Etch Modeling

Semiconductor Manufacturing Process: Etch Modeling

1. Introduction

Etch modeling is one of the most complex and critical areas in semiconductor fabrication simulation. As device geometries shrink below $10\ \text{nm}$ and structures become increasingly three-dimensional, accurate prediction of etch behavior becomes essential for:

  • Process Development: Predict outcomes before costly fab experiments
  • Yield Optimization: Understand how variations propagate to device performance
  • OPC/EPC Extension: Compensate for etch-induced pattern distortions in mask design
  • Design-Technology Co-Optimization (DTCO): Feed process effects back into design rules
  • Virtual Metrology: Predict wafer results from equipment sensor data in real time

2. Fundamentals of Etching

2.1 What is Etching?

Etching selectively removes material from a wafer to transfer lithographically defined patterns into underlying layers—silicon, oxides, nitrides, metals, or complex stacks.

2.2 Types of Etching

  • Wet Etching
  • Uses liquid chemicals (acids, bases, solvents)
  • Typically isotropic (etches equally in all directions)
  • Etch rate follows Arrhenius relationship:
$$ R = A \exp\left(-\frac{E_a}{k_B T}\right) $$

where:
- $R$ = etch rate
- $A$ = pre-exponential factor
- $E_a$ = activation energy
- $k_B$ = Boltzmann constant ($1.381 \times 10^{-23}\ \text{J/K}$)
- $T$ = temperature (K)

  • Dry/Plasma Etching
  • Uses ionized gases (plasma)
  • Anisotropic (directional)
  • Dominant for modern processes ($< 100\ \text{nm}$ nodes)

2.3 Plasma Etching Mechanisms

1. Physical Sputtering
- Ion bombardment physically removes atoms
- Sputter yield $Y$ depends on ion energy $E_i$:

$$ Y(E_i) = A \left( \sqrt{E_i} - \sqrt{E_{th}} \right) $$

where $E_{th}$ is the threshold energy

2. Chemical Etching
- Reactive species form volatile products
- Example: Silicon etching with fluorine

$$ \text{Si} + 4\text{F} \rightarrow \text{SiF}_4 \uparrow $$

3. Ion-Enhanced Etching
- Synergy between ion bombardment and chemical reactions
- Etch yield enhancement factor:

$$ \eta = \frac{Y_{ion+chem}}{Y_{ion} + Y_{chem}} $$

3. Hierarchy of Etch Models

3.1 Empirical Models

Data-driven, fast, used in production:

  • Etch Bias Models
  • Simple offset correction:
$$ CD_{final} = CD_{litho} + \Delta_{etch} $$
  • Pattern-dependent bias:
$$ \Delta_{etch} = f(\text{pitch}, \text{density}, \text{orientation}) $$
  • Etch Proximity Correction (EPC)
  • Kernel-based convolution:
$$ \Delta(x,y) = \iint K(x-x', y-y') \cdot I(x', y') \, dx' dy' $$
  • Where $K$ is the etch kernel and $I$ is the pattern intensity
  • Machine Learning Models
  • Neural networks trained on metrology data
  • Gaussian process regression for uncertainty quantification

3.2 Feature-Scale Models

Semi-empirical, balance speed and physics:

  • String/Segment Models
  • Represent edges as connected nodes
  • Each node moves according to local etch rate vector:
$$ \frac{d\vec{r}_i}{dt} = R(\theta_i, \Gamma_{ion}, \Gamma_{n}) \cdot \hat{n}_i $$
  • Where:
  • $\vec{r}_i$ = position of node $i$
  • $\theta_i$ = local surface angle
  • $\Gamma_{ion}$, $\Gamma_n$ = ion and neutral fluxes
  • $\hat{n}_i$ = surface normal
  • Level-Set Methods
  • Track surface as zero-contour of signed distance function $\phi$:
$$ \frac{\partial \phi}{\partial t} + R(\vec{x}) |\nabla \phi| = 0 $$
  • Handles topology changes naturally (merging, splitting)
  • Cell-Based/Voxel Methods
  • Discretize feature volume into cells
  • Apply probabilistic removal rules:
$$ P_{remove} = 1 - \exp\left( -\sum_j \sigma_j \Gamma_j \Delta t \right) $$
  • Where $\sigma_j$ is the reaction cross-section for species $j$

3.3 Physics-Based Plasma Models

Capture reactor-scale phenomena:

