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00:24
I'm offering a bounty of 50 points for the following, should-be-simple question.
1
Q: Bijection from $A \rightarrow \varnothing$

MunoMy thoughts. We need to prove that: 1 $\forall x,y \in A, \text{ if } f(x) = f(y) \rightarrow x = y$ 2 $\forall y \in \varnothing, \exists x \in A, f(x) = y$. In (1), $f(x) = f(y)$ is false, since neither $f(x)$ nor $f(y)$ have a value, so (1) is vacuously true. Also, $\forall y \in \var...

00:54
@Shaun what do you not like about the selected answer?
01:14
0
Q: What functional equation does the "first in a twin prime pair" indicator function satisfy?

EnjoysMathBasis for the $\Bbb{Z}$-module of eventually vanishing functions on $\Bbb{N}$. Let $M$ be the module of all eventually vanishing functions and for $f \in M$ define $N_f$ to be the vanishing point, i.e. it's the minimal $N_f \in \Bbb{N}$ such that for all $n \gt N_f$ we have $f(n) = 0$. Certain ...

K, I've done it now
Proof completed nearly
 
1 hour later…
02:25
can some help me with this question math.stackexchange.com/questions/219941/…
 
2 hours later…
03:58
When I compute $e^{tA}$ here (i.imgur.com/amXWu0Y.png) I get a different answer than when I compute $YY^{-1}(0)$ here (i.imgur.com/K9ieAdO.png), where the fundamental solutions for $Y$ are shown here (i.imgur.com/gnZhJeN.png) and $Y$ is inverted here (i.imgur.com/75QeXTk.png). What am I doing wrong?
04:21
Morning
Pig
Pig
04:54
@BalarkaSen Hey - sorry I haven't read your previous messages yet
 
1 hour later…
06:18
@Trey where are you having trouble?
06:34
Did you read about the first black valedictorian at Princeton? @robjohn
@skullpatrol Nicolas Johnson? No I haven't ;-P
:D @robjohn
user434058
Is there any general method/procedure to find the maximum and minimum values of $|f(z)|$, where $f(z):\mathbb C\rightarrow \mathbb C$ is a complex function analytic everywhere?
06:52
@FakeMod-Inactiveaccount by Liouville's theorem the maximum (you mean supremum) must be infinity and the infimum must be 0
unless the function is constant
user434058
@LeakyNun Thanksl Now what about constrained optimisation. In the sense that $g(z)=0$ is the constraint and now we are supposed to find the maximum and the minimum values of $f(z)$?
$g(z) = 0$ defines a discrete set of points, unlike what you might expect
(if $g$ is analytic)
so you can't continuously trace through the zeroes of $g$ to maximize/minimize $|f(z)|$
so I don't know how you would do it
user434058
Mostly, I encounter questions where $g(z)=|z|-a$ (where $a$ is a constant). A typical example: Maximize $f(z)=|z^3-z+2|$ under the constraint that $|z|=1$.
user434058
07:02
@LeakyNun you can't. But could you use any complex equivalent of Lagrange Multipliers?
aha, then $g$ isn't analytic
cool fact for you: by Maximum Modulus Principle (MMP), the maximum in $|z| \le 1$ occurs on $|z| = 1$
user434058
@LeakyNun nope :P
user434058
@LeakyNun um... But that won't give the correct answer in my "typical example", which is $\sqrt {13}$...
why not?
are you sure it's $\sqrt{13}$?
user434058
@LeakyNun Oh sorry, it would :P I misread your message...
user434058
07:05
@LeakyNun definitely sure.
user434058
Though I know the long method of using polar form and then applying single variable calculus, however it's too cumbersome and boring :(
$|z|=1$ is a nice submanifold, so Lagrange multipliers should work
user434058
07:24
@Thorgott Could you please explain how (if convenient)?
How do i find range of (x+1) + 4/(x+1) ? without using differentiation @LeakyNun
use differentiation
use AM-GM to find lower bound lol
It's mentioned not to use differentiation
Oops!!
