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AMI Infrar ed Crystalline Materials    221


                                  Refractive* Index at   Absorption
               Wavelength (mm)    25∞C               Coefficient (cm )
                                                                  -1
                3                 2.7026             < 0.01
                4                 2.6971             ”
                5                 2.6922             ”
                6                 2.6886             ”
                7                 2.6865             ”
                8                 2.6846             ”
                9                 2.6825             ”
               10                 2.6797             ”
               11                 2.6766             ”
               12                 2.6749             ”
              ∗ ν 3–5 µm = 163
              † ν 8–12 µm = 173

                               Thermal Change in Index †
                               ∆N/∆T × 10 /°C
                                         −6
                               +147 @ 1.15 µm
                               +98 @ 3.39 µm
                               +98 @ 10.6 µm

              ∗ Melt formed crystal.
              † R. J. Harris, Appl. Opt. 16, 436 (1970).

              TABLE 9.2  Optical Properties of Cadmium Telluride

              reach maximum transmission with no free carrier absorption.  An
                                         −1
              absorption coefficient of 0.002 cm  was measured at 10.6 µm by Laser
              Power Optics. Table 9.2 lists the data found in the AMI product sheet
              for melt-formed crystalline CdTe.

              9.3.1 Conclusions
              The AMI chalcogenide glass compounding process was modified by
              adding a third chamber so plates of large-grain polycrystalline
              cadmium telluride could be produced. Plates with as large as 10-in
              diameter were tried, but failure of the quartz became a problem. Most
              efforts were concentrated on using our regular 8-in chambers. The
              slow freezing rate and the air-controlled directional freeze appear to
              be a reliable method for producing relatively large volumes of
              randomly oriented single-crystal regions. No single preferred growth
              orientation was observed. In general, the plates were well com-
              pounded, free of voids with very little, if any, dendritic growth.
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