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12:24 PM
Observation: D(e^{n 2\pi i x})=n 2\pi i (e^{n 2\pi i x}$ and $E(e^{n 2\pi i x})=e^{n 2\pi i (x+1)}=e^{n 2\pi i x})$ if $n$ is an integer
So that's a simultaneous eigenfunction of $D,E.$
In fact, it's also an eigenfunction of $E^{1/2}.$
 
12:39 PM
@LeakyNun Right, I was bored enough to actually think about that puzzle.
$$\sum_{r=0}^m(-1)^r \begin{pmatrix}m\\ r\end{pmatrix}(x+r)^n = (-1)^m \sum_{r=0}^m(-1)^{m-r} \begin{pmatrix}m\\ r\end{pmatrix}(x+r)^n = (-1)^m \Delta^m x^n = (-1)^m \Delta^{m-n} n! = 0$$
 
12:51 PM
i have $f: S \ ^1 \to \Bbb R $ continuous i need to prove that there exists $x \in S \ ^ 1 $ s.t $f(x) = f(-x)$.
So, suppose there isn't such a point. so define $g(x) = f(x) - f(-x) $ , $g \ne 0$ so we can assume w.l.o.g that $g \gt 0$ . so if we define $h(x) = \dfrac{g(x)}{||g(x)||}$ we have a map $h : S \ ^ 1 \to S \ ^ 1$. how can i get to a contradiction from here? or maybe im not in the right way?
(it is a question in topology course, we learned about retracts maybe i need to use it somehow.)
 
We also know that $g(-x)=-g(x)$
and $h(-x)=-h(x)$
 
What is $-x$ for $x \in S^1$ ?
 
Opposite point
 
Antipodal?
 
12:53 PM
i thought $-x = -(x_1,x_2) = (-x_1,-x_2)$ doesn't it?
 
Yeah, that's the antipodal point
 
It depends how you define $S^1$...
 
huh. ok
 
@Semi you have time?
 
@SteamyRoot $S^n = \left\{ x \in \mathbb{R}^{n+1} : \left\| x \right\| = r \right\}$ from Wikipedia
 
12:54 PM
A common definition is a subset of $\mathbb{C}$, where $-x$ would have a different meaning.
 
@SteamyRoot not really
 
alright, didn't know that :)
 
@LeakyNun How so?
 
@AkivaWeinberger so $h$ must get $0$
 
@SteamyRoot because $-x$ would still be the opposite point.
 
12:55 PM
Oh, right.
In that sense
I was thinking of $e^{i\theta}$ where you consider $\theta \in \mathbb{R}/2\pi \mathbb{Z} \cong S^1$
 
@AkivaWeinberger if $g(-x) = -g(x)$ and $g$ is continuous then $g$ must get a $0$, is that what you meant?
 
It's a question that is commonly asked as "prove there exist two antipodal points on the equator having the same temperature".
 
$h$ is a map $S^1 \to S^0$ though, is it not?
 
@Liad Wait ignore all that
I got confused
Sorry sorry sorry
 
It tends to be easier here if you work with a map $T: [0,2\pi] \to \mathbb{R}$ for the "temperature"
 
12:59 PM
@BalarkaSen what is $S^0$? Two points?
 
everything is ok :P
 
Yes.
 
@Liad You're right
I thought $g$ was from $S^1$ to $\Bbb R^2$ for some reason
or that $h$ was from $S^1$ to $S^1$
But yeah, $g$ is from $S^1$ to $\Bbb R$
 
Well, Liad wrote it wrong.
 
And you define a secondary map $T_a: [0,2\pi] \to \mathbb{R}: \theta \mapsto T(\theta + \pi) - T(\theta)$
 
1:01 PM
@BalarkaSen why would $h$ map $S^1$ to two points?
 
scrolls back up
 
yea, sorry $h: S \ ^ 1 \to \Bbb R -\{0\}$
 
Oh, so he did
 
:P
 
@LeakyNun $|h| = 1$
What are the norm 1 elements in R?
 