Thanks!! Just a glitch
@anakhro It says, on one hand, that $A$ must be zero, yet, on the other, that $A$ can be arbitrary.
what glitch
07:30
Glitch in my mind
@Shaun if a function $A \to \varnothing$ exists then $A$ must be empty
What about this one (x+1) + 4/(x+9) ?@LeakyNun
-8 + (x+9) + 4/(x+9)
I'm really confused in finding range when fn is of type like f(x) + 1/ g(x) ??
@LeakyNun thanks once again
@FakeMod I never thought this through, but you should just be able to translate it back to $\mathbb{R}^2$, apply the usual Lagrange multipliers there and translate it back
user434058
07:37
@Thorgott Oh! That's what I did for the first time. But again, it's cumbersome :) I suppose it's the only method...
I don't see any other method. The behavior of an analytic function on the boundary of a circle can still be rather arbitrary, I think, so holomorphicity may not make that much of a difference
I don't know anything about optimization except Lagrange though, so don't take that as a definite no
@Thorgott You proved smoothness of $\Phi$ on charts, right
user434058
@Thorgott alright Thanks :)
@Pig No worries! I talked to Ted about it extensively, I think I understand the issue now. You raised a good point
Thanks for the discussion!
@Balarka not yet, should I?
I guess I should
wait, the $U_i$ constitute an atlas already
07:53
@Thorgott Given any continuous function $g : S^1 \to \Bbb R$ there exists a continuous function $f : \Bbb D \to \Bbb C$ such that $f$ is holomorphic on the interior of the disk and $\Re(f)|\partial \Bbb D = g$.
In fact you can just demand $g$ to be $L^2$
Then $f$ will similarly be an $L^2$ functions such that ...
wha-
Wild, right?
damn, I knew there was something like this
but I didn't picture it to be that bad
@Thorgott yeah
and on each $U_i$ it's smooth
it agrees on the overlaps $U_i \cap U_j$ by uniqueness
right, so they essentially glue together by definition?
08:00
yup
so gluing together smooth functions on manifolds is for some reason easier than gluing them together on $\mathbb{R}^n$
well, cause $\mathbb{R}^n$ has an atlas only given by one chart, I suppose
haha yeah
the curves $\gamma_x = \Phi(x, \cdot)$ are called the "flowlines" of $X$ (starting at $x$), the map $\Phi$ is just following this flowline for time in $(-\varepsilon, \varepsilon)$. The flowline is a canonical object on the manifold $M$, but you have proved that on $U_i$ this "following the flowline" map is smooth in $x$ parameter - so it must be that it is globally smooth in $x$ parameter
So you do get a smooth map $\Phi : M \times (-\varepsilon, \varepsilon) \to M$. Can you tell me why $\Phi(\cdot, s + t) = \Phi(\cdot, s) \circ \Phi(\cdot, t) : M \to M$, for all $s, t, s + t \in (-\varepsilon, \varepsilon)$?
$\gamma_x$ is basically tracing the path the point $x$ traverses on the manifold if it moves in the direction given by the vector field at each point with time?
Yup
Doing this globally on $x$ paints the picture of a "flow", every point moves time $t$ in the direction given by $X$ at each point of time
I'll think about the homomorphy in a couple minutes (currently in a lecture, but there's a break soon)
08:08
Think of the vector field on $S^1$ given by the unit tangent counterclockwise, which I like to call $\partial/\partial \theta$. The flow along this vector field for time $t$ is given by rotating $S^1$ counterclockwise by angle $t$, so this particular flow keeps rotating $S^1$ counterclockwise forever and ever with unit angular speed
Ya sure
More pictures: Consider the vector field $X = p \, \partial/\partial x + q \,\partial/\partial y$ on $\Bbb R^2$ and scale it to be unit by $T = X/\|X\| = X/\sqrt{p^2 + q^2}$, just for convenience. Note that $X$, hence $T$, is invariant under the action of $\Bbb Z^2$ on $\Bbb R^2$ by vertical/horizontal translations.
Therefore $T$ descends down to a vector field on the torus $T^2 = \Bbb R^2/\Bbb Z^2$.
What does the flow look like?
@BalarkaSen $f$ will be smooth on the interior and $L^2_{1/2}$ up to the boundary :P
08:42
@MikeMiller I was hoping a night of sleep might give me some new insights, but alas. I am trying to figure out your four-line-one-line proof. All I could think of was to take for each $(g,g)$ on the diagonal a small neighbourhood $V_g\times V_g'$, such that for $(x,x')\in V_g\times V_g'$ we have $\vert h(x)-h(x')\vert<\epsilon$.
