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01:00 - 22:0022:00 - 00:00

01:47
What is the derivative of this
$$\frac{d}{dt}\left(\left|x\left(t\right)\right|^3\right)$$
02:25
@Perturbative I don't see how UCT is a special case of AHSS
02:49
@LeakyNun I had seen you asked a question about the PT isomorphism
right
I'm mainly curious on the computation $\pi_4(S^2) = \Bbb Z/2\Bbb Z$
Oh, I am not sure how it relates to that.
Have you seen this?
6
A: Visualize Fourth Homotopy Group of $S^2$

Piotr PstrągowskiOne way I see is the following. To start with, $\pi_{4}(S^{3}) \simeq \pi_{4}(S^{2})$ because of the existence of the Hopf fibre sequence $S^{1} \rightarrow S^{3} \rightarrow S^{2}$ and moreover the isomorphism is given by composition with the Hopf map. Hence, as was observed in the comments, yo...

@anakhro why isnt he a topologist
Why isn't who a topologist?
The author of that paper?
Maybe because he is something else more so?
@anakhro thanks for the paper
03:07
Leaky, are you on a Balarka schedule again?
it's 4 am there, wow
i'm in Hong Kong
TED
I was going to email you.
oh right
so it's 11am now
03:09
It was happening that I was never coming online when you were online.
although I did sleep at 6 and wake up at 9
3 hours is all you need
no i'm tired as heck
@TedShifrin come to the wonderful world of spectral sequences
03:12
wonderful world of dental fetuses, you say?
what?
what reference is that
It rhymes.
so it isn't a reference
it sounds like some monty python thing
8 results on google, so it is possibly something.
Heh, I think they are all random word generators or along those lines.
03:24
Hi everyone, assume that a statement $\phi$ written in first-order logic implies AC in ZF. Can we always find a model of ZF+not $\phi$? Does this question make sense?
Is this assuming you can find a model of ZF?
@KonformistLiberal assuming ZF is consistent, there is a model of ZF+¬AC, hence a model of ZF+¬φ
yeah
so a model of ZF+not AC is always a model of ZF+not phi?
right
because phi implies AC
lol
04:07
@Leaky: There was a spectral sequence in my thesis 40 years ago.
what was it?
I think I needed the cohomology of the flag variety of planes that are subsets of other subspaces.
Standard spectral sequence for a fiber bundle.
 
1 hour later…
05:22
Hello
05:44
Any good source on matrix groups that isn't too advanced? No lie algebras or analysis/topology.
06:23
how about lie groups XD
06:40
lol
I just want to read the basics with a knowledge of only up to the isomorphism theorems for groups, without getting confused with mentions of compact, continuous etc.
So the basics of general linear groups, unitary groups, orthogonal groups, Lorentz group etc.
07:42
@KonformistLiberal there's nothing special about AC here, you can use any independent statement
Hello
Is multiplication of ordered pairs over integers commonly defined somehow ?
or is it just $(a_1,b_1)\cdot (a_2,b_2)=(a_1 a_2,b_1 b_2)$ ?
08:01
I'm trying to find out whether groups $(\Bbb Z_6, +)$ and $(U(\Bbb Z_7), \cdot)$ are isomorphic.
$U(\Bbb Z_7) = \{(2,4),(3,5)\}$
08:47
What do you mean with $U(\Bbb Z_7)$?
09:03
@AlessandroCodenotti the units group of Z/7Z
@flowian yes. so $\Bbb Z^2$ is a ring
@flowian that is wrong. U(Z/7Z) should be {1,2,3,4,5,6}
3 is a generator
3^1 = 3
3^2 = 9 = 2
3^3 = 27 = 6
3^4 = 81 = 4
3^5 = 243 = 5
3^6 = 729 = 1
(or if you want pairs, then U(Z/7Z) = {(1,1), (2,4), (3,5), (4,2), (5,3), (6,6)})
 
1 hour later…
10:16
@Mathei are you here by any chance?
@AlessandroCodenotti what is your question about?
functional analysis?