1:01 PM
10 mins ago, by Liad
i have $f: S \ ^1 \to \Bbb R $ continuous i need to prove that there exists $x \in S \ ^ 1 $ s.t $f(x) = f(-x)$.
So, suppose there isn't such a point. so define $g(x) = f(x) - f(-x) $ , $g \ne 0$ so we can assume w.l.o.g that $g \gt 0$ . so if we define $h(x) = \dfrac{g(x)}{||g(x)||}$ we have a map $h : S \ ^ 1 \to S \ ^ 1$. how can i get to a contradiction from here? or maybe im not in the right way?
 
In any case, $g(x)$ is either positive or negative
and $g(-x)$ is either negative or positive
In either case, IVT.
 
@Leaky Huh? $g$ maps to $\Bbb R$.
 
@BalarkaSen sorry, I see it now
you are right. $h:S^1 \to S^0$.
 
Borsuk-Ulam in dimension 1 is basically IVT, yup.
 
@AkivaWeinberger yea, thanks.
 
1:05 PM
@AkivaWeinberger We should write an expository on the Borsuk-Ulam theorem lol
it came up on a lot of stuff we've done recently
I actually don't even know all the various proofs of B-U.
 
 
1 hour later…
2:49 PM
Fun fact: If Quebec were to become independent, the US would become larger than Canada
@BalarkaSen Is Borsuk–Ulam still true if we replace the antipodal map with any degree -1 map?
 
@AkivaWeinberger That's interesting. I think so.
 
@Bala I have a question for you
Assuming you want to talk about alg geom
 
go ahead
 
Say you have this friendly and nice curve $C$ over a finite field
And you want to map it to $\mathbb P^1$ over the same field
Take $d >> 0$ and $D$ an effective divisor of $C$ of degree $d$
 
2:58 PM
@SimplyBeautifulArt $\operatorname{km}\$^2$ is my favorite unit of measurement
 
Can we find a (degree $d$) map $f: C \to \mathbb P^1$ with fiber $D$ above $0$?
I've been googling this for the past half an hour and I assume it has been answered or at least looked at, but can' t find too much
 
@AkivaWeinberger I think $\$^2$ is almost like saying $\text{radians}^2$
 
@Krijn What's an "effective" divisor?
 
@BalarkaSen No negative coefficients
 
Ah, ok. I was actually thinking about the exceptional divisor in blowups, or something of that sort.
But of course we're working with curves here.
 
3:02 PM
@SimplyBeautifulArt Radians squared is a legit unit of measurement, actually
Measures areas of parts of the sphere
 
Hm, right... didn't think that through too well.
 
You'll see it for apparent size, I think
 
So what does $\$^2$ mean?
 
but how can we be sure any function $f$ can be decomposed into a fourier transform, hence allowing us to exploit the linearity and that $D$ and $E^n$ have simultaneous eigenfunctions $e^{2\pi i x}$ thus allowing us to commute the $E^n$ and $D$ for each term in the expansion?

although I suspect for Akiva's question, I think we should be fine since the fourier transform of a polynomial always exists thus we might be able to use that to show the required commutation relations
although, I felt like when Akiva made that question, he might have a more elegant (read: simpler) way in proving that commutation relation, which probably requires theorems that I either don't know or I don't remember
 
I'm not actually sure if the proof is that simple
 
3:05 PM
NB. I also noticed that $\frac{d}{dx}$ is actually a shift operator in disguise...
 
By the way, note that it's important that these be over polynomials.
$f(x)\mapsto f(x)+\cos(2\pi x)$ commutes with $E$ but not $E^{1/2}$, for example.
(Luckily, there are no nonzero periodic polynomials)
@Secret How so?
 
$$\frac{df(x)}{dx}=\lim_{h\to 0}\frac{f(x+h)-f(x)}{h}=\lim_{h\to 0}\frac{E^hf(x)-f(x)}{h}=\lim_{h\to 0} \left(\frac{E^h-\textrm{id}}{h}f(x)\right)$$
 
Oh yeah
 
@BalarkaSen Yeah, so we are in the easiest case
 
@AkivaWeinberger That's not a very linear operator though, is it?
 
