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5:00 PM
@mercio, dear adviser, any takes on my comments?
 
From t=x to 1, though, it won’t be true. Instead, x-t will be between x-1<0 and 0
 
I have to think more about representations
and also eat something
 
just had fresh pike :-)
 
sorry I'm not giving it much time those days
 
And since the terms of the Fourier series are 1-periodic, we have to extend v=x in a compatible way
 
5:02 PM
@mercio: no prob
 
In particular, v(x)=x+1 for -1<x<0
 
@Semiclassical: So it was an domain issue?
 
I guess so
I can’t check the calculation at the moment, but the explanation seems sound
 
I also think so
How comes your username?
 
Most of my research work has revolved around semiclassical computations in one way or another
Plus I like the word
 
5:10 PM
What is it exactly that your calculating semiclassically?
 
The two big examples are energy levels and level splitting
 
:-) that sound familiar. Solids or molecules?
level splitting by what perturbation?
-- away for 5 min ---
 
the simplest example is a symmetric double well potential
If you had two identical disconnected wells then you’d have a doubly degenerate ground state
But the barrier between the wells is finite, and as a consequence the levels split
...as they’d better, since the potential is symmetric and therefore parity should be a good quantum number
But this splitting is exponentially small and therefore can’t be captured by perturbation theory. Instead you have to proceed from either the WKB approximation or use a saddle point approximation on the path integral
 
this is second order Jahn-Teller, isn't it?
 
Couldn’t tell you. I don’t remember the various terminologies
 
5:19 PM
"this splitting is exponentially small and therefore can’t be captured by perturbation theory" sounds quite interesting
 
The example I remember from textbooks is the level splitting of ammonia?
 
never thought that this could be an issue
 
Closely related to this is the spectrum of a cosine potential
 
@Semiclassical: Yes a kind of strange example for a chemist, this is rather something we'd summarize by non-Born-Oppenheimer effect. But I think its true it could be a 2nd order Jahn-Teller case as well.
As essentially ANY symmetry breaking is somehow the Jahn-Teller effect.
 
Sounds right.
 
5:22 PM
Because in NH3 tunneling is essential. So you need the coupling between nuclear and electronic wave function
And the cases where this coupling is essential often include the Jahn-Teller effect.
 
All of my stuff is 1D, I should note. So nothing terribly realistic
 
The better!
 
The stuff I am torchering people here with sice some days is actually also about some Jahn-Teller consequences.
 
yeah, sounded like it
 
5:25 PM
though I am not sure if THAT kind of effect shows up in 1D as well. Let me think ...
nope unfortunately not, because you have only two irreps.
trivial one and "B".
 
Well, there’s some interesting stuff in the cosine case
 
Since you have both reflection symmetry and a discrete translation symmetry
 
oh you got translation!
then there is chance - but go on
 
Eh, that’s about all I remember
 
5:28 PM
OK :-)
So what I look at is what is the symmetry of the split states.
 
The actual classification of eigenstates by symmetry is pretty easy though
 
after the distortion.
And then you see that there are two cases, one which includes some irrep of a magnetic transition and another case which doesnt.
 
I should note that, in the case I’m describing, one only has the electronic energy levels
In particular, one doesn’t talk about how the lattice may deform in response
 
(in my case also) If you assume now that you have one patricle in the levels.
 
If you do include that, that can lead to a Pierls transition which I think may be more directly related
 
5:31 PM
Ou I see, then thats something slightly different...
Peirls is the Physics name for Jahn-Teller
 
Right
 
in principle
in practice the one is about periodic systems
and the other about "molecules" (subgroups of SO(3))
 
Right.
 
But the rest is the same.
So you look at electronic symmetry breaking?
purely?
 
To some extent, yeah. But I did a few things and it’s hard for me to sum it up
 
5:34 PM
is it a masters thesis?
 
Oh sorry!
No offense indended ;-)
 
Lol, np
 
Physics then I guess?
 
5:36 PM
lol wtf i thought the space force thing was a joke
i cant believe this is real
 
So does it happen then in your systems that the electron density localizes asymmetrically?
in a symmetric well
?
 
