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Mathematics Modeling

1. Crystal Growth (Czochralski Process)

Growing single-crystal silicon ingots requires coupled models for heat transfer, fluid flow, and mass transport.

1.1 Heat Transfer Equation

$$\rho c_p \frac{\partial T}{\partial t} + \rho c_p \mathbf{v} \cdot \nabla T = \nabla \cdot (k \nabla T) + Q$$

Variables:

1.2 Melt Convection Drivers

1.3 Dopant Segregation

Equilibrium segregation coefficient:

$$k_0 = \frac{C_s}{C_l}$$

Effective segregation coefficient (Burton-Prim-Slichter model):

$$k_{eff} = \frac{k_0}{k_0 + (1 - k_0) \exp\left(-\frac{v \delta}{D}\right)}$$

Variables:

2. Thermal Oxidation (Deal-Grove Model)

The foundational model for growing $\text{SiO}_2$ on silicon.

2.1 General Equation

$$x_o^2 + A x_o = B(t + \tau)$$

Variables:

2.2 Growth Regimes

$$ x_o \approx \frac{B}{A}(t + \tau)$$
$$ x_o \approx \sqrt{B(t + \tau)}$$

2.3 Extended Model Considerations

3. Diffusion and Dopant Transport

3.1 Fick's Laws

First Law (flux equation):

$$\mathbf{J} = -D \nabla C$$

Second Law (continuity equation):

$$\frac{\partial C}{\partial t} = \nabla \cdot (D \nabla C)$$

For constant $D$:

$$\frac{\partial C}{\partial t} = D \nabla^2 C$$

3.2 Concentration-Dependent Diffusivity

$$D(C) = D_i + D^{-} \frac{n}{n_i} + D^{2-} \left(\frac{n}{n_i}\right)^2 + D^{+} \frac{p}{n_i} + D^{2+} \left(\frac{p}{n_i}\right)^2$$

Variables:

3.3 Point-Defect Mediated Diffusion

Effective diffusivity:

$$D_{eff} = D_I \frac{C_I}{C_I^*} + D_V \frac{C_V}{C_V^*}$$

Point defect continuity equations:

$$\frac{\partial C_I}{\partial t} = D_I \nabla^2 C_I + G_I - R_{IV}$$
$$\frac{\partial C_V}{\partial t} = D_V \nabla^2 C_V + G_V - R_{IV}$$

Recombination rate:

$$R_{IV} = k_{IV} \left( C_I C_V - C_I^* C_V^* \right)$$

Variables:

3.4 Transient Enhanced Diffusion (TED)

Ion implantation creates excess interstitials causing:

4. Ion Implantation

4.1 Gaussian Profile Model

$$N(x) = \frac{\phi}{\sqrt{2\pi} \Delta R_p} \exp\left[ -\frac{(x - R_p)^2}{2 (\Delta R_p)^2} \right]$$

Variables:

4.2 Pearson IV Distribution

For asymmetric profiles using four moments:

4.3 Monte Carlo Methods (TRIM/SRIM)

Stopping power:

$$\frac{dE}{dx} = S_n(E) + S_e(E)$$

Key outputs:

4.4 Channeling Effects

For crystalline targets, ions aligned with crystal axes experience:

5. Plasma Etching

5.1 Surface Kinetics Model

$$\frac{\partial \theta}{\partial t} = J_i s_i (1 - \theta) - k_r \theta$$

Variables:

5.2 Etching Yield

$$Y = \frac{\text{atoms removed}}{\text{incident ion}}$$

Dependence factors:

5.3 Profile Evolution (Level Set Method)

$$\frac{\partial \phi}{\partial t} + V |\nabla \phi| = 0$$

Variables:

5.4 Knudsen Transport in High Aspect Ratio Features

For molecular flow regime ($Kn > 1$):

$$\frac{1}{\lambda} \frac{dI}{dx} = -I + \int K(x, x') I(x') dx'$$

Key effects:

6. Chemical Vapor Deposition (CVD)

6.1 Transport-Reaction Equation

$$\frac{\partial C}{\partial t} + \mathbf{v} \cdot \nabla C = D \nabla^2 C - k C^n$$

Variables:

6.2 Thiele Modulus

$$\phi = L \sqrt{\frac{k}{D}}$$

Regimes:

6.3 Step Coverage

Conformality factor:

$$S = \frac{\text{thickness at bottom}}{\text{thickness at top}}$$

Models:

6.4 Atomic Layer Deposition (ALD)

Self-limiting surface coverage:

$$\theta(t) = 1 - \exp\left( -\frac{p \cdot t}{\tau} \right)$$

Variables:

Growth per cycle (GPC):

$$\text{GPC} = \theta_{sat} \cdot \Gamma_{ML}$$

where $\Gamma_{ML}$ is the monolayer thickness.

7. Chemical Mechanical Polishing (CMP)

7.1 Preston Equation

$$\frac{dz}{dt} = K_p \cdot P \cdot V$$

Variables:

7.2 Pattern-Dependent Effects

Effective pressure:

$$P_{eff} = \frac{P_{applied}}{\rho_{pattern}}$$

where $\rho_{pattern}$ is local pattern density.