Ted suggested to find a $U$ such that $(g,g')\in \tilde{U}\iff gg'^{-1}\in U$. For a fixed $g\in G$, we have $(g,g')\in V_g\times V_g'$ iff $g'g^{-1}\in (V_g')g^{-1}$, which is indeed a neighbourhood around zero. However, the problem is that I fixed $g$, so this is useless I think. I don't see any other way tho.
Why are you fixing $g$
Consider the map $\varphi: G \times G \to G \times G$ sending $(g,h) \to (g, hg^{-1})$
What is $\varphi(V)$ a neighborhood of?
Or rather, what is $\varphi$ of the diagonal?
@MikeMiller Ah
Sobolev trace lemma says that restricting L^2_k to boundary loses 1/2 of a derivative
For L^p should be 1/p but I always forget some details (does it hold for all k? can I do it for boundary hypersurfaces? I think these are true but I forget)
I should learn this stuff eventually
Next semester I will probably, when I take complex analysis and functional analysis afterwards. Doubtful they'll do proper functional analysis but can't hurt to learn
I think I wrote how to get the result you mentioned from APS somewhere
08:55
Oh possibly
Btw, what are integrable functions which simply satisfy the mean value property? In what sense do they solve $\Delta f = 0$?
@MikeMiller Ah, so, $\phi$ is a homeomorphism, so we know $\phi(V_g\times V_g')$ is open. And since $(g,g)\in V_g\times V_g'$, we know that $\phi(V_g\times V_g')=V_g\times U$, where $U$ is a neighbourhood of the identity. Now, we have $(x,y)\in V_g\times V_g'$ iff $(x,xy^{-1})\in V_g\times U$. However, and this was my problem which is why I fixed $g$, we still don't have $xy^{-1}\in U\implies (x,y)\in V_g\times V_g'$.
What is $V_g \times V_g'$ wtf
Who introduced that
oh, I did before, sorry should have clarified
so $V_g\times V_g'$ is the neighbourhood around $(g,g)$
Yeah I didn't say pick a small neighborhood of one point, that's not going to help you
such that for $(x,y)\in V_g\times V_g'$ we have
o..
right
08:59
You're trying to do this over all of $G$. Why would you restrict to a neighborhood of one point, right?
to START with you have $(g,g') \mapsto |h(g)-h(g')|$, which is a map $H: G \times G \to \Bbb R$
And then $V = H^{-1}(-\epsilon, \epsilon)$ is an open set which contains the diagonal, because $H(g,g) = 0$ for all $(g,g)$ on the diagonal
You're trying to show that there is a neighborhood of the origin $U$ so that if $g' g^{-1} \in U$, then $(g,g') \in V$
It will not help to do this any less than globally, over all of $G$ at once. Anyway, this is the $V$ I was talking about
Try the hint for that
Right, I will think about it, thanks
Hi there, anyone here interested in both surreal numbers and quasicrystals?
09:39
@MikeMiller Right, I finally see it x) So, $\phi$ is a homeomorphism, whose inverse is given by $(x,y)\mapsto (x,y^{-1}x)$. We have $\phi(V)=G\times U$, for some open $U\ni e$. Now, if $gh^{-1}\in U$, then $(g,gh^{-1})\in G\times U$, and hence $(g,h)\in V$.
or actually... I haven't used compactness now, I think
No we don't, @ShaVuklia
We have that $\phi(V)$ contains $G \times \{e\}$
There's no reason to believe that $\phi(V)$ is a product itself though
And indeed you haven't used compactness of $G$ yet. From what I said above, what can you get about $\phi(V)$?
Ah, man x) Right so, for each $g\in G$, we can find a product, $V_g\times U_g$, where $V_g$ is a neighbourhood about $g$, and $U_g$ a neighbourhood about $e$. By compactness of $G$, we only need finitely many to cover $G$. Taking this finite intersection of $U_g$, should give us $U$ then.
don't you know a lemma that means you don't have to do more work?
there should be a lemma that immediately applies to the situation above
oh, tube lemma?
