Anomalously high levels of ion-implanted B diffusivity (table 19) during pulse annealing were attributed to the participation of interstitial Si atoms in the redistribution of migrating B atoms between interstitial and vacancy diffusion mechanisms. At B+ doses of more than 1015/cm2, the high values of B diffusivity were caused by the effect of incompatibility elastic stresses (table 20) that prevented the transition of dopant atoms into lattice sites.
V.F.Stelmakh, J.R.Suprun-Belevich, A.R.Chelyadinski: Physica Status Solidi A, 1989, 112[1], 381-4
Table 19
Ambient Diffusion of B as a Function of B Dose, Si Dose, and Defect Concentration
B (/cm2) | Si (/cm2) | C (/cm3) | D (cm2/s) |
6 x 1013 | 0 | 5 x 1018 | 4 x 10-13 |
6 x 1013 | 6 x 1013 | 1.8 x 1020 | 1 x 10-12 |
6 x 1013 | 1 x 1014 | 2.3 x 1020 | 4 x 10-12 |
6 x 1013 | 6 x 1014 | - | 4 x 10-12 |
6 x 1014 | 0 | 5 x 1019 | 2 x 10-12 |
6 x 1014 | 6 x 1014 | - | 3.5 x 10-12 |
3.7 x 1015 | 0 | 1 x 1020 | 4 x 10-12 |
3.7 x 1015 | 6 x 1013 | 2.5 x 1020 | 4 x 10-12 |
3.7 x 1015 | 1 x 1014 | - | 4 x 10-12 |
3.7 x 1015 | 6 x 1014 | - | 4 x 10-12 |
Table 20
Ambient Diffusion of B as a Function of B Dose, Ge Dose, and Incompatibility Stress
B (/cm2) | Ge (/cm2) | S (N/m2) | D (cm2/s) |
6 x 1014 | 0 | 4 x 107 | 2.5 x 10-13 |
6 x 1014 | 5 x 1015 | - | 8 x 10-14 |
6 x 1014 | 1 x 1016 | - | 5 x 10-14 |
1.3 x 1015 | 0 | 9 x 107 | 4 x 10-13 |
1.3 x 1015 | 5 x 1015 | 6 x 107 | 2.5 x 10-13 |
1.3 x 1015 | 1 x 1016 | 5 x 107 | 1.3 x 10-13 |
2 x 1015 | 0 | 1.5 x 108 | 5 x 10-13 |
2 x 1015 | 5 x 1015 | - | 4 x 10-13 |
2 x 1015 | 1 x 1016 | 1 x 107 | 2.5 x 10-13 |