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Low_resolution_Thesis_CDD_221009_public - Visual Optics and ...

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CHAPTER 2<br />

thickness map, the same base sphere (typically the one corresponding to the anterior<br />

cornea) has to be substracted from both surfaces. The shape of the lens appears more<br />

clearly, as a positive or negative meniscus, depending on the lens power. To study the<br />

lens flexure or conformity to the underlying cornea, each of base spheres has to be<br />

substracted to each from the corresponding surfaces.<br />

2.2.2.4. Representing surfaces<br />

Throughout this thesis we have used different graphical representations for analysing<br />

the optical surfaces measured. Three dimensional scattered points plots (as those<br />

shown in Figs. 2.16 <strong>and</strong> 2.17) are often used to represent raw measurement (or<br />

deviations from a plane or a sphere). Figure 2.18 shows three other representations<br />

used. The same example surface, corresponfing to a highly assymetrical ablation<br />

pattern, is shown in a 2-D color-coded map of elevations (a), a 3-D topography (b)<br />

<strong>and</strong> a radial profile where only the radial coordinate of the points is plotted vs their<br />

heigh (c). To obtain the representations of Figs. 2.18 (a) <strong>and</strong> (b) an interpolation of the<br />

measured points to a regular grid is needed. Depending on the application <strong>and</strong><br />

variability of the data Zernike polinominal expansions, splines or exact interpolation<br />

was used. As opposed to raw sets of data (scattered points), these interpolated data sets<br />

can be directly compared, point by point. To obtain representations as the one shown<br />

in Fig. 2.18 (c), the data sets have to be previously transformed to cilindrical<br />

coordinates. The position of the origin is critical. In the representation of corneal<br />

ablations a biconic fitting was performed to obtain the center of the ablation, which<br />

was used as origin of the cylindrical coordinates. The representation of Fig. 2.18 (c)<br />

can be used with or without previous interpolation of the poins. In rotationally<br />

symetrical ablations this representation provides a thin curve. In assymetrical surfaces,<br />

as the one shown in Fig. 2.18 (c), a wide region of scattered poins appears.<br />

a) b) c)<br />

10<br />

20<br />

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-0.03<br />

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0.01<br />

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100<br />

20 40 60 80 100<br />

-0.07<br />

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-5 0 -5 0 5<br />

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Fig. 2. 18. Different representations of the surfaces used in this thesis. a) Colormap of<br />

elevations. b) Three-dimensional map. C) Radial profile.<br />

2.2.2.5. Operating with surfaces<br />

Calculations are performed on the measured surfaces in different chapters of this<br />

thesis, to estimate physical effects or to obtain different predictions. For example, in<br />

Chapters 3 <strong>and</strong> 5 efficiency effects are calculated by comparing ablation maps. Also,<br />

theoretical calculations of efficiency effects are applied to ablation patterns in flat<br />

surfaces to predict the ablation shape in curved surfaces, or measurements in plastic<br />

are used to predict the outcomes in corneal tissue. In Chapter 8 the thickness map of<br />

contact lenses is calculated by substracting their base surface, alond the redial<br />

76

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