Well, my interest was typically less to do with the form of the wavefunction than the level splitting itself
 
sure, but you will get the WF as well
 
But in both the ground state and first excited state you have the electron being mostly confined to the two wells. The difference is whether it’s s symmetric or antisymmetric combination
 
Oh wait. It seems its really more kind a tunneling
yes its like the ammonia
now I see the connection
 
5:40 PM
So bonding-anti bonding is maybr the better analogy
 
physics sounds like magic to me
lol
 
Guess it would be VERY special case of bonding-antibonding, something we call near-degenrate multi-reference case.
does it sound familiar?
How does the method work you use to calculate the splittings?
 
Basucally it’s just the WKB approximation
 
Thats some very new DFT stuff, isn't it?
 
5:44 PM
in ZFC, Axiom of union just forces the existence of the set which we describe as union, correct?
 
WKB is as old as regular QM stuff
Werner-Kramers-Brillouin I want to say
 
I just checked it on WP, I see never got in touch with that. How many electrons do you have?
or better: do you have inter-electronic interactions to account for?
 
Typically you’re just doing one-electron stuff
 
@Semiclassical: That simplifies life a lot. So you basically need to solve an ODE?
 
Alright, I was given a question you guys may be able to help out with. A friend wants to be able to rank kill-death ratios in a game such that:
-Returns on kills diminish (i.e. the difference in weight between n:m and n+1:m should be less than between n-1:m and n:m)
-If n:m and p:q have the same quotient, but n < p, then n:m is rated less than p:q.

I've tried a few heuristic solutions but none has worked for this yet. Any ideas?
 
5:48 PM
Well, if I was solving an ODE it’d be the Schroedinger equation in which case I’m not doing anything approximate
Main thing is that the tunnel splitting is on the order of exp(-S/hbar) where S is the tunneling action
 
What is the tunneling action?
its the exponential decay rate outside the barrier right?
What is then the "classical" part, if you solve the SE for the potentials and get the tunneling action for different barrires from that.
 
$\int_a^b \sqrt{2m V(x)}\,dx$ for a particle with energy E in a 1D potential, where $a$ and $b$ are the classical minima
Which is computed entirely from knowledge of the potential energy, which is classical
That’s how the tunneling action is defined and calculated
 
vzn
@Rudi_Birnbaum hi, interesting! googled that up & came up with this golem.ph.utexas.edu/category/2013/06/… ams.org/notices/200902/rtx090200212p.pdf
 
The whole point of the WKB approximation is to be able to express QM results in terms of integrals in classical phase space
 
Hi @vzn: Yes that was the "birds and frogs" I was refering to (Freeman Dyson wrote that)
 
5:58 PM
(well, classical configuration space )
 
@Semiclassical OK you calculate the action classically but the WF comes from QM and some "potentials" you get from somewhere.
 
sure. This is all done under the assumption that you know what the potential is
It’s much more simple-minded than something like DFT
 
@vzn : ams.org/notices/200902/rtx090200212p.pdf cvery cool article: "Jokes of nature" that complex numbers & quasicrystals are out there, ...
 
@Rudi_Birnbaum No idea, call me SBA, and I specialize in very fast growing functions.
 
@Semiclassical: Yes since you have only one electron than the Schrödinger eq is a charm ...
 
vzn
6:02 PM
@Rudi_Birnbaum gowers had a very similar essay on "birds vs frogs" using different terms... remarkable it seems dyson does not cite him or vice versa... gowers contrasted grothendieck vs erdos. dpmms.cam.ac.uk/~wtg10/2cultures.pdf
 
@SimplyBeautifulArt: I avoid specialization so its really hard to say what I do ... but my money comes from chemistry teaching and research in university...
 
¯\_(ツ)_/¯
 
vzn
oops my memory may have been off, rereading, he did cite erdos, but maybe he didnt cite grothendieck, but a preeminent "bird" by the classification...
 
@vzn: I see :-) I have read some critics if or how useful it might be to classify 1D quasicrystals for the sake of understanding the Riemann $\rho$s. In case there is no big scepticism I'd be interested in that topic.
 
I’m not sure the two traditions which Gowers described are quite the same distinction as birds vs frogs, though I agree they’re close
 
6:08 PM
I have bookmarked it and will read it soon.
 
