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12:01 AM
@Ted Since you're an expert on complex stuff, do you know a good reference to learn Hecke operators?
 
Question: Do you guys have personal websites?
 
I don't know nothing about no Hecke operators. I mean, I've heard of 'em, but that's it.
They're more number theory :)
@orbit-stabilizer: I have my old one at UGA from being a professor for an eternity, but nothing personal.
 
Well, all the complex analysis people at my uni are actually number theorists, so I guess I have skewed impression
 
@TedShifrin ah okay
 
Yup, @Mathei, and I'm definitely not a complex analyst. But it's hard to do complex geometry/manifolds without knowing some single- and several complex variables.
 
12:06 AM
I didn't mean to imply that you were, but I thought being a complex geometer still makes more of an expert on complex analysis than others
Actually, I'm happy that the exercises in complex analysis 2 don't match the lecture in that we're still doing some Riemann surfaces, although so far, it has been very basic
 
Well, sure, than plenty of "others," but ... also way less than a lot of "others." :)
 
@TedShifrin for two days?
 
Leaky, huh?
 
it's a rick and morty reference lol
 
shrugs
 
12:13 AM
We just globalized some local theorems from single complex variable like open mapping, Riemann's removable singularities, identity theorem and computed the meromorphic function on $\Bbb C \Bbb P^1$, so far
I guess it's better than nothing on Riemann surfaces
 
LOL, but hardly anything interesting other than knowing what a chart is.
 
yeah, I know :(
 
there are a lot of people in this course who have not seen abstract manifolds before
 
Hi @AkivaWeinberger and @LeakyNun
 
12:14 AM
hi
@MatheinBoulomenos they have
everything is a manifold
 
you just have to repeat your definition manifold
(do people even know what "manifold" means in English lol)
it means twice, thrice, ...
 
The ways in which this joke is unfunny are manifold
4
 
I know, @Mathei. I always spent a day on that when i taught Riemann surfaces. I guess I probably had to spend a day on partitions of unity, too, because only people that had had graduate manifolds or undergraduate diff top knew those.
 
Is it correct to assert that there is one homomorphism $f: D_{9} \rightarrow \mathbb{Z}$ on the basis that $f(a^8)=8f(a)=0$ and $f(b^2) = 2f(b) = 0$?
 
12:18 AM
@Argon but $\Bbb Z$ has a non-trivial automorphism so if there is one then there must be another...
 
@Argon yes, more generally, elements of finite order must be mapped to elements of finite order, of which $\Bbb Z$ has only one
 
never mind, it's the trivial one
what am I doing with group theory
 
Haha thanks guys
 
@MatheinBoulomenos if it was non-trivial must there be another?
 
@LeakyNun yes, but that doesn't follow simply because of the fact that there is a nontrivial automorphism
 
12:20 AM
@MatheinBoulomenos hmm?
 
it's the fact that there is a non-trivial automorphism which fixes only the identity element
otherwise you can't be sure that composing with the automorphism actually changes your embedding
 
oh, ok
is there a variation of this in nonsense?
 
For example, consider the homomorphism from a cyclic group of order $2$ to the quaternion group $Q_8$. $Q_8$ has lots of automorphisms, but they all restrict to the identity on the unique subgroup of order 2
 
@TedShifrin yet another neat thing about my surface, and this time it's an algebraic observation
 
If you have two objects $A,B$ in a category $C$, then $\operatorname{Aut}(A)$ acts on $\operatorname{Hom}_C(A,B)$ from the left and $\operatorname{Aut}(B)$ acts on the right by composition (you can also let the whole endomorphism monoids act if you like monoid actions), moreover this two actions are compatible
but that's just a bunch of fancy words for saying that you can compose things
 
12:26 AM
alright
 
$$\begin{vmatrix} 1 & z & x \\ z & 1 & y \\ x & y & 1 \end{vmatrix}=1+2xyz-x^2-y^2-z^2$$
 
@MatheinBoulomenos what is the f.g. of the horn torus?
 
