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

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thermal <strong>annealing</strong> (600 – 700 °C <strong>and</strong> form small aggregates <strong>of</strong> Si interstitials, with the<br />

most stable “magic” clusters being made up <strong>of</strong> 4 <strong>and</strong> 8 atoms (55). For longer anneal<br />

times <strong>and</strong> higher temperatures, the excess interstitials condense into extended defects<br />

(56). This category <strong>of</strong> defects consist <strong>of</strong> {113}’s, perfect dislocat<strong>ion</strong> loops (PDL’s) <strong>and</strong><br />

faulted dislocat<strong>ion</strong> loops (FDL’s) <strong>and</strong> TEM images <strong>of</strong> each are shown in Figure 3.9.<br />

Figure 3.9 TEM images <strong>of</strong> defects present in the<br />

EOR damage area <strong>of</strong> <strong>ion</strong> implanted Si. These are<br />

clusters, {113}s, PDLs, <strong>and</strong> FDLs. From (56).<br />

{113} rod like defects are formed from smaller clusters <strong>and</strong> can become visible<br />

in a TEM from lengths <strong>of</strong> 2 nm (57). The {113} defects are bundles <strong>of</strong> rows <strong>of</strong> Si diinterstitials<br />

that lie on {113} planes <strong>and</strong> which are elongated along direct<strong>ion</strong>s<br />

<strong>and</strong> consist <strong>of</strong> condensates <strong>of</strong> interstitials forming five <strong>and</strong> seven – membered rings (58).<br />

This atomic arrangement provides a way to insert planes <strong>of</strong> self interstitials without<br />

dangling bonds (58). They have a constant width <strong>of</strong> 4 nm. Once {113} defects are<br />

formed, further <strong>annealing</strong> can make the larger {113}’s grow in size at the expense <strong>of</strong> the<br />

smaller ones, thereby reducing the density <strong>of</strong> {113}’s.<br />

Dislocat<strong>ion</strong> loops form in the most densely packed crystal planes for reason <strong>of</strong><br />

<strong>energy</strong> minimisat<strong>ion</strong>. Typically the loops consist <strong>of</strong> circular extra {111} planes <strong>of</strong> Si<br />

interstitials with the lattice elongated along direct<strong>ion</strong>s. Perfect dislocat<strong>ion</strong> loops<br />

52

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