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8:00 PM
2016 is the last year they do a paper version IIRC
the end of an era!
 
:35719754 missed it. ACM is too damn fast.
 
It's a great book for experimental stuff
well, i'm not sure if they'll send it
I tried getting the book before
I don't know how they work exactly
I think it's basically that they just print a big stack of them and send them for free
On the assumption that outside of a laboratory, only a crazy man would order them
(I am that crazy man)
 
@D3075 it's not
@AccidentalFourierTransform no
@Slereah correct, it's a natural transformation of exterior functors
 
Not the functors D:
 
@AccidentalFourierTransform Just $\Lambda^nM$ works if $M$ is $n$-dimensional
 
8:09 PM
what are even the axioms of category theory
I don't know at all
 
@AccidentalFourierTransform elements of $\Lambda^n M$ are "top degree forms"
@AccidentalFourierTransform ?$=n$
@AccidentalFourierTransform Unless you mean $d$ of $\mathrm{vol}$
 
@0celo7 ah thanks. I used to write $T^*$ for $\Lambda$, and $T^{n}$ looked weird. So I wrote $T^_n$ but I guess that it is the same
@0celo7 in my notation, $\mathrm d\text{vol}$ is the volume form itself (not the derivative of anything)
 
@AccidentalFourierTransform $T^*M=\Lambda^1M$ by definition
@AccidentalFourierTransform that's bad notation :P
 
@0celo7 yes it is. Maybe thats not how I used to write it. I really dont remember
its been a long time
 
Oh, what I said above about top-degree forms is wrong. I mean sections of that bundle are top-degree forms.
 
8:13 PM
"some people say that CT is a BYOST theory -- Bring Your Own Set Theory."
 
So that functor thing is wrong too, but I blame @Slereah for being wrong first
 
I'm never wrong
Those were just alternative facts
Apparently the axiomatization of category theory is still basically ZFC
Or ETCS
Basically the same
 
@Slereah how do I upside down $\Pi$?
but not $\coprod$
that's too large
 
$u$?
 
$\small\coprod$
 
no
 
You're tearing me apart @0celo7
 
$\tiny\coprod$
 
\amalg?
 
8:18 PM
is that small enough
 
$M-B=(M-\bar B)\amalg \partial B$
 
Do you mean the disjoint union symbol
$\sqcup$
 
No, he means the coproduct symbol (of which disjoint union is a special case, but the symbols are different)
 
"a category-theoretic construction"
reeeeeeeeee
 
@ACuriousMind My topology professor convinced me coproduct is better than sqcup for that reason
 
8:21 PM
@DanielSank Can you represent the lowpass filter as a system of SDEs? Like you would for e.g. RLC as a system of ODEs effectively. Then the integration would work out as usual (should be a trivial generalization of the ODE).
 
12
Q: Product coproduct sign

JohnI want to have a product sign analogously to $A \amalg B$. I tried $A \Pi B$, but as $\Pi$ isn't a binary operator, this does not look that good. Can you help me?

 
not that I could write down the definition of a coproduct without checking Hatcher...
 
@0celo7 It's that of the product, with all arrows reversed :)
 
@ACuriousMind that's about as helpful as telling @Slereah cohomology is the dual of homology ;)
@ACuriousMind My prof thinks it's strange I prefer cohomology to homology. Is it?
 
@0celo7 To a topologist it is
 
8:30 PM
Why?
 
homology is very natural in terms of cycles
 
Granted, I don't really understand what cohomology is telling me
@ACuriousMind sure
 
But cohomology is...linear functions on cycles. That's not geometric
 
But the arrows go the wrong way in homology
 
Guys, I gotta say, this is one of the nicer chats I've been in on SE.
Some of the other ones... yeeesh.
 
8:31 PM
@DanielSank aww, we <3 you too
Which one is not nice?
 

 The JEE LaunchPad

We love Physics, Chemistry and Mathematics. And we are prepari...
 
@0celo7 Electrical engineering seems awfully hostile.
Two people in one day responded to me with comments that served little purpose other than to stroke their egos.
After I pointed out that someone was wasting time stroking their ego, we got this:
> @MickLH I don't think there is much left when people want to ban words like "victim" and replace it by some terms like "experiencing person"
wat?
 