3:12 PM
While yes under such form, $\textrm{id}$ and $\frac{1}{h}$ will definitely commute with any operator, the issue is that we need to deal with $E^h L$ where $L$ is some linear operator. But that will require proving that $[E,L]\implies [E^n,L]=0,\forall n \in \Bbb{R}$ which is not true for the general case as the periodic counterexample showed, but it might work on polynomials for reasons I need to check out how...
One issue with doing polynomial proofs is I often have no idea what is happening when a polynomial $f(x)$ becomes $f(x+1)$ until I expand it
and that's where things get messy...
 
@SteamyRoot Oh. You're right
Woops
Is $f(x)\mapsto f(x)\cdot\cos(2\pi x)$ good?
 
Meanwhile, the action by the derivative on polynomials is easy to see when we understood that all one variable differential operators have the form $D=\sum_{i=1^n}a_i(x)\frac{d^i}{dx^i}$, thus considering each powers of $\frac{d}{dx}$, each integer application of $\frac{d}{dx}$ on the polynomial effectively shift the polynomial "to the left" if we use the standard basis $\{1,x,x^2,x^3,x^4,...,x^n\}$, and scale its coefficients in a linear manner
 
Don't use $D$ for something other than $\frac d{dx}$, that's confusing
Use like $A$ or something
 
Ok, will do that next time since I timed out
Meanwhile graphically, $E^n$ will translate the graph of the polynomial (or in fact, any function) to the right by $n$ units, however how the coefficients are affected I think I need to work out its matrix representation
 
Hi, $$\textbf{ A classic revived : } \text{this series , is-it converged } \sum\limits_{k=2}^n \frac{1}{\sqrt{k}}\cos(\frac{k^2+1}{k-1}) \text{ ?}$$
 
3:28 PM
@AkivaWeinberger That seems fine, yes.
 
bye
 
@Bala, I' ve just asked it in MSE here, if you' re interested in following it
It' s probably an easy question for someone with the right knowledge
 
in The h Bar, 1 min ago, by 0celouvskyopoulo7
@Secret $d/dx$ is unbounded
in The h Bar, 1 min ago, by 0celouvskyopoulo7
so "converge" is tricky
 
Just saw someone in the engineering building wearing a t-shirt with a statement of the Collatz conjecture on the back
 
O crap, I guess I really need to have a solid background in functional calculus before I started trying to write formal expressions and manipulation on operators...
 
3:40 PM
Did he claim to have proven it?
 
@Astyx sorry didn't get time yesterday to answer your question in more details
 
That font looks suspiciously like the xkcd font...
 
yeah, similar to that. except in red and with a big tree on the back as well.
same font, though.
 
I don't understand how the existence of a real eigenvalue follows in this passage
 
@Astyx could you point me to a more complete calculation of the probabilities you were suggesting for the random walk using that exponent method? It might refresh my memories and I might be able to better answer your question
 
yeah okay, I'll give @Fargle a star.
 
right. I'm surprised I can't seem to find the version of it I saw, though.
 
what are those shirts called where the ape stands up
and is then human
 
3:49 PM
my guess is it's something like "the evolution of man"
 
haha, yes.
 
it's an old image, though, so I wonder where it first comes from.
 
I guess it would be offensive to some.
 
sniped so hard..
 
3:52 PM
lol
 
Linear algebra question. Given a vector $v \in \Bbb{R}^n$, I want to find the matrix such that $\forall v \mapsto (1,1,1,1,...,1)$. How should I approach this problem?
 
did you ever solve that problem semi
 
Ummm.
 
Not yet. I'll be returning to it at some point.
 
You claim to be asking a linear algebra question but the function you describe is everything but linear.
 
3:55 PM
ah I see.
 
@SteamyRoot I think it'd be linear algebra if you asked for the component of $v$ in the 111...1 direction, though.
 
o wait, yes... I forgot the statement of the problem will imply $\mathbf{0}\mapsto (1,1,1,1,...,1)$ which cannot be linear
nvm then...
 
@Semiclassical In that case, yes.
 