so the condition that $x^2+y^2+z^2=1+2xyz$ is equivalent to the vanishing of that determinant.
 
nvm it isn't a manifold
 
moreover, if you take the surface to be $f=1+2xyz-x^2-y^2-z^2=0$
 
12:27 AM
@LeakyNun fundamental groups make sense for general topological spaces
at least if they're path connected
 
what am I doing with my life if it isn't a manifold
then what is it?
@Semiclassical it looks like everytime I'm doing my torus you're doing your cone lol
 
@Semiclassic: Well, that still doesn't settle things for the reason that I indicated. We really only care about the restriction of that quadratic form to the tangent space of your surface, not on all $\Bbb R^3$.
 
then the hessian is $H=2\begin{pmatrix} -1 & z & x \\ z & -1 & y \\ y & x & -1\end{pmatrix}$
 
What's a horn torus?
 
Oh, wait ...
 
12:28 AM
@AlessandroCodenotti a torus with major radius = minor radius
i.e. innermost smallest "circle" becomes a point
 
You're confusing me, @Semiclassic.
 
so I can write that as $f=\det(2I+H/2)=0$ (if I'm not getting the algebra wrong)
 
Its $\pi_1$ is $\Bbb Z$ then
 
hmm
 
I'm not claiming anything re: convexity here, I"m just making an algebraic observation that I thought was cute
 
12:30 AM
We started with $x^2+y^2+z^2-(1+2xyz)$?
 
It's the same as a torus with a disk closing the hole of the donut
 
yeah. though for these purposes I'm finding it better to flip the sign on that, i.e. $1+2xyz-x^2-y^2-z^2=0$
 
simple proof: in a torus, the (1,1)-knot and the Villarceau circle are homotopic
in the horn torus however, the Villarceau circle becomes a vertical circle
therefore we have ab=b, i.e. a=1
so it becomes $\Bbb Z$
 
OK ... My comment still stands. We don't really want the whole determinant ... only the restriction to the tangent plane of the surface is relevant.
 
I think it might actually be the free group on two generators
 
12:31 AM
oh, sure
I'm just saying it's kinda neat
 
@MatheinBoulomenos which two?
the horizontal circle deforms to a point (the center)
 
Oh yeah, nevermind
 
I think it should be $\Bbb Z$, if I'm doing Seifert-Van Kampen right in my head
 
There are all sorts of interesting happenstances with quadrics and cubics.
 
@Semi have you showed it's convex yet?
 
12:32 AM
not yet.
tbh I'm dragging my feet on that right now and I'm just playing around with equations
 
its second fundamental form should be p easy to compute
 
though there is one neat implication of the above
 
deforms to a point in the center
 
namely, the characteristic polynomial of $H$ at $\lambda=-4$ is $\det((-4)I-H)=\det(-2(2I+H/2))$. but I just noted above that the surface could be written as $f=\det(2I+H/2)=0$, so $\lambda=-4$ is an eigenvalue of $H$ for every point on $f=0$.
i dunno what I should conclude from that, but it's neat
 
12:37 AM
something like convex iff the second fund. form is positive (negative) semi-definite is true
 
kk
i'll have to check it out later
mostly I was just surprised to see $\lambda=-4$ as being an eigenvalue of $H$ on the entire surface.
back later
 
@LeakyNun if you consider a standard torus, but with the hole in the middle filled by disk, then this deformation retracts to the horn torus. I find this filled torus easier for visualization/Seifert-Van-Kampen computation. You can set up Seifert-Van-Kampen with a small neighborhood contractible of the center of the disk as one open set and the torus + a punctured neighborhood of the center of the disk as you other open set.
The torus has fundamental group $\Bbb Z^2$, the intersection retracts to a circle which has fundamental group $\Bbb Z$, the contractible open set has trivial fundamental group, amalgamation in this case kills one generator of $\Bbb Z^2$, so we're left with $\Bbb Z$
 
ok
 
I would draw pictures if I could
hope my description is clear enough
 
@MatheinBoulomenos That's not actually needed, but if the space isn't path connected you need to specify at which point are the loops based
 
12:51 AM
Is there reason to believe that orthogonal matrix initialization (as opposed to say, He initialization) can improve performance for shallow (ReLU-activation) neural networks?
 
