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Ion Implantation and Synthesis of Materials - Studium

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1.4 Atomic <strong>and</strong> Planar Densities 5(a)(b)Fig. 1.5. Schematic representation for (a) a single-crystal with crystallographic planesperpendicular to the surface <strong>and</strong> (b) a polycrystalline layer on a single-crystal1.4 Atomic <strong>and</strong> Planar DensitiesTo underst<strong>and</strong> the description <strong>of</strong> ion implantation <strong>and</strong> ion doses, one must knowthe atomic density interplanar distance between planes <strong>and</strong> the number <strong>of</strong>atoms cm −2 on a given plane. In cubic systems with an atomic density <strong>of</strong> Natoms cm −3 , the crystal lattice parameter, a c , is given byac⎛atoms/unit cell ⎞= ⎜ ⎟⎝ N ⎠1/3,(1.1)where, for systems with one atom per lattice point, there are four atoms per unitcell for a face-centered-cubic lattice (Al, Ag, Au, Pd, Pt) <strong>and</strong> there are eight forthe common semiconductors germanium (Ge) <strong>and</strong> silicon (Si), which have thediamond cubic structure. Aluminum has an atomic density <strong>of</strong> 6.02 × 10 22atoms cm −3 , so that the lattice parameter isac 221/3⎛ 4 ⎞−8= ⎜= 4.05 × 10 cm.6.02 × 10 ⎟⎝ ⎠(1.2)The atomic volume can be calculated without the use <strong>of</strong> crystallography. Theatomic density N <strong>of</strong> atoms cm −3 is given byAN = NAρ,(1.3)

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