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3 (lz)2 −1 |⃗r|3 #2 dV× Z π 0 sin3 (θ) P(θ)dθ× 1 2π Z 2π 0 cos2 ˜Ωt− δiso √ 3 τ−φ ! dφ  1/2 = µ0γh 8π √ N r F(2) z × 2 3 , where we definedF (2) q = Z

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