@AlessandroCodenotti only if you're being pedantic
take any point in the intersection
 
hi @TedShifrin
 
To be really pedantic you always need to choose a basepoint, but all the choices give the same group if the space is path connected
 
"See, he has two eyes, but if he crosses them he'll be minus one."
 
@AlessandroCodenotti The same group? You mean isomorphic group
 
12:55 AM
Sure
 
Well, if you're being pedantic you need to distinguish between "same" group and isomorphic group. They're not equal as sets
 
1:18 AM
If you're being really pedantic you need to worry about whether infinite sets exist
2
 
$\displaystyle 1 + \frac x {1-y} + \frac {x^2} {1-2y} + \frac {x^3} {1-3y} + \cdots = ?$
 
@user76284 what are you studying?
 
Neural networks
 
@orbit-stabilizer are you io_cantor?
 
haha yes, I changed my name
@user76284 what are you using to study?
 
1:32 AM
Mostly Google Scholar :P
I'm working on graph neural networks, if you want to be specific
 
Have you read ESL?
 
I haven't. Does it address this issue?
 
I'm not sure. But it does have a neural net section and it's available for free online on the author's website - so no harm in checking
 
Will do. In my experience, though, most textbooks don't cover network initialization in depth :(
Ha, I feel stupid. Turns out the reason my training progress was so slow was because I was plotting a whole graph at every weight update.
 
oh wow
that would do it lol
 
1:37 AM
Now I'm plotting at every 100 or so. What took hours now takes minutes :P
 
Nah
I think the answer is to use AWS and throw tons of gpus at the problem
 
^ Now you're thinking like a data scientist!
 
Hello chat
 
:D
Mathein :D I got 1 week Before exam
do you Think it is enough to go though ring theory part?
 
1:46 AM
Which exam @Kasmir?
 
we only did a Little of it not much
abstract algebra dami
 
I don't know what you did, so it's hard to answer
 
question: does anyone know a quick proof why the cosets form a partition of a group and all cosets are the same size?
I don't like the proof in my book
 
Assume $c\in aH \cap bH$
 
1:47 AM
the partition part comes from equivalence relation
so it need not that every subset have same size
 
Then $c = ah_1 = bh_2$, meaning for any $h_3\in H$, we have that $bh_3 = ah_1h_2^{-1}h_3 \in aH$
 
every coset is the same size
for a subgrouo
 
what dami wrote will show you that each partition coset, will have same size as H
 
for a given subgroup*
 
So $bH \subset aH$, and analogously, $aH \subset bH$, so $aH = bH$
As for showing they have the same size, we want to find a bijection from $H$ to $aH$
So map $h\mapsto ah$
 
1:49 AM
ok im going through your proof
 
This is obviously surjective, and this is injective because $ah_1 = ah_2 \implies h_1 = h_2$
So $H$ and $aH$ are in bijection, so they have the same cardinality
 
@LeakyNun @AkivaWeinberger @anyone_interested So I came up with this interesting idea, and I'm gonna call it structured recursion. More or less, it allows you to use a single thing to represent infinitely many arguments and much much more in particular scenarios involving simple but extremely large amounts of recursion.
 
@Daminark got it, thanks. It's still not completely satisfying, but I understand
 
I suppose I'll use $\newcommand{hardy}{\operatorname{Hardy}} \hardy$ to denote the Hardy hierarchy, since H seems to already be taken in here.
So we have the simple function: $$\hardy(a,n) = \begin{cases}n, &a=0 \\ \hardy(a-1,n+1), & a>0\end{cases}$$
Trivially $\hardy(a,n)=n+a$.
 