  • Plasma Bulk
  • Electron energy distribution function (EEDF)
  • Boltzmann equation:
$$ \frac{\partial f}{\partial t} + \vec{v} \cdot \nabla f + \frac{q\vec{E}}{m} \cdot \nabla_v f = \left( \frac{\partial f}{\partial t} \right)_{coll} $$
  • Sheath Physics
  • Child-Langmuir law for ion flux:
$$ J_{ion} = \frac{4\epsilon_0}{9} \sqrt{\frac{2e}{M}} \frac{V^{3/2}}{d^2} $$
  • Ion angular distribution at wafer surface
  • Transport
  • Species continuity:
$$ \frac{\partial n_i}{\partial t} + \nabla \cdot (n_i \vec{v}_i) = S_i - L_i $$
  • Where $S_i$ and $L_i$ are source and loss terms

3.4 Atomistic Models

Fundamental understanding, computationally expensive:

  • Molecular Dynamics (MD)
  • Newton's equations for all atoms:
$$ m_i \frac{d^2 \vec{r}_i}{dt^2} = -\nabla_i U(\{\vec{r}\}) $$
  • Interatomic potentials: Tersoff, Stillinger-Weber, ReaxFF
  • Monte Carlo (MC) Methods
  • Statistical sampling of ion trajectories
  • Binary collision approximation (BCA) for high energies
  • Acceptance probability:
$$ P = \min\left(1, \exp\left(-\frac{\Delta E}{k_B T}\right)\right) $$
  • Kinetic Monte Carlo (KMC)
  • Sample reactive events with rates $k_i$:
$$ k_i = u_0 \exp\left(-\frac{E_{a,i}}{k_B T}\right) $$
  • Event selection: $\sum_{j < i} k_j < r \cdot K_{tot} \leq \sum_{j \leq i} k_j$

4. Key Physical Phenomena

4.1 Anisotropy

Ratio of vertical to lateral etch rate:

$$ A = 1 - \frac{R_{lateral}}{R_{vertical}} $$
  • $A = 1$: Perfectly anisotropic (vertical sidewalls)
  • $A = 0$: Perfectly isotropic

Mechanisms for achieving anisotropy:

  • Directional ion bombardment
  • Sidewall passivation (polymer deposition)
  • Low pressure operation (fewer collisions → more directional ions)
  • Ion angular distribution characterized by:
$$ f(\theta) \propto \cos^n(\theta) $$

where higher $n$ indicates more directional flux

4.2 Selectivity

Ratio of etch rates between materials:

$$ S_{A/B} = \frac{R_A}{R_B} $$
  • Mask selectivity: Target material vs. photoresist/hard mask
  • Stop layer selectivity: Target material vs. underlying layer

Example selectivities required:

ProcessSelectivity Required
Oxide/Nitride$> 20:1$
Poly-Si/Oxide$> 50:1$
Si/SiGe (channel release)$> 100:1$

4.3 Loading Effects

Microloading

Local depletion of reactive species in dense pattern regions:

$$ R_{dense} = R_0 \cdot \frac{1}{1 + \beta \cdot \rho_{local}} $$

where:
- $R_0$ = etch rate in isolated feature
- $\beta$ = loading coefficient
- $\rho_{local}$ = local pattern density

Macroloading

Wafer-scale depletion:

$$ R = R_0 \cdot \left(1 - \alpha \cdot A_{exposed}\right) $$

where $A_{exposed}$ is total exposed area fraction

4.4 Aspect Ratio Dependent Etching (ARDE)

Deep, narrow features etch slower due to transport limitations:

$$ R(AR) = R_0 \cdot \exp\left(-\frac{AR}{AR_0}\right) $$

where $AR = \text{depth}/\text{width}$

Physical mechanisms:

1. Ion Shadowing
- Geometric shadowing angle:

$$ \theta_{shadow} = \arctan\left(\frac{1}{AR}\right) $$

2. Neutral Transport
- Knudsen diffusion coefficient:

$$ D_K = \frac{d}{3} \sqrt{\frac{8 k_B T}{\pi m}} $$
  • where $d$ is feature diameter

3. Byproduct Redeposition
- Sticking probability affects escape

4.5 Profile Anomalies

PhenomenonDescriptionCause
BowingLateral bulge in sidewallIon scattering off sidewalls
NotchingLateral etching at interfaceCharge buildup on insulators
MicrotrenchingDeep spots at cornersIon reflection at feature bottom
FootingUndercut at bottomIsotropic chemical component
TaperingNon-vertical sidewallsInsufficient passivation

