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01:00 - 13:0013:00 - 00:00

13:02
Please someone look at this
I am really starting to suspect the new age is an age of analysis, given the huge spike in analysis questions here
@AkivaWeinberger I love all the anal: real anal, complex anal, funky anal, harm anal. I just love anal SO MUCH!
Age of Analysis: confirmed
aka The Age of Anal
13:34
O they dried out...
@XanderHenderson Is this true that one should avoid passive voice in the paper?
The passive voice should be avoided.
@XanderHenderson *You should avoid the passive voice
sniped
@Slereah That sentence which was said was the sentence which was meant.
13:43
Although I think "you" is also to be avoided in papers
The author should avoid the passive voice
"You" is terrible.
Rude
(or is it "'You' are terrible"?)
depends how rude you're feeling
We prefer to use "we" in papers. Never "I" and certainly not "you". "You" is to be avoided.
13:44
Perhaps "One should avoid the passive voice"
Same
which is weird because I write it alone
Really? For example, if I want to express something like "The following expression can be brought into the following closed form".
So I suppose it's the royal we
It is the "mathematical we".
How can I rewrite it in active voice?
But I thought there was no royal way to mathematics
13:45
Not the royal we, the mathematical we.
Sometimes, it does appears to me that passive voice cannot be avoided.
The way that I have always interpreted it is that once a result is proved, it is indisputable fact.
Therefore all of us know that it is true, therefore we see how it must be.
*proven
I also have nothing against the passive voice; I was trying to make that clear by using the passive voice to admonish against it.
@Slereah Yuck. No. Proved.
although I beware of "proven results", but maybe that's my physicist ways :p
13:46
Regularize them verbs!
There's a lot of fishy proofs around
Using too much passive voice won't lead to the rejection of the article right?
@quallenjäger No idea. But I would imagine that is WAY down the list.
Over use of the passive voice can be fixed with editing. Uninteresting results or incorrect proofs likely cannot.
I have a horrible style of writing. My supervisor criticized me many times.
I'd say until you have the actual proof you're wanting to write, writing style should be pretty low on your priority :p
It's easier to change phrasing than proving theorem
13:51
Is it common that error occurs on published paper?
In physics certainly :p
Dunno about math
I am currently reading a published paper. Something appears not right to me
I don't know if I am not smart enough to see it or they really did a mistake.
well you can ask here
Errors occur from time to time, but I think that they are reasonably rare in mathematics (at least compared to fields where one might have to gasp experiment).
That being said, one of the first things I did as a graduate student was find a counter-example to a theorem in one of my masters advisor's papers.
Oh I don't even mean experimental things
just that theoretical physicists aren't necessarily big on rigor
13:54
Yes, I know. We make fun of them all the time.
I mean, what the fuck is a Dirac function? That's nonsense, yo!
to be fair they're usually awful bad unphysical counterexample :p
Well technically it is a function
The Dirac distribution, on the other hand... :P
A function on the space of test functions!
There are so many words that are better than function, in that case: continuous linear form, bounded linear functional, distribution, etc
And it certainly isn't a function on the underlying space, which is how I see physicists using it. :P
I use the word maps when the domain or the range is something exotic that is not based on the reals
13:57
But on the other hand there is an embedding of distributions into a space where they are functions!
@Slereah As you say, they are functions on the space of test functions, but that it not the way that I see people using the word "function" in general.
^Dirac distributions as functions :p
actually, is there a difference between maps and functions?
Functions on ${}^*\mathbb{R}$
@Slereah "generalized functions"
which is not the same thing :P
13:59
I mean, we use linear maps instead of linear functions when referring to matrices, for example
It's just $\mathbb R$ with extra numbers!
or, according to their abstract "asymptoic functions"
linear maps are a superset of linear functionals
and between the two sits linear operators
(or map is a synonym for operator, depending on who you talk to)
eh? I always thought linear operators and linear maps are the same thing, bleh, those sloppy quantum physicists...
I never really understood why Todorov uses asymptotic numbers rather than the hyperreal directly
@AkivaWeinberger, will you please look at this?
