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Application and Optimisation of the Spatial Phase Shifting ...

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196 Appendix A: Counting events<br />

<strong>and</strong> with S equal to <strong>the</strong> area unit we <strong>the</strong>n have<br />

( )<br />

ρ = ∫ ∫ ∫ ∫ p 0, 0, A , A , A , A ∂( A , A ) / ∂( x, y)<br />

dA dA dA dA<br />

disl r, x i, x r, y i, y r i r, x i, x r, y i,<br />

y<br />

Ar , x Ai , x Ar , y Ai , x<br />

;<br />

(A.6)<br />

with p(A r , A i , A r,x , A i,x , A r,y , A i,y ) given by (2.1), <strong>the</strong> integration is not trivial; it has been shown in [Ber78,<br />

Eq. 43] that <strong>the</strong> integral is best evaluated in polar co-ordinates, i.e. after conversion to I <strong>and</strong> ϕ, similar to<br />

(2.4). Fortunately, this needed be done only once <strong>and</strong> for all, since <strong>the</strong> "threshold" intensity is fixed to<br />

zero in this case.

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