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Ion Implantation and Synthesis of Materials - Studium

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196 14 Application <strong>of</strong> <strong>Ion</strong> <strong>Implantation</strong> Techniques in CMOS FabricationFig. 14.2. Schematic illustration <strong>of</strong> (a) the intrusion <strong>of</strong> the source <strong>and</strong> drain depletionregions <strong>and</strong> (b) conduction b<strong>and</strong> energy along the surface. The dotted line represents thelong-channel condition, <strong>and</strong> the solid line represents the short-channel condition (afterMuller <strong>and</strong> Kamins 1986)ion straggling during dopant implantation <strong>and</strong> the anomalous dopant diffusionduring thermal annealing (see Chap. 9, Sect. 5). A physical picture <strong>of</strong> these twoeffects can be obtained with the help <strong>of</strong> the modeling program Stanford UniversityProcess Engineering Modeling (SUPREM, Law et al. 1986), which accounts forion straggling <strong>and</strong> dopant diffusion during the activation annealing process.Figure 14.3a, b shows the calculated two-dimensional boron atom distributions,obtained by using SUPREM for 5 keV boron implantation through a 100 nm wideaperture, before <strong>and</strong> after subsequent annealing at 1000°C for 10 s. The maximumlateral penetration depth (measured at the boron concentration <strong>of</strong> 1 × 10 18 cm −3 ) isaround 100 nm for the as-implanted pr<strong>of</strong>ile <strong>and</strong> around 200 nm for annealedpr<strong>of</strong>iles. This anomalous lateral spreading <strong>of</strong> dopants shows the severe challengeto the device scaling. The vertical <strong>and</strong> lateral spreading <strong>of</strong> dopants can bealleviated, but not eliminated, by using ultra low energy ion implantations. Allgroup IV <strong>and</strong> group V dopants show defect-enhanced diffusion phenomena calledtransient enhanced diffusion (TED) (see Chap. 9, Sect. 5). For n-type dopants suchas As <strong>and</strong> Sb, their diffusion is mediated by interaction with vacancies. Thediffusion <strong>of</strong> the p-type dopant B, on the other h<strong>and</strong>, is mediated by the interactionwith Si self interstitials. As <strong>and</strong> Sb have larger masses compared with B. Theheavier mass more easily creates an amorphous substrate layer during ionimplantations. Diffusivities <strong>of</strong> As <strong>and</strong> Sb are also slower than that <strong>of</strong> B. Therefore,the formation <strong>of</strong> B-doped p + ultra shallow junctions is more challenging than that<strong>of</strong> n + shallow junctions.

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