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

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The s<strong>low</strong>er, or initially delayed, regrowth on SOI is also apparent with these<br />

samples. It is most noticeable with the samples annealed for 50s. For the SOI sample,<br />

regrowth to a depth around 20 nm has occurred but the bulk sample has regrown to a<br />

depth <strong>of</strong> approximately 6 nm. The samples annealed for 200s also show a large<br />

difference in the amount <strong>of</strong> damage regrowth between SOI <strong>and</strong> bulk Si. The samples<br />

annealed for 70s appear to show a similar level <strong>of</strong> regrowth between bulk Si <strong>and</strong> SOI.<br />

However for both samples the a/c interface is at a depth where there is a high As<br />

concentrat<strong>ion</strong> <strong>and</strong> hence the regrowth rate is very s<strong>low</strong>. The bulk sample has regrown<br />

by an extra 2nm compared to the SOI sample. With the regrowth rate so <strong>low</strong> in this area<br />

this is a significant difference in depth. Indeed the depth <strong>of</strong> the a/c interface <strong>of</strong> the bulk<br />

Si sample annealed for 70s is close to the depth <strong>of</strong> the SOI sample annealed for 200s.<br />

6.4.4 Discuss<strong>ion</strong><br />

Before the regrowth mechanisms can be considered it is important to discuss the<br />

detail <strong>of</strong> the a/c interfaces. In Figure 6.28a) <strong>and</strong> b) are 2D schematic illustrat<strong>ion</strong>s<br />

showing entirely different possible damage scenarios. In these illustrat<strong>ion</strong>s black<br />

represents fully amorphous Si <strong>and</strong> white represents fully crystalline Si. Different levels<br />

<strong>of</strong> shading <strong>of</strong> grey represent different levels <strong>of</strong> damage between amorphous <strong>and</strong><br />

crystalline. The right h<strong>and</strong> side <strong>of</strong> each illustrat<strong>ion</strong> represents the surface. The<br />

approximate shape <strong>of</strong> the idealised MEIS pr<strong>of</strong>ile (ignoring <strong>energy</strong> straggling <strong>and</strong> system<br />

resolut<strong>ion</strong> convolut<strong>ion</strong>) is given underneath each image. Figure 6.28a) illustrates a<br />

situat<strong>ion</strong> where there is a gradual transit<strong>ion</strong> from the crystalline reg<strong>ion</strong> with increasing<br />

damage until an amorphous layer is reached. In Figure 6.28b) a sharp wavy interface<br />

between fully crystalline <strong>and</strong> fully amorphous Si is presented. Both scenarios would<br />

produce a similar shape in a MEIS pr<strong>of</strong>ile, hence MEIS alone cannot distinguish<br />

between them.<br />

To determine the pr<strong>of</strong>ile XTEM was carried out on the 60 nm SOI sample, preamorphised,<br />

implanted with 3keV As to 1E15 cm -2 , <strong>and</strong> annealed at 550 °C for 600s<br />

(MEIS result Figure 6.25a)). The result is shown in Figure 6.29. It shows that the a/c<br />

interface is indeed wavy in an irregular fash<strong>ion</strong>, over a depth range <strong>of</strong> ~ 14 nm. This in<br />

excellent agreement with the depth range <strong>of</strong> the a/c interface from MEIS results.<br />

165

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