The center of $\Bbb CG$
iirc you can express it in terms of the conjugacy classes
Yes
Wait let me turn on my laptop to write a proper question
It's not clear to me what's the relationship between the size of the conjugacy classes and the matrix rings
For example $\Bbb CS_3\simeq M_2(\Bbb C)\oplus\Bbb C\oplus\Bbb C$. Which factor is coming from which class?
woops yes thanks
When we write $\Bbb CG\simeq\bigoplus M_{n_k}(\Bbb C)$ we have $\sum (n_k)^2=|G|$
And if the conjugacy classes of $G$ are $C_1,\ldots,C_K$ then the center is spanned by $c_n=\sum_{c\in C_n} c$ for $1\leq n\leq K$
10:32
the dimensions correspond to the dimensions of the irreps
which irreps?
so there are two irreps of dimension 1 ($S_3^{ab} = C_2$) and one irrep of dimension 2 (the permutation irrep)
Wait what kind of representations are you talking about?
I only know about unitary representations...
$\Bbb CG$-modules
What do you mean with $S_3^{ab}$?
@LeakyNun Oh ok
10:34
the abelianization
Hmm can you tell me more explicitely what do those representations look like?
the trivial representation sends every $g \in S_3$ to $(1) \in M_1\Bbb C$
the sign representation sends $g$ to $(\operatorname{sgn}(g))$
and the 2-dimensional representation is the one coming from $D_{2 \times 3}$ acting on the plane
in The h Bar, 19 mins ago, by Slereah
Math wizards
in The h Bar, 19 mins ago, by Slereah
Is there a list of like
in The h Bar, 19 mins ago, by Slereah
Linear functionals depending on the type of function space we consider
Uh ok, I guess I actually need to learn some rep theory eventually
in The h Bar, 19 mins ago, by Slereah
ie : what type of integral is a linear functional depending on what function space we consider
10:38
@AlessandroCodenotti so it sends $\rho$ to $\begin{pmatrix} \cos(120^\circ) & \sin(120^\circ) \\ -\sin(120^\circ) & \cos(120^\circ) \end{pmatrix}$
Next time, I am going to just copy the user and then their messages in one to refer, multiple lines clogs the chat
and $\sigma$ to $\begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix}$
they're all unitary
I see, thanks
Do you have a good reference for a quick introduction to this kind of rep theory stuff?
man I forgot so much of this stuff
@AlessandroCodenotti my notes say, we look at the representation $V$
as vector spaces, $V := \Bbb C[G]$
but instead $g \cdot h := ghg^{-1}$
10:48
ok?
Hi, there is a question which I can not to solve it , please can someone help me ? a) prove that h : #R^2 → S^1 × S^1# that defined as : #h(t, s) = (f(t), f(s))# is a Local depomorphism. b) prove that if #L := {(x, y) ∈ R^2| y = ax + b}# is a Straight on the plane איקמ #h|L# is immersion.
@AlessandroCodenotti oh and I believe all reps are unitary since $G$ is finite
We can also think about $V$ as a (finite dimensional) Hilbert space to talk about unitary reps
sure
@AlessandroCodenotti then let $V_1, \cdots, V_m$ be all the irreps of $G$
then we have an $G$-isomorphism $V \cong \bigoplus_{i=1}^m \operatorname{End}_\Bbb C(V_i, V_i)$
send $g$ to $\sum x \mapsto gx$, extend linearly
10:54
I see, makes sense
$ghg^{-1}$ is sent to $x \mapsto ghg^{-1} x$, which is how $g$ acts on $\operatorname{Hom}_\Bbb C(A,B)$ for $G$-reps $A$ and $B$
then take $G$-invariants on both sides
$V^G = \{ \sum a_h h \mid \forall g, \sum a_h ghg^{-1} = \sum a_h h \} = \{ \sum a_h h \mid \forall g, \sum a_{g^{-1} h g} h = \sum a_h h \} = \{ \sum a_h h \mid \forall g, \forall h, a_{ghg^{-1}} = a_h \}$
so a basis is $\{ \sum_{g \in c} g \mid c \in cl(G) \}$
so $\operatorname{dim}_\Bbb C V^G = |cl(G)|$
ok? @AlessandroCodenotti
I'll need to read the details carefully later, but I see how you get the dimensions now
and on the right hand side
$\left( \bigoplus_{i=1}^m \operatorname{End}_\Bbb C(V_i, V_i) \right)^G = \bigoplus_{i=1}^m \operatorname{End}_\Bbb C(V_i, V_i)^G = \bigoplus_{i=1}^m \operatorname{End}_G(V_i, V_i)$
since $V_i$ is simple, $\dim_\Bbb C \operatorname{End}_G(V_i, V_i) = 1$
so $|cl(G)| = m$
@BalarkaSen hey you're finally back!
