Double Diffraction in EUV Masks: Seeing Through The Illusion of Symmetry

Double Diffraction in EUV Masks: Seeing Through The Illusion of Symmetry
by Fred Chen on 05-22-2022 at 7:00 am

Double Diffraction in EUV Masks

At this year’s SPIE Advanced Lithography conference, changes to EUV masks were particularly highlighted, as a better understanding of their behavior is becoming clear. It’s now confirmed that a seemingly symmetric EUV mask absorber pattern does not produce a symmetric image at the wafer, as a conventional DUV … Read More


Demonstration of Dose-Driven Photoelectron Spread in EUV Resists

Demonstration of Dose-Driven Photoelectron Spread in EUV Resists
by Fred Chen on 05-08-2022 at 10:00 am

Demonstration of Dose Driven Photoelectron Spread in EUV Resists

As a consequence of having a ~13.5 nm wavelength, EUV photons transfer ~90% of their energy to ionized photoelectrons. Thus, EUV lithography is fundamentally mostly EUV photoelectron lithography. The actual resolution becomes dependent on photoelectron trajectories.

Photoelectron trajectories in EUV lithography were… Read More


Adding Random Secondary Electron Generation to Photon Shot Noise: Compounding EUV Stochastic Edge Roughness

Adding Random Secondary Electron Generation to Photon Shot Noise: Compounding EUV Stochastic Edge Roughness
by Fred Chen on 04-26-2022 at 6:00 am

Compounding EUV Stochastic Edge Roughness 2

The list of possible stochastic patterning issues for EUV lithography keeps growing longer: CD variation, edge roughness, placement error, defects [1]. The origins of stochastic behavior are now well-known. For a given EUV photon flux into the resist, a limited fraction are absorbed. Since the absorption is less than 5% affected… Read More


EUV Resist Absorption Impact on Stochastic Defects

EUV Resist Absorption Impact on Stochastic Defects
by Fred Chen on 04-03-2022 at 10:00 am

EUV Resist Absorption Impact on Stochastic Defects 1

Stochastic defects continue to draw attention in the area of EUV lithography. It is now widely recognized that stochastic issues not only come from photon shot noise due to low (absorbed) EUV photon density, but also the resist material and process factors [1-4].

It stands to reason that resist absorption of EUV light, which is … Read More


Etch Pitch Doubling Requirement for Cut-Friendly Track Metal Layouts: Escaping Lithography Wavelength Dependence

Etch Pitch Doubling Requirement for Cut-Friendly Track Metal Layouts: Escaping Lithography Wavelength Dependence
by Fred Chen on 03-27-2022 at 6:00 am

Etch Pitch Doubling Requirement

The 5nm foundry node saw the arrival of 6-track standard cells with four narrow routing tracks between wide power/ground rails (Figure 1a), with minimum pitches of around 30 nm [1]. The routing tracks require cuts [2] with widths comparable to the minimum half-pitch, to enable the via connections to the next metal layer with the… Read More


Horizontal, Vertical, and Slanted Line Shadowing Across Slit in Low-NA and High-NA EUV Lithography Systems

Horizontal, Vertical, and Slanted Line Shadowing Across Slit in Low-NA and High-NA EUV Lithography Systems
by Fred Chen on 01-11-2022 at 6:00 am

EUV shadowing across slit

EUV lithography systems continue to be the source of much hope for continuing the pace of increasing device density on wafers per Moore’s Law. Recently, although EUV systems were originally supposed to help the industry avoid much multipatterning, it has not turned out to be the case [1,2]. The main surprise has been the

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Pattern Shifts Induced by Dipole-Illuminated EUV Masks

Pattern Shifts Induced by Dipole-Illuminated EUV Masks
by Fred Chen on 12-19-2021 at 10:00 am

Pattern Shifts Induced by Dipole Illuminated EUV Masks

As EUV lithography is being targeted towards pitches of 30 nm or less, fundamental differences from conventional DUV lithography become more and more obvious. A big difference is in the mask use. Unlike other photolithography masks, EUV masks are absorber patterns on a reflective multilayer rather than a transparent substrate.… Read More


Revisiting EUV Lithography: Post-Blur Stochastic Distributions

Revisiting EUV Lithography: Post-Blur Stochastic Distributions
by Fred Chen on 11-14-2021 at 10:00 am

Revisiting EUV Lithography Post Blur Stochastic Distributions

In previous articles, I had looked at EUV stochastic behavior [1-2], primarily in terms of the low photon density resulting in shot noise, described by the Poisson distribution [3]. The role of blur to help combat the randomness of EUV photon absorption and secondary electron generation and migration was also recently considered… Read More


The Challenge of Working with EUV Doses

The Challenge of Working with EUV Doses
by Fred Chen on 10-25-2021 at 2:00 pm

The Challenge of Working with EUV Doses

Recently, a patent application from TSMC [1] revealed target EUV doses used in the range of 30-45 mJ/cm2. However, it was also acknowledged in the same application that such doses were too low to prevent defects and roughness. Recent studies [2,3] have shown that by considering photon density along with blur, the associated shot… Read More


Blur, not Wavelength, Determines Resolution at Advanced Nodes

Blur, not Wavelength, Determines Resolution at Advanced Nodes
by Fred Chen on 10-05-2021 at 10:00 am

Blur not Wavelength Determines Resolution at Advanced Nodes

Lithography has been the driving force for shrinking feature sizes for decades, and the most easily identified factor behind this trend is the reduction of wavelength. G-line (436 nm wavelength) was used for 0.5 um in the late 1980s [1], and I-line (365 nm wavelength) was used down to 0.3 um in the 1990s [2]. Then began the era of deep-ultraviolet… Read More