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

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produces a device quality regrown layer. On the other h<strong>and</strong> highly damaged Si layers,<br />

even after <strong>annealing</strong> to very high temperatures, always contain residual defects (22).<br />

This is one reason for using a pre-amorphising implantat<strong>ion</strong> (PAI) step prior to<br />

implanting the dopant. It is energetically more favourable for Si to be in a crystal<br />

structure rather than a damaged / amorphous state. Solid phase epitaxial regrowth<br />

(SPER) can proceed from the interface <strong>of</strong> the crystal <strong>and</strong> amorphous reg<strong>ion</strong> in a layerby-layer<br />

fash<strong>ion</strong> upon <strong>annealing</strong> at temperatures <strong>of</strong> 550 °C <strong>and</strong> above (22). The<br />

regrowth rate is temperature dependant <strong>and</strong> increases with increasing anneal<br />

temperature. The regrowth rate also varies with the crystal orientat<strong>ion</strong>, (100) Si regrows<br />

faster than (110) Si, which in turn is faster than (111) orientated Si. This is one reason<br />

for the majority <strong>of</strong> devices being made on (100) Si. (100) Si is also the easiest<br />

orientat<strong>ion</strong> to grow. During the regrowth <strong>of</strong> amorphous layers the implanted dopant can<br />

take up substitut<strong>ion</strong>al lattice posit<strong>ion</strong>s depending on concentrat<strong>ion</strong> (22). For high dopant<br />

concentrat<strong>ion</strong>s some dopant may not be able to be accommodated in the regrown layers<br />

<strong>and</strong> will be swept in front <strong>of</strong> the interface between the amorphous / crystalline interface,<br />

forming a segregated layer at the surface (23, chapter 6) or form clusters.<br />

High anneal temperatures <strong>of</strong> > 1000 °C are typically preferred as they can result<br />

in fewer defects <strong>and</strong> higher levels <strong>of</strong> activated dopant. The thermal budget is the integral<br />

<strong>of</strong> the anneal temperature <strong>and</strong> time, which gives a measure <strong>of</strong> the total heat <strong>energy</strong>.<br />

However higher thermal budgets al<strong>low</strong> for more diffus<strong>ion</strong> <strong>of</strong> the dopant, adversely<br />

affecting both the junct<strong>ion</strong> depth <strong>and</strong> abruptness. It is therefore favourable to optimise<br />

the thermal budget to produce shal<strong>low</strong>er junct<strong>ion</strong>s with high levels <strong>of</strong> activat<strong>ion</strong> (1).<br />

This has led to the development <strong>of</strong> spike <strong>annealing</strong>, in which the wafers are heated to<br />

some higher temperature (usually > 1000 °C) but are not held at this maximum<br />

temperature. Fast ramp up <strong>and</strong> ramp down rates are used. This reduces diffus<strong>ion</strong> as<br />

opposed to the more convent<strong>ion</strong>al rapid thermal processing (RTP), in which the wafer is<br />

held at the maximum anneal temperature for some durat<strong>ion</strong>, usually <strong>of</strong> the order <strong>of</strong><br />

seconds.<br />

At the end <strong>of</strong> the range <strong>of</strong> an amorphising implant will be a reg<strong>ion</strong> essentially<br />

crystalline but containing a substantial number <strong>of</strong> defects. This interstitial rich defect<br />

reg<strong>ion</strong> is termed the end <strong>of</strong> range (EOR) <strong>and</strong> the defects in this area have an important<br />

effect on the behaviour <strong>of</strong> the dopant <strong>ion</strong>s during <strong>annealing</strong> (24, 25). These defects<br />

evolve during <strong>annealing</strong> <strong>and</strong> form extended defects. The dissociat<strong>ion</strong> <strong>of</strong> these extended<br />

defects at high anneal temperatures leads to the release <strong>of</strong> interstitials which sweep<br />

through the lattice <strong>and</strong> interact with the dopant atoms. This results in a burst <strong>of</strong><br />

10

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