Everyday Apparatus
Chemistryopenalex3 min read1 month ago

The Transistor's Next Shrink Isn't Smaller. It's Vertical.

The wall Moore's Law kept hitting wasn't physics. It was the direction engineers had always been building.

A read of All-2D vertical metal-semiconductor field-effect transistor with sub-10 nm channel and contact lengths · openalex

2D materials

Crystalline solids just one or a few atoms thick whose electronic properties differ sharply from their bulk counterparts — graphene and MoS₂ are the main examples here.

Channel length

The distance current must cross between source and drain; the dimension that most directly governs transistor speed, power, and how hard the device is to shrink.

Contact length

The overlap between a metal electrode and the semiconductor; shrink it too far and resistance climbs, but leaving it large wastes the footprint gains from a shorter channel.

Subthreshold swing

Gate voltage needed to change current by a factor of ten; ~62 mV/decade is the room-temperature minimum, and hitting it means the gate has near-perfect channel control.

Heterostructure

A layered stack of different 2D materials assembled to engineer specific electrical behavior — here, graphene electrodes sandwiching hBN insulators, with MoS₂ running up the side.

What it’s not claiming · The authors do not claim that their sub‑10 nm vertical device constitutes a manufacturable replacement for conventional planar MOSFETs or that it instantly solves the mass‑production challenges of modern semiconductor factories.

The computer that guided Apollo to the moon filled a room. The one on your nightstand is millions of times more capable. That staggering gap is the story of a single trick repeated for fifty years: engineers kept making the switches inside a chip smaller, roughly halving them every couple of years, packing more onto the same sliver of silicon. It worked so reliably it got a name and started to feel like a law of nature. Then, about a decade ago, the shrinking began to stall.

To see why, you have to look at one of those switches up close. Each has two parts that matter. There is a channel, the narrow hallway electrons travel down, and there are the contacts, the doorways they enter and leave through. Squeeze both narrower than about ten nanometers, roughly thirty atoms across, and the thing stops behaving like a switch. Electrons leak where they shouldn't. The gate that is supposed to cut the flow cleanly can no longer manage it. Engineers tried, again and again, and kept hitting the same wall. Ten nanometers stopped being a goal and became a ceiling, fixed by everyone's hard experience.

Then a research team asked whether the wall was really made of physics, or of habit. Every chip ever built lays its transistors out flat, carved sideways across the surface like streets on a map. What if you stood the transistor up instead? They built one as a vertical stack of sheets, each just atoms thick, like a tiny club sandwich. And in a stack, the dimensions that decide everything are no longer widths you have to etch. They are the thicknesses of the layers. Thickness is something you can control one atom at a time. The channel and the contacts could both shrink at once, because the limit had never come from the electrons — it came from the direction they were building.

The numbers held. Both the channel and the contacts came in under ten nanometers, and the whole transistor stood less than thirty nanometers tall. It switched cleanly, the "on" state carrying more than ten million times the current of the "off" state, all running on about half a volt. Those are not lab curiosities. They sit right where the industry's most advanced chips are trying to land. The atom-thin sandwich did what the flat carving could not.

One limit remains. A single device on a university bench is a long way from a billion of them stamped out in a factory, and chipmaking is an industrial art refined over sixty years to extraordinary precision. Whether a factory can deposit these gossamer sheets evenly, stack them reliably, and wire them into a working chip is a real and open question, and the paper claims nothing more. But it proved the one thing that mattered. The floor was never a floor. It was a convention. And conventions, unlike physics, are ours to change.

Where this sits

Open question

The critical unresolved issue is whether the atomically thin graphene, hBN and MoS₂ layers can be deposited with wafer‑scale uniformity and high throughput enough to integrate billions of these vertical transistors into practical circuits.

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