8:46 PM
Seen on the site:
> As a theorist, I'm not aware of any experimental method to detect the de Broglie wavelength of particles.
::facepalm::
 
@dmckee Our site?
 
Yeah. Our site.
 
Uh oh.
 
@ACuriousMind Unless, of course, you work on a different version of cohomology than singular.
 
@BalarkaSen sure, but singular is love, singular is life :P
 
8:49 PM
yeah man
@0celo7 Homology is essentially a singular version of cobordism theory, so it's easy to visualize
Cohomology, on the other hand ...
 
Wow, guys go take a look at Electrical Engineering.
Especially the mods might find it interesting. We're a really tame chat by comparison.
 
link please :-)
 
We were talking about git and some guy starting playing some "you don't have kids so you don't know what life is like" card.
Now they're talking smack about liberals etc.
 
Tip: Link to the transcript, not the room, otherwise one enters the room when clicking on the link
 
oops
How to do?
 
8:56 PM
@DanielSank Replace "rooms" by "transcript" in the link
It's also accessible from the "room" menu of the room
 
Wow!
 
@ACuriousMind noted
 
amusing
 
@ACuriousMind if you wanna edit the link please go ahead. I can't anymore.
 
I probably won't go in that room tho
 
8:57 PM
Man, I wish having some rep would give you a slightly longer edit period in chat.
@BalarkaSen Well, in my capacity as a physicist I am presently doing some electrical engineering.
^ Hint hint to all those around here who think physics and engineering are neatly separable.
 
@ACuriousMind I think you mean de Rham
 
Spoiler alert: they're not.
 
in Electrical Engineering, 53 secs ago, by PlasmaHH
@AccidentalFourierTransform or as these days you would probably hear: tää tääää, tää tääää, tää täää
help
me dont understand
 
Let them be.
 
@dmckee ok, I'm gonna bite. How do you detect it?
 
8:59 PM
They seem sick.
 
all drunk
 
@DanielSank Eh, don't be mean just because they are.
 
@ACuriousMind Mean?
 
@0celo7 de Rham is too complicated. forms contain more info than homology alone
*co
 
I really meant it. People who take opportunities to lash out at others for no reason are not well.
@BalarkaSen I like forms tho.
 
9:02 PM
@DanielSank Calling someone "sick" is mean in my perception. If you actually mean that as an assessment of mental health, please don't diagnose people over the internet.
 
@ACuriousMind Oh for... whatever.
 
@DanielSank Yeah, they're great. But I have this strange feeling that I never completely understand what they mean.
Personal failing
 
@ACuriousMind why do we always say fields in qft and other field theories have to be smooth functions?
why not just differentiable? is there a reason?
 
we dont say that because its not true
:-P
 
@D3075 'cause we wanna take derivatives of them and don't really know how many :P
 
9:06 PM
oh ok
@AccidentalFourierTransform example?
i probably won't understand your example btw xD
 
in qft or in other field theories?
 
qft
 
in the operator formalism the fields are distributions, not (smooth) functions
in the path integral formalism you integrate over non-smooth functions too
 
@DanielSank :)
 
(the contribution of smooth functions is typically negligible IIRC)
 
9:09 PM
okay thx
i'll keep that in mind
 
@BalarkaSen Hmm? De Rham is isomorphic to singular
Or are you talking about harmonics?
 
@AccidentalFourierTransform One can, for the actual Wiener path integral measure in 1d, actually show that the differentiable functions are of measure zero :O
 
de Rham admits a natural differential graded algebra structure, which singular doesn't.
 
Oh, I heard a nice talk involving dg-algebras today
 
What even is that
 
9:12 PM
I should find a good resource for the mathematical BV formalism sometime...
 
Functions of bounded variation?
 
Batalin-Vilkowski
 
Algebra?
 
algebraic physics, if you wish
The BV formalism is a way to formulate field theory
 
High school physics?
2
 
9:14 PM
@ACuriousMind I really want to learn about that :-(
 
@BalarkaSen so what does de Rham give you that singular doesn't?
 
