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Euv with fewer mirrors?

Jon Y presents a rare glimpse into a potential paradigm shift in semiconductor manufacturing that bypasses the industry's current obsession with adding complexity. While the global consensus has been that more mirrors equal better resolution, Y introduces a proposal from Professor Tsumoru Shintake that argues for the opposite: a radical simplification of the optical path that could complement, rather than replace, existing giants. This is not merely a theoretical exercise; it is a challenge to the economic and physical limits of the most expensive machines on Earth.

The Mirror Problem

The piece opens by grounding the reader in the brutal physics of current Extreme Ultraviolet (EUV) lithography. Y explains that ASML's current machines rely on a complex chain of twelve reflections to project circuit patterns onto silicon wafers. "A mirror inside ASML's EUV lithography machine reflects just 70% of the EUV light it receives," Y writes, noting that with so many bounces, "Just 1% of the photons hit the wafer." This staggering inefficiency forces the industry to use massive, power-hungry light sources and introduces stochastic defects where quantum effects cause errors because not enough light hits the resist.

Euv with fewer mirrors?

Y's framing is effective because he strips away the mystique of the "black box" machines to reveal a simple arithmetic problem: every mirror absorbs 30% of the light. The industry's solution has been to throw more power at the problem, but Y suggests this approach is hitting a wall. The argument here is that the current path of increasing complexity may be a dead end, or at least a very expensive one. Critics might note that ASML's twelve-mirror system was not chosen arbitrarily but evolved over decades to solve specific distortion issues that simpler systems historically failed to address. Y acknowledges this history but posits that new optical theories might finally make the old, simpler designs viable again.

"ASML chose the number of mirrors they did for a very real reason. It gives them full ability to print specific features on the mask."

Revisiting the Past

The core of Y's narrative is a historical deep dive that reframes the "new" technology as a rediscovery of forgotten engineering. He traces the lineage from early two-mirror systems by pioneers like Professor Hiroo Kinoshita to the more complex six-mirror projection modules adopted by ASML. Y notes that early attempts at two-mirror systems, known as Schwarzschild optics, suffered from "field curvature," where the image projected onto the wafer was curved rather than flat, making it impossible to print large, uniform chips.

Y writes, "The curved reflection gets more pronounced the further away you get from the center, or off-axis." This distortion was the primary reason the industry moved away from simpler optics. However, Y introduces Professor Shintake's work as a potential solution to this century-old problem. Shintake, a physicist with a background in nuclear science and free-electron lasers, applied Petzval field curvature theory to propose a system that uses only two mirrors in the projection module. Y emphasizes that Shintake is not an outsider; he has spent thirty years researching accelerator science and helped build Japan's first X-ray free-electron laser.

The author's choice to highlight Shintake's credentials is crucial. It signals to the reader that this is not a crackpot theory but a serious re-evaluation by a domain expert. Y paraphrases Shintake's realization: after studying over a hundred papers, the professor found that a two-mirror equal-radii system could project a perfectly flat field if the geometry was adjusted correctly. This challenges the assumption that more mirrors are inherently better for resolution.

The Illumination Breakthrough

If the projection system is a refinement of old ideas, Y argues that the true innovation lies in the illumination module. This is where the piece shifts from historical analysis to a description of a clever engineering hack. The challenge in EUV lithography is that the light source must illuminate the mask without the light from different sources colliding or reflecting back into the wrong place.

Y describes Shintake's solution as a "dual line field" system. He quotes the professor directly to illustrate the geometric puzzle: "If you hold two flashlights, one in each hand, and aim them diagonally at a mirror in front of you at the same angle, then the light from one flashlight will always hit the opposite flashlight, which is unacceptable in lithography." Shintake's breakthrough was realizing that by moving the light sources outward while maintaining the angle, the light cones could illuminate the mask without interference.

This arrangement allows for two fixed exposure slits, enabling a scanning process where a spot on the mask is exposed by the first slit and then the second as it moves. Y calls this "very clever," noting that it allows the system to function with fewer mirrors while maintaining the necessary scanning motion. The author suggests that this specific illumination geometry is the key that unlocks the viability of the two-mirror projection system, which had previously been considered impractical.