I see, thanks @Leaky
Hi @Balarka
11:12
@AlessandroCodenotti do you know the result that every $\Bbb CG$-module is semisimple?
Isn't that just a fancy way to state every complex rep of $G$ can be decomposed into irred reps? :P
($G$ has to be a compact Lie group there)
$\Bbb CG$ has an inner product
or maybe $L^2(G)$
oh I remember it being a corollary of the fact that $\operatorname{Hom}(V,W) \to \operatorname{Hom}_G(V,W)$ is a projection
11:17
I don't know algebra but my proof is: "Just average"
:P
right
and $\operatorname{Hom}(V,W)^G = \operatorname{Hom}_G(V,W)$ is a useful fact
oh so in general $V \to V^G$ is a projection
Of course it is.
the formula was $v \mapsto \int_{g \in G} gv \ \mathrm dg$ right
I think we lost @AlessandroCodenotti
@BalarkaSen I've heard that if A->B->C and B->C->D are fibrations then A=ΩD
is this true?
ok brb
11:21
Should be. The shift in the homotopy groups indicates it. I don't know a proof immediately.
So B is the homotopy fiber of C -> D, and B -> C is the fiber inclusion, whose homotopy fiber is A.
So anyway
In two dimensions, there is a trick you can use to get out of labyrinths, by always taking the same direction
But this fail to work in any higher dimension
Is this because of some topological property
True on the plane but not in any higher dimension
11:36
@LeakyNun Yeah alright, this is simple. B is the homotopy limit of C -> D <- pt. A is the homotopy limit of B -> C <- pt. Superimpose these diagrams to get that A is the homotopy limit of pt -> D <- pt.
That's the loopspace indeed.
Cool fact I guess
@BalarkaSen nice
@Slereah I think it’s mainly the Jordan curve theorem
what would be the derivative of $^kx$?
Hi, there is a question which I can not to solve it , please can someone help me ? a) prove that h : #R^2 → S^1 × S^1# that defined as : #h(t, s) = (f(t), f(s))# is a Local depomorphism. b) prove that if #L := {(x, y) ∈ R^2| y = ax + b}# is a Straight on the plane, then #h|L# is immersion.
12:27
@Mathphile $T(k,x)' = (x^{T(k-1,x)})' = T(k-1,x) x^{T(k-1,x)-1} + x^{T(k-1,x)} (T(k-1,x))' \ln x$
$= T(k-1,x) T(k,x)/x + T(k,x) (\ln x) (T(k-1,x))'$
@LeakyNun Any particular theory behind concept of generator? Never heard of it.
are you familiar with linear algebra?
sort of, studying it
it's like the concept of spanning set
lol
ah lol
thanks
12:54
I always thought it was like basis
Could anybody take a look at my question on conditionally sampling from two distributions? https://math.stackexchange.com/q/3304535/47771
This should be a quite natural problem in applications, but I don't know what I need to google to read about it.
13:09
@Notsredt basis is also linearly independent
and doesn't make much sense in the general context of (non-abelian) groups
given $S \subset G$, there's an associated map from (the free group generated by S) to G
in the context of linear algebra, there's an associated map from (the free vector space generated by S) to G
S is linearly independent iff the map is injective, and S is spanning iff the map is surjective
I guess you can define it similarly for non-abelian groups
but then two elements would in general be very unlikely linearly independent
@0xbadf00d try here
I see you have already, sorry.
13:52
@LeakyNun I didn't specifically mean UCT is a special case of AHSS, rather I meant that conceptually it seems to do something more powerful than what UCT does. UCT relates (co)homology with arbitrary $G$ coefficients to (co)homology with $\mathbb{Z}$ coefficients, whereas AHSS relates a (co)homology theory with ordinary homology (by relating the (co)homology groups from one theory with the ordinary (co)homology groups),
and for example UCT does this as well since $H(_; G)$ is an ordinary homology theory for any abelian group $G$. Then again I may be wrong since I'm just learning about these things
14:11
@Perturbative They are not really related. Let's plug in $H^*(-;G)$ as the extraordinary cohomology theory in the AHSS. Call it $h(-)$ for convenience. Then AHSS promises us a spectral sequence starting from $H^*(X;h(pt))$ to $h(X)$. We start from singular cohomology with coefficient groups equal to $h(pt)$. But $h(pt) = G$ in degree zero and is otherwise zero. So you are starting from $H^*(X;G)$ and going to $H^*(X;G)$.
