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U. Glaeser

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1.5 Source and Drain<br />

Figure 1.25 shows the changes of S/D (source and drain) formation process and structure. S/D becomes<br />

shallower for every new generation in order to suppress the short-channel effects. Before, the extension<br />

part of the S/D was called as LDD (Lightly Doped Drain) region and low doping concentration was<br />

required in order to suppress electric field at the drain edge and hence to suppress the hot-carrier effect.<br />

Structure of the source side becomes symmetrical as the drain side because of process simplicity. Recently,<br />

major concern of the S/D formation is how to realize ultra-shallow extension with low resistance. Thus,<br />

the doping of the extension should be done as heavily as possible and the activation of the impurity<br />

should be as high as possible. Table 1.4 shows the trends of the junction depth and sheet resistance of<br />

the extension requested by ITRS 2000. As the generation proceeds, junction depth becomes shallower,<br />

but at the same time, the sheet resistance should be reduced. This is extremely difficult. In order to satisfy<br />

this request, various doping and activation methods are being investigated. As the doping method, low<br />

energy implantation at 2–0.5 keV [48] and plasma doping with low energy [49] are thought to be the<br />

most promising at this moment. The problem of the low energy doping is lower retain dose and lower<br />

activation rate of the implanted species [48]. As the activation method, high temperature spike lamp<br />

anneal [48] is the best way at this moment. In order to suppress the diffusion of the dopant, and to keep<br />

the over-saturated activation of the dopant, the spike should be as steep as possible. Laser anneal [50]<br />

can realize very high activation, but very high temperature above the melting point at the silicon surface<br />

is a concern. Usually laser can anneal only the surface of the doping layer, and thus deeper portion may<br />

be necessary to be annealed by the combination of the spike lamp anneal.<br />

TABLE 1.4 Trend of S/D Extension by ITRS<br />

© 2002 by CRC Press LLC<br />

1999 2000 2001 2002 2003 2004 2005 2008 2011 2014<br />

Technology<br />

node (nm)<br />

180 130 100 70 50 35<br />

Gate length (nm) 140 120 100 85 80 70 65 45 32 22<br />

Extension Xj (nm) 42–70 36–60 30–50 25–43 24–40 20–35 20–33 16–26 11–19 8–13<br />

Extension sheet<br />

resistance (Ω/�)<br />

350–800 310–760 280–730 250–700 240–675 220–650 200–625 150–525 120–450 100–400<br />

Gas / Solid phase diffusion P, B Ion Implantation As, P, B<br />

LDD<br />

S Diffused layer D<br />

P, As, B, BF 2<br />

FIGURE 1.25 Source and drain change.<br />

Extension<br />

Low E Ion Imp.<br />

As, BF 2<br />

LDD (Lightly Doped Drain) Extension Pocket<br />

Pocket / Halo<br />

As, BF2 , In

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