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Semiconductor Manufacturing Process: Physics-Based Modeling and Differential Equations

Keywords: physics based modeling and differential equations, physics modeling, differential equations, semiconductor physics, device physics, transport equations, heat transfer equations, process modeling, pde semiconductor


Semiconductor Manufacturing Process: Physics-Based Modeling and Differential Equations

A comprehensive reference for the physics and mathematics governing semiconductor fabrication processes.

1. Thermal Oxidation of Silicon

1.1 Deal-Grove Model

The foundational model for silicon oxidation describes oxide thickness growth through coupled transport and reaction.

Governing Equation:

$$x^2 + Ax = B(t + \tau)$$

Parameter Definitions:

1.2 Underlying Diffusion Physics

Steady-state diffusion through the oxide:

$$\frac{\partial C}{\partial t} = D_{ox}\frac{\partial^2 C}{\partial x^2}$$

Boundary Conditions:

$$ F_1 = h_g(C^* - C_0)$$
$$ F_2 = k_s C_i$$

Steady-state flux through the oxide:

$$F = \frac{D_{ox}C^*}{1 + \frac{k_s}{h_g} + \frac{k_s x}{D_{ox}}}$$

1.3 Limiting Growth Regimes

RegimeConditionGrowth LawPhysical Interpretation
LinearThin oxide ($x \ll A$)$x \approx \frac{B}{A}(t + \tau)$Reaction-limited
ParabolicThick oxide ($x \gg A$)$x \approx \sqrt{Bt}$Diffusion-limited

2. Dopant Diffusion

2.1 Fick's Laws of Diffusion

First Law (Flux Equation):

$$\vec{J} = -D abla C$$

Second Law (Mass Conservation / Continuity):

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

For constant diffusivity in 1D:

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

2.2 Analytical Solutions

Constant Surface Concentration (Predeposition)

Initial condition: $C(x, 0) = 0$ Boundary condition: $C(0, t) = C_s$

$$C(x,t) = C_s \cdot \text{erfc}\left(\frac{x}{2\sqrt{Dt}}\right)$$

where the complementary error function is:

$$\text{erfc}(z) = 1 - \text{erf}(z) = 1 - \frac{2}{\sqrt{\pi}}\int_0^z e^{-u^2} du$$

Fixed Dose / Drive-in (Gaussian Distribution)

Initial condition: Delta function at surface with dose $Q$

$$C(x,t) = \frac{Q}{\sqrt{\pi Dt}} \exp\left(-\frac{x^2}{4Dt}\right)$$

Key Parameters:

2.3 Concentration-Dependent Diffusion

At high doping concentrations, diffusivity becomes concentration-dependent:

$$\frac{\partial C}{\partial t} = \frac{\partial}{\partial x}\left[D(C)\frac{\partial C}{\partial x}\right]$$

Fair-Tsai Model for Diffusivity:

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

Parameter Definitions:

2.4 Point Defect Coupled Diffusion

Modern TCAD uses coupled equations for dopants and point defects (vacancies $V$ and interstitials $I$):

Vacancy Continuity:

$$\frac{\partial C_V}{\partial t} = D_V abla^2 C_V - k_{IV}C_V C_I + G_V - \frac{C_V - C_V^*}{\tau_V}$$

Interstitial Continuity:

$$\frac{\partial C_I}{\partial t} = D_I abla^2 C_I - k_{IV}C_V C_I + G_I - \frac{C_I - C_I^*}{\tau_I}$$

Term Definitions:

Effective Dopant Diffusivity:

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

where $f_I$ and $f_V$ are the interstitial and vacancy fractions for the specific dopant species.

3. Ion Implantation

3.1 Range Distribution (LSS Theory)

The implanted dopant profile follows approximately a Gaussian distribution:

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

Parameters:

Higher-Order Moments (Pearson IV Distribution):

3.2 Stopping Power (Energy Loss)

The rate of energy loss as ions traverse the target:

$$\frac{dE}{dx} = -N[S_n(E) + S_e(E)]$$

Components:

LSS Electronic Stopping (Low Energy):

$$S_e \propto \sqrt{E}$$

Nuclear Stopping: Uses screened Coulomb potentials with Thomas-Fermi or ZBL (Ziegler-Biersack-Littmark) universal screening functions.