14:02
wait a minute, Slereah knew heaps of anal, thus he might be able to help out, whether he wants to is another story
in particular, he knew hilbert space stuff much MUCH better than I am
@Secret What kind of slander is this
@Slereah well, xanderson has a habit of referring analysis as anal and that becomes an in-joke of math chat
thus I just go with the trend and refer that as anal
@Secret I'll take care of it
cool thanks
Slereah: And based on the h bar and maths chat data, I am pretty sure you knew at least a lot of formalism about hilbert spaces, distribution thoeries, linear operators, complex analysis and some real analysis, so I pretty sure you know most analysis in general, thus I don't think I am slandering you
14:10
I imagine you're not too familiar with the subject
@Secret I went back to the Java backend, connected it to the neural network through Flask. So the bot loaded an old database in which it's still in this room
I'm terrible at analysis
Princessluna: Ah I see
Slereah: Ok
It should be gone, and I'm pingable here for 7 days. If Alisha rejoins, ping me and I'll unsummon her again and make sure it gets saved.
14:28
@AkivaWeinberger, thanks for that answer. :)
Discrete mathematics is the study of mathematical structures that are fundamentally discrete rather than continuous. In contrast to real numbers that have the property of varying "smoothly", the objects studied in discrete mathematics – such as integers, graphs, and statements in logic – do not vary smoothly in this way, but have distinct, separated values. Discrete mathematics therefore excludes topics in "continuous mathematics" such as calculus and analysis. Discrete objects can often be enumerated by integers. More formally, discrete mathematics has been characterized as the branch of mathematics...
hmm...
@Silent Incidentally, I think the answer would be different if we change "bounded" to "totally bounded".
Note that $\Bbb R_{()}$ from your answer is not totally bounded, since you can't cover it with a finite number of balls of radius $\frac12$.
If potential infinity can be ditched since we don't have ideal computers, perhaps it will be a good idea to start studying about discrete analysis and be familiar with the world where things are chunky
(A set is totally bounded, if, for every $\epsilon$, the set can be covered with finitely many balls of radius $\epsilon$)
is that basically the analysis version of compactness in general topology?
14:32
Er, I guess; a metric space is compact iff it's compete and totally bounded.
It's strange that neither completeness nor total boundedness is a topological property and yet their conjunction is
[Looks up to double-check] Conjunction is "and", disjunction is "or"
/thonking/
15:15
O they dried out...
 
2 hours later…
17:03
Hi guys!
I found it interesting that the logic room is a lot more populated than the main chat atm
Oh really
Is its name just Logic?
indeed, and you seemed to found it
It's hard to use chat on phone :D
17:44
hi @ted
Heya @Semiclassic.
Think I have a better way to explain what I was saying the other day re: the gamma function
You need to focus on your other problem:)
If we start from the integral definition $\Gamma(z)=\int_0^\infty u^{z-1}e^{-u}\,du$, and make the substitution $u=ze^{t}$, then it becomes $$\Gamma(z)=z^z e^{-z}\int_{-\infty}^\infty e^{-z(e^t-t-1)}\,dt$$
hey ted, FYI and unrelated, we have preliminary evidence that the chat have entered an Age of Analysis this year, after the Age of Number Theory in 2017, Age of Algebra in 2016-2017 and the Integral Age circa <2015
17:48
There's not that much analysis. I would argue there's been a shift to more geometry (from more topology). Not that I'm biased.
The exponent in that case has an obvious saddle point at $t=0$ which gives the usual $\sqrt{2\pi /z}$ factor.
But it also has an infinity of other saddle points along the imaginary axis.
@Semiclassic: As you know, I no longer have my notes [oh, maybe I did this in the applied math class], but this seems like what I did following Bender/Orszag.
Hi ! @LeylaAlkan
For most purposes, these other saddle don't matter: You're only integrating along the real axis, so why should you care about these other saddle points?
However, if you want to do analytic continuation in $z$, then you want to know what happens to this integral as you deform the contour.
Right, fair enough.
17:51
Ted: Hmm, as you mentioned that, it seems the topology discussion had massively decreased ever since Balarka gone chemistry and I don't see Eric, Balarka and Mike on at the same time that often
And therefore it shouldn't be too surprising that things are rather more involved if you take $z=iy$ with $y\gg 0$.
Mike is around way less, and Balarka has been studying a lot of geometry. So has Akiva. And 0celo is doing geometric analysis, as is Eric.
Fair enough, @Semiclassic. Thanks for thinking about that.
well, I'm doing it more because my advisor asked me to think about it :)
Ah ...
