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Application and Optimisation of the Spatial Phase Shifting ...

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195<br />

Appendix A: Counting events<br />

Intensity level crossings per unit length<br />

In Chapter 2 we have encountered two occasions where probabilistic events had to be counted. The<br />

derivation is similar for both <strong>of</strong> <strong>the</strong>m. The level-crossing problem <strong>of</strong> (2.14) starts from <strong>the</strong> integral<br />

[Bar80]<br />

Nd ( It ) = ∫ δ ( I − It<br />

) ∂ I / ∂ x dx ; (A.1)<br />

d<br />

here N d (I t ) is <strong>the</strong> number <strong>of</strong> times that <strong>the</strong> intensity crosses <strong>the</strong> value I t on a path d (<strong>the</strong> probability for <strong>the</strong><br />

point I=I t being an extremum has measure zero on a straight line). The δ function assures that <strong>the</strong> integral<br />

responds only when I=I t ; to make each such contribution equal to one, i.e. to establish a counting function,<br />

<strong>the</strong> integration over x must be undone by <strong>the</strong> derivative ∂I/∂x; <strong>the</strong> modulus signs ensure that +1 is being<br />

counted for each event. However, since now I x appears, which is not independent <strong>of</strong> I, we need to know<br />

its expectation value at a given I, which requires <strong>the</strong> joint pdf p(I, I x ) <strong>and</strong> changes <strong>the</strong> integral to<br />

N ( I ) = δ ( I − I ) p( I, I ) I dI dx<br />

d t t x x x<br />

d Ix<br />

=<br />

∫ ∫<br />

∫ ∫<br />

d Ix<br />

p( I , I ) I dI dx<br />

t x x x<br />

on integrating over unit length, one obtains <strong>the</strong> density <strong>of</strong> <strong>the</strong> level-crossings,<br />

( )<br />

ρ( I ) = ∫ p I , I I dI ,<br />

t t x x x<br />

I x<br />

;<br />

(A.2)<br />

(A.3)<br />

which is (2.14).<br />

Intensity zero points per unit area<br />

By <strong>the</strong> same line <strong>of</strong> argument as above, we can start from [Ber78, Bar81]<br />

N ( A ) ( A ) ( A , A ) / ( x , y ) dxdy , (A.4)<br />

= ∫∫ δ δ ∂ ∂<br />

disl r i r i<br />

S<br />

where <strong>the</strong> dislocation is expressed by <strong>the</strong> vanishing <strong>of</strong> A r <strong>and</strong> A i , <strong>the</strong> integral is over an area S <strong>and</strong> <strong>the</strong><br />

quantity between <strong>the</strong> modulus signs is <strong>the</strong> Jacobian GJG=FA r,x A i,y – A r,y A i,x F. Obviously, we need<br />

p(A r , A i , A r,x , A i,x , A r,y, A i,y ) to evaluate this integral, or, more specifically, p(0 , 0 , A r,x , A i,x , A r,y , A i,y ) after<br />

<strong>the</strong> δ functions are accounted for. In analogy to above, we write<br />

N<br />

disl<br />

( )<br />

= ∫∫ ∫ ∫ ∫ ∫ p 0, 0, A r, x , A i, x , A r, y , A i, y ∂( Ar , Ai ) / ∂ ( x, y)<br />

dA r, xdA i, xdA r, ydA i,<br />

ydxdy<br />

, (A.5)<br />

S Ar , x Ai , x Ar , y Ai , x

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