You don't pass through $\Bbb Z$-cohomology on the way. The AHSS provides no new information for ordinary cohomology theories.
The AHSS is in some sense a vast generalization of cellular cohomology. What I told you there is the $E^2$ page of a spectral sequence. The $E^1$ page (of the most common derivation of this SS for a CW complex $X$) is $C^*_{cell}(X;h(pt))$. The differential is the cellular differential. When $h$ is an ordinary cohomology theory the story ends after this page.
But in general if $X^k$ is the $k$-skeleton of a CW complex and $f: S^k \to X^k$ is the attaching map for a $(k+1)$-cell, the induced map $h(S^k) \to h(X^k)$ depends on a lot more than just the top cells of $X^k$; it depends also on how they were attached to lower cells. This is in stark contrast to ordinary cohomology (when you just need to know the degree to each top cell, and from there cook up the cellular chain complex)
And that's where the higher differentials come from
@LeakyNun Interesting. I see a lot of concepts sound/feel similar across the intro courses I've done.
 
1 hour later…
15:36
Hello people!
 
2 hours later…
17:57
$P| (p_1)^{a_1}(p_2)^{a_2}..(p_n)^{a_n}$ where P and $p_i$ are primes is not possible when $P>p_i$ for every $p_i$
 
2 hours later…
19:46
Convex polytope question...
Suppose I've got a polytope M in an m-dimensional space, and I project it down to some polytope N in n-dimensional space. If I pick one of the vertices of N, is there anything I can say in general about the dimension of its preimage in M? (i'm assuming that dim(M)=m and dim(N)=n as well)
@Semiclassical well in general it would be m-n right
well, the example that comes to mind is taking a cube and projecting it onto a plane
and if I pick a generic plane, then there's only one vertex of the cube that'll map onto a vertex of its shadow
in which case the preimage is zero dimensional, not one
depends on which vertex really
there are 8 vertices
19:52
Eight vertices of the cube, sure. But I'm asking about vertices of the shadow
And in general the shadow of a cube has six vertices
oh
hmm, this is interesting
(Also, the dimension being m-n only makes sense if m>=n. But that is the context I have in mind.)
I mean, the preimage in that case can be 1D. Take the case where the plane is parallel to a face of the cube
What I'm not at all sure of is whether the preimage of a vertex being 0D is generic or not.
(something something "plane in general position" I guess)
i think this is relevant. not totally sure: mathoverflow.net/q/307951/55904
I think the point is that, while the preimage has to be a face of the original polytope M, there are faces of dimension 0 through dim(M)-1
e.g., vertices themselves count as faces
What does it mean exactly to integrate a function $f\colon G\to\Bbb C$ against the (left) Haar measure on $G$? ($G$ is a locally compact topological group)
(I'm confused by the codomain being $\Bbb C$ instead of $\Bbb R$)
@AlessandroCodenotti $(\int_{g \in G} f(g) \ \mathrm dg) \in \Bbb C$
Sure but how is that integral defined?
20:04
or if you want, $(\int_{g \in G} \Re(f(g)) \ \mathrm dg) + (\int_{g \in G} \Im(f(g)) \ \mathrm dg)i$
Do I split $f$ into real and imaginary part?
Perfect, that makes sense
thanks
> For brevity, we have chosen not to state
or prove such additional results in this article since, thanks to the a priori estimates yielded by
Prop. 9.2, their statements and proofs are similar to the ones given in [50, Theorem 2].
Nice
20:12
someone's doing some hardcore analysis
@Sila shalom
@RyanUnger how are you comfortable with that many symbols
what do you mean this many symbols
20:19
like in your paper
I see a lot of symbols
there's really not that many different symbols
goes with the territory
the hardest thing about mathematical GR is that there's essentially one textbook and it covers the absolute bare minimum basics
everything else is entirely in papers
> This paper has been withdrawn by the author. The paper has been accepted for publication in Communications on Pure and Applied Mathematics.
what?
I mean, I guess the implication is that the journal didn't want there to be a preprint version of an article they're publishing
but the v1 of the preprint is still up, soooo
From the webpage of that journal: The journal primarily publishes papers originating at or solicited by the Courant Institute of Mathematical Sciences
really strange journal
20:32
CPAM is not strange...
mainly publishing papers related to a certain institute is not strange?
