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VECTORIAL ANALYSIS OF POLARIZED LIGHT USING A DICHROIC FILTER    123

                       aligned in the same direction as the organic matrix. The transmission axis of the filter is
                       perpendicular to the orientation of the crystals and linear polymers in the filter. Thus,
                       rays whose E vectors vibrate parallel to the crystal axis are absorbed.  Waves with
                       oblique orientations are partially absorbed, depending on the azimuths of their vibra-
                       tional planes. Filters such as the Polaroid sheet that differentially transmit rays vibrating
                       in one plane while absorbing those in other planes are said to exhibit dichroism; hence
                       the common name, dichroic filter. As we will see in later sections, the Polaroid sheet is
                       a special kind of beam splitter designed to transmit rays vibrating at a certain azimuthal
                       angle as linearly polarized light. For H-series filters that are commonly employed in
                       microscopy, only about 25% of incident random light is transmitted, but the degree of
                       polarization of the transmitted rays is   99%.
                          If two polarizers are oriented so that their transmission axes are perpendicular to
                       each other, they are said to be crossed, and all of the light transmitted by the polarizer
                       (now linearly polarized) is extinguished by the analyzer (Fig. 8-3). The extent to which
                       incident random light is extinguished by two crossed polars is called the extinction fac-
                       tor and is defined as the ratio of the intensity of transmitted light observed for two polars
                       when positioned in parallel and in crossed orientations (I /I ). Extinction factors of

                            5
                         3
                       10 –10 or greater are required for polarization microscopy and can be obtained using
                       two dichroic filters.
                          The role of the analyzer in controlling the transmission of polarized light can be
                       understood from vector diagrams showing the angular orientation (azimuthal angle) and
                       magnitude of the E vectors of rays drawn from the perspective of viewing a ray end on,
                       down its axis of propagation. Figure 8-5 shows a vertically oriented analyzer, four inci-
                       dent waves of linearly polarized light that are equal in amplitude but vibrating in differ-
                       ent planes, and the amplitudes of those waves after transmission through the analyzer. If
                       each incident wave is resolved into its horizontal and vertical components, it can be seen
                       that the entire vertical component of each ray passes through the analyzer. Further, the
                       amplitudes of the vertical component and the transmitted ray rapidly decrease as the
                       plane of vibration of the incident ray approaches an azimuth perpendicular to the trans-
                       mission axis of the analyzer.













                               Analyzer


                                   Excluded
                                   Transmitted

                       Figure 8-5
                       Transmission through an analyzer of linearly polarized rays vibrating in different planes. A
                       linearly polarized ray vibrating at an azimuthal angle different from the transmission axis of
                       an analyzer can be resolved into its horizontal and vertical components using principles of
                       vector math. The amplitude of the transmitted ray is equal to the vertical vector component.
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