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18:44
I am trying to prove if f has a right inverse then it's surjective
let g be the right inverse of f
then we know f o g = id_B
so let g(b)=a
then $$f(a) = f(g(b)) = (f\circ g)(b) =b$$
but how does this prove that for all b in B, there exists an a in A such that b=f(a)
@LeakyNun yes there is a counterexample, I saw one once but I forgot it
Hi @Ted!
Hi @Mathein
How are you doing?
@Maximus: You have it. You just didn't say it quite clearly. Start with $b\in B$. Now what?
Doing just fine, Mathein, thanks. You?
now you let g(b)=a @TedShifrin
18:49
Oh, it's a @Fargle
And then you show $f(a)=b$, so you've done what you wanted, @Maximus.
Heya @Ted
I'm doing well. I'm helping a friend with his bachelor thesis, which is quite fun
Better than doing your own, Mathein? :P
yo yo yo chat
Yo @EricS
18:50
@TedShifrin I'll start my own next semester
how goes it
howdy @EricSilva
there's still some stuff I have to do
@TedShifrin yes but I am confused. we let b in B so this means b is a random element in B and we force g(b)=a, how do we know there exists this a such that g(b)=a
Ah, cool, Mathein.
18:51
because I took the approach of taking all courses I find interesting instead of taking those that are required :D
Because $g$ is a function from $B$ to $A$, so $g(b)$ is some element of $A$. You just named it $a$.
but how do we know it maps it to an element there
maybe that particular b doesnt get mapped
What is a function?
or we assume it does
@MatheinBoulomenos i did this too! my last year of college is gonna have like no math bc i was a fool lol
18:51
Functions always map the entire domain.
oh right
so that means there exists at least an element a in A such that g(b)=a correct?
oh that makes total sense now, since g always maps the whole domain and f takes whatever g mapped then we will get B back, yes?
Not at least, @Maximus. Precisely one. You really need to understand completely the definition of a function.
So, @Fargle, how goes the fun with Hatcher?
yes sorry, that's what I meant
there exists precisely one element
@TedShifrin I'm pretty lost with it at the moment, so I'm trying to give it a break.
You could forget naming it $a$, and just say $f(g(b)) = b$.
Wow, I thought you were doing great, @Fargle.
18:54
I also found out that some nonsense I did for fun might actually help in the bachelor thesis of my friend
Oh, that's fun, @Mathein.
@Fargle, you on summer break?
@TedShifrin There's some point somewhere at which something isn't clicking, so I'm kind of just proverbially spinning my tires in mud.
Yep.
Well, I spent my career spinning tires, Fargle, so it's just a sign you're progressing.
yeah that makes sense, Thanks @TedShifrin !
18:56
I'm sure this is quite well-known, but I didn't saw it before so I tried to work it out on my own: I called it "Tensor products of $G$-sets", like when you have a right $G$-set $X$ and a left $G$-set $Y$ and you use these actions to identify elements in $X \times Y$. I thought this looked like a tensor product, so I tried to work out as much analogous results to those for tensor products of modules as possible
this might help to describe some rep theory stuff that came up in the thesis
Oh, that's sorta like the associated bundle construction, @Mathein.
what do you mean by "spinning tires"
ACtually, it's usually spinning wheels, not tires :P
Hi, demonic @Alessandro. All done?
18:57
\o
Oh no. It's a @Balarka
Yes, as far as diffgeo is concerned (the exam went very well), but I'll do an algebraic number theory presentation next week which will also be my last exam
I'm proud that you did me proud. :) ... Are you sad that it's almost all over?
Not execissively, I'm looking forward to begin my master in October
19:01
I can't believe we've spent so many years in this chat.
@TedShifrin what if g does the following:
g(b_1)=a
g(b_2)=a
g(b_3)=a
then how would f take a back to all 3 of the b's ?
what i mean in our proof
how do we know we don't have the case I outlined
If $g$ is a right inverse of $f$, $g$ must be injective.
yes but we never mentioned this in the proof
You can prove that in a similar fashion. You don't need to. It follows from your proof.
yeah I know that g technically has f as a left inverse so it's injective
in what way it follows from the proof?
