Home Knowledge Base High-NA EUV lithography

High-NA EUV lithography is the next-generation patterning system that increases the numerical aperture of the EUV projection optics from 0.33 to 0.55 — shrinking the minimum printable half-pitch from ~13 nm to ~8 nm in a single exposure. ASML's EXE:5000 (first shipment 2024, ~€350M per tool) is the only High-NA scanner; Intel is the lead customer (Intel 14A, ~2026), with TSMC and Samsung following. High-NA extends EUV lithography one or two more nodes beyond what current 0.33-NA systems can resolve, pushing the industry toward angstrom-scale patterning without falling back to costly multi-patterning.

Resolution — Rayleigh's equation. The minimum resolvable half-pitch (HP) in optical lithography:

$$\text{HP} = k_1 \cdot \frac{\lambda}{\text{NA}}$$

For current EUV ($\lambda$ = 13.5 nm, NA = 0.33, $k_1$ ≈ 0.3–0.4): HP ≈ 12–16 nm. For High-NA ($\lambda$ = 13.5 nm, NA = 0.55, $k_1$ ≈ 0.3–0.4): HP ≈ 7–10 nm. The 67% increase in NA delivers a proportional improvement in resolution — the same physics that drives microscope objectives, now at 13.5 nm wavelength with all-reflective optics in vacuum.

Depth of focus — the trade-off. Increasing NA narrows depth of focus (DoF):

$$\text{DoF} = k_2 \cdot \frac{\lambda}{\text{NA}^2}$$

At 0.55 NA: DoF drops by $(0.55/0.33)^2 \approx 2.8\times$ compared to 0.33 NA — from ~100 nm to ~35–45 nm. This razor-thin focus budget demands: (1) flatter wafers (global planarity <10 nm), (2) ultra-precise wafer stage leveling (real-time topography correction), (3) thinner resist stacks (~20–30 nm), and (4) tighter CMP uniformity across every underlayer.

Anamorphic optics — the enabling innovation. Simply scaling a 0.33-NA lens to 0.55 NA would require mirrors too large to manufacture. ASML's solution: an anamorphic (non-rotationally-symmetric) optical design that magnifies 4× in one axis and 8× in the perpendicular axis. This keeps mirror sizes manageable but means the mask field shrinks from 26×33 mm (standard EUV) to 26×16.5 mm in the scanning direction — exactly half the field area. Consequence: die sizes larger than 26×16.5 mm require field stitching (two exposures bonded at the overlap), which adds complexity and edge-placement error at the stitch boundary.

ParameterCurrent EUV (0.33 NA)High-NA EUV (0.55 NA)Impact
Numerical aperture0.330.5567% higher resolution
Wavelength13.5 nm13.5 nmSame EUV source
Min half-pitch (k₁=0.33)~13 nm~8 nmEnables 14A / A14 nodes
Depth of focus~100 nm~35–45 nm2.8× tighter → thinner resist
Mask magnification4× (symmetric)4× × 8× (anamorphic)Half field in scan direction
Exposure field26 × 33 mm26 × 16.5 mmLarge dies need stitching
Source power needed250–500 W500–800 W (target)Higher dose demand
Resist thickness30–40 nm20–30 nmThinner → pattern collapse risk
Overlay budget~2 nm<1.5 nmTighter stage/metrology
Throughput target150–200 WPH150+ WPH (goal)Must match 0.33 NA economics
Tool cost~€180M (NXE:3800)~€350M (EXE:5000)2× cost → must print 2× more layers/tool

The half-field problem. Because the exposure field is halved in one dimension, any chip larger than ~26×16.5 mm must be exposed in two stitched shots. For AI accelerators (H100 die = 814 mm², MI300X chiplet = ~700 mm²), this means either: (a) redesigning the chip to fit within the half-field (costly), (b) stitching with sub-1 nm overlay accuracy (challenging), or (c) using High-NA only for the most critical layers (metal/via pitches below ~20 nm) while keeping the rest on 0.33-NA EUV or immersion (the expected initial approach).

Resist challenges. Thinner resist (~20–25 nm) with reduced photon shot noise requires higher EUV dose — but EUV source power is finite, so throughput degrades without mitigation. Metal-oxide resists (MOx, e.g. tin-oxide-based inorganic resists) offer 2–3× better EUV absorption than chemically-amplified resists (CAR) at the same thickness, enabling adequate dose at production throughput. Dry-development resists (no wet puddle) reduce pattern collapse in the high-aspect-ratio features that thin resist creates.

Source power. Current EUV sources deliver 250–500 W of in-band 13.5 nm power to the intermediate focus. High-NA needs 500–800 W to maintain throughput at the higher dose demanded by thinner resist and finer features. ASML/Trumpf's tin-droplet laser-produced-plasma (LPP) source is being scaled with higher-repetition-rate CO₂ lasers (~100 kHz) and optimized tin-droplet targeting. Reaching 800 W in-band is the critical path item for High-NA productivity parity with 0.33-NA tools.

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  <text x="150" y="402" fill="#6f6f6a" font-size="7" text-anchor="middle">2020</text>

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Economics — the $350M question. A single EXE:5000 costs roughly €350M — nearly twice the NXE:3800 (€180M). To justify the investment, each High-NA tool must process enough wafers at enough layers to amortize its cost over production volume. Intel's calculus: High-NA eliminates the need for EUV double-patterning (which uses two 0.33-NA exposures per layer), so one High-NA shot replaces two 0.33-NA shots at critical metal layers — effectively doubling the throughput per critical layer and justifying the tool premium. The break-even requires High-NA throughput to reach at least 150 WPH (wafers per hour) at production dose.

What High-NA means for AI chip manufacturing. The tightest metal pitches on next-generation AI accelerators (18–20 nm M1 pitch at Intel 14A / TSMC A14) are below what 0.33-NA EUV can resolve in a single exposure. Without High-NA, these layers would require EUV double-patterning — doubling litho cost and halving effective throughput at the most expensive process step. High-NA makes single-exposure patterning at 8–10 nm half-pitch practical, keeping Moore's Law cost scaling alive for the transistor-dense accelerator dies that power frontier AI training.

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