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In  the  very  low  (cryogenic)  temperature  region,  where  the
            quantum  mechanical  nature  of  energy  storage  in  all  solids

            manifests itself with larger and larger effect, the law fails for all

            substances.  In  1912  Debye  realized  that, inconsistent  with the Einstein
            model, low-energetic excitations of a solid material were not oscillations
            of a single atom, but collective modes propagating through the material.
            Such  vibrations  can  be  considered  to  be  sound  waves,  and  their

            propagation speed is the speed of sound in the material. Moreover, these
            modes only accept energy in discreet amounts.
            Quantum theory uses the concepts of phonons, which are “quasi-particles”

            with definite energies and directions of motion, to treat the vibrations. The
            concept of phonon is analogous with photons of the electromagnetic wave.


                                          4.4 Crystallographic Defect


            Crystalline  solids  exhibit  a  periodic  crystal  structure.  The  positions  of

            atoms or molecules occur on repeating fixed distances, determined by the
            unit cell parameters. However, the arrangement of atoms or molecules in
            most  crystalline  materials  is  not  perfect.  The  regular  patterns  are
            interrupted by crystallographic defects.

            Point defects are defects that occur only at or around a single lattice point
            Vacancy defects (fig.4.4.1a) are lattice sites which would be occupied in a
            perfect crystal, but are vacant. If a neighboring atom moves to occupy the

                                                                    vacant site, the vacancy moves
                                                                    in the opposite direction to the
                                                                    site which used to be occupied

                                                                    by  the  moving  atom.  The
                                                                    stability  of  the  surrounding
                                                                    crystal  structure  guarantees
                     a                 b                c           that the neighboring atoms will

                                                                    not simply collapse around the
                                 Figure 4.4.1
                                                                    vacancy.  In  some  materials,
            neighboring  atoms  actually  move  away  from  a  vacancy,  because  they

            experience attraction from atoms in the surroundings. A vacancy (or pair
            of vacancies in an ionic solid) is sometimes called a Schottky defect.
            A  nearby  pair  of  a  vacancy  and  an  interstitial  is  often  called  a  Frenkel

            defect or Frenkel pair (fig.4.4.1b). This is caused when an ion moves into
            an interstitial site and creates a vacancy.




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