Low_resolution_Thesis_CDD_221009_public - Visual Optics and ...
Low_resolution_Thesis_CDD_221009_public - Visual Optics and ...
Low_resolution_Thesis_CDD_221009_public - Visual Optics and ...
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CHAPTER 2<br />
surface before <strong>and</strong> after the ablation. Furthermore, the measurement of the ablation<br />
efficiency effects is obtained after comparing the ablation pattern on flat surfaces from<br />
the ablation pattern on spheres (Chapters 3 <strong>and</strong> 5). The simulation of the threedimensional<br />
shape of a contact lens fitted on the eye results from the comparison of<br />
the anterior cornea <strong>and</strong> the anterior surface of the contact lens fitted. These two<br />
surfaces are also compared to obtain the conformity or flexure of the lens to the<br />
underlying cornea. All these applications are described hereinafter.<br />
2.2.2.1. Ablation patterns from flat surfaces<br />
In flat samples ablated with a laser, the measurement of the surface elevation pattern<br />
(or profile) should directly provide a measurement of the ablation pattern. However, in<br />
most cases the raw measurements of flat surfaces are affected by tilt. This happens<br />
when the support of the samples in the profilometry system is not perfectly parallel to<br />
the translation of the probe tip in contact profilometers (as that used in Chapter 3), or<br />
if the support of the samples is not perfectly perpendicular to the optical axis of the<br />
instrument in non-contact profilometers (Chapters 4 <strong>and</strong> 5). Tilt also appears if the<br />
sample is not perfectly plano-parallel.<br />
To remove this tilt, the non-ablated zone is fitted by a plane surface (a line in the<br />
case of a profile). That plane (or line) is subtracted from the measured surface. The<br />
location of the non-ablated zone is an input parameter, indicated as the ring between<br />
two given radii. The corrected measurement is more symmetrical than the original<br />
measurement (see Fig. 2. 16). Section 2.1.1.2 describes a cross-validation procedure of<br />
the measurement <strong>and</strong> the processing algorithms based on measuring the sample with<br />
different tilts <strong>and</strong> orientations (Fig. 2. 7). This cross-validation demonstrates (with the<br />
same sample) that the residual asymmetry obtained is in fact in the original sample,<br />
<strong>and</strong> is not an artifact introduced by the measurement procedure or the algorithms.<br />
0.08<br />
j j g p<br />
0.06<br />
0.04<br />
0.02<br />
0<br />
-0.02<br />
-0.04<br />
-0.06<br />
-0.08<br />
6<br />
4<br />
2<br />
0<br />
Y<br />
-2<br />
-4<br />
-6<br />
-4 -2 0 2 4 6<br />
j X<br />
j<br />
Fig. 2. 16. Removing tilt from topographies measured on flat ablated surfaces. The<br />
non-ablated zone (green points) of the measured elevation map (blue points) is fitted<br />
to a plane surface. This plane surface is subtracted from the measured surface to give<br />
the corrected measurement (red), which is more symmetrical than the original<br />
measurement (blue). The residual asymmetry is in the original sample, <strong>and</strong> is not<br />
introduced as an artifact of the measurement procedure, as can be demonstrated by<br />
measuring the sample with different tilts <strong>and</strong> orientations (Fig. 2. 7 <strong>and</strong> Section<br />
2.1.1.2)<br />
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