Let $H$ act on $G$ from the right by right multiplication. orbits under this action are left cosests, and the orbits of a group action always form a partition
 
1:57 AM
@orbit-stabilizer another proof of the first fact which may be more satisfying (if not, chances are no proof will be) is that cosets are equivalence classes of the relation $a\sim b \iff ab^{-1}\in H$
 
We can then extend this function: $$\hardy(a_1, a_0,n) = \begin{cases} \begin{cases} n, &a_1=0 \\ \hardy(a_1-1, n, n), & a_1>0 \end{cases}, & a_0=0 \\ \hardy (a_1, a_0-1, n+1), &a_0>0 \end{cases}$$
 
Oh there's what @Mathei said too
 
And further: $$\hardy(a_2, a_1, a_0,n) = \begin{cases} \begin{cases} \begin{cases}
n, &a_2=0 \\ \hardy(a_2-1, n, n, n), & a_2>0 \end{cases}, &a_1=0 \\ \hardy(a_2, a_1-1, n, n), & a_1>0 \end{cases}, & a_0=0 \\ \hardy (a_2, a_1, a_0-1, n+1), &a_0>0 \end{cases}$$
 
I think group actions are more fitting, given your name @orbit-stabilizer :P
 
Oh that just makes it triviali
trivial*
thanks!
orbits make everything easier :)
 
1:59 AM
I agree, group actions are awesome
 
However, this entire expression can easily be simplified and expanded using structured recursion. Imagine if we had this cool $ω$ such that $$H(a_n, \dots, a_0, n) = H(ω^na_n + \dots + ω^0a_0, n)$$
From here, we can devise some interesting rules:
If $a_0>0$, subtract 1 from it and put it with the $n$.
Otherwise, if they are all zero, return $n$.
Otherwise, rewrite $\omega^ka_k = \omega^k(a_k-1) + \omega^{k-1}\omega$ for the rightmost non-zero $a_k$ and change the last $\omega$ into $n$.
Fairly basic rules. And if we further generalize and say that these rules can extend into the exponents....
Then we can get things like $$H(ω^ω, n)$$
Whereupon we would change the exponent $ω$ into $n$ to get $$H(ω^n,n)$$which in our original notation would be $H(1,0,0,0,\dots,0,n)$.
IMHO, notation like this is quite beautifully written.
And we can move onto things like $$H(ω^ω2, n) = H(ω^ω + ω^ω, n) = H(ω^ω + ω^n, n) = H(ω^ω + ω^{n-1}ω, n) = \dots$$
Or $H(ω^{ω+1}, n)$ simplifying into $H(ω^ωω, n) = H(ω^ωn, n) = \dots$
 
what are the relationships between group theory and combinatorics? I feel like they must exist since group theory is all about permutations and how they interact with each other (cayley's theorem)
 
But we can actually go much further than this with structural recursion. Imagine a new function called $ψ$ that produces exponents and exponents of $ω$'s, where more arguments works analogously to the above. Then give $ψ$ a new thing called $Ω$ which behaves like $ω$ in the hardy hierarchy!
Shoot, I forgot to use \hardy instead of H. Sorry if I've confused anybody.
 
I was lost from the first line :D
 
@orbit-stabilizer :P
Then skip to the first math formula thingy. It's not terrible to understand what's going on for the first few lines.
@SimplyBeautifulArt btw, $\hardy(a_1, a_0, n) = (n+a_0)\times2^{a_1}$.
@SimplyBeautifulArt And this is approximately tetrational level strength.
@SimplyBeautifulArt And for natural $n$, this is approximately Knuth's up-arrow strength.
I mean for natural $n$ in the largest subscript of $a_k$. Not $n$ as in the second argument of the function :-/
 
2:26 AM
hi @Daminark
I was wondering if you would like to discuss something ?
 
Sure!
 