Isn't Annals that way?
No, of course not
CPAM is one of the best analysis journals, and Courant is very analysis-heavy. So it's not strange.
It is published by Princeton, but as most journals, it publishes whatever is submitted to it (that meets its standards)
20:36
I'm pretty sure CPAM is that way too. Yau talks about it in his book.
The first Calabi conjecture related paper was in CPAM, because Caffarelli liked it.
@RyanUnger The passage I quoted above is the first thing it says in their description
Yau wasn't affiliated with Courant.
Yeah and I'm saying that's a strange sentence. You can't trust everything on the internet.
they might publish other stuff. They might even work exactly as all other journals. But the phrase is weird to me
It is from the journal's own description
"primarily" is a bit of an escape clause here
That was a tounge in cheek remark
The "solicited by" is key
You submit your paper to a Courant professor and if they like it, it can be submitted to the journal
That's what it seems like
20:40
Sure, and that seems strange to me as I said. I know the journal has a good reputation (I had seen the name before even though it is way outside my own field), but for any up-and-coming journal any sentence like that would have been a huge red flag
Kyoto should publish a journal containing papers approved by Mochizuki. Oh wait, don't they already do that?
No, it was only a rumor that it was going to be published by PRIMS
(or possibly it really was, but they realized how bad it would look, no way to know)
@TobiasKildetoft so just looking through the recent papers, most of the authors are one degree of separation from Courant faculty
(these are the people I recognize)
Urgh I'm stuck on a computation not working out... It's been a while since this last happened, very annoying
what are you computing
20:48
I'm checking that a thing those notes defined really is a *-algebra, but I'm doing some stupid mistake in checking that $(ab)^\ast=b^\ast a^\ast$ because it's not working
I have a locally compact group $G$ with it's left Haar measure $\mu$ and its modular function $\Delta\colon G\to\Bbb R^+$. I look at $C_c(G)$, the space of complex valued functions on $G$ with compact support, and I want to turn this vector space of functions into a *-algebra
what's the modular function
If you fix $g\in G$ then $\mu_g$ defined by $\mu_g(E)=\mu(Eg)$ is also a left invariant measure, so it must differ from $\mu$ by a constant, $\Delta(g)$ is the constant such that $\mu_g=\Delta(g)\mu$
$\Delta$ is actually a (continuous) group homomorphism $G\to\Bbb R^+$
The multiplication is convolution, $(ab)(g)=\int_G a(h)b(h^{-1}g)\mathrm{d}\mu(h)$, while the involution is defined by $a^\ast(g)=\Delta(g)^{-1}\overline{a(g^{-1})}$
oh right
I remember this
Terminology question
So I get $(ab)^\ast(g)=\Delta(g)^{-1}\overline{(ab)(g^{-1})}=\Delta(g)^{-1}\int_G\overline{a(h)b(h^{-1}g^{-1})}\mathrm{d}\mu$
while $(b^\ast a^\ast)(g)=\int_Gb^\ast(h)a^\ast(h^{-1}g)\mathrm{d}\mu=\Delta(g)^{-1}\int_G\overline{b(h^{-1})a(g^{-1}h)}\mathrm{d}\mu$
21:02
Suppose I have n-by-m complex matrices $A,B$. Then the Hilbert-Schmidt inner product is just $\langle A,B\rangle = \mathrm{Tr}(A^* B)$ where $*$ is hermitian conjugate
And here I'd like to use $\int_G f(ax)\mathrm{d}\mu(x)=\int_G f(x)\mathrm{d}\mu(x)$ to conclude, but I have something wrong
Supposes now I have some positive-definite m-by-m matrix $\rho$. Then I think that $\mathrm{Tr}(\rho A^* B)$ should also be an inner product
(I'm allowing $\rho$ to be complex, so it's necessarily Hermitian by definition of PD)
Is there a name for how that relates to the standard H-S inner product?