But I explained it so awkwardly before that I wanted to correct the point
17:53
hmm, interesting... should continue to observe closely then
By comparison, the full asymptotics for $\Gamma(iy)$ (which i'm stealing from another source) are
$$
\Gamma(i y)\sim \sqrt{2\pi}(i y)^{iy-1/2}e^{-i y}\left(1+\frac{1}{12iy}-\frac{1}{288y^2}+\cdots \right)(1-e^{-2\pi y})^{-1/2}$$
Oh, @Semiclassic, I found it in my applied math lecture notes. Interesting, I also got Stirling out of the difference equation.
the stuff in front is just what you get from stirling's formula. the stuff in the middle is the usual asymptotic series
and what's left is there because the reflection formula should give $|\Gamma(iy)|=\sqrt{\dfrac{\pi}{y\sinh \pi y}}$ for $y>0$.
the upshot, as I understand it, is that the effect of all those additional saddle points at $z=2\pi i k$ along the imaginary axis is to give that factor of $(1-e^{-2\pi y})^{-1/2}=1+\frac12 e^{-2\pi y}+\mathcal{O}(e^{-4\pi y})$
(there's a thesis out there which does this in a lot more detail)
I see. That shouldn't be too hard to check. I'm looking back at my asymptotics notes from that class.
Anonymous
I'm a bit confused about this terminology: My textbook (Axler) calls $\Bbb{F}^{n}$ a set of functions from $\{1,2,3,...,n\}$ to $\Bbb{F}$. It also says that the elements of $\Bbb{F}^{n}$ are a list of numbers. I'm not sure how a list of numbers can be function from $\{1,2,3,...,n\}$ to $\Bbb{F}$.
18:00
@Blue simple: the k-th element is just f(k)
(0,1,0,3) is precisely the function that sends 1 to 0; 2 to 1; 3 to 0; 4 to 3
if nothing else, the figure on page 103 (page 127 in the pdf file) is worth glancing at
By a list of numbers, you mean an ordered $n$-tuple $(x_1,x_2,\dots, x_n)$, so, as Leaky said, $x_k = f(k)$.
@TedShifrin sniped :P
18:01
I was typing more info than you, Leaky.
Anonymous
Oh. It's a set of functions from $\{1,2,3,..,n\}\to\Bbb{F}$. I missed that. Thanks!
I'm trying to avoid looking at their thesis too much because there's so much detail that I fear going blind :P
Hello
Hi Demonark.
How's it going?
18:03
The main tedious bit of all of this is that there's Stokes phenomenon going on along the imaginary axis for $\Gamma(z)$
I know Gibbs phenomenon. Who's Stokes phenomenon?
@Semiclassical jeez
so many equations
ikr
short description: if you look at the coefficients of an asymptotic series, you'll often find that they need to be different in different sectors of the complex plane
@BalarkaSen I'm on a ski trip, and while tumbling down the slopes and almost dying I dreamed up two more Hodge theorem proofs for you, I think.
18:06
hi Eric.
Probably you should be paying attention to the skiing and not the almost dying, 0celo.
and unless one handles the error terms very carefully, you'll incorrectly conclude that those coefficients must change discontinuously across the imaginary axis
Well I was paying attention to the skiing but when you're on the ground in pain, elliptic PDE comes naturally
For a more quantitative description:
@Eric done with finals?
just finished my Foucault paper and now i am free
18:07
0celo, it probably should be parabolic PDE.
hi @Sha
@TedShifrin I wasn't flying through the air
just falling to the ground
omg hi @Ted! do you know any logic by chance:p
As $|z|\to \infty$ with $|\theta|<\pi$ where $\theta=\text{arg }z$,
$$\Gamma(z)\sim \sqrt{2\pi}z^{-1/2}e^{-z}\left(1+\frac{1}{12z}+\frac{288z^2}+\cdots +S(\theta)e^{\pm 2\pi i z}\right)$$
and certainly not at the speed of light, so not hyperbolic either
Very little, @Sha. You should ask @Alessandro. He's our resident logician.
18:09
where $S(\theta)=0$ if $|\theta|<\pi/2$, $S(\pm \pi/2)=1/2$, and $S(\theta)=1$ otherwise.
alright, if he comes around, I'll do that
also, it's the plus sign in the exponent if im(z)>0
But parabolic eqns are more painful than elliptic, 0celo.
@BalarkaSen So there's a very nice proof where you derive a p-form Poincare inequality for forms orthogonal to the kernel of the Laplacian. This gives you nice control for an existence theorem.
The main point is that $S(\theta)$ changes discontinously to this order of approximation.
That's Stokes phenomenon.
18:11
@Semiclassical does this have anything to do with the stokes layer in fluid dyanmics
Ah, interesting how we label "phenomenon" all these sorts of discontinuity/overshoot things.
No idea. It wouldn't terribly surprise me, given how boundary layers in fluid mechanics are related to the method of multiple scales (which is just a version of asymptotic analysis)
But then it could just reflect the fact that Stokes did a lot of stuff
yeah, true
Oh, @TedShifrin, my advisor gave me a copy of this Wu book on Bochner stuff
You mentioned it some years ago
Yes, Wu's an old, old friend of mine. Great writer.