5. Mathematical Foundations

5.1 Surface Evolution Equation

General form for surface height $h(x,y,t)$:

$$ \frac{\partial h}{\partial t} = -R_0 \cdot V(\theta) \cdot \sqrt{1 + |\nabla h|^2} $$

where:
- $R_0$ = baseline etch rate
- $V(\theta)$ = visibility/flux function
- $\theta = \arctan(|\nabla h|)$

5.2 Ion Angular Distribution

At wafer surface, ion flux angular distribution:

$$ \Gamma(\theta, \phi) = \Gamma_0 \cdot f(\theta) \cdot g(E) $$

Common models:

  • Gaussian distribution:
$$ f(\theta) = \frac{1}{\sqrt{2\pi}\sigma_\theta} \exp\left(-\frac{\theta^2}{2\sigma_\theta^2}\right) $$
  • Thompson distribution (for sputtered neutrals):
$$ f(E) \propto \frac{E}{(E + E_b)^3} $$

5.3 Visibility Calculation

For a point on the surface, visibility to incoming flux:

$$ V(\vec{r}) = \frac{1}{2\pi} \int_0^{2\pi} \int_0^{\theta_{max}(\phi)} f(\theta) \sin\theta \cos\theta \, d\theta \, d\phi $$

where $\theta_{max}(\phi)$ is determined by local geometry (shadowing)

5.4 Surface Reaction Kinetics

Langmuir-Hinshelwood mechanism:

$$ R = k \cdot \theta_A \cdot \theta_B $$

where surface coverages follow:

$$ \frac{d\theta_i}{dt} = s_i \Gamma_i (1 - \theta_{total}) - k_d \theta_i - k_r \theta_i $$
  • $s_i$ = sticking coefficient
  • $k_d$ = desorption rate
  • $k_r$ = reaction rate

5.5 Plasma-Surface Interaction Yield

Ion-enhanced etch yield:

$$ Y_{etch} = Y_0 + Y_1 \cdot \sqrt{E_{ion} - E_{th}} + Y_{chem} \cdot \frac{\Gamma_n}{\Gamma_{ion}} $$

where:
- $Y_0$ = chemical baseline yield
- $Y_1$ = ion enhancement coefficient
- $E_{th}$ = threshold energy (~15-50 eV typically)
- $Y_{chem}$ = chemical enhancement factor

6. Modern Modeling Approaches

6.1 Hybrid Multi-Scale Frameworks

Coupling different scales:

Plasma Etch — RIE and Pattern Transfer reactive ions + radicals selectively remove material through a patterned mask — the subtractive half of lithography RIE Chamber Showerhead (gas inlet + upper electrode) Plasma (ions + radicals + electrons) CF₄, Cl₂, SF₆, O₂, Ar, C₄F₈... ions ↓ wafer ESC chuck (RF bias, He cooling) RF power source → RF bias → Etch Profile Control anisotropic (ideal, vertical) isotropic (undercut) CD control: ±1 nm (EUV node) Selectivity: > 10:1 (etch:mask) Aspect ratio: > 60:1 (3D NAND) Etch Technologies CCP RIE: capacitively coupled, dielectric etch ICP/TCP: inductively coupled, high-density metal etch ALE: atomic layer etch (1 monolayer/cycle, precision) Cryo-etch: -100°C, passivation-free HAR Si etch Wet etch: isotropic, used for cleans and sacrificial release Advanced Node Challenges HAR etch (3D NAND): 200+ layers, > 8 μm deep LELE etch budget: sub-nm CD uniformity needed GAA nanosheet release: selective SiGe vs Si removal BEOL low-k damage: plasma damages porous dielectric Equipment: Lam Research, TEL, Applied Materials Etch Steps per Transistor (advanced node) Fin/NS etch pattern the channel Gate etch define gate length Spacer etch self-aligned structures Contact etch HAR vias to S/D Trench etch Cu damascene wiring Etch is the pattern transfer engine: lithography defines the pattern, etch carves it into silicon — at atomic precision. Modern chips have 60+ etch steps — each one must hold sub-nanometer uniformity across a 300mm wafer.

