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88   Ophthalmic Lenses























                               Fig. 8.5: Principle of anti-reflection coating
                  However, in practice it is impossible to attain total extinction of reflection
               just by depositing a single layer of coating on the lens. In fact, the reflection
               could be almost eliminated by meeting two conditions:
               1. The refractive index of the coating is the square root of that of the lens
                  material.

                                      n  film =   n  Substrate
               2. The thickness of the coating, multiplied by its refractive index, is exactly
                  one – quarter of a wavelength of light or any odd number of quarter
                  wavelengths.
               Unfortunately, this is not always obtainable. Crown glass with a refractive
               index of 1.523 would need a material with an index of 1.234, whereas the
               most suitable material available for glass is Magnesium Fluoride which
               has a refractive index of around 1.38. So it is not very well suited for crown
               glasses but its performance is better on higher index materials. Also the
               two necessary conditions can be met for only one wavelength. This is the
               reason why single layer anti-reflection coating cannot reduce the reflectance
               in the entire range of visible spectrum. Single layer coatings are designed
               to give their maximum effect in the middle and brightest region of the
               visible spectrum. The reflectance gradually increases towards both violet
               and red ends of the spectrum. As a result, the coated surface presents the
               characteristics of purplish appearance which is described as bloom.

               MULTILAYER ANTI-REFLECTION COATING
               The limitations of the single layer antireflection coating can be overcome
               by multilayer coating which are now capable of almost extinguishing
               surface reflections from one end of the visible spectrum to the other. The
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