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Ion Implantation and Synthesis of Materials - Studium

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88 7 Displacements <strong>and</strong> Radiation DamageNormal AtomInterstitial AtomPath <strong>of</strong> Primary ParticlePath <strong>of</strong> Primary Knock-OnFig. 7.5. Schematic <strong>of</strong> a highly damaged volume <strong>of</strong> material, formed when the mean freepath between collisions, λ d, approaches the atomic spacing <strong>of</strong> the target atoms. The densecascade is referred to as a displacement spike (after Brinkman, 1956)mean deposited energy density in the spike by3θ D = kT B2(7.14)where k B is Boltzmann’s constant.The quench time, t q , for a thermal spike <strong>of</strong> radius r is extremely small <strong>and</strong> canbe estimated bytq2= r4DT(7.15)(Davies 1983), where D T is the thermal diffusivity <strong>of</strong> the target. Using Au as anexample, with D T = 0.7 cm 2 s −1 . <strong>and</strong> assuming r = 8 nm, results in a quench time≈ 2 × 10 −13 s.

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