Home Knowledge Base Lithography Light Sources

Lithography Light Sources are the precision photon generators that provide the illumination for projecting circuit patterns onto silicon wafers — where the wavelength of light fundamentally determines the minimum feature size achievable, driving the progression from mercury lamps (436 nm) to excimer lasers (193 nm) to tin plasma EUV sources (13.5 nm) across four decades of semiconductor advancement.

Lithography Wavelength Evolution

EraWavelengthSourceMin FeatureNode
g-line436 nmMercury lamp350 nm500nm
i-line365 nmMercury lamp250 nm350nm
KrF248 nmKrF excimer laser150 nm250-180nm
ArF dry193 nmArF excimer laser65 nm130-65nm
ArF immersion193 nm (water lens)ArF excimer laser38 nm45-7nm
EUV13.5 nmSn plasma (LPP)8 nm7nm-2nm

Excimer Laser (DUV — 193nm/248nm)

EUV Source (13.5nm)

1. Tin droplet dispenser creates 25 μm tin droplets at 50,000/second. 2. Pre-pulse laser flattens droplet into pancake shape. 3. Main CO₂ laser (25 kW) hits flattened droplet → creates 500,000°C plasma. 4. Plasma emits EUV light at 13.5 nm. 5. Multilayer mirror collects and focuses EUV light toward the reticle.

EUV Source Challenges

High-NA EUV

Lithography light sources are the fundamental enabler of Moore's Law — the ability to generate shorter wavelengths of light with sufficient power, spectral purity, and reliability has been the pacing technology for every node advancement in the semiconductor industry's history.

semiconductor lithography sourceduv sourceeuv sourceexcimer laserlight source lithography

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