The behavior of electrons in a material depend on the material. Crystals and sheets of graphene are special because of their periodicity, i.e. the inability to distinguish one location in the lattice from another over long distances. The wavefuntions of electrons are to first order due to this periodic potential.
Crystals are also interesting mathematically because there is a finite number of possible lattices that can exist, and it isn't even that many. All the useful and interesting effects of doping semiconductors is the result of throwing some contaminants in to disrupt the perfect periodicity of the silicon crystal and therebey make junctions that can ultimately be used for computation etc. "Holes" are sort of emergent quasiparticles with charge +1.
I think a key term in the article is "moire". When two regular patterns are overlayed and then twisted or offset, they interfere to produce a new emergent pattern, sometimes with radically different periodicity than the original. The electrons must now inhabit this very artificial pattern of pottentials that is neither a crystal or a doped crystal and may not occur in nature at all. Plus there are probably effects caused by the material being nearly 2d.
Very exciting stuff, emergent complexity seems to be a major theme in physics so far this century.
> Here, we devise a theory that incorporates the quantum geometry of the electron bands into the electron–phonon coupling, demonstrating the crucial contributions of the Fubini–Study metric or its orbital selective version to the dimensionless electron–phonon coupling constant. We apply the theory to two materials, that is, graphene and MgB2, where the geometric contributions account for approximately 50% and 90% of the total electron–phonon coupling constant, respectively. The quantum geometric contributions in the two systems are further bounded from below by topological contributions
> Here, we devise a theory that incorporates the quantum geometry of the electron bands into the electron–phonon coupling, demonstrating the crucial contributions of the Fubini–Study metric or its orbital selective version to the dimensionless electron–phonon coupling constant. We apply the theory to two materials, that is, graphene and MgB2, where the geometric contributions account for approximately 50% and 90% of the total electron–phonon coupling constant, respectively. The quantum geometric contributions in the two systems are further bounded from below by topological contributions
There is emergence in complex fluid attractor systems.
I've never seen a good clear explanation of "fractionalization" - the way that that systems can contain excitations that act like particles with charges that are a fraction of the electron charge. A typical non-explanation:
Couldn't an effective theory/mean-field theory have almost any emergent behavior depending on the underlying configuration space/system? Kind of like how one can build a domain-specific language out of an expressive enough underlying language it's implemented in
Maybe, but getting fractional charges out of a system with charges that are integer multiples of the electron charge is no mean feat, and I want to understand the math behind this in detail. Someone knows, but I haven't found any clear explanations.
I'm no physics expert but I do make programmable crystals for a living. One of my favorite applications of adiabatic quantum computers is the simulation of physical materials such as [1] wherein we see emergent phenomena like fractional magnetization. My contribution to this paper was to find the configuration of qubits equivalent to the material in question. What's really cool about experiments like this is that you can directly observe the spin configurations that give rise to the fractional states -- if you're sufficiently motivated, you could reproduce the experiment and paw through the data yourself (disclaimer: that may require you to pay my employer for QPU access). For the less motivated, see figure 3.
The way my inner child handwaves it away: you have the electron wavefunction spread out, say, it’s equally likely to be in one of 2 points in space. If you only look at one of these 2 points, you are likely to measure only half an electron.. until an adult (say, you) corrects me (using the Feynman Dirac hand/belt trick)
That explains having a 50% chance of seeing an electron somewhere, not seeing an entity of charge 1/2. It's like a weather report saying there's a 50% chance of rain doesn't mean you're going to see little raindrops cut in half.
If you look at the experiments, they don’t mention observing a single entity of fractional charge, it is always in terms of aggregate behavior under EM fields: conductance(1) inferred from shot noise (2), or density (3)
Personally, I find it curious that people talk about detecting single photons, but in these fractional charge experiments, nobody mentions detecting a single quasiparticle.
As for the math, nobody says it outright, or even in a single paragraph, but a fractional charge (“filling fraction”) of p/q does correspond to p “normal” charges distributed over q degenerate states (q=2 equivalent locations I used in the naive example)
> Personally, I find it curious that people talk about detecting single photons, but in these fractional charge experiments, nobody mentions detecting a single quasiparticle.
You detect a single photon when it perturbs an apparatus like a photon multiplier; you detect a single quasiparticle when it perturbs a split stream of electrons.
The apparent difference is that photons can travel through free space and strike such an apparatus from afar; while quasiparticles definitionally cannot. However, I’ve read about experiments that measure a single anyon on a dot by wrapping electron interferometry around it, which is measuring the lone quasiparticle on that dot.
I still think my point, originally about 1 electron split into 2 locations, or “ends” of string (but devolving to a complaint about casual ignorance of the central issue in publications) hasn’t been completely destroyed, because here you are measuring interference of 2 anyons, somewhat like measuring the interference of a photon “with itself” in a double split experiment.
The broader point could be that the effect of a single photon is “localized”, but here to see the effect, you have to move 1 anyon in a “complete path” around the other, recalling the Feynman/Dirac belt in my top level comment, a trick I said an adult should try to correct me with :)
> the world is far more complicated than a human can grasp in their lifetime
Language plays a big part in this "grasping" process. Without language we would not have been able to build upon past experience and get to where we are now. It now preserves more knowledge than any one human can ever learn. We often think intelligence is an individual trait, but it is made of concepts and methods discovered by a social process based on language. A single human can't bootstrap to that level on his own.
I wonder if the moire materials can tuned as a dynamic metamaterial to absorb or dump a lot of charge, based on their rotational geometry. That charge plateau seems like a quite powerful trick
Crystals are also interesting mathematically because there is a finite number of possible lattices that can exist, and it isn't even that many. All the useful and interesting effects of doping semiconductors is the result of throwing some contaminants in to disrupt the perfect periodicity of the silicon crystal and therebey make junctions that can ultimately be used for computation etc. "Holes" are sort of emergent quasiparticles with charge +1.
I think a key term in the article is "moire". When two regular patterns are overlayed and then twisted or offset, they interfere to produce a new emergent pattern, sometimes with radically different periodicity than the original. The electrons must now inhabit this very artificial pattern of pottentials that is neither a crystal or a doped crystal and may not occur in nature at all. Plus there are probably effects caused by the material being nearly 2d.
Very exciting stuff, emergent complexity seems to be a major theme in physics so far this century.