There is growing awareness that EUV lithography is actually an imaging technique that heavily depends on the distribution of secondary electrons in the resist layer [1-5]. The stochastic aspects should be traced not only to the discrete number of photons absorbed but also the electrons that are subsequently released. The electron… Read More
EUV’s Pupil Fill and Resist Limitations at 3nm
The 3nm node is projected to feature around a 22 nm metal pitch [1,2]. This poses some new challenges for the use of EUV lithography. Some challenges are different for the 0.33NA vs. 0.55NA systems.
0.33 NA
For 0.33 NA systems, 22 nm pitch can only be supported by illumination filling 4% of the pupil, well below the 20% lower limit for
ASML- US Seeks to Halt DUV China Sales
-If you can’t beat them, embargo them
-It has been reported US wants ASML to halt China DUV tools
-US obviously wants to kill, not just wound China chip biz
-Is this embargo the alternative to failed CHIPS act?
-Hard to say “do as I say, not as I do”- but US does anyway
First EUV ban now DUV ban? Are process & yield… Read More
ASML EUV Update at SPIE
At the 2022 SPIE Advanced Lithography Conference, ASML presented an update on EUV. I recently had a chance to go over the presentations with Mike Lercel of ASML. The following is a summary of our discussions.
0.33 NA
The 0.33 NA EUV systems are the production workhorse systems for leading edge lithography today. 0.33 NA systems are… Read More
Obscuration-Induced Pitch Incompatibilities in High-NA EUV Lithography
The next generation of EUV lithography systems are based on a numerical aperture (NA) of 0.55, a 67% increase from the current value of 0.33. It targets being able to print 16 nm pitch [1]. The High-NA systems are already expected to face complications from four issues: (1) reduced depth-of-focus requires thinner resists, which… Read More
The Electron Spread Function in EUV Lithography
To the general public, EUV lithography’s resolution can be traced back to its short wavelengths (13.2-13.8 nm), but the true printed resolution has always been affected by the stochastic behavior of the electrons released by EUV absorption [1-5].
A 0.33 NA EUV system is expected to have a diffraction-limited point spread… Read More
Double Diffraction in EUV Masks: Seeing Through The Illusion of Symmetry
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
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
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
Intel and the EUV Shortage
In my “The EUV Divide and Intel Foundry Services” article available here, I discussed the looming EUV shortage. Two days ago, Intel announced their first EUV tool installed at their new Fab 34 in Ireland is a tool they moved from Oregon. This is another indication of the scarcity of EUV tools.
I have been tracking EUV system production… Read More
Podcast EP100: A Look Back and a Look Ahead with Dan and Mike