Anyway, lets interprete a 1D quasicrystal as a surreal number. The surreal numbers of day $\omega$ e generated from a sequence of right, left operations. If we take for example the Fibonacci chain which is encoded as a series of such two different symbols, we would obtain a day $\omega$ surreal number.
As the Fibonacci chain is not a uniquely defined sequence of symbols (the paricular sequence depends on how it was generated exactly, e.g. substition, multigrid, cur and project, ...) I ask myself how the corresponding set of surreal numbers is composed.
09:49
ye okay, that is nicer x)
Yes, the whole point of this setup is that you wanted a sort of tube around the diagonal, right?
But there isn't a "diagonal tube lemma"
So we use the group structure to turn the diagonal into a slice
At which point we just have the tube lemma
@Rudi_Birnbaum how high are you
I haven't read the chat guidelines .I am new here. Hope it is not very strict chat which kicks you out for asking question.
Nobody here has the power to kick you
if you read the chat description you'll see "Just ask; don't ask to ask."
09:54
The worst case scenario is that nobody can / wants to answer your question, which can happen
@MikeMiller Oh, that's what that $\phi$ did. Right:D thanks, that makes it more intuitive.
@LeakyNun Its not easy to quantify ...
That was why I did it in the first place :)
It possibly has a nice answer: I conjecture, that the difference between two such Fibonacci-chain surreal numbers is a finite day generated number.
The idea is that the different Fibonacci chains are identical up to a finitely long sequence of elements.
@LeakyNun So what I am aiming at would be Freeman Dysons proposal of a classification of 1D-quasicrytals.
(Of his "birds and frogs" talk)
10:21
Jo zeeeas @Rudi
@MikeMiller ?
@robjohn At that moment... ;)
@MikeMiller Ah, I thought I was still in the room. I must have floated off...
10:57
@EdwardEvans Zeeeaas @Edward
wia gäds?
bist in DE oder GB?
@Rudi_Birnbaum how dare you call Britain gross! :P
@LeakyNun right, UK is anyway more accurate ..
Gross Britain
@Balarka Ok, I claim that for a function $\Phi\colon M\times(-\varepsilon,\varepsilon)\rightarrow M$ satisfying $\Phi(p,0)=p$ for all $p\in M$, the following two properties are equivalent.
1. $\Phi(p,s+t)=\Phi(\Phi(p,s),t)$ for all $p\in M$ and $s,t$ such that $|s|,|t|,|s+t|<\varepsilon$ and $d\Phi(p,-)\vert_0=X(p)$ for all $p\in M$.
2. $d\Phi(p,-)\vert_t=X(\Phi(p,t))$ for all $p\in M,|t|<\varepsilon$.
Suppose $\Phi$ satisfies 1., then $d\Phi(p,-)\vert_t=d\Phi(p,t+\cdot)\vert_0=d\Phi(\Phi(p,t),-)\vert_0=X(\Phi(p,t))$ (hard abuse of notation), so $\Phi$ satisfies 2.
@Rudi bin noch in DE hehe
Hast den lockdown gut überstanden?
11:10
Jaaa für mich war's eh business as usual
Was meinst wie das weitergeht?
irgendwie hab ich nichtmal was gemerkt hahaha
Ich hab ehrlich gesagt keine Ahnung, aber mich freut's wenn ich von daheim aus arbeiten kann hahaha
(ehrlich gesagt: mich auch ...) lol
nächste Woche muss ich mal in die uni und einen Lehrfilm aufnehmen
das erste mal seit 2 Monaten...
wird hart, aber was tut man nicht für die Studis
11:12
ooof, ich halte einen Seminarvortrag in einem Monat ungefähr, den ich auch von daheim halten werde lol
Sind deine Leute daheim ok?
Ja denen geht's gut, aber die englische Regierung ist echt kacke
BoJo ...lol
aber eigentlich ned lustig
ja überhaupt nicht, aber man kann nur halb lachen lol
Absoluter Trottel
und dann der krasse Typ da sein Beraterkumpel wie heisst der?
11:15
Dominic Raab?
Dominic Cummings
?
Humor ist, wenn man trotzdem lacht
ahhhh kann sein
Dominic Raab ist der Außenminister lol
irgendwie hab ich seit der Parlamentwahl angefangen die britische Politik zu ignorieren
und die Tagen zu zählen bis ich die deutsche Staatsbürgerschaft beantragen kann hahahaha
@Thorgott ja
The Germans have taken over the chat
11:27
d'Deeeeitschn
;-)
Germs?
