Page 185 - Materials Science and Engineering An Introduction
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5.6 Diffusion in Semiconducting Materials  •  157


                             Now, from Equation 5.13,
                                                                         1/2
                                                                 Q 0
                                               x j = c (4D d t d )ln a  b d
                                                              C B 1pD d t d
                                                                     2
                                                 = c (4)(1.51 * 10 -17  m /s)(7200 s) *
                                                                                         1/2
                                                               18
                                                       3.44 * 10  atoms/m 2
                                       lnC                                            S s
                                                20
                                                                            2
                                                         3
                                          (1 * 10  atoms/m )2(p)(1.51 * 10 -17  m /s)(7200 s)
                                                            -6
                                                 = 2.19 * 10  m = 2.19 
m
                          (c)  At x   1 
m for the drive-in treatment, we compute the concentration of B atoms using
                             Equation 5.11 and values for Q 0  and D d  determined previously as follows:
                                         Q 0         x 2
                                 C(x, t) =     expa -   b
                                       1pD d t      4D d t
                                                                                      -6
                                                    18
                                            3.44 * 10  atoms/m 2               (1 * 10  m) 2
                                      =                             expc -          -17  2        d
                                                          2
                                        2(p)(1.51 * 10 -17  m /s)(7200 s)  (4)(1.51 * 10   m /s)(7200 s)
                                               23
                                      = 5.90 * 10  atoms/m 3
                  M A T E R I A L S                   O F       I M P O R T A N C E

                                    Aluminum for Integrated Circuit Interconnects

                 ubsequent to the predeposition and drive-in heat                           Interconnects
              Streatments just described, another important step   4  m
              in the IC fabrication process is the deposition of very
              thin and narrow conducting circuit paths to facilitate
              the passage of current from one device to another;
              these paths are called interconnects,  and several are
              shown in Figure 5.11, a scanning electron micrograph
              of an IC chip. Of course, the material to be used for
              interconnects must have a high electrical conductiv-
              ity—a metal, because, of all materials, metals have
              the highest conductivities. Table 5.3 gives values for
              silver, copper, gold, and aluminum, the most conduc-
              tive metals. On the basis of these conductivities, and
              discounting material cost, Ag is the metal of choice,
              followed by Cu, Au, and Al.
                 Once these interconnects have been deposited,
              it is still necessary to subject the IC chip to other  Figure 5.11  Scanning electron micrograph of an
              heat treatments, which may run as high as 500 C. If,   integrated circuit chip, on which is noted aluminum
              during these treatments, there is significant diffusion   interconnect regions. Approximately 2000 .
              of  the interconnect metal into the silicon,  the elec-  (Photograph courtesy of National Semiconductor Corporation.)
              trical functionality of the IC will be destroyed. Thus,
              because the extent of diffusion is dependent on the  of D in silicon. Figure 5.12 plots the logarithm of D
              magnitude of the diffusion coefficient, it is necessary   versus 1/T  for the diffusion,  into silicon,  of copper,
              to select an interconnect metal that has a small value   gold, silver, and aluminum. Also, a dashed vertical line

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