So you know little bit about differential forms
 
A bit, yeah
 
so suppose we define the following differential form on complex manifold. $dz = dx + i dy \in Hom(T_U,\mathbb{C})$
why is $Hom(T_U,\mathbb{C}) = \Omega_{U,\mathbb{R}} \otimes \mathbb{C}$?
under what field we are tensoring ?
C ?
if it is C then yeah it is trivial
 
$\Omega_{U,\mathbb{R}}$ is what exactly?
Real differential forms on $U$?
 
2:34 AM
yeah
I am pretty sure we are tensoring here with respect to C
otherwise it odesn't make sense
 
I don't think we are, a priori $\Omega_{U,\mathbb{R}}$ isn't a priori a complex vector space
$T_U$ here is the tangent bundle of $U$?
 
yeah
 
And homomorphisms meaning, a map such that its restriction to each tangent space is a vector space homomorphism?
 
yeah
 
Well wait a sec $dz$ is a 1-form, so it's a map from $U$ to $T^*U$
Oh wait nevermind
I see, so if you evaluate $dz$ at a point $p$ you do get an element in $\text{Hom}(T_pU,\mathbb{C})$
 
2:43 AM
yeah
dz \in Hom(T_p U,\mathbb{C}) i.e
if $\alpha \in T_pU$ we have $dz(\alpha) \in C$
 
Well, not exactly
 
?
 
$dz(p):T_pU \to\mathbb{C}$
So $dz(p)(\alpha) \in\mathbb{C}$ is what you really have going on
The differential (1-)form is the map from the manifold to the cotangent bundle, when you evaluate it at a point you get your element of the cotangent bundle
 
sure yeah
yeah a 1 form is a section of the cotagent bundle yeah
 
Also may I see where you've found this? Maybe reading in a neighborhood will help give an idea
 
2:48 AM
Hodge Theory and Complex Algebraic Geometry I:
 
Okay got it, section 3.2?
OH you're thinking about $\mathbb{C}$ as a real vector bundle?
That would make more sense to me actually
Oh I found where you are
Okay so keep in mind here that $U$ isn't a complex manifold in general, it's an open subset of $\mathbb{C}$
The tangent bundle of $U$ is trivial, so $TU = U\times\mathbb{C}$
So $\Omega_{U,\mathbb{R}}$ has a basis $\{dx,dy\}$ and $\mathbb{C}$ has a basis $\{1,i\}$
Their (real) tensor product is the set of things generated by $\{dx\otimes 1, dx\otimes i, dy\otimes 1, dy\otimes i\}$
 
3:06 AM
yeah @Daminark
One sec Their is also
 
First off, now I'm completely convinced this is a real tensor product
 
oh
yeah I agree with you
the result follows from the basis of the
 
does anyone know graph theory?
 
thing tensor product you considered above
It follows right away I guess @Daminark
 
Now I'm actually doubtful of what I said though
That's a basis if we consider it as a $C^{\infty}(U)$-module
Not as a real vector space
 
3:12 AM
@ForeverMozart nope but im taking graph theory next semester
 
I already passed the PhD prelim in graph theory but I need some help with terminology lol
I forgot the words
 
@Forever eh..? Chances are you know a lot more graph theory than me but try your luck?
 
1
Q: Graph theory term and notation for "splitting" a point into more points

Forever MozartSuppose $v$ is a vertex in a graph $G$. Is there a name for the process of replacing $v$ with $d(v)$ (the degree of $v$) many vertices, one attached to each edge coming into $v$? For instance if $V(K_3)=\{v_0,v_1,v_2\}$ are the vertices of the "triangle" graph, then doing my process at any one ...

 
@ForeverMozart I'm almost sure there's a wikipedia page for that.
And, actually, you can generalize that
 
@Adeek so I'm starting to get a grip on this
 
3:19 AM
Take two graphs, and add an edge from each node of one graph to each node of the other
 
So, what's an element of $\text{Hom}_{\mathbb{R}}(T_U,\mathbb{C})$?
 
so possibly one of the products listed here: en.wikipedia.org/wiki/Graph_product
 
they are R linear maps from the vector spaces $T_U$ and $\mathbb{C}$
 
Nope
Call it $f$, we have that $f:U\times\mathbb{C} \to \mathbb{C}$ such that $f(u,z+w) = f(u,z) + f(u,w)$, all that. Meaning it takes a point
 
?
 
