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

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Figure 3.11 Relat<strong>ion</strong>ship between implantat<strong>ion</strong> dose <strong>and</strong> <strong>annealing</strong>, on the type <strong>of</strong><br />

defects formed.<br />

Figure 3.12 Schematic two-dimens<strong>ion</strong>al representat<strong>ion</strong>s <strong>of</strong> direct diffus<strong>ion</strong><br />

mechanisms <strong>of</strong> an element A in a solid, via a) interstitial lattice sites <strong>and</strong><br />

b) substitut<strong>ion</strong>al lattice sites.<br />

Figure 3.13 Schematic two-dimens<strong>ion</strong>al representat<strong>ion</strong> <strong>of</strong> indirect diffus<strong>ion</strong><br />

mechanisms <strong>of</strong> an element A in a solid. Ai, As, V, <strong>and</strong> I denote<br />

interstitially <strong>and</strong> substitut<strong>ion</strong>ally dissolved foreign atoms, vacancies, <strong>and</strong><br />

silicon self-interstitials, respectively. AV <strong>and</strong> AI are defect pairs <strong>of</strong> the<br />

corresponding defects.<br />

Figure 4.1 Inelastic <strong>energy</strong> loss rates as a funct<strong>ion</strong> <strong>of</strong> <strong>energy</strong> for H in Si <strong>and</strong> He in<br />

Si <strong>and</strong> SiO2.<br />

Figure 4.2 MEIS scattering configurat<strong>ion</strong>.<br />

Figure 4.3 Graph <strong>of</strong> the inelastic <strong>energy</strong> loss rates, indicating how the <strong>energy</strong> loss<br />

values used in the surface approximat<strong>ion</strong> (blue lines) differs slightly<br />

from reality (green lines).<br />

Figure 4.4 Different orientat<strong>ion</strong>s <strong>of</strong> a Si Crystal. R<strong>and</strong>omly oriented, planar aligned,<br />

<strong>and</strong> aligned along the [110] direct<strong>ion</strong>.<br />

Figure 4.5 a) Shadow cone produced by a surface atom. b) Ions steered into the<br />

open channel.<br />

Figure 4.6 a) Schematic illustrat<strong>ion</strong>s <strong>of</strong> particles undergoing dechannelling,<br />

channelling <strong>and</strong> backscattering. b) Illustrat<strong>ion</strong> <strong>of</strong> the divergence <strong>of</strong> a<br />

collimated beam through an amorphous layer, which results in a high<br />

level <strong>of</strong> dechannelling.<br />

Figure 4.7 a) Plot <strong>of</strong> a Gaussian distribut<strong>ion</strong> b) The error funct<strong>ion</strong> in MEIS spectra<br />

is typically <strong>of</strong> the form <strong>of</strong> the integral <strong>of</strong> the Gaussian distribut<strong>ion</strong>. The<br />

st<strong>and</strong>ard deviat<strong>ion</strong> is indicated.<br />

Figure 4.8 The effects <strong>of</strong> <strong>energy</strong> straggling <strong>and</strong> the system resolut<strong>ion</strong>. For an ideal<br />

pr<strong>of</strong>ile a), <strong>energy</strong> straggling causes a broadening <strong>of</strong> the <strong>low</strong> <strong>energy</strong> edge<br />

b). The system resolut<strong>ion</strong> causes a broadening <strong>of</strong> both the leading <strong>and</strong><br />

<strong>low</strong> <strong>energy</strong> edges c).<br />

Figure 4.9 The effect <strong>of</strong> convoluting different ideal peak shapes with a single<br />

Gaussian funct<strong>ion</strong>. a) A layer that is wide compared to the width <strong>of</strong> the<br />

Gaussian. b) A very thin layer. c) A layer with a width similar to the<br />

Gaussian. d) An interface with a broad <strong>energy</strong> distribut<strong>ion</strong>.<br />

Figure 4.10 Illustrat<strong>ion</strong> <strong>of</strong> the Daresbury MEIS facility.<br />

Figure 4.11 MEIS Azimuthal alignment axes.<br />

Figure 4.12 MEIS analyser <strong>and</strong> detector scattering configurat<strong>ion</strong>.<br />

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