Page 211 - Chalcogenide Glasses for Infrared Optics
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IR Imaging Bundles Made fr om Chalcogenide Glass Fibers       187

              using a microscope at 5X. The top image shows the cladding rings
              around each fiber. Note the space between the fibers covered by the
              cladding. The second image is made when visible light is transmitted
              through the bundle. The image illustrates how much area is inactive
              when you use clad fibers, at least when using the AMI method in
              drawing fibers and making ribbons. The measured spacing between
              the 100-µm fibers is 160 µm, thus limiting resolution by the bundle.
              Figure 8.5 shows the transmitted image by the bundle of the “O”
              pattern as recorded using the 1.5X objective on the microscope. The
              “O” pattern covers to 1 to 1.8 lp/mm and is clearly resolved. Note the
              coarseness of the image due to the thick cladding.
                 It was pointed out earlier that AMI developed an As-Se glass with
              a low softening point (131°C) and a large thermal expansion coeffi-
                                -6
              cient (∆L/L = 27  × 10 /°C) to use for molding chalcogenide glass
              lenses in a joint program with Lockheed Martin in Orlando. The glass
              was designated Amtir 4. Fiber drawn from this glass proved our con-
              clusion that chalcogenide glasses with the best physical properties do
              not make the best fibers. The ir transmission of C4 glass is similar to
              that of C1 except it drops off a little faster around 12 µm because the
              composition does not contain tellurium. The refractive index is 2.6
              compared to 2.8 for C1 glass. Fibers with a core diameter of 50 µm can
              be drawn unclad at 10 m/min without breaking. The time required to
              pull the 4000 to 5000 m of fiber for a bundle is greatly reduced. The
              finished bundle is flexible enough that it can be placed in the sample
              area of our FTIR, and the transmission of the bundle can be measured
              holding each end in place. The results are not quantitative but rather


























                              “O” Resolution Pattern 1–1.8 lp/mm
              FIGURE 8.5  Transmitted image of the “O” pattern by the C2 bundle.
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