A visco-elastic oxide growth model has been developed at our institute using FEM as the simulation environment [80]. The model is three-dimensional and does not rely on a simple expression for the interface motion, but rather relies on calculations of oxidant diffusion and oxide volume expansion in three dimensions to move the FEM mesh appropriately. A major limitation of FEM analysis is related to the mesh used for simulations. As either the time or space increments are decreased, or the mesh is made finer, the number of calculations necessary to simulate oxide growth can increase by a factor dependent on the model itself [34], [159]. Some models also do not account for orientation dependence adequately or the error can be a non-linear function which can amplify significantly with further iterations [229].

The model presented in [80] is based on a few main equations. The first equation is meant to describe oxidant diffusion

(72) |

where is the Laplace operator, is the oxidant concentration in the material, and is the temperature dependent low stress diffusion coefficient. is the strength of a spatial sink and not a simple reaction coefficient at a sharp interface

(73) |

where is the maximal possible strength of the sink.

The next equation is meant to deal with the dynamics of

(74) |

where is the volume expansion factor (=2.25) for the reaction from Si to SiO, and is the number of oxidant molecules incorporated into a unit of SiO volume.

The volume increase of the generating oxide occurs successively and not abruptly because of the diffuse interface concept. A volume increase of the oxidized material is calculated using the and values. After a given time , the normalized additional volume is given by

An important aspect of (3.4) is that the sum of over all time steps must not exceed 125%, which is the maximum volume expansion of the material during oxidation.

Since the principal axis components of the residual strain tensor are linearly proportional to in the form

(76) |

the normalized additional volume directly loads the mechanical problem. Using Hook's law, the stress tensor is given by

where is the so-called material matrix, constructed in Lame's form [80], is the strain tensor, is the residual strain tensor, and is the residual stress tensor. The material matrix is rebuilt and (3.6) becomes

(78) |

where is the Young's modulus, is the Poisson ratio, and are the shear strain components.

The effective shear modulus can be added to to handle elastic and visco-elastic materials. For elastic materials

(79) |

while for visco-elastic materials

(80) |

where is the Maxwellian relaxation time constant and is the effective shear modulus.

L. Filipovic: Topography Simulation of Novel Processing Techniques