19:05
If $g(b)=g(b')$, then $f(g(b))=f(g(b'))$ because $f$ is a function. Therefore ...
ah right
@TedShifrin Apparently Mather describes the Whitney stratification criterions as an intrinsic definition in terms of blowups, it seems
@Maximus I just meant "unable to gain traction"
Right, @Balarka. See the brief discussion of Nash blow-up and Chern-Mather classes in one of the little papers I sent you. :)
Ahh looking
It's the local Morse theory paper, yes?
19:10
No, the Whitney umbrella paper.
Hmm let's see where I put it
Ah found it
Boy, math was so ugly pre-LaTeX.
I kinda like the grainy typesetting fonts
It's classy
This was IBM Selectric typewriter.
And then scanning the reprint.
Ugh.
$\LaTeX$ is one of my top 5 things.
19:13
@Mathei That is the right perspective on that construction
pre-Latex is a myth
See the original Spivak 5 volumes, @EricSilva.
Ah of course this captures the idea.
the world has only existed since the original release in the 80s
everything that predates it is just a cover up
And it's about to stop existing.
19:14
bye bye world
@TedShifrin i have these on pdf but i dont like looking at old typeface lmao
My preferred typewriter has always been a Clark Nova
No, given the choice, I'd rather read TeX. But I'm not so fond of the default font.
@MikeMiller yeah, I managed to prove Hom-Tensor adjunction and the analog of Eilenberg-Watts (at least the part about tensor products) so far
@Mathein should be proud that I even normalized the Whitney umbrella :P
19:17
what's a Whitney umbrella?
A thing with a singularity that never goes away if you blow up any order of times
There's probably some categorical notion that encapsulates all similar constructions but I don't know what it is
Whitney is a really good umbrella manufacturer, they make umbrellas with no holes
truly cutting-edge
pls no cronenberg
@MikeMiller it's apparently "tensor products of functors" which works for monoidal categories
19:18
@Mathein: $x^2w-yz^2=0$ in $\Bbb P^3$.
But I haven't checked the details
the arguments for Eilenberg-Watts both in the homological algebra case and in the group action case seem quite specific
@Mathein Ah that makes sense, I remember seeing that come up in bar construction-like things in equivariant homotopy theory
you need coends to describe that and I didn't do coends so far
@EricSilva pls *more cronenberg
Yeah coends are valuable to the categorists
19:20
what is the meaning of your existence if you don't like cronenberg fam
@MikeMiller apparently coends also give a really description of geometric realization
i recognize that Cronenberg is interesting but i just get kinda get queasy at his particular brand of body horror
I think there's a coend formula for Kan extensions which you would like
@Mathei Yeah
what kind of body horror do you like
That's encapsulated in what I just said
19:22
do you prefer this
Balarka is throwing up at this conversation
The Cronenbwrg is fine though
I have the paper "this is the (co)end, my only (co)friend" bookmarked, I want to read it at some point not too far in the future
@MikeMiller That's some good body horror right there
Uncontrollable vomiting caused by reading nlab
Hellraiser $(\infty, 1)$
@Balarka I'm reading this paper my advisor sent me, you'd love it: pdfs.semanticscholar.org/b44b/…
i dont really have any feelings about the hellraiser movies
19:23
@BalarkaSen I looked for a counterexample because Leaky asked me and I just found a concrete and understandable counterexample on nlab
this doesnt bother me tho
I was shocked, to say the least
@Daminark I have seen it
Akiva read it with undivided attention once
@MikeMiller I like that they use integral notation. It's like category theorists are making fun of analysts
Ah, it's so quiet here without DogAteMy.
19:25
It really is
Even topologists write an integral sign for evaluation on the fundamental class, Mathein.
I just abuse notation and write the class for its evaluation
Well, it's well-known that Mike is abusive.
@TedShifrin hmm we didn't do that in our alg top lecture
notation is made to be abused
19:26
@Eric Hellraiser 1 is rly good Hellraiser 2 is ok to aight
Well, I smack anyone who writes $\int_a^x f(x)\,dx$.
