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The Crystal Lattice System
                                                        c
                                                ab
                             assume that the vectors  ,   and   are perpendicular. The Bravais lattice
                             is inherently symmetric with respect to translations q  : this is the way we
                                                                       j
                             construct it. The remainder of the symmetries are related to rotations and
                             reflections. There are   crystal systems: hexagonal, trigonal, triclinic,
                                               7
                             monoclinic, orthorhombic, tetragonal and cubic. In addition, there are
                             14   Bravais lattice types, see Figure 2.12. These are grouped into the fol-
                             lowing six lattice systems in decreasing order of geometric generality (or
                             increasing order of symmetry): triclinic, monoclinic, orthorhombic, tet-
                             ragonal, Hexagonal and cubic. The face-centered cubic (fcc) diamond-
                             like lattice structure of silicon is described by the symmetric arrangement
                             of vectors shown in Figure 2.13 (I). The fcc lattice is symmetric w.r.t. 90 o
                             rotations about all three coordinate axes. Gallium arsenide´s zinc-blende
                             bcc-structure is similarly described as for silicon. Because of the pres-
                             ence of two constituent atoms, GaAs does not allow the same transla-
                             tional symmetries as Si.


                Primitive    We associate with a lattice one or more primitive unit cells. A primitive
                Unit Cell    unit cell is a geometric shape that, for single-atom crystals, effectively
                             contains one lattice point. If the lattice point is not in the interior of the
                             primitive cell, then more than one lattice point will lie on the boundary of
                             the primitive cell. If, for the purpose of illustration, we associate a sphere
                             with the lattice point, then those parts of the spheres that overlap with the
                             inside of the primitive cell will all add up to the volume of a single
                             sphere, and hence we say that a single lattice point is enclosed. Primitive
                             cells seamlessly tile the space that the lattice occupies, see Figure 2.14.

                Wigner-Seitz   The most important of the possible primitive cells is the Wigner-Seitz
                Unit Cell    cell. It has the merit that it contains all the symmetries of the underlying
                             Bravais lattice. Its definition is straightforward: The Wigner-Seitz cell of
                             lattice point  p   contains all spatial points that are closer to  p   than to any
                                        i                                    i
                             other lattice point q  . Its construction is also straight-forward: Consider-
                                             j
                             ing lattice point  p  , connect  p   with its neighbor lattice points  q  . On
                                            i         i                            j
                             each connection line, construct a plane perpendicular to the connecting
                             line at a position halfway along the line. The planes intersect each other


                42           Semiconductors for Micro and Nanosystem Technology
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