3.3 Boltzmann Transport Equation

For rigorous treatment (typically solved via Monte Carlo methods):

$$\frac{\partial f}{\partial t} + \vec{v} \cdot abla_r f + \frac{\vec{F}}{m} \cdot abla_v f = \left(\frac{\partial f}{\partial t}\right)_{coll}$$

Variables:

3.4 Damage Accumulation

Kinchin-Pease Model:

$$N_d = \frac{E_{damage}}{2E_d}$$

Parameters:

4. Chemical Vapor Deposition (CVD)

4.1 Coupled Transport Equations

Species Transport (Convection-Diffusion-Reaction):

$$\frac{\partial C_i}{\partial t} + \vec{u} \cdot abla C_i = D_i abla^2 C_i + R_i$$

Navier-Stokes Equations (Momentum):

$$\rho\left(\frac{\partial \vec{u}}{\partial t} + \vec{u} \cdot abla\vec{u}\right) = - abla p + \mu abla^2\vec{u} + \rho\vec{g}$$

Continuity Equation (Incompressible Flow):

$$abla \cdot \vec{u} = 0$$

Energy Equation:

$$\rho c_p\left(\frac{\partial T}{\partial t} + \vec{u} \cdot abla T\right) = k abla^2 T + Q_{reaction}$$

Variable Definitions:

4.2 Surface Reaction Kinetics

Flux Balance at Wafer Surface:

$$h_m(C_b - C_s) = k_s C_s$$

Deposition Rate:

$$G = \frac{k_s h_m C_b}{k_s + h_m}$$

Parameters:

Limiting Cases:

RegimeConditionRate ExpressionControl Mechanism
Reaction-limited$k_s \ll h_m$$G \approx k_s C_b$Surface chemistry
Transport-limited$k_s \gg h_m$$G \approx h_m C_b$Mass transfer

4.3 Step Coverage — Knudsen Diffusion

In high-aspect-ratio features, molecular (Knudsen) flow dominates:

$$D_K = \frac{d}{3}\sqrt{\frac{8k_B T}{\pi m}}$$

Parameters:

Thiele Modulus (Reaction-Diffusion Balance):

$$\phi = L\sqrt{\frac{k_s}{D_K}}$$

Interpretation:

5. Atomic Layer Deposition (ALD)

5.1 Surface Site Model

Precursor A Adsorption Kinetics:

$$\frac{d\theta_A}{dt} = s_0 \frac{P_A}{\sqrt{2\pi m_A k_B T}}(1 - \theta_A) - k_{des}\theta_A$$

Parameters:

5.2 Growth Per Cycle (GPC)

$$GPC = n_{sites} \cdot \Omega \cdot \theta_A^{sat}$$

Parameters:

6. Plasma Etching

6.1 Plasma Fluid Equations

Electron Continuity:

$$\frac{\partial n_e}{\partial t} + abla \cdot \vec{\Gamma}_e = S_{ionization} - S_{recomb}$$

Ion Continuity:

$$\frac{\partial n_i}{\partial t} + abla \cdot \vec{\Gamma}_i = S_{ionization} - S_{recomb}$$

Drift-Diffusion Flux (Electrons):

$$\vec{\Gamma}_e = -n_e\mu_e\vec{E} - D_e abla n_e$$

Drift-Diffusion Flux (Ions):

$$\vec{\Gamma}_i = n_i\mu_i\vec{E} - D_i abla n_i$$

Poisson's Equation (Self-Consistent Field):

$$abla^2\phi = -\frac{e}{\varepsilon_0}(n_i - n_e)$$

Electron Energy Balance:

$$\frac{\partial}{\partial t}\left(\frac{3}{2}n_e k_B T_e\right) + abla \cdot \vec{q}_e = -e\vec{\Gamma}_e \cdot \vec{E} - \sum_j \epsilon_j R_j$$

