First-principles study on the electronic structure of Pb10−xCux(PO4)6O (x=0, 1)
arxiv.org
arxiv.org
You meant the calculations can't show it's a superconductor, but can only show that some materials aren't?
If this is correct, then it is expected that it will be very hard to produce good samples, because when impurity atoms are introduced in a crystal it is very difficult to control the final positions of the atoms, when there is little energy difference between alternatives.
Minor differences in heat treatment can cause great differences in the electrical and magnetic properties of the samples.
So it is likely that some time will pass until we will know for sure whether this material can be a superconductor, unless some laboratory gets very lucky.
I suppose that the reason why the Korean team was not really ready to publish their results is because they are not able yet to produce material samples in a reproducible manner.
Papers about failed experiments are worth a lot more than no papers about failed experiments. Alas, it is rare.
:heart:
People have been trying to get there for decades.
It almost feels like we're on the brink of some revolutionary discoveries: quantum computers, room-temperature superconductors, fusion, general artificial intelligence. Unless it's all hype. I'm reluctant to be optimistic.
Maybe the AI can help us develop a quantum computer with which we'll find useful materials to build a fusion reactor!
So, very much a quantum mechanical effect.
Because reasoning about the real deal sounds like it would be rather difficult for me (and likely too difficult for me without significant assistance, at least, within any reasonable about of time for me to spend on this), I want to make up a toy model now.
Say I have a single-electron Hilbert space and a single electron Hamiltonian on it (where, I would later maybe add terms for interactions between the electrons, and/or a space for how the surrounding material can change in ways tied to the electrons). Below a certain energy level, I want to say that the eigenspace of the single electron Hamiltonian for each lower energy level, is finite-dimensional, and also the spectrum is discrete. (and, I want to consider the electrons only with energies below this threshold.)
For any wavefunction in the single-electron Hilbert space, there is a corresponding creation operator acting on the Fock space.
Now, I imagine that without any interactions, the concept of a cooper pair is probably inapplicable. But, I am imagining that when we add in the interactions, that, at least at low energies, the Fock space obtained from the single-electron Hilbert space, should work as a Hilbert space for the many-particle system with interactions between electrons (and then, I guess take the tensor-product with another Hilbert space representing how nuclei can change, when handling that part).
Everything in the Fock space can be obtained as a linear combination of applications of some number of creation operators to the vacuum state. As such, a state with a single cooper pair can be expressed as a linear combination of states obtained by applying two creation operators to the vacuum state.
Unless this "linear combination" can be done with only a single term, this would be an entangled state, right?
I would think that there should be creation operators for cooper pairs, consisting of a linear combination of products of two creation operators for electrons?
A Cooper pair is a composite object, and you absolutely need to consider the atomic lattice of the superconductor.
So you end up with your electron being entangled with all the surrounding atoms in the lattice. And all other electrons.
please, issue corrections in the comments if you have a second