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Application and Optimisation of the Spatial Phase Shifting ...

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2.2 First-order speckle statistics 29<br />

Fig. 2.17: Left: phase distribution <strong>of</strong> sample speckle field; [–π,π) represented as grey shades from black to white.<br />

Right: zero crossings <strong>of</strong> A r (x, y), black lines, <strong>and</strong> <strong>of</strong> A i (x, y), white lines. Red dots: positive, green dots:<br />

negative singularities.<br />

The figure shows that <strong>the</strong> zero-crossings <strong>of</strong> A r (x, y) <strong>and</strong> A i (x, y) intersect at all angles between 0 <strong>and</strong> 90°<br />

[Fre94a], <strong>and</strong> also explains easily why dislocations always appear <strong>and</strong> vanish pairwise: it is impossible for<br />

<strong>the</strong> closed zero contours <strong>of</strong> A r (x, y) <strong>and</strong> A i (x, y) to generate only one new intersection. This is also <strong>the</strong><br />

reason why <strong>the</strong>y alternate in sign – also called topological charge – on paths along any zero-crossing<br />

contour [Shva94, Fre94b, Fre95d]. When <strong>the</strong> zero-crossings <strong>of</strong> A r (x, y) <strong>and</strong> A i (x, y) touch, <strong>the</strong>y do so<br />

tangentially <strong>and</strong> generate a zero-amplitude line, or "edge" dislocation [Nye74, Bas95], <strong>of</strong> infinitesimal<br />

length in <strong>the</strong> x-y plane, that instantly splits up into <strong>the</strong> two "screw" dislocations as <strong>the</strong> zero crossings <strong>of</strong><br />

A r (x, y) <strong>and</strong> A i (x, y) intersect, i.e. as we shift our x-y-plane in z direction <strong>and</strong> <strong>the</strong> wavefield evolves in<br />

space. The trajectories <strong>of</strong> <strong>the</strong> singularities can be thought <strong>of</strong> as dark lines that pierce <strong>the</strong> x-y-plane <strong>and</strong> are<br />

orientated mostly in z direction [Ber78]. Their shape in space has been referred to as "snake-like" [Bar83];<br />

<strong>the</strong> process <strong>of</strong> pair creation or annihilation <strong>the</strong>refore corresponds to turning points <strong>of</strong> <strong>the</strong>se trajectories<br />

where <strong>the</strong> z component <strong>of</strong> <strong>the</strong>ir direction vector changes sign.<br />

The abovementioned z-direction scan <strong>of</strong> <strong>the</strong> speckle field gives us <strong>the</strong> opportunity to track <strong>the</strong> loci <strong>of</strong> <strong>the</strong><br />

dislocations slice by slice to see whe<strong>the</strong>r a pair <strong>of</strong> dislocations that has appeared toge<strong>the</strong>r will also vanish<br />

toge<strong>the</strong>r, <strong>and</strong> how one should imagine <strong>the</strong> zero-intensity trajectories in space. Fig. 2.18 presents <strong>the</strong> zerointensity<br />

lines in <strong>the</strong> very centre <strong>of</strong> <strong>the</strong> sample phase field; <strong>the</strong> colouring helps to distinguish <strong>the</strong>m. If <strong>the</strong>y<br />

end, it means that <strong>the</strong>y have moved out <strong>of</strong> <strong>the</strong> sample volume or that <strong>the</strong>ir tracking is discontinued for<br />

clarity <strong>of</strong> <strong>the</strong> representation.

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