@LeakyNun So what did you mean by ZFC is just sentences in logic and why is it bad
 
vzn
@Rudi_Birnbaum the n-category cafe blog alludes to fractal aspects of Riemann which is a key interest of my own. have found a lot of fractal properties in Collatz conjecture over the yrs. are you a student? there are also some deep connections between Riemann and QM theory, have collected misc refs on that over the yrs...
 
With bird vs frog, the distinction seems to be one of scope: look at lots of of problems at once vs focus on one at a time
Whereas the traditions that Gowers proposes are more to do with whether mathematics is a search for a systematic understanding vs building up a range of techniques and methods
 
vzn
@Semiclassical gowers calls it theory building vs problem solving & think a key part/ insight of his essay is that they are complementary & not mutually exclusive. like yin + yang :) ☯
 
@vzn: I'm docent. There is one recent one where a guy uses some $t^-1 xp -px t$ Hamiltonian to prove the Riemann hypothesis. One of a thousand to solve it, but I think the ansatz itself is regarded still ineteresting
RH is then to show that the operator is self-adjoined
 
6:16 PM
Yeah, that was a Bender paper
 
because one can show that the zeros are its eigenvalues.
The Bender was the "serious" one. But then one followed from some "unknown" guy who claimed to have shown it - on second I'll pass the link ...
 
There was a stack question on it at the time
Ah. I wasn’t aware of a follow up
Right, the MSE question:
52
Q: Riemann hypothesis: is Bender-Brody-Müller Hamiltonian a new line of attack?

Slava KashcheyevsThere is a beautiful paper in Physical Review Letters [PRL 118, 130201 (2017), DOI:10.1103/PhysRevLett.118.130201] by Carl Bender, Dorje Brody, and Markus Müller (BBM) on a Hamiltonian approach to the Riemann Hypothesis. The paper is surprisingly easy to follow for a physicist. BBM define a H...

 
A Frederick Moxley
I am not sure if this can be called follow up, since he implies he solved the RH....
 
The main reason for skepticism I’ve seen raised is that similar arguments apply to zeta functions which are known to not satisfy the RH
So those arguments can’t by themselves be sufficient
 
Ah
I once in while thought about how to construct Operators that have prime number eigenvalues. Then there was something which I still do not understand properly but which dampened my interest in prime somehow very strongly.
 
6:24 PM
@Maximus will you be here an hour later?
 
The story I linked in the comments is a fun side story btw (though of course I think it’s intesting since I linked it)
 
It is that the 2D sequence $(m+1)(n+1)$ with $n,m\in \Bbb N$ produces all interges except any prime. that looks simple is simple and somehow demystifies the primes in my eyes a bit... dunno
 
vzn
@Semiclassical thx for digging that up, reminds me, am now organizing my riemann bookmarks + added that one... have been meaning to blog on this...
 
@Semiclassical: Oh great Belizzard himself replied.. I'll read that :-) Thanks
 
@Rudi_Birnbaum Where?
 
6:34 PM
@Semiclassical: In the MSE post you linked : math.stackexchange.com/questions/2211278/…
 
@LeakyNun yes
 
6:54 PM
Is anyone able to explain this proof to me?
 
What is example 3.3?
 
Here but it's kind of how they start the proof
I am assuming they are trying to use comprehension
 
From "Therefore" on it is clear, isn't it?
 
nevermind they are using comprehension
we assume P is true, so x in P
so we let A = P to conclude there exists a B such that x \in B iff x in A and P(x, P, Q)
with B being the original set
 
7:28 PM
Unless I'm mistaken, the isomorphisms in the category of $k$-vector spaces are just... the invertible $k$-linear transformations right?
 
@ÍgjøgnumMeg right
 
Okay lol, sanity check
learning the language
thanks
 
@Rudi_Birnbaum sure, but where in there? his answer has been there a while
 
We need more insanity checks around here ... :)
4
 
7:43 PM
lol
A category needn't have infinitely many objects right?
Sorry if these are silly questions!
no of course not
a group is a groupoid with one object
So if I want to describe a groupoid that isn't a group I can take $\operatorname{Obj}(C) = \lbrace V_1, V_2\rbrace$ with $V_1, V_2$ $k$-vector spaces and then $\operatorname{Hom}_C(V_1, V_2)$ as the identity maps on $V_1$ and $V_2$ respectively and then an invertible linear transformation (and its inverse)? Or is this cheating?
(the linear transformation should map $V_1$ to $V_2$, not just any old linear transformation lol)
 
Hi, @Alessandro. All done graduated?
 