Turns out they did a 2017 reprint and he picked up two of them
18:13
@TedShifrin the main novelty about Stokes phenomenon in the last decades is that one doesn't have to settle for S(theta) being discontinuous
Oh cool. Well, Wu's still alive and kicking.
It's nicely written, and also why I have a newfound interest in Hodge's theorem.
Yes, he's a great teacher and expositor.
One can get a smooth description of what happens across the imaginary axis, it just requires more work
I don't like the one I usually think about (from Gilkey)
Warner's is very long
18:14
Warner's tries to use minimal amounts of analysis.
Jost's is...Jost. I don't think it's quite right.
I'm not really interested in the rigorous bounds on the error term (which is where much of the equations in that thesis come from)
I think Griffiths pretty much stole Warner's argument for their treatment in Griffiths/Harris. I've forgotten now.
But there's also just a lot of careful manipulation going on
@TedShifrin Well he does this stuff with Fourier but if you're going to do that, might as well do pseudos a la Gilkey or Lawson--Michelson.
18:15
@Semiclassic: Does your adviser have a good reason for having you look at this?
Wells has a proof using PsiDO.
Yes, that's true.
He's curious about it as a warm-up example for stuff involving the parabolic cylinder function
But I found his exposition less clear and certainly less detailed than Gilkey.
the main point there being that it's got a similar-looking integral representation
I no longer have any of these books. Oh well.
And I'm about to have to move in a few weeks, and I'm regretting the number of books I do still have.
18:16
So it'd be nice to understand how the story for the gamma function works as a warm-up for the parabolic cylinder function
I see.
@TedShifrin Anyway, I think I can do a proof by mimicking the proof that $\int f=0\implies \Delta u=f$ for some $u$
You just have to work a bit harder because the kernel of $\Delta$ on $\Omega^p$ is more complicated than on $\Omega^0$
And this requires very little analysis.
There's also a temptation on my part to get really into this stuff since this kind of 'resurgent analysis' of integral representations is something I've had an interest in for a while now.
Semiclassic: You really are a mathematician at heart.
I'm a certain kind of mathematician, at any rate.
proving rigorous error bounds isn't something that excites me, so I'm probably not an analyst
18:20
Right, that makes you more a physicist.
Yeah.
I live on the line :P
Like the Maginot line ...
Error bounds don't really excite us, it's the fact that we can bound errors that does...?
Yeah, great precedent there :P
@0celo7 That's fair.
@Ted where are you heading?
18:21
To the building next door, Demonark. But it's still a royal pain.
@Semiclassical It's just a part of the life I guess
In that spirit, I do find it interesting when there are neat things to be said about how fast the error goes down.
@0celo7 Write up all those Hodge proofs for me and I'll look into it three weeks from now
Oh, look, it's a Balarka.
An example being the rates at which Fourier series coefficients decrease based on how smooth the function is.
18:27
Sure, @Semiclassic, you can be sure I taught that and emphasized it in my applied class.
My favorite example in that vein being stuff like $f(x)=\sqrt{1-m \sin^2 x}$.
That's analytic in the neighborhood of the real line, so the Fourier coefficients decrease like $c_n\sim a^{-n}$ for some $a>1$.
on the other hand, when $m\to 1^{-}$ there's a kink at $x=\pi$.
Hence there's some interesting stuff going on for how the coefficients behave asymptotically as $m\to 1^-$
ok, time to go back out
cheerio
Don't break too many legs, 0celo.
"too many"
See you Ocelot
18:30
@Semiclassic: I'm going back to geometry. :)
@TedShifrin Morwen Thistlethwaite (maybe you know him) said when he was at Cambridge, all the rich kids when to Switzerland and broke their legs
I haven't done a lot with that matrix stuff I was doing this week, since the main prof I talk to about it is out of town
I'm not rich, and not in Switzerland, so maybe I'll be safe
But I think he'll like the use of the spectral factorization once I get a chance to talk with him again
18:31
@0celo7 but you broke both conditions so it's like a double negative
Is this observation trivial?
:( crap
I've met him, 0celo.
@Daminark double negatives either make him safer or in danger 50/50 chance
18:43
(I wonder who in the world had time and decided to make that, but wow does it come in handy)
WOW! SUPER COOL
who knew the sun had a face :P
@Daminark i dont understand what u mean, that's 100% real footage of the actual sun
oshit
18:59
@Daminark I'm bookmarking this
Hi
@ShaVuklia I heard you have a logic question
Feel free to add more intuitive answers (i.e. interpretations of the value of the p.d.f., which changes from r.v. to r.v.) to the following question.
