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

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The higher temperature anneals carried out at 700 °C for 15s <strong>and</strong> 1050 °C spike<br />

anneal, shown in Figure 6.25d) with their faster regrowth rates produced a fully regrown<br />

layer, with less As visible in the regrown layer <strong>and</strong> hence a clear segregated peak.<br />

In summary <strong>of</strong> these results, the wide amorphous / crystalline transit<strong>ion</strong> reg<strong>ion</strong>s<br />

observed in the MEIS spectra fol<strong>low</strong>ing anneals where regrowth is not completed are<br />

unique for SOI. The continued visibility <strong>of</strong> the As in the regrown layer, typical for the<br />

regrowth <strong>of</strong> SOI pre-amorphised samples, is also an unusual feature.<br />

6.4.3.3 Bulk Si, 60, 100 nm SOI, PAI, 3 <strong>and</strong> 1 keV BF2<br />

Experiments similar to the ones reported above were carried out using BF2<br />

<strong>implants</strong>. Samples were produced from bulk Si, 60 nm, <strong>and</strong> 100 nm SOI wafers,<br />

respectively. All samples were pre-amorphised with 40 keV Xe to a dose <strong>of</strong> 1E14<br />

<strong>ion</strong>s/cm 2 , <strong>and</strong> implanted with 1 or 3 keV BF2 + to a dose <strong>of</strong> 7E14 <strong>ion</strong>s/cm 2 .<br />

MEIS results for the 3 keV BF2 <strong>implants</strong> into bulk Si are shown in Figure 6.26a)<br />

for anneals at 550 °C for 600s <strong>and</strong> at 600 °C for 60s. For both samples, the regrowth has<br />

proceeded in the convent<strong>ion</strong>al SPER manner as is usual for bulk Si. There is no wide<br />

transit<strong>ion</strong> layer from amorphous to crystalline. The anneals have not produced complete<br />

regrowth, since there remains a ~ 4 nm wide Si surface peak after the 550 °C anneal <strong>and</strong><br />

a ~ 3 nm wide Si surface peak after the 600 °C anneal. The growth <strong>of</strong> the oxide layer<br />

thickness only partially accounts for the width <strong>of</strong> these layers.<br />

MEIS results for 60 nm SOI samples using identical implant condit<strong>ion</strong>s are<br />

shown in Figure 6.26b), the only difference with this set <strong>of</strong> samples is the wafer<br />

material, i.e. SOI. Si damage pr<strong>of</strong>iles with wide a/c interfaces similar to those in the PAI<br />

As implanted samples (sect<strong>ion</strong> 6.4.3.2) are also seen with these samples. The sample<br />

annealed at 550 °C for 600 s has a very broad transit<strong>ion</strong> from crystalline to amorphous<br />

Si taking place over a depth <strong>of</strong> ~ 14 nm. The sample annealed at 600 °C for 60 s also<br />

has high level <strong>of</strong> residual damage at a depth from 6 to 16 nm, behind a 6 nm wide<br />

highly damaged / amorphous surface peak. The samples annealed at 650 °C <strong>and</strong> 700 °C<br />

for 15 s both show good regrowth. This is in contrast to the As implanted sample<br />

annealed at 650 °C for 15s, shown in 6.25c), which is not yet fully regrown, attributed<br />

to the effect <strong>of</strong> the high As concentrat<strong>ion</strong> s<strong>low</strong>ing down the regrowth.<br />

Lastly the 100 nm SOI wafer was pre-amorphised <strong>and</strong> then implanted with<br />

1 keV BF2 to a dose <strong>of</strong> 7E14 <strong>ion</strong>s/cm 2 . An equivalent 3 keV BF2 implanted sample was<br />

not available. It is not likely that the different BF2 <strong>energy</strong> will cause a fundamentally<br />

different behaviour. The results are shown in Figure 6.26c) <strong>and</strong> they prove almost<br />

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