Germknödel
11:48
I have to "find a condition" such that the image of an ideal under a ring-homomorphism $f$ is again an ideal.
I think the task is strange, since I could say $f$ is surjective and I'm obviously done - but what is the minimal condition for this?
Or, wait, is this condition minimal? If $f$ is not surjective I can always choose a field for the target Ring, and then $f$ yields a non-ideal as image as long it does not map everything to zero, right?
@Alessandro I feel like functional analysis is just the triangle inequality with extra steps
There's an extra "functional" in your sentence
rofl
just about to have a seminar talk on semisimple rings and Artin-Wedderburn
and then directly after a talk on local fields lol
AND my copy of Lang's algebra is arriving today; I have a wheelbarrow ready to transport it up to my room once it arrives
Nice, good luck for your talks!
12:05
@EdwardEvans lol
this one?
@Thorgott Excellent
I claim you can just extend that to an actual homomorphism $\Bbb R \to \text{Diff}(M)$ by going $\varepsilon/2$-much everytime
12:28
Can I find this limit $$ \lim_{n\to \infty} \frac{q^n \pi}{n !} \left(\frac{\pi}{4}\right)^n $$
why not $2\varepsilon$?
Please guide me
The most I can think is that the denominator grows faster than numerator and hence the limit may be zero.
ratio test will do the job
@Knight Use Stiriling's approximatio
that's way overkill
12:37
$n! \approx \sqrt{ 2 \pi n} (n/e)^n$
boom
Solved now?
the limit is trivial, Stirling's approximation is not, there's no reason to use it
I just stated why
13:17
Out of curiosity, is there any way to swap the antidiagonal elements of a 2x2 matrix using matrix multiplication?
That is: $$\begin{bmatrix}a&b \\c&d \end{bmatrix} =\begin{bmatrix}? &?\\?&?\end{bmatrix} \begin{bmatrix}a&c \\b&d\end{bmatrix} \begin{bmatrix}?&? \\?&?\end{bmatrix}$$
@Thorgott What is ratio test? (if that reply was for me)
@Thorgott I mean, you don't know if the flow exists at time $\varepsilon$. You know it exists at time $\varepsilon/2$, so you extend it to exist for $(-\varepsilon, \varepsilon) \cup (\varepsilon/2 - \varepsilon, \varepsilon/2 + \varepsilon) = (-\varepsilon, 3\varepsilon/2)$
And so on
@EdwardEvans Listening to Autumn Eternal by Panopticon
Seems good
@Knight if $\limsup\Big\lvert\frac{a_{n+1}}{a_n}\Big\rvert<1$, then $a_n\rightarrow0$
@Thorgott Basically what I am saying is for any $t \in \Bbb R$, choose $n \in \Bbb Z$ such that $n\varepsilon/2 < t < (n+1)\varepsilon/2$. Then define the flow as follows: For notational ease I will denote $\Phi_t(x):=\Phi(x, t)$. Define $\Phi_t := \Phi_{\varepsilon/2}^{\circ n} \circ \Phi_{t - n\varepsilon/2}$
@Thorgott Thank you.
13:28
Where $\Phi^{\circ n}_{\varepsilon/2} = \Phi_{\varepsilon/2} \circ \Phi_{\varepsilon/2} \circ \cdots \circ \Phi_{\varepsilon/2}$, $n$ times.
What I was thinking of is each real having a unique representative in $(-\varepsilon,\varepsilon)$ $\mod2\varepsilon$
These are well defined, because a-priori you knew $\Phi_s$ makes sense for $s \in (-\varepsilon, \varepsilon)$
but I actually can't take steps that large, so that doesn't make sense
Yeah what you said just needed to be modified a little I think
Great, so we have proved flowing along a vector field on a compact manifold always makes sense
compactness doesn't play a role in extending $t$ to all of $\mathbb{R}$, I take it?
13:32
given these transformations how do you find the "net" transformation that is some combination of the two? $x\mapsto x^2$ and $(1-x) \mapsto (1-x)^2$
is there such a thing?
