Page 157 - Photodetection and Measurement - Maximizing Performance in Optical Systems
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Control of Ambient Light

            150   Chapter Seven

                                       Color corrected laser protection
                           100
                           90
                           80
                         Transmission (%)  60
                           70

                           50
                           40
                           30
                           20
                           10
                            0
                             400 420 440 460 480 500 520 540 560 580 600 620 640 660 680 700
                                              Wavelength (nm)
                        Figure 7.9 Almost arbitrary wavelength filtering responses are possible
                        with the new synthesis tools and manufacturing techniques of “rugate”
                        filters. These use a deposited film of continuously varied refractive
                        index, rather than the Hi-Lo stacks of conventional interference filters.
                        The curve shows a filter for visual use with color-correction and strong
                        suppression of a small band of wavelengths around 532nm. Figure sup-
                        plied and reproduced by permission of Advanced Technology Coatings
                        Ltd., Plymouth U.K.



                        Company’s original range. These are cheaper than colored glass filters, but
                        generally do not offer as high suppression. A selection of long-wavelength pass
                        filters is available from about 395nm (Type “1A”) in the blue to 852nm (“87C”)
                        in the near IR. In addition, there are a few bandpass filters in the visible wave-
                        length range. Being plastic, they are easily cut to size for custom applications
                        and quick tests.
                          Another way to obtain very high suppression of particular wavelengths, espe-
                        cially with a long-pass characteristic, is to use pure, simple liquids. For example
                        ethyl acetate in aqueous solution is transparent in the visible, but absorbs
                        strongly below about 255nm. Carbon tetrachloride performs similarly. Figure
                        7.11 shows a dilute solution of acetone (ª50ml/ml in water). The absorption is
                        a smooth peak centered on 270nm (lower curve), which is useful to absorb the
                        254nm mercury line. As the concentration is increased (upper curve), this looks
                        more and more like an edge filter, which shifts to longer wavelength. It remains
                        very transparent in the visible range. The ultimate absorption is much greater
                        than 3AU, which is the measurement limit of the spectrometer used for this
                        spectrum. The convenience of a liquid filter lies mainly in wide-range adjust-
                        ment of the absorption strength (via concentration), very high absorption at
                        large thicknesses and the ability to form complex shapes. Transition metal ions
                        in aqueous solution are also useful, having strong visible colors which can be
                        used to absorb relatively narrow spectral regions. These metal ions often can


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