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U. Glaeser

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1.2 Downsizing below 0.1<br />

© 2002 by CRC Press LLC<br />

µµµµ m<br />

In digital circuit applications, a MOSFET functions as a switch. Thus, complete cut-off of leakage current<br />

in the “off” state, and low resistance or high current drive in the “on” state are required. In addition,<br />

small capacitances are required for the switch to rapidly turn on and off. When making the gate length<br />

small, even in the “off” state, the space charge region near the drain—the high potential region near the<br />

drain—touches the source in a deeper place where the gate bias cannot control the potential, resulting<br />

in a leakage current from source to drain via the space charge region, as shown in Fig. 1.6. This is the<br />

well-known, short-channel effect of MOSFETs. The short-channel effect is often measured as the threshold<br />

voltage reduction of MOSFETs when it is not severe. In order for a MOSFET to work as a component<br />

of an LSI, the capability of switching-off or the suppression of the short-channel effects is the first priority<br />

in the designing of the MOSFETs. In other words, the suppression of the short-channel effects limits the<br />

downsizing of MOSFETs.<br />

In the “on” state, reduction of the gate length is desirable because it decreases the channel resistance<br />

of MOSFETs. However, when the channel resistance becomes as small as source and drain resistance,<br />

further improvement in the drain current or the MOSFET performance cannot be expected. Moreover,<br />

in the short-channel MOSFET design, the source and drain resistance often tends to even increase in<br />

order to suppress the short-channel effects. Thus, it is important to consider ways for reducing the total<br />

resistance of MOSFETs with keeping the suppression of the short-channel effects. The capacitances of<br />

MOSFETs usually decreases with the downsizing, but care should be taken when the fringing portion<br />

is dominant or when impurity concentration of the substrate is large in the short-channel transistor<br />

design.<br />

Thus, the suppression of the short-channel effects, with the improvement of the total resistance and<br />

capacitances, are required for the MOSFET downsizing. In other words, without the improvements of<br />

the MOSFET performance, the downsizing becomes almost meaningless even if the short-channel effect<br />

is completely suppressed.<br />

To suppress the short-channel effects and thus to secure good switching-off characteristics of MOSFETs,<br />

the scaling method was proposed by Dennard et al. [3], where the parameters of MOSFETs are shrunk<br />

or increased by the same factor K, as shown in Figs. 1.7 and 1.8, resulting in the reduction of the space<br />

charge region by the same factor K and suppression of the short-channel effects.<br />

2<br />

In the scaling method, drain current, Id<br />

( = W/<br />

L × V / tox),<br />

is reduced to 1/<br />

K.<br />

Even the drain current is<br />

reduced to 1/<br />

K,<br />

the propagation delay time of the circuit reduces to 1/<br />

K,<br />

because the gate charge reduces<br />

2<br />

to 1/<br />

K . Thus, scaling is advantageous for high-speed operation of LSI circuits.<br />

2<br />

If the increase in the number of transistors is kept at K , the power consumption of the LSI—which<br />

2<br />

is calculated as 1/<br />

2fnCV as shown in Fig. 1.7—stays constant and does not increase with the scaling.<br />

Thus, in the ideal scaling, power increase will not occur.<br />

FIGURE 1.6<br />

Source<br />

Leakage Current<br />

0 V<br />

Space Charge<br />

Region<br />

Short channel effect at downsizing.<br />

0 V<br />

Gate<br />

V dd (V)<br />

Drain

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