Page 66 - Chalcogenide Glasses for Infrared Optics
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44    Cha pte r  T w o

                    This equation has been applied to the study of bonding in organic
                                                        36
              and inorganic compounds including oxide glasses.  For a molecular
              compound of the form A B C , where x, y, and z are the atomic frac-
                                   x  y  z
              tions of the constituents A, B, and C, the molar refraction becomes
                                R = xR + yR  + zR
                                     A    B    C
              where R , R and R are the atomic (or ionic) refraction values result-
                     A   B,   C
              ing from their presence in the molecule. The approach applies well to
              the covalent bonded chalcogenide glasses so that single values for
              each element can be determined and used in many different glass
              compositions. The atomic refraction values should be close to the
              cube of their accepted covalent radii. Calculating directly from
              accepted covalent radii would yield low values because the atomic
              spheres are loosely packed. Amorphous selenium was chosen as the
              starting point in calculating atomic refraction values for use with
              chalcogenide glasses.Using available experimental data. The atomic
              refraction for selenium was calculated and used as a reference. The
              index wavelength chosen was 5 µm. The atomic refractions for silicon,
              germanium, phosphorus, arsenic, sulfur, and tellurium were calcu-
              lated from the cube of their covalent radii and normalized to selenium.
              From these atomic refraction literature-derived values, the molar
              refractions for the 28 glass compositions used in the density plot of
              Fig. 2.15 were calculated and compared to the measured values.
              Agreement was  ±4.1 percent. The results are given in Table 2.5.
              Another approach that yielded better agreement was to treat the glass
              formulas of atomic refraction values for glasses with different con-
              centrations of the same elements as simultaneous equations and solve
              directly for the experimental atomic refraction values of each con-
              stituent element. When the 28 glass compositions were recalculated,
              the agreement with experimental values was ±1.1 percent. Table 2.6
              lists the atomic refraction values determined from the literature and
              from solving the simultaneous equations. Values from glasses based
              on S, Se, and Te are given for comparison.
                 An illustration of the worth of the method follows: The refrac-
              tive index for chalcogenide glasses at 5 µm can be calculated within
              a few percent by using the density vs. molecular weight plot in
              Fig. 2.15 and the atomic refraction values in Table 2.6 to calculate
              molar refraction:


                                R = xR  + yR + zR
                                     A     B   C
                                     2
                                            2
              Then solve for N from R = (N – 1)/(N  + 2) × molecular weight/density.
                 This procedure was applied to 20 As-Se-Te glasses reported by
                                                5
              Jerger and Billian at Servo Corporation.  The accurate values they
              reported and the values estimated agreed within +3 percent. The results

              are shown in Table 2.7.
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