@DIRAC1930 it depends on the goals. sometimes the goal is just to do abstraction and generalisation. but some generalisation is stupid, yes. one's intuition guides the kind of abstraction that might lead to interesting results.
@SillyGoose sure (but then you could argue if you're engaging in this meta-study of notions of aesthetics you're again not using your own aesthetic sense :P)
@Allie I've recently been binge-ing upon essentially exact solutions to few-electron wavefunctions, especially He and Li and H2, some of which are even without Born-Oppenheimer approximation.
both :P but i am a very squeamish person. also why i didnt go into synthesis, i am very clumsy and also very afraid of spilling some nasty chemical on myself
This article lists notable unsolved problems in biology.
== General biology ==
=== Evolution and origins of life ===
Origin of life. Exactly how, where, and when did life on Earth originate? Which, if any, of the many hypotheses is correct? What were the metabolic pathways used by the earliest life forms? How did genetic code originate? What was the molecular mechanism that allows the association of the amino acids with their triplet codons? What were the biochemical paths from individual bio-building blocks like amino acids or nucleic acids to functional polymers such as proteins and D...
> Laughter: While it is generally accepted that laughing evolved as a form of social communication, the exact neurobiological process that leads humans to laugh is not well understood.
@Allie still, it is extremely exciting to see evidence that quantum theory gets > 40 digits agreement with experiment in all kinds of phenomena, from 2 electrons to 6 electrons, to Rydberg atoms, etc.
The following is a list of notable unsolved problems grouped into broad areas of physics.
Some of the major unsolved problems in physics are theoretical, meaning that existing theories seem incapable of explaining a certain observed phenomenon or experimental result. The others are experimental, meaning that there is a difficulty in creating an experiment to test a proposed theory or investigate a phenomenon in greater detail.
There are still some questions beyond the Standard Model of physics, such as the strong CP problem, neutrino mass, matter–antimatter asymmetry, and the nature of dark matter...
Well, the Hylleraas method means that the resulting wavefunctions have electron-electron separation as part of their coördinates, which makes it difficult to plot the wavefunctions in space
@RyderRude Well, the problem is of course general. The point is that you cannot decide for every Hamiltonian (from a certain class) whether or not is has a spectral gap, roughly speaking
@Allie But I still want to plot those wavefunctions in space just as to see, especially to see what the handling of the Kato cusp conditions causes the wavefunctions to change.
> Locality: Are there non-local phenomena in quantum physics?[98][99] If they exist, are non-local phenomena limited to the entanglement revealed in the violations of the Bell inequalities, or can information and conserved quantities also move in a non-local way?
@Allie I wonder if it is possible to merge the Hylleraas method with the method that treats the nuclei with Dirac equation too, i.e. fully SR in everything. However, I'm wary of trying to compute the Bethe logarithm in this context. It will be hell.
im honestly not sure. the way i think of it (and it might be a complete cop-out/wrong answer, but) is that they are just the orbitals that naturally arise from an N-electron wave function
so if you want some way to extract a one-electron wave function from the N-electron one, the eigenfunctions of the 1-RDM seems like a somewhat natural way to do that. but again, may be completely talking out of my ass
@TobiasFünke definitely let me know! i am interested too
interestingly, Heisenberg was bothered by this non locality of Copenhagen interpretation, and he proceeded to re-define Copenhagen interpretation to mean that the collapse is not a physical process, but it only happens in the mind of the observer
this completely contradicts the previous usage of Copenhagen interpretation. it is where the idea that "no one really knows was Copenhagen interpretation means" originates
@RyderRude idk if this is his position. he and others, mostly philosophers (but not exclusively) say that most people dismiss the two-step argument in Bell's original paper, and thus come to the wrong conclusion (they do not a priori claim that "realism" is true, but rather that "local" must be false)-- but their work is criticized, too, in a lot of papers
vey roughly speaking. Here on PSE, there are some users also holding this position. wait a sec.
I was watching a video of Tim Maudlin where he talks about how the CHSH version of Bell’s inequalities do not assume determinism and only assume locality. He said that it is a common misconception that Bell assumed determinism and that in the CHSH version, he was explicit about not assuming that....
