In a DRAM chip, the memory array contains features which are the most densely packed, but at least they are regularly arranged. Outside the array, the regularity is lost, but in the most difficult cases, the pitches can still be comparable with those within the array, though generally larger. Such features include the lowest metal… Read More
Author: Fred Chen
Stitched Multi-Patterning for Minimum Pitch Metal in DRAM Periphery
A Perfect Storm for EUV Lithography
Electron blur, stochastics, and now polarization, are all becoming stronger influences in EUV lithography as pitch continues to shrink
As EUV lithography continues to evolve, targeting smaller and smaller pitches, new physical limitations continue to emerge as formidable obstacles. While stochastic effects have long been… Read More
Variable Cell Height Track Pitch Scaling Beyond Lithography
Two approaches compared
With half-pitch approaching 10 nm, EUV patterning is heavily impacted by stochastic effects, which are aggravated from reduced image contrast from electron blur [1]. A two-mask (“LELE”: Litho-Etch-Litho-Etch) approach was proposed to pattern core features for self-aligned double patterning (SADP)… Read More
A Realistic Electron Blur Function Shape for EUV Resist Modeling
Peak probability at zero distance actually makes no sense
In lithography, it is often stated that the best resolution that can be achieved depends on wavelength and numerical aperture (NA), but this actually only applies to the so-called “aerial” image. When the image is actually formed in the resist layer, it also depends on an… Read More
Rethinking Multipatterning for 2nm Node
Whether EUV or DUV doesn’t matter at 20 nm pitch
The International Roadmap for Devices and Systems, 2022 Edition, indicates that the “2nm” node due in 2025 (this year) has a minimum (metal) half-pitch of 10 nm [1]. This is, in fact, less than the resolution of a current state-of-the-art EUV system, with a numerical aperture… Read More
Resist Loss Model for the EUV Stochastic Defectivity Cliffs
The occurrences of notorious stochastic defects in EUV lithography have resulted in CD or corresponding dose windows with the lower and higher bounds being characterized as “cliffs” [1-3], since the defect density increases exponentially when approaching these bounds. The defects at lower doses have been attributed to the… Read More
Stochastic Effects Blur the Resolution Limit of EUV Lithography
Conventionally, the resolution limit of a lithography system with wavelength l and numerical aperture NA is given by half-pitch = 0.25 wavelength/NA. With the use of EUV lithography, however, electron blur needs to be added [1]. The impact of this blur is to reduce the contrast [2]. Blur reduces the modulation amplitude by a factor… Read More
Can LELE Multipatterning Help Against EUV Stochastics?
Previously, I had indicated how detrimental stochastic effects at pitches below 50 nm should lead to reconsidering the practical resolution limit for EUV lithography [1]. This is no exaggeration, as stochastic effects have been observed for 24 nm half-pitch several years ago [2,3]. This then leads to the question of whether … Read More
Stochastic Pupil Fill in EUV Lithography
Pupil fill tradeoff again
EUV lithography continues to be plagued by its stochastic nature.
This stochastic nature is most clearly portrayed by the random fluctuation of the absorbed photon number at a given location. For example, consider an absorbed dose of 10 mJ/cm2 amounts to 6.8 photons of energy 92 eV absorbed in a square … Read More
Application-Specific Lithography: Patterning 5nm 5.5-Track Metal by DUV
At IEDM 2019, TSMC revealed two versions of 5nm standard cell layouts: a 5.5-track DUV-patterned version and a 6-track EUV-patterned version [1]. Although the metal pitches were not explicitly stated, later analyses of a 5nm product, namely, Apple’s A15 Bionic chip, revealed a cell height of 210 nm [2]. For the 6-track … Read More
TSMC 2025 Technical Symposium Briefing