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

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The “zero” depth point in the MEIS depth pr<strong>of</strong>iles is always taken at the sample<br />

surface, <strong>and</strong> the depth <strong>of</strong> the a/c interface is measured in relat<strong>ion</strong> to the surface. XRD<br />

however takes the “zero” point <strong>of</strong> the depth scale at some depth in the reg<strong>ion</strong> <strong>of</strong> the<br />

amorphous to crystalline interface as it is only sensitive to the crystalline material <strong>and</strong><br />

hence does not “see” the amorphous Si. Obviously this point is at a different depth for<br />

each sample. The other difference between the techniques that affects the<br />

recrystallisat<strong>ion</strong> depth measured, results from differences in criteria for the end point.<br />

The depths in MEIS are based upon the a/c interfaces <strong>and</strong> as such the regrown layer<br />

thickness is determined by subtracting the depth <strong>of</strong> the a/c interface fol<strong>low</strong>ing <strong>annealing</strong><br />

from the depth <strong>of</strong> the original a/c interface. In XRD the end point is the strained reg<strong>ion</strong><br />

around the EOR defects. This would be deeper than the a/c interface. The regrown layer<br />

thickness is given from the distance between this point <strong>and</strong> the reg<strong>ion</strong> <strong>of</strong> strain near to<br />

the zero depth point be<strong>low</strong> the a/c interface, i.e. the distance between reg<strong>ion</strong> 1 <strong>and</strong> 3<br />

shown in Figure 6.21a).<br />

In Figure 6.23 the strain pr<strong>of</strong>iles obtained from XRD measurements (Figure<br />

6.21a)) have been rescaled by a shift <strong>of</strong> each pr<strong>of</strong>ile for direct comparison to the MEIS<br />

spectra in the fol<strong>low</strong>ing way. The EOR damage reg<strong>ion</strong>, which causes the strongest<br />

contrast in XRD curves, has been arbitrarily located at the back edge <strong>of</strong> the asimplanted<br />

Si amorphous layer <strong>and</strong> its posit<strong>ion</strong> has been kept fixed during the <strong>annealing</strong>,<br />

as would be expected for EOR defects in this temperature range. The peak is located at<br />

a depth <strong>of</strong> 13.5 – 16.5 nm. As a result <strong>of</strong> this rescaling <strong>of</strong> the depth, Figure 6.23 shows<br />

the disordered Si pr<strong>of</strong>ile from MEIS superimposed by the lattice strain pr<strong>of</strong>ile from the<br />

fits <strong>of</strong> the XRD curves. The a/c interface from XRD always aligns with the back edge <strong>of</strong><br />

the Si peak in MEIS (i.e. area <strong>of</strong> strong lattice disorder).<br />

155

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