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handbook of modern sensors

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138 4 Optical Components <strong>of</strong> Sensors<br />

(A)<br />

(B)<br />

(C)<br />

Fig. 4.13. Concept <strong>of</strong> a Fresnel lens.<br />

detectors. Fresnel lenses may be fabricated <strong>of</strong> glass, acrylic (visible and near-infrared<br />

range), or polyethylene (far-infrared range). The history <strong>of</strong> Fresnel lenses began in<br />

1748, when Count Buffon proposed grinding out a solid piece <strong>of</strong> glass lens in steps<br />

<strong>of</strong> the concentric zones in order to reduce the thickness <strong>of</strong> the lens to a minimum and<br />

to lower energy loss. He realized that only the surface <strong>of</strong> a lens is needed to refract<br />

light, because once the light is inside the lens, it travels in a straight line. His idea<br />

was modified in 1822 by Augustin Fresnel (1788–1827), who constructed a lens in<br />

which the centers <strong>of</strong> curvature <strong>of</strong> the different rings receded from the axis according<br />

to their distances from the center, so as to practically eliminate spherical aberration.<br />

The concept <strong>of</strong> that lens is illustrated in Fig. 4.13, where a regular plano-convex<br />

lens is depicted. The lens is sliced into several concentric rings. After slicing, all rings<br />

still remain lenses which refract incident rays into a common focus defined by Eq.<br />

(4.24). A change in an angle occurs when a ray exits a curved surface. The section<br />

<strong>of</strong> a ring marked by the letter x does not contribute to the focusing properties. If all<br />

such sections are removed, the lens will look like it is shown in Fig. 4.13B and will<br />

fully retain its ability to focus light rays. Now, all <strong>of</strong> the rings may be shifted with<br />

respect to one another to align their flat surfaces (Fig. 4.13C). A resulting near-flat<br />

lens is called Fresnel, which has nearly the same focusing properties as the original<br />

plano-convex lens.AFresnel lens basically consists <strong>of</strong> a series <strong>of</strong> concentric prismatic<br />

grooves, designed to cooperatively direct incident light rays into a common focus.<br />

The Fresnel lens has several advantages over a conventional lens, such as low<br />

weight, thin size, ability to be curved (for a plastic lens) to any desirable shape, and,<br />

most importantly, lower absorption loss <strong>of</strong> light flux. The last feature is very important<br />

for the fabrication <strong>of</strong> mid- and far-infrared lenses where absorption in the material<br />

may be significant. This is the reason why polymer Fresnel lenses are used almost<br />

exclusively in the far-infrared motion detectors.<br />

Two common types <strong>of</strong> Fresnel lenses are presently manufactured. One is a<br />

constant-step lens (Fig. 4.14A) and the other is a constant depth lens (Fig. 4.14B). In<br />

practice, it is difficult to maintain a curved surface <strong>of</strong> each small groove; hence, the<br />

pr<strong>of</strong>ile <strong>of</strong> a groove is approximated by a flat surface. This demands that the steps be<br />

positioned close to each other. In fact, the closer the steps, the more accurate the lens.<br />

In a constant-step lens, a slope angle ϕ <strong>of</strong> each groove is a function <strong>of</strong> its distance<br />

h from the optical axis.As a result, the depths <strong>of</strong> the grooves increase with the distance

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