8
Q: What does the value of a probability density function (PDF) at some x indicate?

jesterIII understand that the probability mass function of a discrete random-variable X is $y=g(x)$. This means $P(X=x_0) = g(x_0)$. Now, a probability density function of of a continuous random variable X is $y=f(x)$. Wikipedia defines this function $y$ to mean In probability theory, a probability...

I can't seem to remember the names in probability, cdf, pdf, density, they're all too similar
19:09
@Astyx it's excellent
pdf is probability density function I think
portable digital file
@Astyx cimer
c'est tres tilu
:P
"tilu" isn't something you'd say :p
And that kind of language should only be used with people you are very familiar with
i'm in a frenzy now
19:11
Else you look like a thug or something
je verlan tous
Your french seems to have improved at least
@Astyx the one for absolutely continuous variables that you integrate to get the probability?
cepar que je lanver?
Yeah I think
19:12
@MikeMiller portable document format?
@Leaky Non et cette phrase était juste incompréhensible à vrai dire
whatever
lmao
that's the goal, verlan until tu peux pas prendcom
PDF often refers to the Portable Document Format in computing. PDF or PdF may also refer to: == In mathematics, science, and technology == === In biology and medicine === Parkinson's Disease Foundation, in medicine Pigment dispersing factor, in biology === In computing and telecommunications === Package Definition File, System Center Configuration Manager Page Description File, used in variable data publishing Pop Directional Formatting, Unicode character U+202C, a formatting character that cancels a previous bi-directional formatting character Printer Description File, describing cap...
19:14
user image
3
@Astyx one should edit a french wiki page to verlan every mot
i hate this meme
@EricSilva I'll keep using it; CHANGE MY MIND :P
you can do w.e. u want my dude
I liked it originally
"I drink piss" was a classic
19:15
you won't change my mind
change my mind
@MikeMiller pee is stored in the balls
that's a 50/10
How is the pushforward measure of the random variable called in English? Distribution or density?
hard to not love
its just such a perfect summary of Steve Crowdy boi
19:35
Poisson summation is cool
the content is sorta obvious---Fourier transform of a periodic function should be related to the Fourier series coefficients---but it's still really powerful.
20:07
@AlessandroCodenotti hey thanks for getting back at me, but the question is solved!
I see, what kind of logic are you dealing with?
we've just been introduced to Stone duality
and we are also doing stuff with interpretations
like, those are two separate topics we cover
I'm glad the question is solved because I don't know anything about Stone duality :P it's a topic I should read something about though
o lol, yea well my question had to do with atoms, and it was actually something very simple, but it took me hours
I wanted to show that each finite BA has an atom, but I forgot a very simple thing, which resulted in me complicating a lot
@Alessandro I think it's the distribution
And that should be the CDF
The density is gonna be the Radon-Nikodym derivative of the distribution wrt the Lebesgue measure, and that's sometimes called PDF
If I remember this right
 
2 hours later…
21:48
@Daminark makes sense, so you need an absolutely continuous variable to have a PDF
Suppose that $V$ is a vector space with some involution $*$ (e.g., matrices with conjugate transpose). If $\phi : V \to \Bbb{C}$ is some linear functional, is it true that $\overline{\phi(v)} = \phi(v^*)$?
Is the involution also linear?
@AlessandroCodenotti Yes.
Anyone able to answer this quick question? Suppose A and B are symmetric matrices. What are necessary and sufficient conditions for Tr(AB) = 0?
Let me restate the problem as follows: Let A be a symmetric, square real matrix. For which rank-1 positive (non-negative) definite matrices B is it true that Tr(AB) = 0?
22:07
If I'm not mistaken $\Bbb C^2$ as a $\Bbb C$ vector space with $*(x,y)=(y,x)$ and $V((x,y))=x$ is a counterexample
 
1 hour later…
23:21
hey @AlessandroCodenotti
ah he's gone
Hello
How's it going ?
I'm good, just doing my homework and wasting time on stackexchange
Homework on what topic if i may ask ?
23:31
measure theory
you?
Well i am trying to practise for entrance exams for uni right now
thanks
23:54
I would once again like to invite anyone with better harm anal knowledge than myself to have a look at this question.
According to the exercise the OP posted, I am an idiot (which is an entirely reasonable conclusion), but I would like to know in what specific way I am an idiot.
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