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+++
title = "Interface model"
weight = 11
+++
# Rough interface models
### Interface model
The mathematical model for one interface must be specified through one of
```python
ba.SelfAffineFractalModel(...)
ba.LinearGrowthModel(...)
```
These models define the behavior of autocorrelation function of roughness
or, better to say, its Fourier spectrum in the full range of spatial
frequencies from 0 to infinity.
##### Self-affine fractal model
```python
ba.SelfAffineFractalModel(sigma, hurst, lateral_corr_length, max_spatial_freq=0.5)
```
where
- `sigma`, $\sigma$, is the root-mean-square amptitude of out-of-plane
(transversal) fluctuation.
- `hurst`, $H$, is a fractal exponent `H` with `0<H<1`.
The smaller $H$ is, the more serrate the surface profile looks.
- `lateral_corr_length`, $\xi$, is the lateral (in-plane) correlation length.
- `max_spatial_freq`, $\nu_{max}$, is a cut-off spatial frequency.
This is the K-correlation model of
[Palasantzas 1993](https://doi.org/10.1103/PhysRevB.48.14472).
The autocorrelation spectrum is
$$
S(\nu)=\dfrac{4 \pi H \sigma^2\xi^2}{(1+(2\pi\nu)^2)^{1+H}} ,\quad
for \quad \nu<\nu_{max}
$$
In case there is no cut-off, the real-space roughness correlation
function at the interface is expressed as:
$$
< U(x, y) U(x', y')> = \sigma^2 \frac{2^{1-H}}{\Gamma(H)} \left(
\frac{\tau}{ξ} \right)^H K_H \left( \frac{\tau}{ξ} \right),
\quad \tau=[(x-x')^2+(y-y')^2]^{\frac{1}{2}}
$$
where $U(x, y)$ is the height deviation at position $(x, y)$.
The main property is that it remains nearly constant at low $\nu$
and transitions into a straight line on a log-log scale at high $\nu$,
exhibiting an inflection point between these two regions.
##### Linear growth model
```python
ba.LinearGrowthModel(particle_volume, damp1, damp2, damp3, damp4, max_spatial_freq=0.5)
```
where
- `particle_volume`, $\Omega$, is the volume of particle (atom, molecule, cluster)
coming to the surface during film deposition,
- `damp1-damp4`, $a_1-a_4$, are damping coefficients, responsible for replication
of underlying roughness and the growth of the new independent one,
- `max_spatial_freq`, $\nu_{max}$, is a cut-off spatial frequency.
This is the model described by [Stearns 1993](https://doi.org/10.1063/1.109593)
and extended by [Stearns and Gullikson 2000](https://doi.org/10.1016/S0921-4526(99)01897-9).
The model describes the evolution of the roughness spectrum on
the top surface of a growing film.
Its autocorrelation spectrum depends not only on the model parameters
but also on the film thickness
and the spectrum of the underlying interface.
Therefore, the model _cannot_ be applied directly to the substrate.
The autocorrelation spectrum is
$$
S_{above}(\nu)=S_{below}(\nu)e^{-b(\nu)t} + \Omega\dfrac{1-e^{-b(\nu)t}}{b(\nu)}, \quad
for \quad \nu<\nu_{max}
$$
where
$t$ - film thickness,
$b(\nu) = \sum{a_i\nu^i}$ - relaxation function
An essential property of the model is that it describes not only autocorrelation
but also cross-correlation properties.
Therefore, it _does not_ require [cross-correlation](../xcorr) to be specified separately.
|