Key phenomena:

7.3 Contact Mechanics

Hertzian contact pressure:

$$P(r) = P_0 \sqrt{1 - \left(\frac{r}{a}\right)^2}$$

Pad asperity models:

8. Lithography

8.1 Aerial Image Formation

Hopkins formulation (partially coherent):

$$I(\mathbf{x}) = \iint TCC(\mathbf{f}, \mathbf{f}') \, M(\mathbf{f}) \, M^*(\mathbf{f}') \, e^{2\pi i (\mathbf{f} - \mathbf{f}') \cdot \mathbf{x}} \, d\mathbf{f} \, d\mathbf{f}'$$

Variables:

8.2 Resolution and Depth of Focus

Rayleigh resolution criterion:

$$R = k_1 \frac{\lambda}{NA}$$

Depth of focus:

$$DOF = k_2 \frac{\lambda}{NA^2}$$

Variables:

8.3 Photoresist Exposure (Dill Model)

Photoactive compound (PAC) decomposition:

$$\frac{\partial m}{\partial t} = -I(z, t) \cdot m \cdot C$$

Intensity attenuation:

$$I(z, t) = I_0 \exp\left( -\int_0^z [A \cdot m(z', t) + B] \, dz' \right)$$

Dill parameters:

8.4 Development Rate (Mack Model)

$$r = r_{max} \frac{(a + 1)(1 - m)^n}{a + (1 - m)^n}$$

Variables:

8.5 Computational Lithography

9. Device Simulation (TCAD)

9.1 Poisson's Equation

$$\nabla \cdot (\epsilon \nabla \psi) = -q(p - n + N_D^+ - N_A^-)$$

Variables:

9.2 Carrier Continuity Equations

Electrons:

$$\frac{\partial n}{\partial t} = \frac{1}{q} \nabla \cdot \mathbf{J}_n + G - R$$

Holes:

$$\frac{\partial p}{\partial t} = -\frac{1}{q} \nabla \cdot \mathbf{J}_p + G - R$$

Variables:

9.3 Drift-Diffusion Current Equations

Electron current:

$$\mathbf{J}_n = q n \mu_n \mathbf{E} + q D_n \nabla n$$

Hole current:

$$\mathbf{J}_p = q p \mu_p \mathbf{E} - q D_p \nabla p$$

Einstein relation:

$$D = \frac{k_B T}{q} \mu$$

9.4 Advanced Transport Models

10. Yield Modeling

10.1 Poisson Yield Model

$$Y = e^{-A D_0}$$

Variables:

10.2 Negative Binomial Model (Clustered Defects)

$$Y = \left(1 + \frac{A D_0}{\alpha}\right)^{-\alpha}$$

Variables:

10.3 Critical Area Analysis

$$Y = \exp\left( -\sum_i D_i \cdot A_{c,i} \right)$$

Variables:

Critical area depends on:

11. Statistical and Machine Learning Methods

11.1 Response Surface Methodology (RSM)

Second-order model:

$$y = \beta_0 + \sum_{i=1}^{k} \beta_i x_i + \sum_{i=1}^{k} \beta_{ii} x_i^2 + \sum_{i<j} \beta_{ij} x_i x_j + \epsilon$$

11.2 Design of Experiments (DOE)

Design TypeApplication
Full factorialComplete parameter space exploration
Fractional factorialScreening many factors
Central compositeRSM fitting
Box-BehnkenEfficient quadratic modeling
TaguchiRobust design optimization

11.3 Statistical Process Control (SPC)

Process capability indices:

$$C_p = \frac{USL - LSL}{6\sigma}$$
$$C_{pk} = \min\left( \frac{USL - \mu}{3\sigma}, \frac{\mu - LSL}{3\sigma} \right)$$

11.4 Machine Learning Applications

MethodApplication
Neural NetworksProcess-property prediction
Gaussian Process RegressionSurrogate modeling
Random ForestDefect classification
Bayesian OptimizationRecipe tuning
Convolutional Neural NetworksDefect detection in images
Recurrent Neural NetworksTime-series process data

12. Multi-Scale Modeling

12.1 Modeling Hierarchy

ScaleLengthMethodExample
Quantum< 1 nmDFT, ab initio MDReaction barriers
Atomistic1–100 nmClassical MDSurface diffusion
Mesoscale100 nm – 1 μmKinetic Monte CarloDopant clustering
Continuum> 1 μmFEM, FDMProcess simulation
SystemWafer/dieStatisticalYield modeling

12.2 Bridging Methods

13. Key Mathematical Toolkit

13.1 Partial Differential Equations

13.2 Numerical Methods

13.3 Optimization Techniques

13.4 Stochastic Processes

14. Modern Challenges

14.1 Random Dopant Fluctuation (RDF)

Threshold voltage variation:

$$\sigma_{V_T} \propto \frac{1}{\sqrt{W \cdot L}} \cdot \frac{t_{ox}}{\sqrt{N_A}}$$

14.2 Line Edge Roughness (LER)

Power spectral density:

$$PSD(f) = \frac{2\sigma^2 \xi}{1 + (2\pi f \xi)^{2(1+H)}}$$

Variables:

14.3 Stochastic Effects in EUV Lithography

14.4 3D Device Architectures

Modern modeling must handle:

14.5 Emerging Modeling Approaches

mathematicsmathematical modelingsemiconductor mathcrystal growth mathczochralski equationsdopant segregationheat transfer equationslithography math

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