But that's not what was asked, so yeah.
 
The closest to an answer of the original question would be to embed $\mathbb{R}^n$ in $\mathbb{R}^{n+1}$ by $i(x_1,\dots,x_n) = (x_1, \dots, x_n, 1)$
 
3:57 PM
@Semiclassical So the lady said that if I do part time I would be considered by the Ontario government as a full-time student and get full-time funding, and I'd be able to live on campus. She said the part-time application costs like 58 bucks. It turns out it costs 145 bucks, so now she's looking into it to see if I can get it for 58 bucks.
Hey zee.
 
And then consider the matrix given by all zeros except the last column, consisting of only ones.
 
@Dodsy Good. Keep plugging away at that.
 
Zee
Hey dod
 
Because that matches the affine map $x \mapsto 0 x + 1$ on $\mathbb{R}^n$...
 
Zee
Well it sounds to me like you got accepted where you want
Yet you ain't happy...
 
3:59 PM
bureaucratic limbo is never fun.
 
Thanks semi.
Great to have some support!
 
even if it can lead somewhere good, it's still not a pleasant place to be.
 
Zee
It sure is fun
Bureaucratic limbo is where you can hack the system so to speak
 
Right up until the system hacks you.
 
Zee
The systems is always hacking you so it don't matter
 
Zee
Oh god
 
SMACK ONNNNNNN
 
That's right, I'd forgotten that he was previously a skeptic.
Reminds me, there was something I got in my campus mail slot lately
 
if he was a schitzophrenic, we would've nailed all three of the people you need to convince:

Convince yourself
Convince your friend
Convince a skeptic
 
And apparently a bunch of other physics people (e.g. grad students)
 
4:03 PM
What was it
 
which was an anti-global warming booklet from the Heartland Institute
 
hm interesting
 
I tossed it. Anyone who is going to try to convince you that way is doing propaganda.
 
Ok guys, I got the matrix representation of $\frac{d}{dx}$ in polynomial space. Not sure how much that will help on the proof:
In $\textrm{P}^n(\Bbb{R})$. using the standard basis
$$\frac{d}{dx}=\begin{pmatrix}
0 & 0 & 0 & 0 & \cdots & 0 \\
n & 0 & 0 & 0 & \cdots & 0 \\
0 & n-1 & 0 & 0 & \cdots & 0 \\
0 & 0 & n-2 & 0 & \cdots & 0 \\
0 & 0 & 0 & n-3 & \cdots & 0 \\
\vdots & \vdots & \vdots & \vdots & \ddots & \vdots \\
0 & 0 & 0 & 0 & \cdots & 0 \\
\end{pmatrix}$$
 
4:05 PM
I am currently computing the matrix reprsentation for the shift operator also, though this one is indeed messy because going from $x^n$ to $(x+1)^n$ suddenly you have a pascal triangle of coefficients need to add to the polynomials for each power of x
 
One connection worth noting re: E and D
If we do a Taylor series on $Ef(x)=f(x+1)$, we get
$$Ef(x) = f(x+1)=f(1)+xf'(1)+\frac{x^2}2 f''(1)+\cdots$$
hang on. I need to say this differently to get the conclusion I want.
Let me write $E_y f(x)=f(x+y)$.
 
$E^y$, @Semiclassical
 
oh, sure.
$$E^y f(x) = f(x+y)=f(y)+x f'(y)+\frac{x^2}2 f''(y)+\cdots$$
 
By the way, @Secret, re: convergence
Say I have the following infinite polynomial in $D$: $a_0+a_1D+a_2D^2+\dotsb$
 
which I can rewrite in operator form as $$f(x+y)=\left(1+x \dfrac{d}{dy}+\frac{x^2}{2}\dfrac{d^2}{dy^2}+\cdots\right)f(y)$$
 
4:12 PM
(which could be something horrible like $a_n=n!$ or something, doesn't matter)
That always converges when applied to a polynomial, because it turns into a finite sum.
High enough powers of $D$ would just send our polynomial to 0.
($D=\frac d{dx}$)
 
Therefore $E^y f(x) = f(x+y)=e^{x (d/dy)}f(y)$.
 
right, so polynomial space formed a finite support in functional space at least for the differential operator
 
Yup. And (with $x=1$) $~E=e^D$!
 
blarg. I should've expanded in powers of $y$.
 