Nope, I have the number theory presentation on Friday
I tried it today and it's about 2 hours and a half long instead of an hour.... I decided that if the intermediate results need an hour to be explained they might as well be the topic of the presentation instead
 
Well, is the presentation for your colleagues or for faculty?
 
Heya @Ted.
 
7:57 PM
heya @Fargle
 
@TedShifrin colleagues
 
Aha. So the question is whether the intermediate results are interesting enough in and of themselves. Sometimes it's better just to quote some black-box results to prove more interesting things.
 
Someone please i have another question. When/if an infinite sum can go inside a function: like infinitesum ln(f(x)) = ln ( infinitesum f(x) ) ?
 
But it's a standard phenomenon that people underestimate the time by a factor of 3 or so ... and you should allow for interruptions/clarifications/questions.
@valer: That's a big vague a question. But uniform convergence of the series might be the answer.
@Fargle: You got my recent answer?
 
Yes, I did. I appreciate it.
 
8:00 PM
Nah they're pretty interesting, I'm going to show how factorization of primes works in cyclotomic extensions, but I'll also prove a more general result about factorizing primes first. I'll also show why in the Galois extension case the factorizations have a simpler form
 
Oh, OK, that sounds not just technical but interesting.
Make sure you intersperse plenty of examples.
 
@Alessandro Nice!
 
We dealt with quadratic extensions in class so it's not completely new either for my classmates but a generalisation
 
@Maximus i'm here now
 
Just make sure you have examples ... and maybe examples illustrating why hypotheses are needed, etc.
One of the standard mistakes I've seen — even in graduate presentations and seminar talks — is dry theorem proofs without concrete examples illustrating the ideas and the need for hypotheses.
 
8:04 PM
That's good advice, thanks, I'll make sure to have examples ready
 
I try to give only bad advice :P
 
@ÍgjøgnumMeg that's ok
or just construct the category abstractly by giving the 2 objects and 4 morphisms
 
@LeakyNun As in, a satisfactory answer to "describe a groupoid that is not a group" would be "a category with $2$ objects, the identity morphisms on these objects, and an isomorphism/its inverse"?
 
yes
 
ha nice, thanks
 
8:08 PM
Awww, I waited, but now I have to brb myself. In case I am not back on time we can talk tomorrow or some other time since I come here often @LeakyNun
 
sorry @Maximus
 
no worries
 
@ÍgjøgnumMeg You would say there are two objects $X$ and $Y$, and $\operatorname{Mor}(-,-)$ is always a singleton, and you could also give the composition table but that's quite enough
 
Fair, the exercise is labelled as "Unimportant exercise" anyway
 
LOL ... I don't think I'd ever write such a label. I mean, I did have an Exercise 0, which was a standard joke, but ... really!
 
8:11 PM
@ÍgjøgnumMeg recall that a category is a set of objects, and for every two objects a set of morphisms, satisfying some axioms
so you just have to give the objects and morphisms
 
Is the collection of all sums of commutators in $B(\mathcal{H})$ topologically closed, where $\mathcal{H}$ is some Hilbert space? Closed with respect to the strong operator topology would be nice, but if it's closed with respect to any of the standard topologies on $B(H)$, I would be interested in knowing.
 
oh and the composition function @ÍgjøgnumMeg
 
By the way, by commutator I mean ring commutator; i.e., $[X,Y] = XY-YX$ for $X,Y \in B(\mathcal{H})$.
 
