Page 45 - A Practical Guide from Design Planning to Manufacturing
P. 45

The Evolution of the Microprocessor  21

        at the end of processing is the actual gate length (L GATE ). Also, the source
        and drain regions within the silicon typically reach some distance under-
        neath the gate. This makes the effective separation between source and
        drain in the silicon less than the final gate length. This distance is called
        the effective channel length (L EFF ). It is this effective distance that is the
        most important to transistor performance, but because it is under the
        gate and inside the silicon, it can not be measured directly. L EFF  is only
        estimated by electrical measurements. Therefore, L GATE  is the value most
        commonly used to compare difference processes.
          Gate oxide thickness is also measured in more than one way as shown
        in Fig. 1-10. The actual distance from the bottom of the gate to the top of
        the silicon is the physical gate oxide thickness (T OX-P ). For older processes
        this was the only relevant measurement, but as the oxide thickness has
        been reduced, the thickness of the layer of charge on both sides of the oxide
        has become significant. The electrical oxide thickness (T OX-E ) includes the
        distance to the center of the sheets of charge above and below the gate oxide.
        It is this thickness that determines how much current a transistor will pro-
        duce and hence its performance. One of the limits to future scaling is that
        increasingly large reductions in the physical oxide thickness are required
        to get the same effective reduction in the electrical oxide thickness.
          While scaling channel length alone is the most effective way to reduce
        delays, the increase in leakage current prevents it from being practical.
        As the source and drain become physically closer together, they become
        more difficult to electrically isolate from one another. In deep submicron
        MOSFETs there may be significant current flow from the drain to the
        source even when the gate voltage is below the threshold voltage. This
        is called subthreshold leakage. It means that even transistors that
        should be off still conduct a small amount of current like a leaky faucet.
        This current may be hundreds or thousands of times smaller than the
        current when the transistor is on, but for a die with millions of tran-
        sistors this leakage current can rapidly become a problem. The most
        common solution for this is reducing the oxide thickness.
          Moving the gate terminal physically closer to the channel gives the
        gate more control and limits subthreshold leakage. However, this




            +  +   +   +   +  +   +
          +  +   +  +    +  +   +   +  Poly

             T OX-P     T OX-E         SiO 2
          −    −  −  −  −  −  −  −  −  −  −
         −  −                    −   −  Si   Figure 1-10 Gate oxide thickness.
           −                        −
   40   41   42   43   44   45   46   47   48   49   50