Page 82 - Semiconductor For Micro- and Nanotechnology An Introduction For Engineers
P. 82

The Vibrating Uniform Lattice
                    ω k()










                                                      k  ω k()      k   ω k()    DOS
                Figure 2.26. The computed phonon density of state diagram for a simplistic silicon
                model, shown together with the computed phonon dispersion diagram. Notice that peaks
                in the density of states diagram occur at positions where ∂ω ∂k⁄  =  0  [2.13].



                                               2
                                              ∂ u
                                             ρ-------- =  ∇• σ =  ∇• ( C:ε)       (2.73)
                                                2
                                              ∂t
                                                        T
                             Remember that  u =  u u u    . It is simplest to first evaluate
                                                  1  2  3
                             σ =  C:ε   (here for a cubic-symmetry crystal) in the engineering notation
                             of (2.38) and (2.40)

                                                        C:ε

                                 C  11  C  12  C 12       ε 11   C ε +  C ε +   C ε
                                                                                 12 33
                                                                  11 11
                                                                          12 22
                                 C  12  C  11  C 12       ε 22   C ε +  C ε +   C ε
                                                                          11 22
                                                                                 12 33
                                                                  12 11
                                 C 12  C 12  C 11         ε 33   C ε +  C ε +   C ε
                                                                  12 11
                                                                                 11 33
                                                                          12 22
                              =                        ⋅      =
                                            C            2ε             2C ε
                                             44            23             44 23
                                               C         2ε             2C ε
                                                 44        31             44 31
                                                   C     2ε             2C ε
                                                     44    12             44 12
                                                                                  (2.74)
                             ant then to transform the result back to the usual tensor notation

                             Semiconductors for Micro and Nanosystem Technology      79
   77   78   79   80   81   82   83   84   85   86   87