Page 71 - Semiconductor For Micro- and Nanotechnology An Introduction For Engineers
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The Crystal Lattice System
                             Since the potential energy is located in the bonds and not the lattice site,
                             and therefore depends on the positions of the neighboring lattice sites,
                                     2
                             the term d udX⁄  2   is replaced by its lattice equivalent for the lattice site
                                               ⁄
                             i ( 2u –  u  –  u  ) a 2  . This finite difference formula expresses the
                                  i  i 1   i +  1
                                      –
                                                 u
                                                                i
                             fact that the curvature of   at the lattice site   depends on the next-neigh-
                             bor lattice positions. This step is necessary for a treatment of waves with
                             a wavelength of the order of the interatomic spacing. If we use the sim-
                             pler site relation, we only obtain the long wavelength limit of the disper-
                             sion relation, indicated by the slope lines in Figure 2.20. We now look for
                             solutions, periodic in space and time, of the form
                                         (
                                           ,
                                                          (
                                       uX t)       =  exp [  jkX –  ωt)]          (2.53)
                                              X =  ia              X =  ia
                             which we insert into equation (2.52) and cancel the common exponential
                                          2     E
                                                 (
                                       – ρω =  –  ----- 2 –  exp [ kia] –  exp  – [  kia])  (2.54)
                                                 2
                                                a
                             Reorganizing equation (2.54), we obtain

                                              (
                                           2E 1 –  cos [ ka])   E     ka
                                     ω =   ----------------------------------------- =  2 -------- sin  ------  (2.55)
                                                                 2
                                                   2
                                                 ρa            ρa     2
                             Equation (2.55) is plotted in Figure 2.20 on the left, and is the dispersion
                             relation for a monatomic chain. The curve is typical for an acoustic wave
                             in a crystalline solid, and is interpreted as follows. In the vicinity where
                                                                             ⁄
                                                                                    ⁄
                             ω   is small, the dispersion relation is linear (since  sin [ ka 2] ≈  ka 2  )
                             and the wave propagates with a speed of  E ρ⁄   as a linear acoustic
                             wave. As the frequency increases, the dispersion relation flattens off,
                             causing the speed of the wave ∂ω ∂k⁄   to approach zero (a standing wave
                             resonance).

                1D Diatomic   Crystals with a basis, i.e., crystals with a unit cell that contains different
                Dispersion   atoms, introduce an important additional feature in the dispersion curve.
                Relation
                             We again consider a 1D chain of atoms, but now consider a unit cell con-
                             taining two different atoms of masses m   and M  .


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