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

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The as-implanted sample, with a broad As distribut<strong>ion</strong> (seen from MEIS), does<br />

not provide sufficient density contrast to be visible in SR.<br />

In terms <strong>of</strong> the behaviour <strong>of</strong> the oxide layer, both MEIS <strong>and</strong> SR show the SiO2<br />

layer growing in thickness with increasing thermal budget. The measurements <strong>of</strong> the<br />

width <strong>of</strong> the SiO2 are in reasonable agreement, within the experimental accuracy <strong>and</strong> are<br />

given in Table 6.1. The small differences may be simply due to different measurement<br />

criteria. MEIS shows that the oxide peaks appear to contain a reg<strong>ion</strong> <strong>of</strong> suboxide<br />

(Figure 6.4c), which are not included in the oxide widths in Table 6.1, based on FWHM.<br />

It is not clear how the SiO2 layer is defined in the SR measurements.<br />

To conclude this comparison sect<strong>ion</strong>, it has been shown that the combined use <strong>of</strong><br />

MEIS <strong>and</strong> SR can provided complementary <strong>and</strong> addit<strong>ion</strong>al in<strong>format<strong>ion</strong></strong>. MEIS has<br />

provided the essential starting point for an unambiguous modelling <strong>of</strong> the SR curves.<br />

SR with the better depth resolut<strong>ion</strong> gives the width <strong>of</strong> the segregated As layer to be 0.7<br />

nm. Within the accuracy <strong>of</strong> the two techniques they give good agreement on the depth<br />

<strong>of</strong> the segregated peak <strong>and</strong> the trends in the oxide layer width.<br />

6.2.4 Reduct<strong>ion</strong> in implant <strong>energy</strong> – 1 keV As implantat<strong>ion</strong> <strong>and</strong> <strong>annealing</strong><br />

In terms <strong>of</strong> improvements in junct<strong>ion</strong> depth a common trend in manufacturing<br />

has been to reduce the implant <strong>energy</strong>. In this sect<strong>ion</strong> the results <strong>of</strong> 1 keV As<br />

implantat<strong>ion</strong> are presented as a comparison to the 3 keV results described in sect<strong>ion</strong><br />

6.2.3. It is shown that diffus<strong>ion</strong> is far more critical in determining the final junct<strong>ion</strong><br />

depth than the implantat<strong>ion</strong> <strong>energy</strong> <strong>and</strong> hence a reduct<strong>ion</strong> in beam <strong>energy</strong> may not<br />

necessarily lead to an improvement in junct<strong>ion</strong> depth.<br />

6.2.4.1 Experimental<br />

MEIS <strong>and</strong> SIMS analysis was carried out on a similar batch <strong>of</strong> samples to the<br />

previous set but with a 1 keV implant instead <strong>of</strong> 3 keV. The dose was again 2E15 cm -2 .<br />

As with the previous samples, <strong>implants</strong> were carried out into crystalline (NoPAI) <strong>and</strong><br />

pre-amorphised (PAI) wafers. The pre-amorphising implant was a 130 keV Xe to a dose<br />

<strong>of</strong> 2E14 cm -2 , producing a 100 nm amorphous layer (13). Samples were annealed with a<br />

furnace anneal at 600 °C for 20 min, rapid thermal annealed at 1000 °C for 5s <strong>and</strong><br />

1025 °C for 10s, <strong>and</strong> spike annealed at 1050 °C. MEIS analysis was performed using a<br />

100 keV He + beam. The results <strong>of</strong> the [332] blocking direct<strong>ion</strong> are presented here. The<br />

shal<strong>low</strong>er implantat<strong>ion</strong> does not require as large an <strong>energy</strong> separat<strong>ion</strong> <strong>of</strong> the peaks as in<br />

the case <strong>of</strong> a 3 keV implant <strong>and</strong> so the [332] direct<strong>ion</strong> with its better depth resolut<strong>ion</strong><br />

132

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