The grain-boundary diffusion of dopants was reviewed. Literature data for thick and thin samples were analyzed by using an homogeneous semi-infinite substrate. It was concluded that grain-boundary diffusion could be readily analyzed by using the correct model. It was shown that the ratio of grain boundary to bulk diffusivity ranged from 103 to 105 and was a function of temperature and dopant type. Data obtained from thin-film systems were shown to be consistent with the Gilmer-Farrell thin-film model. This model was used to deduce that the diffusion could be described by:

D(cm2/s) = 4 x 10-3exp[-1.71(eV)/kT]

A.D.Buonaquisti, W.Carter, P.H.Holloway: Thin Solid Films, 1983, 100[3], 235-48

 

Table 89

Diffusivity Ratios of 30Si and P in Si during Oxidation at 800 to 1100C

 

Temperature (C)

30Si

P

Interstitial Mediation (%)

1100

1.53

2.69

50.2

1000

2.46

4.09

57.5

900

5.16

8.39

60.5

800

14.57

23.60

61.4

 

obtained from thin-film systems were shown to be consistent with the Gilmer-Farrell thin-film model. This model was used to deduce that the diffusion could be described by:

D(cm2/s) = 4 x 10-3exp[-1.71(eV)/kT]

A.D.Buonaquisti, W.Carter, P.H.Holloway: Thin Solid Films, 1983, 100[3], 235-48

 

Table 89

Diffusivity Ratios of 30Si and P in Si during Oxidation at 800 to 1100C

 

Temperature (C)

30Si

P

Interstitial Mediation (%)

1100

1.53

2.69

50.2

1000

2.46

4.09

57.5

900

5.16

8.39

60.5

800

14.57

23.60

61.4

 

Figure 13

Diffusion of P and Si in Si

 

Table 90

Grain Boundary Diffusion of P in Polycrystalline Si

 

Temperature (C)

Dδ (cm3/s)

566

4.96 x 10-25

639

6.00 x 10-24

693

1.26 x 10-23

793

5.66 x 10-22

980

8.26 x 10-20