"This two-slit arrangement lets the two illumination cones to be [positioned] without colliding with the light from the opposite flashlights."

Practical Constraints and Future Outlook

Y does not shy away from the physical realities of implementing this system. He notes that to enlarge the field size to a commercially viable level, the machine would need to be significantly taller than current tools. "Shintake's proposal increases the distance between the object and the image... to the very limit allowed by modern semiconductor fabs' ceilings: About 2 meters or 6 foot, 6 inches," Y writes. He even adds a touch of humor, noting this is "just a bit taller than a Michael Jordan, the semiconductor industry's widely-accepted standard for height increment."

This detail is important because it grounds the theoretical proposal in the physical constraints of real-world factories. While the industry has gotten used to the massive footprint of High-NA EUV tools, a machine that pushes the ceiling limit introduces new logistical challenges. Y suggests that fab operators might be less phased by this now than they would have been a decade ago, given the scale of current equipment. However, he also wonders about the "second-order effects of such a big device," acknowledging that size is not the only factor in manufacturing efficiency.

The author concludes by reiterating that Shintake is careful not to frame this as a replacement for ASML. "Shintake makes it clear to me that his system no way challenges ASML's. In fact, it should complement it," Y writes. This is a nuanced position that avoids the hype of a "disruptor" narrative. Instead, it suggests a future where fabs might use a mix of lithography machines: the complex, high-cost ASML systems for the most critical layers, and these simpler, more efficient systems for others.

"Perhaps fabs in the future adopt a mix of lithography machines - doing some very complicated layers with those machines and others with simpler mirrors."

Bottom Line

Jon Y's analysis is a masterclass in separating the signal from the noise in semiconductor hype. The strongest part of the argument is the rigorous historical context that shows how the industry's current complexity is a specific solution to specific problems, not an inevitable law of physics. The biggest vulnerability remains the sheer scale of the proposed machine and the difficulty of manufacturing mirrors with the required precision at a larger physical footprint. Readers should watch for whether the "dual line field" illumination can be scaled to the throughput speeds required by high-volume manufacturing, as efficiency is the only metric that matters to the industry's bottom line.

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Euv with fewer mirrors?

Has it really been so long since I last did a newsletter? That is kind of crazy. Time moves so fast.

Like as I wrote before, I want to thank Professor Shintake as well as Dr. Patrick Naulleau of EUV Tech for their help and consultation. They are the true experts of this domain.

I do want to note that ASML chose the number of mirrors they did for a very real reason. It gives them full ability to print specific features on the mask. Simplifying the number of mirrors that away so we should keep this in mind. Perhaps fabs in the future adopt a mix of lithography machines - doing some very complicated layers with those machines and others with simpler mirrors.

A mirror inside ASML's EUV lithography machine reflects just 70% of the EUV light it receives.

With 10-12 reflections in the machine, this can get inefficient. Just 1% of the photons hit the wafer. Electrical power efficiency is said to be less than 0.2%.

It also contributes to troublesome stochastic defects, since not enough EUV photons hit the resist to overcome quantum effects.

So a recent paper from Professor Tsumoru Shintake at the Okinawa Institute of Science & Technology caught my eye.

It proposes a simplified setup with radically fewer mirrors. But Shintake makes it clear to me that his system no way challenges ASML's. In fact, it should complement it.

I think this thing can work. In today’s video, I want to walk you through this interesting new thing cooking up in beautiful Okinawa.

Beginnings.

We should begin with a brief overview of a commercial EUV lithography system. I am not going to cover everything, just enough to get you through this video.

First, we need EUV light, 13.5 nanometer wavelength light. The light source creates it in a number of ways - lasers hitting tin droplets, particle accelerators, whatever you want.

A mirror then collects the light and sends it through the Illumination module, which spreads out the light and makes it as uniform as possible for the mask.

That light then bounces off a photomask, a special mirror with the chip design printed onto it.

The reflected light then goes through an Optical Projection module that reduces the size of the pattern on the mask's field by some ratio and focuses it.

Finally, the light hits the resist-coated wafer. Ideally at the exact ...