When it matures, you’re right back to the same heat constraint considerations, just with faster chips.
> Rather than allowing heat to build up, what if we could spread it out right from the start, inside the chip?... To do that, we’d have to introduce a highly thermally conductive material inside the IC, mere nanometers from the transistors, without messing up any of their very precise and sensitive properties. Enter an unexpected material—diamond.
> ... my research group at Stanford University has managed what seemed impossible. We can now grow a form of diamond suitable for spreading heat, directly atop semiconductor devices at low enough temperatures that even the most delicate interconnects inside advanced chips will survive... Our diamonds are a polycrystalline coating no more than a couple of micrometers thick.
> The potential benefits could be huge. In some of our earliest gallium-nitride radio-frequency transistors, the addition of diamond dropped the device temperature by more than 50 °C.
It sounds like the most important part of the article (and another cool quote) is this:
>Until recently we knew how to grow it only at circuit-slagging temperatures in excess of 1,000 °C.
So basically, the big breakthrough was low-temp growth of a diamond lattice. Very cool they can do it at such a low temperature. It must be a crazy low temp - probably under 100C?
"we were able to find a formula that produced coatings of large-grained polycrystalline diamond all around devices at 400 °C, which is a survivable temperature for CMOS circuits and other devices."
Learnt that in Physics lab.
Not to say that it can't be done, only that the process window is not very large and the propensity for deleterious carbon soot is very high. Likely this will generate some very fun, highly integrated problem statements before we see this available for sale.
Getting heat out of the chip is such a painful and important struggle. I hope this works on a real process line. Too many benefits on the table to ignore.
Edit: Grammar, clarity
https://www.powerelectronicsnews.com/diamond-semiconductors-...
Edit: Because they are polycrystalline, and produced with a very new and novel technology.
"Our diamonds are a polycrystalline coating no more than a couple of micrometers thick."
> The high p-n junction built-in voltage (4.9V, compared to 2.8V in SiC) and short carrier lifetimes limit the advantages of bipolar diamond devices to only ultra-high voltages (> 6kV) and low switching frequencies.
Nobody is thinking about using diamond for the silicon CMOS logic in a computer, though they may replace the gallium arsenide we use for motor control some day.
"Before my lab turned to developing diamond as a heat-spreading material, we were working on it as a semiconductor. In its single-crystal form—like the kind on your finger—it has a wide bandgap and ability to withstand enormous electric fields. Single-crystalline diamond also offers some of the highest thermal conductivity recorded in any material, reaching 2,200 to 2,400 watts per meter per kelvin—roughly six times as conductive as copper. Polycrystalline diamond—an easier to make material—can approach these values when grown thick. Even in this form, it outperforms copper.
"As attractive as diamond transistors might be, I was keenly aware—based on my experience researching gallium nitride devices—of the long road ahead..."
BTW, the thermal conductivity of C-12 diamond at cryogenic temperature is even higher, reaching something like 41000 W/m K at 104 K.
Isotopically purified silicon has also been considered due to its higher thermal conductivity, but the effect there at room temperature is not nearly as dramatic.
Weirdly, I read UV damage in C-12 diamond is reduced by a factor of 10 vs. natural diamond, I understand because this damage process is mediated by phonons. No relevance to the chip use case (unless UV damage in photolithography could be important?), but I found it interesting.
On an unrelated note, I like the writing style of this article a lot. This is how science journalism should be. It reminds me of how Scientific American used to be before it was ruined. Is IEEE Spectrum always like this? I might have to subscribe to the print version. I want articles like this floating around my house for my kids to discover.
If a chip were to be stacked as tall as it was wide, are we talking 10x, 100x, 100,000x?
I guess for N stacks you're still paying N chips worth of wafer, and Nx the amount of defects.
The packaging usually has the stacked dies offset in a staircase pattern so that the contacts at the edge are exposed for every die. The alternative is through-silicon vias (TSVs), which theoretically would allow stacking until you have a mass of chips that is roughly a cube, but achieving that without having a defective connection somewhere in the stack is approximately impossible.
This is probably not an issue for thermal TSVs, because of the heat spreader layer between each silicon layer, but it would become an issue for power TSVs, as each layer would (presumably) require an independent supply of power.
That said, mentioned temperature gains are absolutely and utterly insane even if they come with some high-frequency issues.
This on top of all the through-silicon-vias and backside power delivery would make even the crustiest of engineers weep...
"Oxygen-assisted monodisperse transition-metal-atom-induced graphite phase transformation to diamond: a first-principles calculation study"
I think it's pay-walled unfortunately. https://pubs.rsc.org/en/content/articlelanding/2024/ta/d4ta0...
Not sure I understand this. Is this a requirement for real-world use? What happens if the outside of the coating isn't atomically flat? What makes this hard to do?
Caveat: For older processes, built on a larger scale (>1 micron), these kinds of details may not matter, in which you are right to question this point. But if you want to implement on cutting edge manufacturing processes, these details absolutely do matter.
To put this in perspective, in cutting edge process nodes, I've seen senior engineers argue bitterly over ~1 nm in a certain critical dimension. That's (roughly) about 5 atoms across, depending on how much you trust the accuracy of the metrology.
So, if ANY layer isn't "flat" (or otherwise to spec within tolerance), the next layer in the semiconductor patterning stack will tend to translate that bumpiness upward, or cause a deformity in adjacent structure. This is (almost) always bad. These defects cause voids, bad electrical/thermal contacts and characteristics, misshapen/displaced structures, etc, etc
Crystallization in thin-film (especially conformal/gap-filling films) is a tough job which many poor PhD students have slaved over. Poly crystalline material is arguably harder to control in some key ways vs mono crystalline, since you don't have direct control the specific crystal grain orientation and growth direction. That is, some grain orientations will grow quickly, and others growing slowly. You can imagine the challenge then of getting the layer to terminate growth without ending up too jagged on the ~nm scale. After that you also get into the fun world of crystal defects, grain size, and deciding if you need to do some more post-processing (do I risk planarizing?)
Hopefully I have captured some of the pieces involved in an understandable way.
Edit: clarity
I confess to being a nerd that appreciates this “joke”
djoldman•6h ago