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Alfredo Dubra's PhD thesis - Imperial College London

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3. Data processing<br />

maximum value within the annular section s min < r < s max is found. The position<br />

of the maximum was only determined with 1 pixel accuracy. Sub-pixel search of<br />

the maximum by interpolation would not provide any advantage in our case because<br />

the algorithm that reconstructs the wavefront from the slope of the phase maps only<br />

uses integer values of shear amplitude. If we assume that the error in the maximum<br />

position determination is half a pixel, then the relative error for a typical shear value<br />

(30 pixels) is about 2%. In practice the error of the algorithm is higher, due to noise<br />

in the image acquisition and pixelation.<br />

3.2.4 Tests<br />

The value of the autocorrelation at the side peaks can not be determined theoretically<br />

unless one knows the image function A and the shear ⃗s. However, we can estimate it<br />

roughly if we use the fact that the actual overlapping of the images over areas with<br />

non-zero values is small in comparison with the non-overlapping areas. Evaluating<br />

formula 3.1 for ⃗r = −⃗s (and expanding the denominator) gives,<br />

∫ ∫ [<br />

C AA (−⃗s; ⃗s) = 1 A( r ⃗′ )A( r ⃗′ + ⃗s) + A( r ⃗′ )A( ⃗ ]<br />

r ′ + 2⃗s) d 2 r ′<br />

2 + 2 ∫ ∫ [ A 2 ( r ⃗′ ) + A( r ⃗′ )A( r ⃗ ] , (3.2)<br />

′ + ⃗s) d 2 r ′<br />

which shows that if the overlap between the two sheared images is small, then the value<br />

of the normalized autocorrelation at the side peaks is around 0.5. This is the case<br />

for our filtered interferograms that only have non-negligible values at the edges of the<br />

pupil and tear features. This can be clearly seen in figures 3.5 and 3.6, where the first<br />

columns show raw interferograms, the images in the second columns are the band-pass<br />

filtered interferograms and the three dimensional plots are the central region of the<br />

autocorrelation. By comparing the values of the autocorrelation side peaks indicated<br />

in the figures, and the filtered interferograms, it can be seen that other than when the<br />

tear surface is so rough that the fringes can not be recognized, the values at the side<br />

peaks are close to 0.5. More interesting is that even in the situation when the fringes<br />

can not be identified at all, the side peaks seem clearly identifiable, illustrating the<br />

robustness of the algorithm.<br />

49

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