6.2 Sheath Physics

Bohm Criterion (Sheath Edge Condition):

$$u_i \geq u_B = \sqrt{\frac{k_B T_e}{M_i}}$$

Child-Langmuir Law (Collisionless Sheath Ion Current):

$$J = \frac{4\varepsilon_0}{9}\sqrt{\frac{2e}{M_i}}\frac{V_0^{3/2}}{d^2}$$

Parameters:

6.3 Surface Etch Kinetics

Ion-Enhanced Etching Rate:

$$R_{etch} = Y_i\Gamma_i + Y_n\Gamma_n(1-\theta) + Y_{syn}\Gamma_i\theta$$

Components:

Yield Parameters:

Surface Coverage Dynamics:

$$\frac{d\theta}{dt} = s\Gamma_n(1-\theta) - Y_{syn}\Gamma_i\theta - k_v\theta$$

Terms:

7. Lithography

7.1 Aerial Image Formation

Hopkins Formulation (Partially Coherent Imaging):

$$I(x,y) = \iint TCC(f,g;f',g') \cdot \tilde{M}(f,g) \cdot \tilde{M}^*(f',g') \, df\,dg\,df'\,dg'$$

Parameters:

Rayleigh Resolution Criterion:

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

Depth of Focus:

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

Parameters:

7.2 Photoresist Exposure — Dill Model

Intensity Attenuation with Photobleaching:

$$\frac{\partial I}{\partial z} = -\alpha(M)I$$

where the absorption coefficient depends on PAC concentration:

$$\alpha = AM + B$$

Photoactive Compound (PAC) Decomposition:

$$\frac{\partial M}{\partial t} = -CIM$$

Dill Parameters:

ParameterDescriptionUnits
$A$Bleachable absorption coefficientμm⁻¹
$B$Non-bleachable absorption coefficientμm⁻¹
$C$Exposure rate constantcm²/mJ
$M$Relative PAC concentrationdimensionless (0-1)

7.3 Chemically Amplified Resists

Photoacid Generation:

$$\frac{\partial [H^+]}{\partial t} = C \cdot I \cdot [PAG]$$

Post-Exposure Bake — Acid Diffusion and Reaction:

$$\frac{\partial [H^+]}{\partial t} = D_{acid} abla^2[H^+] - k_{loss}[H^+]$$

Deprotection Reaction (Catalytic Amplification):

$$\frac{\partial [Protected]}{\partial t} = -k_{cat}[H^+][Protected]$$

Parameters:

7.4 Development Rate — Mack Model

$$R = R_{max}\frac{(a+1)(1-M)^n}{a + (1-M)^n} + R_{min}$$

Parameters:

8. Epitaxy

8.1 Burton-Cabrera-Frank (BCF) Theory

Adatom Diffusion on Terraces:

$$\frac{\partial n}{\partial t} = D_s abla^2 n + F - \frac{n}{\tau}$$

Parameters:

Step Velocity:

$$v_{step} = \Omega D_s\left[\left(\frac{\partial n}{\partial x}\right)_+ - \left(\frac{\partial n}{\partial x}\right)_-\right]$$

Steady-State Solution for Step Flow:

$$v_{step} = \frac{2D_s \lambda_s F}{l} \cdot \tanh\left(\frac{l}{2\lambda_s}\right)$$

Parameters:

8.2 Rate Equations for Island Nucleation

Monomer (Single Adatom) Density:

$$\frac{dn_1}{dt} = F - 2\sigma_1 D_s n_1^2 - \sum_{j>1}\sigma_j D_s n_1 n_j - \frac{n_1}{\tau}$$

Cluster of Size $j$:

$$\frac{dn_j}{dt} = \sigma_{j-1}D_s n_1 n_{j-1} - \sigma_j D_s n_1 n_j$$

Parameters:

