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Study of radiation damage in silicon detectors for high ... - F9

Study of radiation damage in silicon detectors for high ... - F9

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28 2. Operation and Radiation Damage <strong>of</strong> Silicon Detectorsab c de f ghFigure 2.6: Various possible defect congurations. Simple defects are: a) vacancy V, b)<strong>in</strong>terstitial <strong>silicon</strong> atom I, c) <strong>in</strong>terstitial impurity atom, d) substitutional impurity atom (e.g.phosphorus as donor). Examples <strong>of</strong> defect complexes are: e) close pair I-V, f) divacancy V-V,g) substitutional impurity atom and vacancy (e.g. VP complex), h) <strong>in</strong>terstitial impurity atomand vacancy (e.g, VO complex)capture processes and thus aect<strong>in</strong>g the leakage current. They can act as donors or acceptors, chang<strong>in</strong>g the eective dopant concentrationN eff thus aect<strong>in</strong>g the full depletion voltage. Increased capture probability decreases charge carrier lifetime thus decreas<strong>in</strong>g thecharge collection eciency.2.3.1 Leakage CurrentDefects generated due to ir<strong>radiation</strong> may <strong>in</strong>troduce energy levels <strong>in</strong> the band gap. Mostdefects have one energy level with two charge states as was also assumed <strong>in</strong> the derivation<strong>of</strong> the generation rate <strong>in</strong> the depleted region (section 2.1.5). Acceptors are negativelycharged when occupied by an electron and neutral when empty, while donors are positivelycharged when unoccupied but neutral otherwise. Some <strong>of</strong> the defects however have morethan one energy level and more charge states. Such an example is divacancy (V 2 ) withthree energy levels <strong>in</strong> the band gap, giv<strong>in</strong>g four charge states [28].As shown <strong>in</strong> section 2.1.5 the largest contribution to the leakage current comes

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