(And with $x=h$, $~E^h=e^{hD}$)
 
4:13 PM
so that $E^y f(x) = f(x+y)=e^{y (d/dx)}f(x)$.
i.e. $E^y = e^{y(d/dx)}$.
With, yeah, the suggestive implication being $E=e^{d/dx}$.
 
Another way to get the same result, by the way (and I don't know if you know this, Semi)
 
you use this in QM a lot, but written in terms of the momentum operator
 
but earlier Secret pointed out that$$D=\lim_{h\to0}\frac{E^h-I}h.$$
 
in which case you'd prove it via the commutation relation
Oh, nice.
 
And then use L'Hôpital.
That gives you $D=\ln E$.
Which implies $E=e^D$ as well ^_^
 
4:16 PM
I know the reverse of it: $\left(1+\frac{1}{n}D\right)^n\to e^D=E$ as $n\to \infty$.
 
Yeah that's Newton's something or something
 
yeah.
 
As 0celo have noted, that limit form will probably be an issue if we are working outside the polynomials (to be checked by some functional analysis people), but for polynomials, I think we will be fine because the differential operator is bounded in polynomial space
 
(In fact, since $E=e^D$ essentially is equivalent to Taylor's theorem, and the above limit is the definition of the derivative, that manipulation doubles as like the shortest proof of Taylor's theorem ever)
@Secret Right. And as I noted, the problem is false outside of the polynomials
$f(x)\mapsto f(x)\cos(2\pi x)$ being the example of something that commutes with $E^1$ but not $E^{1/2}$
 
Typically in physics you'd instead restrict it by only considering periodic $f(x)$.
I have in mind Bloch's theorem like I said elsewhere.
 
4:19 PM
@AkivaWeinberger Taylor's theorem?
 
Hi, 0celoubskyopoulo7!
 
(Is that Greek?)
 
Ask @BalarkaSen
 
But yeah, write that as $E^h=e^{hD}$, apply it to a function $f$ at $x$, and then do a substitution in the variables I think
I can post a fuller version later
 
4:20 PM
What's nice, as I said earlier, is that if $f(x)$ is periodic then $f(x)$ can be written as a sum of complex exponentials $e^{2\pi i n x}$.
 
i.e. fourier series expansion
 
Right.
 
Not to be too pedantic, but with Fourier series one has to be careful with the words "can be written as."
 
in which case $E e^{2\pi i n x}=e^{2\pi i n}e^{2\pi i n x}= e^{2\pi i n x}$.
 
Hello!! Do you maybe know which function has the following graph: https://lp.uni-goettingen.de/get/image/5182 ?
Is it maybe a cosine function?
 
4:22 PM
I can write anything as a series of something, that doesn't mean the series has to converge or converge nicely.
 
Yeah. In physics I'd also want it to be square-integrable
since wavefunction and all that.
 
At least that. But just square integrable doesn't mean the derivative has any meaning.
 
Sure. You'd also want it to be smooth (so long as you're not doing some kind of delta-function potential).
$De^{2\pi i n x} = 2\pi i n e^{2\pi i n x}$.
 
@0celouvskyopoulo7 get out of here you pedant :P
 
So $E$ acts as the identity operator on these eigenfunctions and $D$ just multiplies by $2\pi i n$.
 
4:25 PM
I am ok with pedantics to ensure us not fall into wrong places
 
It's physics, I'm sure all functions are continuous and infinitely differentiable and all that jazz
 
yeah, and we do sometimes deal with distributions loosely...
 
e.g. in h bar we talked about a horror paper where you have power series expansions on delta functions
 
Additionally, we have that $e^{2\pi i x }e^{2\pi i n x} = e^{2\pi i (n+1)x}$
 
4:27 PM
There's a variation on classical logic in which the excluded middle fails and all functions are continuous
 
So multiplying by $e^{2\pi i x}$ shifts us by one index.
 