@AccidentalFourierTransform Several talks in our physical mathematics seminar dealt with it recently, I have a decent high-level understanding but nothing detailed
 
:: is envious ::
 
I think physicists tend to call it the "antifield formalism" for some reason
 
Ah
That's in Weinberg
Made approximately zero sense
 
It's also in Henneaux/Teitelboim
but there it's fullblown BV-BRST
 
Haven't heard that in a while
 
@ACuriousMind and, again, made almost approximately zero sense
something about ghosts of ghosts
and ghosts of ghosts of ghosts
 
The ghosts are pure BRST, nothing to do with BV
 
Ok what is with these prodigies in my engineering classes
This guy has specific heat values memorized
Who the hell does that?
 
9:20 PM
@ACuriousMind ok then it made literally zero sense :-P
4180
 
Ignore that.
 
@AccidentalFourierTransform you integrate only on non-smooth functions, even
 
@0celo7 I think I was wrong about my previous statement. Singular cochain complex does admit a commutative differential graded algebra structure, since cup product can be defined on cochains.
Oh well!
 
@BalarkaSen I was thinking about cup, but I don't know what a differential graded algebra is.
 
@AccidentalFourierTransform Ghosts of ghosts are what you get when the gauge transformations themselves can have gauge transformations
 
9:25 PM
@Slereah wat
 
Smooth functions have measure $0$
 
It's basically a cochain complex with a cup product and a differential which is compatible with the cup product. Don't worry about it
Anyway, it is true that forms contain more information than cohomology.
 
@ACuriousMind e.g. in sugra, right?
 
A nice example I recently got to know: If a closed manifold admits a nowhere zero form then it fibers over the circle.
 
$h_{\mu\nu}\to h_{\mu\nu}+\partial_{(\mu}A_{\nu)}$, and $A_\mu\to A_\mu+\partial_\mu B$
 
9:28 PM
@ACuriousMind Double ghosts???? D:
 
@BalarkaSen form of what degree?
 
1-form, sorry
 
@AccidentalFourierTransform Simplest example is whenever you have a higher gauge field, like the Kalb-Ramond field in ST or the C-field in M-theory
 
Speaking of forms, I really need to read de Rham's book
 
9:31 PM
Is there any gauge simpler than $U(1)$
 
Yeah, wire gauge.
 
They are $\mathrm{U}(1)$ theories, but the gauge field is not a 1-form, but a higher p-form
 
@BalarkaSen how does the proof go?
 
@DanielSank you silly man
 
It see what You're saying now
 
9:32 PM
@Slereah I was in the Silliman college at Yale...
 
Sorry I'm walking and my fingers are cold. It's hard to type
 
The gauge trafo $C\mapsto C + \mathrm{d}\Lambda$ has higher trafos $\Lambda \mapsto \Lambda + \mathrm{d}\chi$.
 
but that doesnt work in $U(1)$, right?
 
Sure it does
$C$ is a three-form
 
hmm
ok so $\Lambda^2$ and $\chi^1$
but $\Lambda$ is defined up to a closed form, so $\Lambda\to\Lambda+\mathrm d\chi$ is trivial
 
9:35 PM
@BalarkaSen using a metric, doesn't that mean any closed manifold with zero Euler characteristic fibers over the circle?
 
@0celo7 Sorry, I messed again. I meant a closed 1-form.
 
@AccidentalFourierTransform Yes and no - it's trivial and that's why it's a gauge transformation
 
yeah reading it back it made no sense lol
 
Like, $A\mapsto A+\mathrm{d}\Lambda$ is also trivial, since it does not change $F$
 
@BalarkaSen ok, how does the proof go?
 
9:36 PM
Anyone here who has to deal with mechanical drawings, this is really useful: gdandtbasics.com/feature-control-frame
 
@0celo7 Yeah, you get a closed 1-form by dualizing a nonzero vector field on the manifold
 
I doubt it'll be closed...
 
@0celo7 I don't know yet but I suspect what's happening is this. Look at the kernel of $\omega$ on $TM$: that a codimension 1 distribution. Because $\omega$ is closed, that's integrable. So you have a codimension 1 foliation.
 
