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For a Gaussian atom distribution of size ro and peak density no n (r) = no e- r2 /2 ro2. The total number of atoms is N= (2π) 3/2 no ro3 and the peak optical depth is b0 = 2π n0 σ0 r0. σ0 is the weak-field resonance light scattering cross section.
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For a Gaussian atom distribution of size ro and peak density no n (r) = no e- r2 /2 ro2. The total number of atoms is N= (2π) 3/2 no ro3 and the peak optical depth is b0 = 2π n0 σ0 r0. σ0 is the weak-field resonance light scattering cross section.
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