Page 42 - Chalcogenide Glasses for Infrared Optics
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Chalcogenide Glasses      21

              Hughes, Martin Marietta, and Westinghouse in several programs.
              Amtir 1 is still the major FLIR glass produced by AMI. Standard pro-
              duction is 9-kg plates 8-in diameter. AMI has produced 35 tons of
              Amtir 1 glass from 1978 to 2007.
                 Later, in 1991 after the TI 1173 patent expired, the Night Vision
              Laboratory provided a letter contract to qualify  AMI as a second
              source of the glass which AMI renamed Amtir 3. It is interesting to
              note that in the United States during the period from 1950 to the pres-
              ent, only three glass compositions have been produced in ton quanti-
              ties: arsenic trisulfide, TI 1173 (Amtir 3), and TI 20 (Amtir 1). No other
              widely used new compositions have emerged. The reason in part is
              due to the considerable effort required to identify, produce, and char-
              acterize a new glass composition to the state that optical designers,
              system designers, and corporate management are willing to use it in
              a new system. Even if a new, better glass emerged, there would be
              great reluctance to redesign a system once it is in production.


        2.2  The Periodic Table and Glass Formation
              Previously, it was pointed out that efforts to find and develop chalco-
              genide glasses for infrared systems were most successful using ele-
              ments from the IVA, VA, and VIA groups of the periodic table. This
              statement is to point out that the periodic table is not an inexhaustible
              supply of elemental combinations that should be investigated. The
              three groups named have fueled investigations of many systems:
              binary, ternary, or those containing even more elements. A review of
              other materials transparent in the infrared but from different elemen-
              tal families may help to explain why some elements are favored more
              than others. Figure 2.1 presents a shortened version of the periodic
              table of the elements. Outlined are the families of the elements from
              which infrared optical materials are formed.
                 As indicated in the chart, the alkali halides form from the IA alkali
              metal elements Li, Na, K, Rb, and Cs in combination with the group
              VIIA halogens F, Cl, Br, and I. The alkaline earth halides form from
              the IIA alkaline earth metal elements Be, Mg, Ca, Sr, and Ba in combi-
              nation with the VIIA halogen elements F, Cl, Br, and I. Notice also in
              Fig. 2.1 that a change in Pauling electronegativity  is indicated as one
                                                      27
              moves up or down in the chart or from left to right. On the left, the
              value decreases going from lighter alkali and alkaline earth elements
              to heavier. Thus, Cs and Ba have the lowest values for the two fami-
              lies. Conversely, Pauling electronegativity is indicated to be increas-
              ing with atomic number going across the chart from IA elements to
              VIIA elements. At the same time on the right of the chart, Pauling
              electronegativity increases going up the chart from the heavier halo-
              gens to the lighter elements. Fluorine in the top right corner has the
              highest value, 4.0, one unit higher than its next row element Cl.
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