249 karma · joined July 22, 2016
Having taught low-temperature condensed matter labs, a big part of the grade is figuring out what went wrong, and either correcting for it, or at least acknowledging that it went wrong. The student needed to give more information about the experimental setup (what instruments did they use? four point or two point resistance? resistivity vs resistance? what is R_0?) and why they think the experiment didn't work. It looks to me like they had something miswired, so they only measured noise.
It's worth reiterating that while graphene can have some niche uses in "the real world", the main reason that it is so highly prized within academia is that it is a superb platform for studying fundamental physics, as in this work. Maybe in the future this will lead to room-temperature superconductors or something along those lines. Maybe not. Nobody jokes about how the Higgs boson has failed to leave the lab.
These days, common practice is to cut the graphene with an AFM or laser prior to stacking.
> Creating a working device typically takes them dozens of tries. And even then, each device behaves differently, so specific experiments are almost impossible to repeat.
This is frustrating. You can make two twisted bilayer graphene samples at 1.10 degrees precisely (to within 0.01 degrees), and they will show completely different phase diagrams. One will superconduct, but the other will not. Things like that.
What I learned recently is that every transport paper's twist angle report is wrong. The two hypothetical samples are actually probably not both 1.10 degrees. The uncertainty in twist angle should be of order 10-20%, rather than <1%. I even made this same mistake in my own paper last year!
When creating these TBG samples, we used to literally tear the graphene in half, to get accurate relative alignment of the two halves. It was very clever, but it imparts a huge amount of strain to the two layers, generally of order 0.1-0.3%. This seems like a small amount, but moire patterns are extremely sensitive to this (roughly strain amount divided by twist angle, but the twist angle is very small), so the unit cell area gets modified by anywhere from 5-30%. In transport measurements, we can only measure moire unit cell area, but not twist angle. The number 1.10 +\- 0.01 deg is calculated assuming no strain, and this is an incorrect assumption. An STM paper from 2019 first pointed this out, but it was just a couple sentences buried in the supplemental material, and I (and most others) completely missed it.
Even four years after moire materials took over the condensed matter world, we still don't understand the basics of how the materials work. It's very exciting, hot stuff.
Of course what he did was mega illegal and he knew it, but it's still sad.
Still, thoroughly enjoyed it.
This is not the first time a tetraquark has been measured, but instead it's the first time a tetraquark with two charm quarks and no charm antiquarks. That's still nice work, but I was initially confused by the headline ("didn't they discover those already?").
https://en.wikipedia.org/wiki/Kung-Fu_Chess https://www.youtube.com/watch?v=fVob7meb83w
Many of the cool excitonic properties that he describes were recently (last 10 years ish) seen in a class of materials known as TMDCs: https://en.wikipedia.org/wiki/Transition_metal_dichalcogenid...
Condensed matter physics is the largest field of physics by number of PhDs granted, but I feel like it gets a disproportionately low amount of pop sci coverage.
https://en.wikipedia.org/wiki/Hofstadter%27s_butterfly
In the '70s, Hofstadter wrote about this neat fractal pattern that would show up in the band structure of a material in a sufficiently large magnetic field. Specifically, the magnetic field strength times the crystal unit cell area needed to be big. Magnetic field strength is limited by how much current you can put around a superconducting solenoid. Unit cell area is generally something that you can't change for ordinary crystals: it's just set by the chemistry of the material.
Back in 2012-ish, a few groups managed to artificially increase the area of the unit cell by multiple orders of magnitude by aligning the graphene with hexagonal boron nitride, which has the same crystal structure and a very similar size. When aligned, the moire pattern itself has a large size, and that was enough to see the butterfly.
You may have noticed that literally every experimental paper on this stuff has Kenji Watanabe and Takashi Taniguchi as authors. This is because they grow the best hBN crystals in the world and they give them for free to pretty much any researcher who asks nicely. This is amazing and without them the whole field would be way worse off. Their crystals are the bulk sort that needs scotch tape to use, much like graphite needs scotch tape to isolate graphene. I don't think CVD hBN is nearly as good as their stuff yet. The hBN provides an encapsulating dielectric for the graphene, and is critical to getting high-quality devices.
That's just one example of a problem with scaling this stuff, and there are others as well. The field is working to improve these things though, since right now it's super difficult to reproduce any given piece of physics. I think at this point there are exactly 3 ferromagnetic TBG devices in the world, for instance.
Regardless of whether graphene has left the lab and made it into consumer electronics or not, it's still super interesting for academics.
Source: I work on this stuff.