</strong> Eq. 2.36. <strong>The</strong> red loop <strong>of</strong> current produces a magnetic<br />

field at the point (ρ,z). <strong>The</strong> magnetic field is decomposed into components<br />

parallel to ˆz and to ˆρ.<br />

42

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