$\begin{cases}1,&x=0\\0,&x\ne0\end{cases}$ isn't well-defined because it doesn't talk about things that are neither zero nor not zero :P
@Secret ??
Like, $\sum a_n\delta^n$?
 
@AkivaWeinberger Good
I reject classical logic
 
in The h Bar, 2 days ago, by ACuriousMind
Mar 16 at 18:29, by 0celo7
He's Taylor expanding a Dirac delta holy shit
 
So something like $\delta(x+y)=\delta(x)+\delta'(x)y+\cdots$.
 
4:29 PM
Oh god wow
 
$5 if you can make that precise.
 
How can you reject Aristotle?
 
What, so $\delta(0)=\delta(-1)+\delta'(-1)+\dotsb$??
 
Probably one way to do it is to Fourier transform in $x$, expand in powers of $y$ there, and then inverse Fourier transform back.
 
That's just infinity equals zero
@Secret On the train ride home I found a hole in my solution
but then I found a way to fix it
 
4:31 PM
@AkivaWeinberger $\delta'(1)$ is pretty badly defined.
 
I mean, the Fourier transform of $\delta(x-y)$ in $x$ is just $e^{i k y}$ I think.
modulo an overall constant etc.
 
@Semiclassical Correct
 
So you'd be doing $1+i k y-\frac{k^2}{2}y^2+\cdots$
...hrm. And then you'd be asking about the inverse Fourier transforms of $k^p$.
 
Those are not Schwartz functions, good luck.
 
Yeeah.
 
4:33 PM
(Neither is $1$, which is why the delta is not a function.)
 
What makes me think there could still be some logic to it is what it would seem to mean physically.
Namely: Suppose I start with a point charge at $x=y$
And then move the charge just a little.
How does the charge distribution change?
...but, that seems kinda silly now that I think of it.
i mean, it sorta makes sense that the difference in charge distribution would be something like a dipole.
(which is what $\delta'$ more-or-less is as I remember)
But that's just the linear term.
 
yeah it's a limit of dipole looking things
 
I think this does have some interpretation in terms of multipole moments or some such
But uh
 
so the idea would be that one dip cancels the original delta and the spike is the new one
 
Yeah.
As usual with the dirac delta, it's probably best to think in terms its effect on an actual integral
e.g. $f(x)=\int_{\mathbb{R}} f(y)\delta(x-y)\,dy$
 
4:38 PM
how about setting $y=0$ for simplicity
 
$-f'(x)=\int_{\Bbb{R}} f(y)\delta'(x-y)dy$ if I recall...
 
$y=0$ or $x=0$?
In the way I've written it just now I'd say $x=0$ since i'm integrating over $y$.
But I've also managed to reverse how I said it above, blah
So I'll say $f(y)=\int_{\mathbb{R}} f(x)\delta(y-x)\,dx$.
 
NB this is how engineers use $\delta'$
In mathematics, the unit doublet is the derivative of the Dirac delta function. It can be used to differentiate signals in electrical engineering: If u1 is the unit doublet, then ( x ∗ u 1 ) ( t ) = d x ( t ) d t {\displaystyle (x*u_{1})(t)={\frac {dx(t...
 
@Secret yeah.
Hence dipole kind of thing
I imagine, in fact, that it really is a dipole thing once you go to a point charge in 3-space and take $\nabla$ of the 3D dirac delta
 
@Semiclassical ...hmm
one of us got switched
 
4:43 PM
Yeah, probably me.
If I want to say "the point charge is at $x=y$"
then I'd better have $y$ as a free variable not a dummy one
anyways. If I formally expand $\delta(x-y)=\sum_k \delta_k(x) (-)^k y^k$ and expand the LHS as $f(y)=\sum_k f^{(k)}(0) y^k$
then I can identify each side term-by-term in $y$
 
that's pretty painful lol
 
Not going to argue with that.
and get $f^{(k)}(0)=(-1)^k \int_{\mathbb{R}} \delta_k (x) f(x)\,dx.$
 
@Semiclassical I won't argue that $\delta^{(k)}$ doesn't make sense...in fact what you're doing is just deriving the action of the $k$-th distributional derivative of $\delta$.
 
