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

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damage evolut<strong>ion</strong> behaviour observed is strongly influenced by, on the one h<strong>and</strong>, the<br />

proximity <strong>of</strong> the surface, that acts as a nucleat<strong>ion</strong> centre for a fract<strong>ion</strong> <strong>of</strong> the interstitials<br />

produced along the collis<strong>ion</strong> cascade <strong>and</strong> on the other by the operat<strong>ion</strong> <strong>of</strong> dynamic<br />

<strong>annealing</strong> effects even at room temperature. These cause a substantial reduct<strong>ion</strong> in the<br />

disorder at depths where the interstitial <strong>and</strong> vacancy distribut<strong>ion</strong>s, which for <strong>low</strong><br />

energies are closely overlapping, have their maxima.<br />

The work reported here consists <strong>of</strong> a detailed MEIS study <strong>of</strong> the mode <strong>of</strong><br />

damage evolut<strong>ion</strong> as a funct<strong>ion</strong> <strong>of</strong> implant dose <strong>and</strong> its correlat<strong>ion</strong> with dopant<br />

movement for 2.5 keV As <strong>and</strong> 2 keV Sb <strong>ion</strong>s implanted into Si at room temperature to<br />

doses from a few times 10 13 cm -2 upwards.<br />

It will be seen that for both As <strong>and</strong> Sb <strong>ion</strong> implantat<strong>ion</strong>, the <strong>energy</strong> deposit<strong>ion</strong><br />

rate is sufficiently high for the Si matrix to become amorphised at room temperature for<br />

doses above 10 14 cm -2 . This study exploits the ability <strong>of</strong> MEIS to provide quantitative<br />

in<strong>format<strong>ion</strong></strong> on either the As or Sb <strong>implants</strong> <strong>and</strong> the Si damage depth distribut<strong>ion</strong>s.<br />

MEIS shows the operat<strong>ion</strong> at room temperature <strong>of</strong> a damage accumulat<strong>ion</strong> process for<br />

<strong>low</strong> doses that is explained in terms <strong>of</strong> interstitial trapping at pre-existing nucleat<strong>ion</strong><br />

sites formed by the oxide / Si crystal interface <strong>and</strong> the planar growth <strong>of</strong> the amorphous<br />

layer from the surface inwards into the bulk through the accumulat<strong>ion</strong> <strong>of</strong> point defects<br />

produced in the collis<strong>ion</strong> cascade. In particular, this work shows a novel dopant<br />

movement correlated to the growth <strong>of</strong> the amorphous layer that is driven by differences<br />

in the energetics <strong>of</strong> accommodat<strong>ion</strong> <strong>of</strong> these heavy <strong>ion</strong>s in damaged crystalline <strong>and</strong><br />

amorphous Si.<br />

5.2 Experimental<br />

Implants <strong>of</strong> 2.5 keV As <strong>ion</strong>s into Cz, p-type Si (100) samples <strong>of</strong> resistivity 10 –<br />

20 Ω cm were performed under UHV condit<strong>ion</strong>s using the ultra-<strong>low</strong> <strong>energy</strong> <strong>ion</strong><br />

implanter at Salford (21). Sb <strong>implants</strong> at 2 keV, were carried out in p-type (100) Si<br />

wafers <strong>of</strong> resistivity <strong>of</strong> 2– 10 Ω.cm at Applied Materials. In all cases the targets were<br />

held at room temperature <strong>and</strong> all <strong>implants</strong> were performed through the native oxide.<br />

The MEIS <strong>studies</strong> reported were carried out using a nominally 200 keV He <strong>ion</strong><br />

beam <strong>and</strong> the double alignment configurat<strong>ion</strong>, in which the [ 1 1 1]<br />

channelling direct<strong>ion</strong><br />

was combined with the [332] <strong>and</strong> [111] blocking direct<strong>ion</strong>s. Using a 200 keV He beam,<br />

sufficient separat<strong>ion</strong> <strong>of</strong> the dopant <strong>and</strong> Si peaks could be obtained for the [332] blocking<br />

direct<strong>ion</strong>. Results from the [332] direct<strong>ion</strong> only are presented here. The overall depth<br />

resolut<strong>ion</strong> obtained for these condit<strong>ion</strong>s was better than 0.7 nm (20). Energy spectra<br />

106

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