@AlessandroCodenotti this is really hard
like a mayor problem of rep theory basically
e.g. "it's the H-S inner product with respect to $\rho$" or "it's the H-S inner product weighted by $\rho$"
Leaky explained to me that it depends on the dimensions of the irreps
21:10
why know that there are as many conjugacy classes as there are representations, but is there are nice correspondence? The general answer I think is that we don't know
I guess determining those dimensions is really hard in general
no
what if you have multiple irreps of the same dimension
there's a correspondence worked out for $S_n$ over $\Bbb C$ I think
Then you have multiple factors $M_{n_k}(\Bbb C)$ with the same dimension?
yes but which factor corresponds to which conjugacy class?
you don't have a canonical correspondence
Oh ok, I see your point
I was mostly interested in how to determine the $n_k$ though, which was answered by Leaky
21:12
oh okay
yeah that follows from how you prove Artin-Wedderburn basically
(I guess my question just comes down to whether there's standard terminology for weighted norms/inner products)
@MatheinBoulomenos I keep hearing about this theorem, I will have to learn it and its proof eventually!
@AlessandroCodenotti these are complex functions?
@Alessandro wait a moment what did Leaky tell you lol
21:14
It's in the transcript, after the message I wrote and you just replied to
leaky is in trouble
@MatheinBoulomenos The correspondence for $S_n$ also works out in a similar way for other finite Coxeter groups
so the thing is
the matrix factors correspond to irreps
though it gets a bit more complicated
and the dimensions are the degree of the matrix rings
but this is not related to sizes of conjugacy classes
I was confused there
@TobiasKildetoft thanks
I was about to ping you :)
21:16
Oh yeah, I was assuming it was related, but I was wrong
@AlessandroCodenotti there are as many irreps as conjugacy classes
There is another way to go about the one for $S_n$ that also works out nicely (and gives the same answer which is a bit surprising). But that one does not work out as nicely for the other Coxeter groups
Is there a name for the general correspondence problem?
but the dimensions of the irreps and the sizes of the conjugacy classes are not (known to be) related
at least I don't know a relation
the size of the conjugacy classes sum to the order of the group. the sum of the squares of the dimension of irreps (or the matrix factors) sum to the order of the group. So it seems unlikely that there is a relation between two kinds of quantities which are related like that
lol that sounds weird
21:17
Got it, thanks
you know what I mean
@AlessandroCodenotti the algebra C[G] can be decomposed to sum of matrix groups, with dimensions corresponding to the dimensions of the irreps
"unlikely that there is a relation between two kinds of quantities which are related like that"
Well, there is a relation...namely, they're both related to the underlying group itself.
21:19
But that's not a very useful relation in this context, heh
not really no
Thanks for you help @Leaky @Mathei
The KL basis allows for a way that directly associates 2-sided ideals to partitions in such a way that the ideal gives the same irrep as one would associate to the partition via Specht modules
Do you also happen to know what am I messing up in my Haar measure computations above?
I only did like Haar measures on locally profinite groups
21:20
this also works out for other Coxeter groups, except one no longer gets an irrep
there everything is basically locally constant
so integrals are actual sums
so I don't know
@TobiasKildetoft hmm, I need to learn about this
$\Delta(g)^{-1}\int_G\overline{a(h)b(h^{-1}g^{-1})}\mathrm{d}\mu = \Delta(g)^{-1}\int_G\overline{a(g^{-1} h)b((g^{-1} h)^{-1}g^{-1})}\mathrm{d}\mu = \Delta(g)^{-1}\int_G\overline{a(g^{-1} h)b(h^{-1})}\mathrm{d}\mu$
@AlessandroCodenotti where's the problem?
I don't see why the second integral is equal to the first
You're multiplying on the left by $g^{-1}$, right? So you get $b(g^{-1}h^{-1}g^{-1})$
@MatheinBoulomenos KL theory is pretty cool. Also really weird and I have no idea how they could ever have come up with it in the first place.
I don't have much time for rep theory right now sadly
21:28
@AlessandroCodenotti I'm multiplying g^-1 to h
not to the input of the function, whatever it happens to be
Oh of course
Thanks, that was dumb
@AlessandroCodenotti (shameless plug) it's on my blog ;)
along with one lemma that has a triple application of Zorn lol
I think "the Hilbert-Schmidt inner product weighted by $\rho$" is as good as I'll get
> Not wishing the Germans to know that he was an expert in hydrodynamics, since he feared that if they found out he would be forced to undertake war work for them, Leray claimed to be a topologist. He worked only on topological problems for the years he was held captive in the camp.

Although he had undertaken some topological work it was not easy for Leray to work on the topic without reading topological literature. He was able to obtain some papers through Hopf who was at this time in Zürich but much of Leray's work was done independently of the developments which had taken place in the s
oh wow
I didn't know that
01:00 - 22:0022:00 - 00:00

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