@LeakyNun which is something like Hom(B, C) x Hom(A, B) --> Hom(A, C) right?
 
well, Mor instead of Hom
 
8:13 PM
What's the difference? lol
 
we use Mor to denote the set of morphisms (used in the definition of category, but not really much afterwards)
and for Hom, it's a functor
 
Ah I see
I was under the impression that the distinction was purely based on preference
 
I've never seen Mor except in the definition
 
ha fair, that's good because Hom looks nicer to me
 
@ÍgjøgnumMeg we also sometimes equip Hom with other structures, e.g. in an abelian category, the Homs are abelian groups
 
8:22 PM
@Semiclassical so why was there a problem with (f1g)(x):=int_0^1(t-1/2)g(x-t)dt? i agree that for g(x)=x it should be -x^2/2 + x/2 - 1/12 and not just -1/12, but how do we get that?
 
@user193319: You might ask Demonark (@Daminark) if he's thought about your question.
 
@PeterSheldrick because $g(x)\neq x$ on $[0,1]$, at least not if $g$ is supposed to be expressible as a Fourier series
 
@LeakyNun Right, for instance the hom sets of $R$-modules are abelian groups
 
i'm not convinced by my own argument here, if anyone wants to check the reasoning
 
and the category of $R$-modules is an abelian category if I'm not mistaken
 
8:23 PM
facecpalm i edited that into nonsense
 
@ÍgjøgnumMeg indeed, it is an abelian category
 
context: $k, h$ are mappings on well ordered sets, $k$ is order-preserving
 
so we have a functor $\mathcal C^{op} \times \mathcal C \to \mathbf{Ab}$
 
$g(x)=x$ on $[0,1]$ but not outside of it. in particular, $g(x-t)\neq x-t$ for all $t\in [0,1]$
 
Thus $k(a) \prec \min \left({E \setminus h\left[ {S_a} \right]}\right)$.


This implies that $k(a) \notin h\left[ {S_a} \right]$.

As $k$ is order preserving, we must have that $k(a) \succeq \min \left({E \setminus h\left[ {S_a} \right]}\right)$.
doesn't feel right to me
 
8:26 PM
heya @GFauxPas.
 
hi Ted
seeking a contradiction here
not sure I have one
 
@LeakyNun Nice, thanks
 
You'll have $g(x-t)=x-t$ for $t\in[0,x)$. But for $t\in (x,1]$ you'll have (by periodicity) $g(x-t)=g(x-t+1)=x-t+1$ since $x-t+1\in [0,1]$ when $t>x$
Hence you have to divide up your integral into two parts, one for $t\in[0,x)$ and the other for $t\in (x,1]$
 
Is the argument just what you have here or was there something before? What you have here seems to assume I know what you're talking about.
 
@GFauxPas can you give me the full context?
 
8:28 PM
Oh, good, better for @Leaky to think.
 
I guess that's not enough context. proofwiki.org/wiki/User:GFauxPas/Sandbox , "proof of lemma"
 
@GFauxPas the lemma is crap
surely there's an order-preserving mapping from $2$ to $1$
 
so if $A \cong B$ in the category then $\operatorname{Aut}(A) \cong \operatorname{Aut}(B)$ under the map $f \mapsto f^{-1}$ (now in $\textbf{Grp}$)
 
It's an exercise from Munkres, and I haven't found a mistake in Munkres before
 
No, Munkres does not make mistakes.
I don't even remember any in the typewritten version of his book we had before it got published.
Not that I'm paying attention ...
 
8:32 PM
do you know him personally Ted?
 
@Semiclassical okay how about x-floor(x) - how do we calculate the integral of that?
 
Yes, @GFauxPas. I took topology from him as an undergraduate (and diff. top. from Guillemin and algebra from Artin). I was a lucky boy.
Now you know why I've made my students suffer so :D
 
nice :)
 
@PeterSheldrick: Draw a picture!
 
@Ted Your students will be telling people on Math.stack 3.0 Chat that they took lessons from Ted
 
8:33 PM
@TedShifrin Munkres is still one of my favorite books to this day. I'm a bit envious of the fact that you got to learn from the man himself. And from both of those others.
 
@GFauxPas well the lemma would be correct if the mapping is injective
 
Munkres was a bit stiff and formal, but for that course when I was a second-year student it was perfect. I wouldn't have liked it so much for an advanced course like algebraic topology. But he was great for me then. And we interacted some when I went back to MIT as a postdoc. He was always kind.
 
