Identical sets of thermal oxidation and nitridation experiments were performed because selectively perturbing equilibrium point-defect concentrations by using these surface reactions was a means for identifying the relative importance of various atomic-scale diffusion mechanisms. Bounds were obtained on the fractional contributions of self-interstitials, vacancies and concerted exchange mechanisms to diffusion at 1100 and 1000C (tables 4 and 5). The bounds were found by simultaneously solving a system of equations while making only very conservative assumptions. It was found that B diffused via a self-interstitial mechanism.

Fractional Contributions of Microscopic Diffusion Mechanisms for Common Dopants and Self-Diffusion in Silicon. A.Ural, P.B.Griffin, J.D.Plummer: Journal of Applied Physics, 1999, 85[9], 6440-6. See also: Applied Physics Letters, 1998, 73[12], 1706-8

 

Table 5

Diffusivity Enhancement or Retardation for B in Si

Temperature (C)

Method

Factor

1100

oxidation

3.07

1100

nitridation

0.421

1000

oxidation

4.70

1000

nitridation

0.341