Yeah, it won't. In 3 dimensions you need it to be irrotational
Unless I'm missing something important I doubt that's always the case
 
since $\omega$ is nowhere zero, you get a nowhere zero transverse vector field on the foliation.
Flowing along that tells you nearby leaves are diffeomorphic. Aka, you have a codim 1 foliation with diffeomorphic leaves
Now that's not sufficient, because you can get things like the irrational foliation on the torus. So I think a generic perturbation of this foliation should be a fiber bundle over the circle
@0celo7 Ah, yes, of course.
 
9:49 PM
@BalarkaSen Oh, so an actual fiber bundle?
 
Yes.
 
@BalarkaSen Hmm. Is there a more rigorous argument here or is it supposed to be obvious?
Oh, compact manifold
Yeah, sure
That argument is used in morse theory
 
Ya, it's sort of like that gradient flow argument.
 
Gradient flow is also something I want to understand
@BalarkaSen generic perturbation?
@DanielSank what's this about contour integration?
 
You can perturb a foliation; foliate a ball cross manifold so that each slice is a union of leaves
 
10:01 PM
sorry, foliate a ball cross manifold?
 
I don't understand the question
You just foliate $D^k \times M$
 
@BalarkaSen yeah, but how is that a "perturbation" of the original one?
 
By restricting it to be the original foliation on $0 \times M$
It's just a homotopy idea
 
@BalarkaSen what's the reference?
I still dunno what you're trying to tell me
 
Candel-Conlon, the book I am reading right now
I don't know what's so hard about what I am saying but whatever
 
10:09 PM
@0celo7 Talk about it in the EE room.
 
@DanielSank But why?
 
@0celo7 Because it's funny.
 
@BalarkaSen Def. 2.4.5?
 
probably? I don't have it in front of me
 
@BalarkaSen What is $C^{1,0+}$?
 
10:16 PM
who cares. C^1 manifold with C^0 foliation I guess
or something.
 
I can't get over how cool this is: $$\int_0^T f(t) dW_t = \mathcal{N} \left(0, \int_0^T f(t)^2 \, dt \right) \, .$$
 
That doesn't seem like the right attitude for learning the subject...
 
i don't care about technicalities
 
^ Mah man!
 
everything is smooth, every foliation is smooth. i'm happy
 
10:20 PM
@DanielSank what is that?
 
@0celo7 It's a stochastic integral. Allow me to explain.
Suppose I have a Gaussian distribution $\mathcal{N}(0, \sigma)$.
That reads: Normal (Gaussian) distribution with mean 0 and std deviation $\sigma$.
Now suppose I have a variable $x$ which is formed by sampling the Gaussian twice and summing the results.
What, dear @0celo7, is the distribution of $x$?
 
every integrable function is also square-integrable too, right?
 
Wait, I'm searching through my complex analysis book for a good integral
 
wait no, $1/\sqrt x$
 
@AccidentalFourierTransform No.
Yes.
 
10:21 PM
and if it is non-singular?
 
Do you mean bounded?
 
@0celo7 Ok, it means the foliation is integral to a C^0 subbundle.
 
Compact support?
 
10:23 PM
@AccidentalFourierTransform I'm thinking of a function that has integral equal to some series
But the square of the series diverges
...does that even happen?
 
@0celo7 talk about stochastic integrals later?
 
@DanielSank ahhh
I can't find an integral
 
ahhh what?
 
Is a scattering amplitude cheating?
 
@0celo7 Generally speaking, no, scattering amplitude is not cheating.
I don't even know what that means.
 
10:28 PM
@AccidentalFourierTransform For a bounded set you have $L^2\subset L^1$
 
cool thanks <3
 
@AccidentalFourierTransform well you said no compact support
You have $L^2\not\subset L^1$ in general but I can't think of a bounded function example
 
bounded set means compact support? I thought you meant that for bounded functions ...
 
Also, you want a function in $L^1-L^2$ so that doesn't even help
@AccidentalFourierTransform no
my brain is failing right now
 
whatever, I just need some integrals to converge. I think Im going to go with "for $f$ a Schwartz function..." and forget about the details
 
10:31 PM
@AccidentalFourierTransform Oh, yeah, I'm stupid.
Still no, that's not even integrable.
 
lol
I just bit a hang-nail and Im losing a lot of blood
 
@AccidentalFourierTransform If $|f|\le M$, then $\int f^2=\int |f|^2\le M\int |f|$.
 