Yeah, it doesn't, because what you proved gives us a uniform $\varepsilon > 0$ irregardless of $x \in M$ for which $\Phi_t(x)$ is defined for all $|t| < \varepsilon$.
In general, given a vector field on a noncompact manifold, this $\varepsilon$ will vary point-to-point. Indeed, take the example of the vector field on $\Bbb R$ I gave by pushing $d/dt$ forward along a diffeomorphism $\tanh^{-1} : (0, 1) \to \Bbb R$ so that the norm of the vector in the resulting vector field on $\Bbb R$ gets very huge as you go towards infinity. There $\varepsilon$ varies from point-to-point so much that you cannot obtain a uniform $\varepsilon > 0$ that works.
@SimplyBeautifulArt nvm lol
right, but if we have one $\varepsilon$ for a range of $x$, then we can always extend to all of $\mathbb{R}$ (but not necessarily to all of $M$)
I think if you inspect the proof closely you will be able to obtain a smooth function $\varepsilon : M \to \Bbb R_{+}$ such that $\Phi_{t}(x)$ is well-defined for all $|t| < \varepsilon(x)$.
Right
that's saying the solution interval of the IVP depends smoothly on the parameter
sounds believable
13:36
Yeah
Can some help me with this?
$f(x)=\frac {2020^{2x}}{2020+2020^{2x}}$. Find $\sum f(\frac {k}{2019})$ with k from 1 to 2019.
@Thorgott You remember the notion of tangentspacewise dot product I defined earlier, before the flow story?
@BalarkaSen what is this, German?
I'm still in the process of convincing myself this $\Phi_t$ is still additive
13:47
Fair enough. It's instructive to understand this in terms of the flowlines
Does this site do migrations any more?
@EnlightenedFunky no. unfortunately, for migrations, one should seek their closest embassy
like I have a question a meta, and I want it migrated and I remember when I opened my account they can migrate their question to the main stack
Like it was a whole a thing the question title would or some where around there would say migrated from MathOverFlow.SE
@Thorgott What does additivity mean in this context?
$\Phi_{s+t}=\Phi_s\circ\Phi_t$
13:54
Additive in time parameter
okay.
Ok, say we have $m\varepsilon/2\le s<(m+1)\varepsilon/2$ and $n\varepsilon/2\le t<(n+1)\varepsilon/2$. Then $\Phi_s\circ\Phi_t=\Phi_{\varepsilon/2}^{\circ m}\circ\Phi_{s-m\varepsilon/2}\circ\Phi_{\varepsilon/2}^{\circ n}\circ\Phi_{t-n\varepsilon/2}$. But $s-m\varepsilon/2<\varepsilon/2$, so these commute (and the choice of $\varepsilon/2$ really was the right one), hence $\Phi_s\circ\Phi=\Phi_{\varepsilon/2}^{m+n}\circ\Phi_{s-m\varepsilon/2}\circ\Phi_{t-n\varepsilon/2}$.
Now we are guaranteed to have $(m+n)\varepsilon/2\le s+t<(m+n+2)\varepsilon/2$. If, in fact, $s+t-(m+n)\varepsilon/2<\var
fuck
ok was just missing a dollar
Ya we extended something additive in (-eps, eps) additively to all of R so you expect that to be additive
Good to write down the details though
yeah, it's not surprising
just had to figure out that I can commute them through to collect exponents and then the case distinction
13:58
I should also convince myself this is smooth in $t$ still
wait, that's obvious
u should join leagues with feynhat
but is it jointly smooth still
no wait, I'm being nonsensical
for each $t\in\mathbb{R}$, $\Phi_t\colon M\rightarrow M$ is smooth as composition of smooth functions (in fact, all diffeomorphisms, so itself a diffeomorphism)
but, if I fix $p\in M$, is $t\mapsto\Phi_t(x)$ smooth?
right thats what i meant when i said think in terms of flowlines
this follows from uniqueness, and the fact that smooth functions on open things glue to smooth functions when they agree on overlap
Anonymous
Hi. If $A$ is a non-abelian normal simple subgroup of a group $G$ and $C$ is the centralizer of $A$ in $G$, could someone explain why $A\cap C = 1$?
