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Damage formation and annealing studies of low energy ion implants ...

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Sputtering <strong>and</strong> atomic mixing play an important role in SIMS analysis, discussed in<br />

chapter 4, in the sense that the former is the basis <strong>of</strong> the technique <strong>and</strong> the latter places<br />

an undesirable limit on the resolut<strong>ion</strong>.<br />

3.2.3.3 Range shortening<br />

As the implanted <strong>ion</strong> concentrat<strong>ion</strong> increases during an implantat<strong>ion</strong>, the<br />

stopping power <strong>of</strong> Si changes slightly from being the stopping in pure Si to the<br />

combinat<strong>ion</strong> <strong>of</strong> stopping powers <strong>of</strong> the Si <strong>and</strong> dopant, as determined by Braggs rule (see<br />

sect<strong>ion</strong> 4.2.1.2). An increased stopping power leads to a concept called range shortening<br />

whereby the range <strong>of</strong> an implant reduces slightly with increasing fluence. This is most<br />

applicable with a high concentrat<strong>ion</strong> <strong>of</strong> implanted dopants.<br />

3.3 Annealing<br />

3.3.1 Introduct<strong>ion</strong><br />

Fol<strong>low</strong>ing <strong>ion</strong> implantat<strong>ion</strong> it is necessary to anneal the damaged wafers to<br />

restore the crystal lattice structure <strong>and</strong> electrically activate the implanted dopant <strong>ion</strong>s.<br />

The dopant <strong>ion</strong>s must be located on regular substitut<strong>ion</strong>al lattice sites. Tradit<strong>ion</strong>ally<br />

furnace <strong>annealing</strong> was used for this with temperatures from approximately 600 °C<br />

upwards, with timescales <strong>of</strong> minutes or hours. Furnace <strong>annealing</strong> in the reg<strong>ion</strong> <strong>of</strong><br />

600 °C would leave behind a large number <strong>of</strong> defects <strong>and</strong> require a second higher<br />

temperature anneal to remove them.<br />

Rapid thermal <strong>annealing</strong> (RTA), using for example arc or halogen lamps, has<br />

more recently been employed. Far higher temperatures, e.g. >1000 °C <strong>and</strong> shorter<br />

anneal durat<strong>ion</strong>s, e.g. seconds, are common. Spike <strong>annealing</strong> (SA) is a variant, applied<br />

to minimise diffus<strong>ion</strong>, carried out using the same type <strong>of</strong> RTA equipment. SA has a<br />

“zero” dwell time at the maximum temperature <strong>and</strong> uses rapid ramp up <strong>and</strong> down rates,<br />

e.g. 200 °Cs -1 <strong>and</strong> 70 °Cs -1 respectively are typical.<br />

All these types <strong>of</strong> <strong>annealing</strong> operate in the heat balance regime, which is where<br />

equilibrium between deposited <strong>and</strong> lost power is established <strong>and</strong> results in a steady state<br />

heat balance throughout the wafer. The timescales involved in this regime are t>10 -2 s<br />

(36).<br />

Other types <strong>of</strong> <strong>annealing</strong> include flash <strong>annealing</strong>, where a short durat<strong>ion</strong> pulse<br />

(10 -6 < t < 10 -2 s) from flash lamps will rapidly raise the temperature, creating a<br />

temperature gradient through the wafer. This is the thermal flux regime.<br />

42

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