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4.4.2 Segregation Model

  At the early stage of a diffusion process equilibrium at the material interface is not reached, hence, we have to define a diffusion flux tex2html_wrap_inline4781 across the interface box area which accounts for the segregation kinetics, as given by (4.4-4), where tex2html_wrap_inline5909 denotes the transport coefficient.

  equation1742

tex2html_wrap_inline5909 determines how fast any disturbance of the equilibrium conditions at the interface is compensated by the dopant flux across the interface. After thermal equilibrium is reached the ratio of the concentrations on each side of the boundary are given by the according segregation coefficient m.

Generally, segregation coefficients are extracted form experiments under certain process conditions. It is possible to trace the dopant concentration across the interface with SIMS analysis, followed by the extraction of the segregation data to obtain good simulation results. Unfortunately, segregation behavior is influenced by other process conditions like local hydrogen or florine content in the material layers. Advanced process technologies are even able to control the segregation process. During the fabrication of the gate oxide it is common to blow in nitrogen at the end of the oxidation process for several seconds. This short term nitridation affects the segregation conditions at the gate oxide interface significantly. Thus the oxide layer represents a stable diffusion barrier for dopants [Mat93].

Generally, the silicon/silicon dioxide interface is of vital importance for process development. The most commonly used p-type dopant, boron, exhibits strong tendencies to accumulate in the oxide (m ;SPMlt; 1), where phosphorus shows the opposite segregation behavior (m ;SPMgt; 1). Segregation data [Plu86] for several dopants at the silicon/silicon dioxide interface are given in Table 4.4-1.

 

Segregation Parameters
P tex2html_wrap_inline5301 tex2html_wrap_inline5303
tex2html_wrap_inline5909 tex2html_wrap_inline5929 cm/s

Boron

m 1126.0 tex2html_wrap_inline5937
tex2html_wrap_inline5909 tex2html_wrap_inline5929 cm/s

Arsenic

m 30.0
tex2html_wrap_inline5909 tex2html_wrap_inline5929 cm/s

Phosphorus

m 30.0
tex2html_wrap_inline5909 tex2html_wrap_inline5929 cm/s

Antimony

m 30.0
Table 4.4-1: Segregation parameter for the most common dopants given for the Si- tex2html_wrap_inline4711 material interface. For k and m an Arrhenius law tex2html_wrap_inline5981 is assumed.

 


next up previous contents
Next: 4.4.3 Poly-/Monosilicon Model Up: 4.4 Material Interface Models Previous: 4.4.1 Conduction Model

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