9. Chemical Mechanical Polishing (CMP)

9.1 Preston Equation

$$MRR = K_p \cdot P \cdot V$$

Parameters:

9.2 Contact Mechanics — Greenwood-Williamson Model

Real Contact Area:

$$A_r = \pi \eta A_n R_p \int_d^\infty (z-d)\phi(z)dz$$

Parameters:

9.3 Slurry Hydrodynamics — Reynolds Equation

$$\frac{\partial}{\partial x}\left(h^3\frac{\partial p}{\partial x}\right) + \frac{\partial}{\partial y}\left(h^3\frac{\partial p}{\partial y}\right) = 6\mu U\frac{\partial h}{\partial x}$$

Parameters:

10. Thin Film Stress

10.1 Stoney Equation

Film Stress from Wafer Curvature:

$$\sigma_f = \frac{E_s h_s^2}{6(1- u_s)h_f R}$$

Parameters:

u_s$ — substrate Poisson's ratio

10.2 Thermal Stress

$$\sigma_{th} = \frac{E_f}{1- u_f}(\alpha_s - \alpha_f)\Delta T$$

Parameters:

u_f$ — film Poisson's ratio

11. Electromigration (Reliability)

11.1 Black's Equation (Empirical MTTF)

$$MTTF = A \cdot j^{-n} \cdot \exp\left(\frac{E_a}{k_B T}\right)$$

Parameters:

11.2 Drift-Diffusion Model

$$\frac{\partial C}{\partial t} = abla \cdot \left[D\left( abla C - C\frac{Z^*e\rho \vec{j}}{k_B T}\right)\right]$$

Parameters:

11.3 Stress Evolution — Korhonen Model

$$\frac{\partial \sigma}{\partial t} = \frac{\partial}{\partial x}\left[\frac{D_a B\Omega}{k_B T}\left(\frac{\partial\sigma}{\partial x} + \frac{Z^*e\rho j}{\Omega}\right)\right]$$

Parameters:

12. Numerical Solution Methods

12.1 Common Numerical Techniques

MethodApplicationStrengths
Finite Difference (FDM)Regular grids, 1D/2D problemsSimple implementation, efficient
Finite Element (FEM)Complex geometries, stress analysisFlexible meshing, boundary conditions
Monte CarloIon implantation, plasma kineticsStatistical accuracy, handles randomness
Level SetTopography evolution (etch/deposition)Handles topology changes
Kinetic Monte Carlo (KMC)Atomic-scale diffusion, nucleationCaptures rare events, atomic detail

12.2 Discretization Examples

Explicit Forward Euler (1D Diffusion):

$$C_i^{n+1} = C_i^n + \frac{D\Delta t}{(\Delta x)^2}\left(C_{i+1}^n - 2C_i^n + C_{i-1}^n\right)$$

Stability Criterion:

$$\frac{D\Delta t}{(\Delta x)^2} \leq \frac{1}{2}$$

Implicit Backward Euler:

$$C_i^{n+1} - \frac{D\Delta t}{(\Delta x)^2}\left(C_{i+1}^{n+1} - 2C_i^{n+1} + C_{i-1}^{n+1}\right) = C_i^n$$

12.3 Major TCAD Software Tools

Processes and Governing Equations

ProcessPrimary PhysicsKey Equation
OxidationDiffusion + Reaction$x^2 + Ax = Bt$
DiffusionMass Transport

abla^2 C$ |

ImplantationBallistic + Stopping$\frac{dE}{dx} = -N(S_n + S_e)$
CVDTransport + KineticsNavier-Stokes + Species
ALDSelf-limiting AdsorptionLangmuir kinetics
Plasma EtchPlasma + SurfacePoisson + Drift-Diffusion
LithographyWave Optics + ChemistryDill ABC model
EpitaxySurface DiffusionBCF theory
CMPTribology + ChemistryPreston equation
StressElasticityStoney equation
ElectromigrationMass transport under currentKorhonen model

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