Page 22 - Chalcogenide Glasses for Infrared Optics
P. 22

CHAPTER 1






                                         Transmission of


                                           Light by Solids









        1.1 Solids
              In nature, material exists as gas, liquid, or solid. Gas atoms or mole-
              cules are free to move within the confines of their container. Liquids
              move to fill the shape of their container while solids are rigid in shape.
              There is about a 1000-fold increase in density in going from gas to the
              condensed state of liquid or solid. The atoms or molecules come
              much closer together as a liquid and closer still as a solid. The dense
              solid may have a precise three-dimensional spatial arrangement for
              the atoms making up the solid that covers thousands of neighbors in
              all three directions. When the long-range order is perfect, the solid
              may be referred to as single-crystal. Or the order may be maintained
              over limited atomic distances and be referred to as polycrystalline.
              The atoms or molecules of liquids are free to move within their
              arrangements continuously in any direction and are said to have no
              long-range three-dimensional order. Order found is that of nearest
              neighbors or second nearest neighbors or even more, but not long
              range in the structural sense. Depending on elemental composition,
              when the atoms or molecules of a solid come close together, they
              begin to share their electronic bonding states, which results in forma-
              tion of an energy structure for the solid. When excited, bonding
              valence electrons are elevated into a higher conduction band state
              and are free to travel through the solid as charge if an electric field is
              applied. The energy difference between the valence state and the free
              conduction state is called the bandgap of the solid. The vacancies left
              in the valence band are called holes and can constitute charge flow
              moving in the opposite direction to the field. The band structure is
              well developed and precise in crystalline solids with good crystalline
              perfection. Liquids and amorphous solid glasses are condensed states
              but without long-range three-dimensional orders. A glass is referred
              to as a disordered solid. The energy band structure may exist, but the


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