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

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with are comparatively small, ~ 0.5 nm, but effort was put into this area in an effort to<br />

maximise the high resolut<strong>ion</strong> potential <strong>of</strong> the technique.<br />

4.2.3.1 Stopping powers<br />

At an early stage it was observed that a variat<strong>ion</strong> <strong>of</strong> up to 9 % existed between<br />

depth pr<strong>of</strong>iles converted from MEIS spectra taken on the same sample using 100 keV or<br />

200 keV He + beam energies. An example <strong>of</strong> these depth pr<strong>of</strong>iles is shown in the top <strong>of</strong><br />

Figure 4.17, including data taken using a 150 keV beam. The discrepancy in the peak<br />

centres is indicated with dashed lines. The cause <strong>of</strong> this discrepancy was an incorrect<br />

slope <strong>of</strong> the inelastic loss curve. There have recently been a number <strong>of</strong> <strong>studies</strong> with the<br />

aim to improve the accuracy <strong>of</strong> stopping powers (32, 33, 34, 35). The solut<strong>ion</strong> that<br />

produced consistent depth scales was found with the release <strong>of</strong> the 2003 vers<strong>ion</strong> <strong>of</strong><br />

SRIM. The stopping powers have been significantly improved from the last major<br />

update in SRIM 1998 (20). The updated <strong>energy</strong> loss rates are compared with those <strong>of</strong><br />

the SRIM 2000 vers<strong>ion</strong> in Figure 4.18. The use <strong>of</strong> the new inelastic loss data largely<br />

eliminated the discrepancy at the two energies as demonstrated in the depth pr<strong>of</strong>iles in<br />

the bottom <strong>of</strong> Figure 4.17.<br />

88

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