I cant think right now
@0celo7 ah thats it
wait
yes
ok, thanks $\varepsilon >$
 
If $f$ is complex you omit the first $=$
@DanielSank Ok, educate me
@DanielSank Yes
@DanielSank Ugh. Convolution?
I'd have to get out my probability notes
 
@0celo7 Well, the results winds up being that you sum the $\sigma^2$'s.
 
10:37 PM
@DanielSank But is convolution the correct approach?
 
@0celo7 yeah
 
Then the convolution integral would spit out a Gaussian I imagine
Complete the square and all that
 
@0celo7 Nah just use Fourier transforms. Convolutions are products in Fourier land.
 
Right, and fourier transform of Gaussian is Gaussian
 
Anyway, so $x$ has distribution $\mathcal{N}(0, 2 \sigma^2)$.
Ok so now suppose we are summing infinitely many Gaussians.
Suppose we invent notation $\int_0^T dW_t = \mathcal{N}(0, T)$.
(I just changed the notation so the second argument in $\mathcal{N}$ is the $\sigma^2$ instead of $\sigma$. Sorry.
 
10:40 PM
are we talking about wieners
 
@Slereah Yes.
 
good old wieners
 
@DanielSank ok
 
@0celo7 Ok so now ask yourself what you get form $$\int_0^T f(t) dW_t$$
Just kind of think about it and see what you expect.
 
I have no clue what that symbol is supposed to mean...
 
10:42 PM
@0celo7 which?
 
$\int_0^T f(t)dW_t$
 
Isn't it just the gaussian measure
 
I means add a continuum of Gaussian distributed random variables, indexed by $t$, each one weighted by $f(t)$.
@Slereah I don't know what that means.
 
$$dW_t \approx \prod e^{-x(t)^2} dt$$
Or something
 
@BernardoMeurer haha holy shit Fantano gave it a "not good"
 
10:44 PM
Or is it $dx$
 
@DanielSank Umm, assuming $f(t)$ modified each variance by $f^2$ (?), then would it be $\int_0^T f(t)^2dt$?
in the $\sigma^2$ slot
 
(is there any standard name for the set of bounded and integrable functions?)
 
isn't that just the set of test functions?
Oh wait, I guess they don't have to be smooth
 
@AccidentalFourierTransform not that I know of
I lied
 
@0celo7 Which is what I wrote.
 
10:48 PM
@AccidentalFourierTransform $L^1\cap L^\infty$
@DanielSank ok, but what about it
what is it telling me?
 
Is $L^\infty$ the set of bounded functions?
 
hmm I think im gonna go with "bounded and integrable function". $f\in L^1\cap L^\infty$ feels slightly pedantic :-P
 
It tells you how to make sense of stochastic integral notation, which allows you to solve some problems easily.
 
$||f||_\infty=\max f<\infty$?
 
@0celo7 see here.
 
10:50 PM
@AccidentalFourierTransform less pedantic?
 
@AccidentalFourierTransform $||f||_\infty=\mathrm{ess\,sup}\,(|f|)=\inf\{M\in\bar{\Bbb R}:\mu([|f|\ge M])=0\}.$
 
What is the ass sup
 
thats my def. of $\max$
 
essential supremum
@AccidentalFourierTransform I doubt it, but ok
 
10:52 PM
YOU DONT KNOW ME
 
I think I've got you figured out
@Slereah It's the set of functions that are a.e. equal to a bounded function.
 
Sounds like you almost everywhere answered his question then
 
@AccidentalFourierTransform so what are you trying to do?
analysis?
 
lol I wish
Im playing around with basic field theory
and I want to make sure that all Fourier transforms are well-defined and all the generators of symmetries are well-defined
nothing fancy
 
So you know the Stone theorem?
 
10:57 PM
as I said, in the end I might go with "everything is a Schwartz function" and forget about the details
classical field theory
 
@0celo7 Diffractive scattering. Any kind of diffractive scattering is sensitive to wave-length. Do it with massive particles and you are measuring the de Broglie wavelength of the particle.
And that is why people need to do an advanced lab course just as badly as they need demanding whiteboard electives.
 
youre just bragging
 

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