As I said, their approach is criticized in many papers, too. ^^ I don't have the knowledge (yet) to "decide" what I find more plausible-- I am annoyed by the overloaded words lol
as I said, check the scholarpedia article (for me the site somehow does not work right now)
he is not an author, IIRC, though
there is some article "What Bell really did" or so by him. (and also check the critique article by Werner)
in Tumulka's QM book the argument is outlined, too... and if you search a bit you will find many more articles, and also the opponents arguing against it
@SillyGoose it's a theorem about relations between certain expressions in c/a operators. There are no dynamics involved, so I don't understand where "free" or "interacting" would enter
er i guess i am confused about the following facts
(1) a VeV by construction doesn't allow non-particle-number-conserving "scattering events" to survive, e.g. $\langle 0 \lvert a^\dagger a^\dagger \lvert 0 \rangle = 0$
(2) Wick's theorem should be general as you stated, so how do I get contributions from NPNC "scattering events"?
the $P$ is a permutation on the set $\{1, 2, ...\}$ from which $r := t_r$ takes its values. The notation $P'_r$ means apply permutation $P$ to $r$ then turn it into a primed coordinate.
to me Wick's theorem is a purely combinatorial statement about the relationship between time-order and normal-order, as in e.g. this answer by Qmechanic
if we ultimately reduce every scattering computation into an LSZ like computation, which is heuristically the VeV of some time-ordered set of fields, how do you ever get NPNC contributions
if someone is interested, there is also a "Wick's theorem" for stat. mech; a starting point is Une démonstration simplifiée du théoreme de wick en mécanique statistique by Gaudin (1960)
@DIRAC1930 i didn't get too far in :P it seems like it is kind of neat for taking the theory from a phenomenological perspective. it is a bit terse for me. i found online notes by fradkin and etc. more illuminating.
i felt like i was wasting time reading L&L9, but perhaps it would be good to go back to after already knowing the theory so that time is not wasted thinking if a step is being skipped or etc.
But in cases where the action has multiple minima, do all of those paths satisfy the EL equation? Im having trouble making sense of this in regards to how this relates to the initial
@Allie The E-L equations are local differential equations you can solve as an initial value problem. Each path you obtain in this way is a stationary point of the action with respect to variations adhering to the boundary value problem where the start and end point of that path are the given boundaries
@Allie he says that the diagonal form of the 1-RDM "is characterized by the fact that all bond orders are vanishing" (and argues that thus the name is appropriate) -- do you know what this means? (the quote is from his paper "Quantum Theory of Many-Particle Systems. I", right below eq. 74)
it's a not particularly precise phrase that just means you're treating the field classically, not as a quantum field so that photons could be generated or whatever
you've literally asked the same question about the same situation (scattering off an external field)
@SillyGoose You keep being strangely vague about what setting you're talking about. The standard "fermion field" in relativistic QFT is the Dirac field, which has two sets of c/a operators. You've written down a number operator for one set. What exactly is "the free fermion field" you want to ask about here?
but anyway, of course the number density operator for the particles created by some creation operator $c^\dagger$ is just $n = \sum_\sigma c_{k\sigma}^\dagger c_{k\sigma}$. That's how number operators work.
@TobiasFünke that might be, but so far I haven't seen any "field" here and the goose switches confusingly between obviously talking about condensed matter stuff and then referencing Schwartz (which is a hep-th book as far as I know :P) so I really find it hard to tell what's going on
@TobiasFünke Then can you tell me why the chemical potential is considered as a part of the Hamiltonian. In BCS, for example they add it before minimizing as a "constraint", which mathematically is ok, but I don't really see the physical meaning. It's very reminiscent of the exponent of the density matrix in the GCE, but I would like a stronger motivation
@SignorFeynman it is not part of the Hamiltonian, no. It is when you consider the grand canonical ensemble, i.e. situation where the number of particles is not fixed
i think i am conflating just counting up all the particles (number) and actually keeping track of their locations in addition to counting them up (density)
I mean, in the GCE I know how it appears. On the other hand, in SC books they often just "manually" define $\mathcal{H}=H-\mu N$ and use it e.g. in the variational principle for energy. It is not as "natural" as the way it appears in the GCE density matrix, or in the entropy variational principle 🤔
@SignorFeynman hmhmhm. I mean it appears when you e.g. want to minimize the energy but also let the particle number vary (as you seem to know), where BCS is, I suppose, an instance of that. but I've never seen a claim that this is the Hamiltonian
well, wait a second
at least the point is true when $H$ and $N$ commute
which shouldn't be the case for the BCS hamiltonian
Btw one has to be careful with using $\int \mathrm{d}x \psi^\dagger j^\mu \psi$ when it comes to the Dirac theory since it gives the wrong expression. However one can add an extra term allowed by an operator ordering ambiguity so everything works out
hm okay i think there is a rather simple explanation for my wrong computation getting the right answer. physically in the situation of a simple fermion gas, the particle density actually is just constant within the fermi surface. so if i count all particles and divide by the volume i will get the same answer as properly computing the density.
but indeed in no other circumstance will just counting up the particles work.
yeah, I think the idea is to get the gap equation, and then extract $\mu$ from the desired average particle number; this probably has to be done iteratively or so; once you have determined those quantities, you get the coefficients $u_k,v_k$ and can determine the BCS state
This state by definition yields the minimal energy and the (desired) average particle number
and in contrast to the "usual" CGE cases from e.g. stat. mech, the hamiltonian and the number operator do not commute, so we expect that the ground state does not have a well-defined particle number (which we know already for the BCS state)