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CHAPTER 3<br />

28<br />

DIFFRACTIVE LENS THEORY<br />

The advantages of using diffractive lenses and the intended application<br />

for them have been discussed in the preceding chapters. In this chapter, the<br />

discussion will focus on the basic operating principles and fabrication methods<br />

of diffractive lenses. It is necessary to point out there is a hierarchy of<br />

components that can be thought of as diffractive lenses. The operating effect of<br />

these components can be based on diffraction by a Fresnel zone plate (FZP).<br />

The operating principal of the FZP is thus considered first. This theory is then<br />

extended to discuss binary diffractive lenses, kinoforms, and multilevel<br />

approximations to the kinoform. The diffraction efficiency and method of<br />

fabrication of diffractive lenses are also discussed.<br />

3.1 Basic Principles<br />

For a general case, a diffractive lens illuminated by a plane<br />

monochromatic wave (Figure 3-1) splits the incoming wave into many spherical<br />

waves or diffraction orders. The foci of the lens occur where these diffracted<br />

orders cross the optical axis. The diffraction angle of each order is controlled by<br />

the period of the lens and may be calculated using the grating equation. The<br />

amount of light directed into each of these orders is in turn determined by the<br />

shape of the lens which modulates the phase of the incoming wave.<br />

The principle of operation of a diffractive lens may be better understood<br />

by first examining the zone construction of Fresnel. 31,32 A monochromatic

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