6.2 Machine Learning Integration

  • Surrogate Models
  • Train neural network on physics simulation outputs:
$$ \hat{y} = f_{NN}(\vec{x}; \vec{w}) $$
  • Loss function:
$$ \mathcal{L} = \frac{1}{N} \sum_{i=1}^{N} \|y_i - \hat{y}_i\|^2 + \lambda \|\vec{w}\|^2 $$
  • Physics-Informed Neural Networks (PINNs)
  • Embed physics constraints in loss:
$$ \mathcal{L}_{total} = \mathcal{L}_{data} + \alpha \mathcal{L}_{physics} $$
  • Where $\mathcal{L}_{physics}$ enforces governing equations
  • Virtual Metrology
  • Predict CD, profile from chamber sensors:
$$ CD_{predicted} = g(P, T, V_{bias}, \text{OES}, ...) $$

6.3 Computational Lithography Integration

Major EDA tools couple lithography + etch:

1. Litho simulation → Resist profile $h_R(x,y)$
2. Etch simulation → Final pattern $h_F(x,y)$
3. Combined model:

$$ CD_{final} = CD_{design} + \Delta_{OPC} + \Delta_{litho} + \Delta_{etch} $$

7. Challenges at Advanced Nodes

7.1 FinFET / Gate-All-Around (GAA)

  • Fin Etch
  • Sidewall angle uniformity: $90° \pm 1°$
  • Width control: $\pm 1\ \text{nm}$ at $W_{fin} < 10\ \text{nm}$
  • Channel Release
  • Selective SiGe vs. Si etching
  • Required selectivity: $> 100:1$
  • Etch rate:
$$ R_{SiGe} \gg R_{Si} $$
  • Inner Spacer Formation
  • Isotropic lateral etch in confined geometry
  • Depth control: $\pm 0.5\ \text{nm}$

7.2 3D NAND

Extreme aspect ratio challenges:

GenerationLayersAspect Ratio
96L96~60:1
128L128~80:1
176L176~100:1
232L+232+~150:1

Critical issues:
- ARDE variation across depth
- Bowing control
- Twisting in elliptical holes

7.3 EUV Patterning

  • Very thin resists: $< 40\ \text{nm}$
  • Hard mask stacks with multiple layers
  • LER/LWR amplification:
$$ LER_{final} = \sqrt{LER_{litho}^2 + LER_{etch}^2} $$
  • Target: $LER < 1.2\ \text{nm}$ ($3\sigma$)

7.4 Stochastic Effects

At small dimensions, statistical fluctuations dominate:

$$ \sigma_{CD} \propto \frac{1}{\sqrt{N_{events}}} $$

where $N_{events}$ = number of etching events per feature

8. Industry Tools

8.1 Commercial Software

CategoryTools
TCAD/ProcessSynopsys Sentaurus Process, Silvaco Victory Process
Virtual FabCoventor SEMulator3D
Equipment VendorLam Research, Applied Materials (proprietary)
Computational LithoSynopsys S-Litho, Siemens Calibre

8.2 Research Tools

  • MCFPM (Monte Carlo Feature Profile Model) - University of Illinois
  • LAMMPS - Molecular dynamics
  • SPARTA - Direct Simulation Monte Carlo
  • OpenFOAM - Plasma fluid modeling

9. Future Directions

9.1 Digital Twins

Real-time chamber models for closed-loop process control:

$$ \vec{u}_{control}(t) = \mathcal{K} \left[ y_{target} - y_{model}(t) \right] $$

9.2 Atomistic-Continuum Coupling

Seamless multi-scale simulation using:
- Adaptive mesh refinement
- Concurrent coupling methods
- Machine-learned interscale bridging

9.3 New Materials

Modeling requirements for:
- 2D materials (graphene, MoS$_2$, WS$_2$)
- High-$\kappa$ dielectrics
- Ferroelectrics (HfZrO)
- High-mobility channels (InGaAs, Ge)

9.4 Uncertainty Quantification

Predicting distributions, not just means:

$$ P(CD) = \int P(CD | \vec{\theta}) P(\vec{\theta}) d\vec{\theta} $$

Key metrics:
- Process capability: $C_{pk} = \frac{\min(USL - \mu, \mu - LSL)}{3\sigma}$
- Target: $C_{pk} > 1.67$ for production

Summary

Etch modeling spans from atomic-scale surface reactions to reactor-scale plasma physics to fab-level empirical correlations. The art lies in choosing the right abstraction level:

ApplicationModel TypeSpeedAccuracy
Production OPC/EPCEmpirical/ML★★★★★★★☆☆☆
Process DevelopmentFeature-scale★★★☆☆★★★★☆
Mechanism ResearchAtomistic MD/MC★☆☆☆☆★★★★★
Equipment DesignPlasma + Feature★★☆☆☆★★★★☆

As geometries shrink and structures become more 3D, accurate etch modeling becomes essential for first-time-right process development and continued yield improvement.

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