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The Crystal Lattice System
                             ficients of continuum theory, acoustic dispersion, specific heat, thermal
                             expansion and heat conduction. In fact, going beyond our current goals, it
                             is possible to similarly treat dielectric, piezoelectric and elastooptic
                             effects. However, the predictions are of a qualitative nature in the major-
                             ity of cases, mainly because the interatomic potential of covalently
                             bonded atoms is so hard to come by. In fact, in a sense the potential is
                             reverse engineered, that is, using measurements of the crystal, we fit
                             parameters that improve the quality of the models to make them in a
                             sense “predictive”.

                Chapter Goal Our goal for this chapter is to explain the observed crystal data with pref-
                             erably a single comprehensive model that accounts for all effects.


                Chapter      Our road map is thus as follows. We start by stating some of the relevant
                Roadmap      observable data for the three materials  Si SiO   and  GaAs  , without
                                                                ,
                                                                     2
                             more than a cursory explanation of the phenomena.

                             Our next step is to get to grips with the concept of a crystal lattice and
                             crystal structure. Beyond this point, we are able to consider the forces
                             that hold together the static crystal. This gives us a method to describe
                             the way the crystal responds, with stress, to a strain caused by stretching
                             the lattice. Then we progress to vibrating crystal atoms, progressively
                             refining our method to add detail and show that phonons, or quantized
                             acoustic pseudo “particles”, are the natural result of a dynamic crystal
                             lattice.

                             Considering the phonons in the lattice then leads us to a description of
                             heat capacity. Moving away from basic assumptions, we consider the
                             anharmonic crystal and find a way to describe the thermal expansion. The
                             section following presents a cursory look at what happens when the regu-
                             lar crystal lattice is locally deformed through the introduction of foreign
                             atoms. Finally, we leave the infinitely-extended crystal model and briefly
                             consider the crystal surface. This is important, because most microsys-
                             tem devices are build on top of semiconductor wafers, and so are repeat-



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