CHAPTER 1:   MOS TRANSISTOR MODELS   29
In order to provide the full expression in the saturation region, Eq. (l-25a) must
                      be multiplied by the same factor (1 + Xvds) as in Eq. (1-20). The same parameter À
                      can be used in strong and weak inversion.
                         For the weak inversion region, the transconductance gm is again obtained by taking
                      the derivative of ids versus Vgs in Eq. (l-25a), which yields
                                                     W    Ido              VGSQ \       iDSQwi
                                            SmWl =        , rr, /   eXp                                   (1-256)
                                                     L nkT/q              nkT/q J       nkT/q
                         The transconductance is now directly proportional to the current. The transconduc
                      tance is sketched on a bilogarithmic scale versus the current in Fig. l-10a. The change
                      in slope from 1 to 1/2, going from weak to strong inversion, is clearly seen.
1-6-2    Transconductance-Current Ratio
                      The transconductance is the most important parameter of the MOST because it re
                      flects the transfer efficiency from input to output. A better criterion, however, is its
                      transconductance to current ratio gm/iDS- This ratio shows how efficiently the current
                      is used to generate transconductance.
        FIGURE 1-10   (a) gm and, (b) gm/lDS of MOST in saturation.