Hellraiser n > 2 are a clusterfuck
Just read the book tbh
Corporal punishment in math
@MikeMiller it's been years since i watched the first one so ill have to revisit now that im more snobby than i used to be and actually appreciate things
I like hellraiser $\aleph_0$ the most
19:27
[garbled radio transmission] REPEAT: DO NOT ENGAGE (with Hellraiser n>2)
@TedShifrin im gonna write this exclusively from now on
Be prepared to be smacked, Eric.
@Ted I write $\int_a^x f$
@TedShifrin that smack is quite well-deserved
and do change of variables anyway
19:28
Delearn English just write unparseable integrals
not every abuse of notation is justified
31 mins ago, by MatheinBoulomenos
I'm sure this is quite well-known, but I didn't saw it before so I tried to work it out on my own: I called it "Tensor products of $G$-sets", like when you have a right $G$-set $X$ and a left $G$-set $Y$ and you use these actions to identify elements in $X \times Y$. I thought this looked like a tensor product, so I tried to work out as much analogous results to those for tensor products of modules as possible
I very much try to stick with $\int_a^x f(x')\,dx'$
@Balarka: That's fine. But what if you don't have an $f$, but a formula? :D
19:28
@TedShifrin $\int_x^x x(x)\;\text{x}x$
@MatheinBoulomenos in what sense is it a tensor product?
@LeakyNun why did you quote that?
ah
smacks @Fargle with multiplicity
@MatheinBoulomenos to ask you a question afterwards :)
or as I prefer to write my functions and variables, $$\int_0^1 2(3) d4$$
19:28
well, the construction looks the same to me
Well, I did ask for it.
@Semiclassical i dont like primes bc sometimes my x is a function
@MikeMiller i just screeched at this
it's not perfect, no
my usual default in cases like that is $u$
I love how Fargle still wrote \mathrm{x} at the end
i like t and s
19:29
What a nerd
i tend to stay away from x tbh
the page refreshed for some reason and I assumed I got banned for that integral
for single variable
LOL, I've been banned for words less offensive than that.
19:30
\mathrm, ugh
i can't get myself to ever bother with that
@MikeMiller honestly u deserve to
@LeakyNun I mean, in the tensor product, you quotient out stuff like $xr - ry$ and in the tensor product for $G$-sets I quotient out by the equivalence relation generated by stuff like $xg \sim gy$
is there a joke here i dont comprehend with my peanut brain @Mike
its bad
@MatheinBoulomenos i see
19:31
Also there's a Hom-Tensor adjunction for that construction
real pet peeve: $\frac{\mathrm{d}}{\mathrm{d}d}$
derivative w/r/t distance?
$\frac{\mathrm{d}}{\mathrm{d}d} d^d$
@LeakyNun if you want, it's on my blog: wlou.blog
19:32
hi @loch
@TedShifrin I get the Nash blowup. You're taking the closure of the image of a given stratum (of a smooth stratified space, embedded in a smooth manifold) by the Gauss map to get the limiting tangent planes. What about the secants?
using $d$ as a variable in calculus contexts is a bad time
I see
what about using $\int$ as a variable
Secants aren't there unless you do the secant variety.
19:32
Im currently writing on a third blog post with applications in representation theory
and yet you're forced to do it in physics when you talk about capacitors, since people seem to insist on $d$ as the plate separation
$\frac{d}{d\int} = \text{Id}$ is the fundamental theorem of calculus?
@MikeMiller good $\int$hit
use $s$ gdi
there's a nice proof of Mackey's formula with this approach
19:33
@TedShifrin It's the crucial part of a Whitney stratified space!
You want limiting secants to be contained in the limit plane
I thought you wanted limiting tangent lines to be contained in the limit plane
@MikeMiller Both
That's condition A and B
I assumed if you had secant lines it would imply tangent linez
Right. So I haven't thought about it, but you could frame it by saying that a map on $X\times X-\Delta$ (for $X$ the smooth stratum) extends to the blow-up.
@TedShifrin Yeah that's exactly what Mather does
@MikeMiller That is correct
19:34
Not with bad singularities, Mike. You're doing secants on the smooth stratum.