@ÍgjøgnumMeg surely $f$ isn't sent to $f^{-1}$...
 
bleh why not?
 
8:37 PM
because $f^{-1}$ is still a member of $\operatorname{Aut}(A)$
 
oh right hahaha
makes sense
I guess
$f$ maps to something like $f \circ \varphi$ where $\varphi : A \to B$ is the isomorphism
dunno if that even makes sense I'm just "typing out loud"
 
you're almost there
@GFauxPas why $h(a) \ne e_0$?
 
@Semiclassical, @TedShifrin hmm im almost there but there is a sign problem
if g(x)=x-floor(x) then int_0^1(t-1/2)*g(x-t)dt=int_0^x(t-1/2)*g(x-t)dt+int_x^1(t-1/2)*g(x-t)dt=int_0^x(t-1/2)*(x-t-0)dt+int_x^1(t-1/2)*(x-t-1)dt=x^2/2-x/2-1/12 but it should be -x^2/2+x/2-1/12
 
mathematics is always correct up to indexing error and sign error
so treat i as i+1
and then by induction...
 
order-increasing mappings are always injective I thought
 
8:43 PM
@GFauxPas ok
 
because if $h(a) \succ \text{ anything }$, then $h(a)$ can't be minimal
 
@GFauxPas also, $k(\alpha) \prec \min(E \setminus h[S_\alpha])$ actually implies that $k(\alpha) \in h[S_\alpha]$
 
okay if t>=x then g(x-t)=(x-t)-floor(x-t)=x-t + 1 and not x-t - 1
thanks everyone
struggle ;)
 
hmm
 
Right $f\circ \varphi$ can't be an automorphism of $B$ because $f$ is an automorphism of $A$
unless $B = A$ I guess
 
8:46 PM
even if $h$ isn't given as order-preserving?
 
@GFauxPas because $\min(..)$ is the minimum item that isn't in $h[S_\alpha]$
 
It would be nice if $h[S_a] = S_{h(a)}$ but I don't know if that's ture
 
i.e. everything below it is in $h[S_\alpha]$
@GFauxPas I believe it's true
 
proofwiki.org/wiki/… I'm looking at this, I did this yesterday
but now I'm second guessing what I did yesterday
 
@GFauxPas just use the product trick
the one you felt unjustified last time
idk if you have convinced yourself of its veracity now
 
8:55 PM
i dont remember what that is
 
given wosets $A$ and $B$, consider the set $\{(a,b) \in A \times B \mid \exists~\text{order preserving bijection}~S_{A,a} \to S_{B,b}\}$
 
oh, well, let me finish it this way first, in Munkres's exercises
 
claims:
1. if (a,b1) and (a,b2) are in the set, then b1=b2
2. if (a1,b) and (a2,b) are in the set, then a1=a2
3. the set exhausts either all of A or all of B
4. in the first case, it is an injection A->B with connected image
5. in the second case, its inverse is an injection B->A with connected image
 
oh I don't need equivalence between $h[S_a]$ and $S_{h(a)}$, it's enough to have subsets I think
 
this is found in Jech's Set Theory
 
8:58 PM
let me try that
okay fixed I think
 
9:56 PM
Anyone here familiar with the convolution theorem of the Fourier Transform?
 
@Maximus hi
 
Hey, you can write stuff now
but I have to do work so I will read it when I can
 
10:21 PM
consider $\int \Psi^*\dfrac{\partial^3 \Psi}{\partial x^3}$. If i do integration by parts on this by taking $u = \Psi$ and $v = \dfrac{\partial^2 \Psi}{\partial x^2}$. The integral should become: $-\int \dfrac{\partial^2 \Psi}{\partial x^2}dx$
right?
assume limits $(-\infty, +\infty)$
And ignoring the boundary term
Now consider the integral -$\int \dfrac{\partial^2 \Psi^*}{\partial x^2}\dfrac{\partial \Psi}{\partial x}$ I can't figure out how to apply by parts on this?
After by parts the resulting integral should be the same as the previous result but with a changed sign
Will I have to apply by parts twice?
nvm got it
 
10:59 PM
Is it actually possible to receive send a text message then delete it?
 

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