Right.
There's a certain kind of logic to this, but I won't pretend that what I'm doing is terribly logical on the whole
If I do some vigorous hand-waving as regards integration by parts, that basically does give $\delta_k(x) = \delta^{(k)}(x)$.
 
But the problem is that if $f$ has Taylor series like that, you have $f\in C^\omega$. But $C^\omega\cap \mathscr D=\{0\}$. So you need to work in $\mathscr S\cap C^\omega$. I don't know what topology that has.
(Besides the subspace topology.)
 
4:48 PM
Formally, this all has a certain coherence.
Rigorously....oh, look, a convenient distraction! flees
 
@Semiclassical Another thought. $\delta$ is a limit of gaussians in $\mathscr D'$. Those are $C^\omega$. Maybe the limit of their Taylor series has a meaning as a Taylor series for $\delta$.
 
maaaybe.
It usually does help to think in terms of approximations rather than the dirac delta itself.
 
@Semiclassical wait, wasn't the integral over $y$?
$x$ is fixed...
 
(Reading all of this makes me wish I had a solid functional analysis background, so I can participate in the investigation...)
 
4:53 PM
@0celo7 I swapped it, remember?
13 mins ago, by Semiclassical
So I'll say $f(y)=\int_{\mathbb{R}} f(x)\delta(y-x)\,dx$.
 
Oops. Well still, a Taylor series coefficient does not depend on the dynamical variable
So it should be $\delta_k(0)$
 
Yeah.
Probably wasn't worth worrying about in any case.
 
It isn't.
But there was a paper that assumed $\delta$ was an analytic function.
 
In fairness, as you say, you can pick an approximation of $\delta$ which is analytic
and do the arguments on that.
but uh, coulda-woulda-shoulda
 
Yeah. The paper made about 0 sense unless you read the conclusion. They were trying to derive formal expressions that could be approximated numerically with Gaussians.
 
4:56 PM
ahhh
 
@Semiclassical In particular, they needed a Taylor expansion of $\delta(x)$ so they could define $\delta(-i\partial_x)$.
 
Guys, here's the shift operator's matrix representation in the standard polynomial basis (and this is why I so hate to expand polynomials) :

Interestingly, its upper antitriangular
In $\textrm{P}^n(\Bbb{R})$. using the standard basis. Let $\begin{pmatrix}x \\ y\end{pmatrix}={}^xC_y$
$$E^k=\begin{pmatrix}
{}^nC_0k^0 & {}^{n-1}C_0k^0 & {}^{n-2}C_0k^0 & {}^{n-3}C_0k^0 & \cdots & {}^{0}C_0k^0 \\
{}^nC_1k^1 & {}^{n-1}C_1k^1 & {}^{n-2}C_1k^1 & {}^{n-3}C_1k^1 & \cdots & 0 \\
{}^nC_2k^2 & {}^{n-1}C_2k^2 & {}^{n-2}C_2k^2 & {}^{n-3}C_2k^2 & \cdots & 0 \\
{}^nC_3k^3 & {}^{n-1}C_3k^3 & {}^{n-2}C_3k^3 & {}^{n-3}C_3k^3 & \cdots & 0 \\
{}^nC_4k^4 & {}^{n-1}C_4k^4 & {}^{n-2}C_4k^4 & {}^{n-3}C_4k^4 & \cdots & 0 \\
 
@Semiclassical Their formula for the Fourier transform:
$$\tilde g(y)=\sqrt{2\pi}\mathrm e^{\mathrm ixy}\delta(\mathrm i\partial_x-y)g(x).$$
 
@0celo7 friends don't let friends drink and derive.
4
is my reaction to that
 
4:59 PM
$$\int_\Bbb Rg\,\mathrm dx=2\pi \delta\mathopen{}\left(\mathrm i \frac{\mathrm d}{\mathrm dt}\right) \mathclose{}g(t).$$
 

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