dopant diffusion

Dopant diffusion is the thermally driven movement of impurity atoms (B, P, As, Sb) through the silicon crystal lattice at elevated temperatures, redistributing dopant concentration profiles introduced by ion implantation or surface deposition. The process follows Fick's laws of diffusion: J = -D × (dC/dx) where J is the dopant flux, D is the diffusion coefficient, and dC/dx is the concentration gradient. The diffusion coefficient follows an Arrhenius relationship: D = D₀ × exp(-Ea/kT), where D₀ is the pre-exponential factor, Ea is activation energy (~3-4 eV for common dopants in Si), k is Boltzmann's constant, and T is absolute temperature. Diffusion increases exponentially with temperature—at 1100°C, boron diffuses roughly 100× faster than at 900°C. Diffusion mechanisms in silicon: (1) vacancy-mediated (dopant atom exchanges position with a neighboring vacant lattice site—dominant for arsenic and antimony), (2) interstitial-mediated (dopant atom moves between lattice sites through interstitial positions—dominant for boron and phosphorus), (3) kick-out mechanism (interstitial atom displaces a substitutional dopant, which then diffuses as an interstitial until it re-enters a substitutional site). Transient enhanced diffusion (TED): after ion implantation, excess point defects (interstitials and vacancies) created by implant damage dramatically accelerate dopant diffusion above equilibrium rates during the first few minutes of annealing. TED is the primary obstacle to forming ultra-shallow junctions—even brief anneals can push boron junctions 5-20nm deeper than expected. Diffusion management at advanced nodes: minimizing thermal budget (spike, flash, and laser annealing), using heavy ions (As instead of P for n-type, BF₂ instead of B for p-type), and using diffusion-retarding co-implants (carbon co-implant traps excess interstitials, reducing boron TED by 50-90%).