3:21 AM
$T_U$ is the tangent bundle, it isn't a vector space but rather a vector bundle, so it's a smooth map from $T_U$ to $\mathbb{C}$ that restricts to a vector space homomorphism on the fibers
 
It is also a R vector space
 
Are you sure about that? On a general manifold the tangent bundle isn't a vector space
@Eric halp
 
oh wait
no your right I was thinking of the tangent space at a point.
 
Oh phew
 
what
 
3:25 AM
Well anyway, you want to think about currying here. It takes in $(u,z)$ and spits out a complex number such that it restricts to a homomorphism $\mathbb{C}\to\mathbb{C}$, this means it's a mapping from $U$ to $\text{Hom}_{\mathbb{R}}(\mathbb{C},\mathbb{C})$
 
So there is a correspondence between tensor maps
and Homs
I think that is where we get that directly
 
Hey guys, please give me some hints regarding this integral!
 
Okay so now that we understand one side, I think I'm starting to get the picture of the other side but I'm having a bit of difficulty expressing this formally
@Eric I'm trying and probably doing a miserable job at finding out why $\text{Hom}_{\mathbb{R}}(T_U,\mathbb{C}) \cong \Omega_{U,\mathbb{R}}\otimes \mathbb{C}$
 
what is $T_{U}$
 
3:31 AM
Tangent bundle of $U$, where $U$ is an open subset of $\mathbb{C}$
 
and what is $\Omega_{U, \mathbb{R}}$
i would write $TU$ but ok
 
Real differential forms on $U$
Yeah same, but the book is using this notation so I'm trying to be consistent about it
 
@Daminark How to enable mathjax in chat?
 
first of all are we tensoring over R or C?
 
If you look at the room description on the top-right hand side of the screen, you'll see a link, and follow the instructions
@Adeek Probably $\mathbb{R}$, since $\Omega_{U,\mathbb{R}}$ isn't even a complex vector space, and we're looking at real homomorphisms
 
3:34 AM
yeah
 
what does Hom mean here, do you mean that
it's like a bundle map
 
That's what I'm guessing here
 
youre complexifying so it's definitely tensoring over R
 
hm
 
@Daminark on the level of fibers do you know why this is true
 
3:39 AM
yeah
 
it's just saying that $\text{Hom}_{\mathbb{R}}(V, \mathbb{C}) \cong V^{\ast} \otimes_{\mathbb{R}} \mathbb{C}$
 
I think this is the correct term: AMALGAMATION
In graph theory, a graph amalgamation is a relationship between two graphs (one graph is an amalgamation of another). Similar relationships include subgraphs and minors. Amalgamations can provide a way to reduce a graph to a simpler graph while keeping certain structure intact. The amalgamation can then be used to study properties of the original graph in an easier to understand context. Applications include embeddings, computing genus distribution, and Hamiltonian decompositions. == Definition == Let G {\displaystyle G} and H ...
 
Yeah, that's something I buy
 
yeah i mean the isomorphism is just $f_{1} \otimes 1 + f_{2} \otimes i \mapsto f_{1} + if_{2}$
so what do you think happens on the level of the bundle
(your bundle is trivial so this should be very easy)
 
Well, if we have $\omega_1\otimes 1 + \omega_2\otimes i$, that gives us $\omega_1 + i\omega_2$. If you evaluate that at a point $u\in U$, you get your map from $\{u\}\times \mathbb{C}$ to $\mathbb{C}$
That's a bundle homomorphism because differential forms act linearly on the tangent vectors, so yeah I'm happy now
@Adeek does this make sense?
 
3:55 AM
yeah
thanks a lot @Daminark @EricSilva
 
@Daminark being happy is good
 
It seems we all find happiness in our own strange places
 
birth is a curse and existence is a prison
 

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