Page 187 - Materials Science and Engineering An Introduction
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Summary   •  159

                   Fick’s First Law  •  Diffusion flux is defined in terms of mass of diffusing species, cross-sectional area, and
                                   time according to Equation 5.1.
                                 •  Diffusion flux is proportional to the negative of the concentration gradient according
                                   to Fick’s first law, Equation 5.2.
                                 •  Concentration profile is represented as a plot of concentration versus distance into the
                                   solid material.
                                 •  Concentration gradient is the slope of the concentration profile curve at some specific point.
                                 •  The diffusion condition for which the flux is independent of time is known as steady state.
                                 •  The driving force for steady-state diffusion is the concentration gradient (dC/dx).

               Fick’s Second Law—  • For nonsteady-state diffusion, there is a net accumulation or depletion of diffusing
                 Nonsteady-State   species, and the flux is dependent on time.
                       Diffusion  •  The mathematics for nonsteady state in a single (x) direction (and when the diffusion
                                   coefficient is independent of concentration) may be described by Fick’s second law,
                                   Equation 5.4b.
                                 •  For a constant surface composition boundary condition, the solution to Fick’s second
                                   law (Equation 5.4b) is Equation 5.5, which involves the Gaussian error function (erf).


                     Factors That   •  The magnitude of the diffusion coefficient is indicative of the rate of atomic motion
               Influence Diffusion  and depends on both host and diffusing species as well as on temperature.
                                 •  The diffusion coefficient is a function of temperature according to Equation 5.8.

                     Diffusion in   •  The two heat treatments that are used to diffuse impurities into silicon during inte-
                  Semiconducting   grated circuit fabrication are predeposition and drive-in.
                       Materials      During predeposition, impurity atoms are diffused into the silicon, often from a
                                        gas phase, the partial pressure of which is maintained constant.
                                      For the drive-in step, impurity atoms are transported deeper into the silicon so
                                        as to provide a more suitable concentration distribution without increasing the
                                        overall impurity content.
                                 •  Integrated circuit interconnects are normally made of aluminum—instead of metals such
                                   as copper, silver, and gold that have higher electrical conductivities—on the basis of diffu-
                                   sion considerations. During high-temperature heat treatments, interconnect metal atoms
                                   diffuse into the silicon; appreciable concentrations will compromise the chip’s functionality.


              Equation Summary

              Equation                                                                              Page
              Number        Equation           Solving For                                        Number
                                  M
               5.1            J =              Diffusion flux                                       143
                                  At
                                   dC
               5.2          J = -D             Fick’s first law                                     143
                                    dx
                                    2
                            0C     0 C
               5.4b            = D             Fick’s second law                                    145
                             0t    0x 2
               5.5    C x - C 0  = 1 - erfa  x  b  Solution to Fick’s second law—for constant surface composition   146
                      C s - C 0       21Dt
                                      Q d
               5.8       D = D 0 expa -   b    Temperature dependence of diffusion coefficient      149
                                     RT
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