@Semiclassical $\frac{\mathrm{d}}{\mathrm{d}d} \mathfrak{d}(\partial(d), \mathscr{d}(d))$
5
Think about my example to Asaf with the surface $x^3=y^2$. Limiting secants don't get you tangents to the $z$-axis.
On this notational nauseous note, I leave to eat lunch.
Or should that be nauseating notional note?
@TedShifrin It doesn't satisfy the limit secants condition
good alliteration
19:36
Right, @Balarka.
Oh, OK.
what does $ f(x) $ mean
Mike is saying if it satisfies the limiting secants condition, then it satisfies the tangent line condition
OK. Right.
Bye for now.
Cool example anyhow :)
Bye
19:37
See you Ted!
@Semi same, never saw the appeal, I just write $\int stuff dx$
Or sometimes without the $x$, it depends
$\int f$
If it's clear
@MikeMiller yes, and taylor's theorem says that $\exp{d}=\operatorname{Id}$ locally, for functions that are nice enough
@Semiclassical ok in actuality if i wanna differentiate wrt something that's like a distance i use r and write $d/dr$
but hot take: i pronounce it dee durr
yeah
i tend to avoid $r$ for that because one uses $r$ so much in electrodynamics already
I am starting to use $\partial_t$ for $d/dt$ a lot these days
It's really convenient
@MatheinBoulomenos Better to say $e^d = 1$ :D
therefore the derivative operator is identically zero on analytic functions
19:39
Please stop @Mike @Mathein
but i also like using $s$ for the radial coordinate in cylindrical coordinates, so it's not entirely consistent
@MikeMiller right. So $\exp$ is not only $2\pi i$-periodic, but also $d$-periodic? thonk
@Balarka i write notation like $\partial_{t}$ for a tangent vector p much exclusively
Taylor's theorem says every section of a smooth fibration satisfies the h-principle locally with respect to any open partial differential relation
That's what Taylor's theorem is
$d/d|x|$ :P
19:41
It's just an h-principle
and then i write either $\frac{\partial}{\partial t}$ or $\frac{d}{dt}$ depending
I'm pretty sure I change notation for partial derivatives every 3 days
i pronounce the $\partial$ symbol as th-
hehehe mathein got rekt in algebra
so $\partial/\partial t$ is thatheet
19:42
@BalarkaSen it's analysis
it's h principle
$f_x$, $D_xf$, $\partial_x f$, $\frac{\partial f}{\partial x}$, $\int^{-1} f dx$, and so on
@Mathein I bumped into the algebraist that gave me the inverse limit problem today at lunch
@BalarkaSen ah
"I bumped into the algebraist" did you survive?
19:47
He liked my ideas/approach, told me not to spend too much time on it, and told me an obscene solution by Waterhouse
@Daminark No I didn't
He started teaching me what a Deligne Mumford stack is
It was like 3 hours long conversation
zombalarka
what's so obscene about that solution?
Ended with the conclusion that geometers don't understand orbifolds
These are obscene people man
19:48
whatever
lmao don't take it personally. I'm just memeing
I thought it was a clever solution
@Daminark i love how literally all of these are fine till you get to the last one
and then u take a sharp turn into crazytown
But algebra people have always ever been obscene. I have been reading a book on intersection homology. Beautiful stuff developed by topologists, Goresky and MacPherson. But here comes butting in the algebraists with their leader in charge Deligne and does perverse things with it
yes, Deligne did some stuff with perverse sheaves
@Balarka if anything topology is the obscene thing, like check out this picture of cobordism
That's just lewd
19:52
If a Mickey Mouse pair of pants is obscene to you I recommend getting help
Mickey Mouse?
No no no he's studying to do surgery on people, not on manifolds
This is just anime pants
"the category with compact oriented 2-dimensional cobordisms as morphisms, is the free symmetric monoidal category on a commutative Frobenius monoid object"
TQFTs are pretty cool though
That's how I learnt basic category theory and how to relate it to geometry
relate it to geometry sometimes people just miss the point...
Yo anyone know the assumptions needed on this theorem in order for it to be true? I would like to prove it. $e^f$ is measurable if and only if $f$ is measurable
Perhaps something to do with Borel measure?

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