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

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contain no stacking fault, but faulted dislocat<strong>ion</strong> loops have a stacking fault in the {111}<br />

plane (59), as illustrated in Figure 3.10.<br />

Figure 3.10 Structure <strong>of</strong> a) faulted dislocat<strong>ion</strong> loops <strong>and</strong> b) perfect dislocat<strong>ion</strong> loops.<br />

Faulted dislocat<strong>ion</strong> loops contain a {111} stacking fault. From (60).<br />

Dislocat<strong>ion</strong> loops (perfect <strong>and</strong> faulted) act as nucleat<strong>ion</strong> sites for Si interstitials<br />

released from {113} defects during <strong>annealing</strong> at temperatures <strong>of</strong> 800 °C <strong>and</strong> above. This<br />

is termed a conservative Ostwald ripening process. The density <strong>of</strong> the dislocat<strong>ion</strong> loops<br />

will increase while the density <strong>of</strong> the {113} defects will decrease by a similar amount<br />

(73). For temperatures <strong>of</strong> 1000 °C <strong>and</strong> greater, perfect dislocat<strong>ion</strong> loops start to<br />

dissociate leaving large highly stable faulted dislocat<strong>ion</strong> loops that will be stable at<br />

1050 °C. A PDL can act as a sink for a {113} defect <strong>and</strong> a source for FDL at the same<br />

time (57). The dependence <strong>of</strong> the <strong>format<strong>ion</strong></strong> <strong>of</strong> the different types <strong>of</strong> defects on the<br />

implantat<strong>ion</strong> dose is illustrated in Figure 3.11.<br />

53

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