for some reason I have a mental barrier in my head that's telling me smooth functions on open sets don't glue together that easily
14:04
the sticky point ur thinking about is smooth functions on closed intervals agreeing on endpoints of the closed intervals dont glue to a smooth function
yeah lol
but since we're doing (-eps, eps) U (-eps + eps/2, eps + eps/2) and you have smooth curves defined on each of those intervals which agree on the intersection by uniqueness, the whole thing glues to a smooth curve
I was just trying to construct a counter-example using bump functions and realized I'm being an absolute buffoon
no this is a fine point
it tells you that the gluing lemma is not really the sheaf axiom
the fact that they glue together here is just stating that smoothness is a local property, essentially
14:06
cuz the most useful form of the gluing lemma is gluing continuous functions over closed guys which is stronger than gluing them over open guys
ya that smooth functions form a sheaf, to be precise :)
actually, they agree on the overlap, because of additivity, no?
but well, additivity follows from uniqueness, so same thing, I guess
@Triskelion if a nontrivial element of $A$ centralized $A$ then that would be in $Z(A)$, but centers are normal subgroups...
@Thorgott ye thats true
ok, after two days, I think I'm finally ready to believe you that flows are a thing
next thing i wanted to tell you that if you have a vector field such that for a long stretch of time nothing happens on a region in the manifold then the topology of the manifold is trivial on that region
Your life would have been easier if you didn't believe
That's too vague bro I don't know what that means
14:13
i will tell him what it means
i have to clickbait first
Anonymous
@BalarkaSen Oh, and centers are also supposed to be abelian subgroups (which isn't admissible here as $A$ is non-abelian). So contradiction, I see. Thanks!
I need to explain to you this theorem of Fenichel once I understand if
no thats the wrong contradiction
Social Experiment: having a vector field such that for a long stretch of time nothing happens on a region (gone wrong, nearly trivialized the topology)
2
@MikeMiller see, this is scary
i misread fenichel as fenchel even though u gave me a heads up
awful
Anonymous
14:16
@BalarkaSen Non-abelian simple groups are also centerless I think
correct, you need simplicity
abelianity is just to avoid Z/p
Why are you guys splitting the domain into pieces? Is it to avoid saying things like 'whenever it is defined'? Wouldn't additivity follow trivially from uniqueness: For all $s$, $t \mapsto \Phi_{s+t}(p)$ defines a curve starting at $\Phi_s(p)$, which is by definition uniqueness $t \mapsto \Phi_{t}(\Phi_s(p))$? (Of course I have completely overlooked the fact that $s+t$ may not even be in the domain, but whenever it is, additivity holds).
it follows from uniqueness sure
we are splitting it into pieces precisely to define it everywhere
additivity on the initial interval (whenever defined) followed from uniqueness
Ah okay. Global flows? Have you assumed something about the field? (Sorry, I haven't been following this discussion).
Anonymous
14:21
@BalarkaSen Heh, I momentarily thought that non-abelian groups only have non-abelian subgroups. Which is, of course, terribly false.
pedants joining leagues
time to scurry
this discussion started two days ago, I'd be worried had you been following
the manifold was assumed to be compact
oh... okay. So, on compact manifold all fields are global?
Yes, Thorgott is writing down a proof, though you can too
14:24
Can? Probably. Will? Strong No.
I'm not sure what that means, what we've been discussing is that a smooth vector field on a compact manifold generates a unique, global flow
Yes, I was asking if you can always extend local flow (which always exists) to $\Bbb R \times M$.
thats indeed what thorgott means by a global flow
Cool.
You chatted up with the monk yet?
14:28
if you have a flow on $(-\varepsilon,\varepsilon)\times M$, you can extend it to $\mathbb{R}\times M$, this is what we did above
he told me probabilistic geometry is just a geometry bundle over a measure space
but you can't necessarily extend on $I\times U$ to $I\times M$ if $M$ is non-compact, it seems
@BalarkaSen shivers
also, if we have that it's smooth in $x$ and smooth in $t$ if we fix the other each, it's also smooth in $(x,t)$, right? cause an atlas on the product manifold is given by the products of charts
oof, no. not even true for a function $f : \Bbb R^2 \to \Bbb R$
ah C^1
ok
continuous partials imply multivariable differentiability, thats what you need
14:33
@BalarkaSen Were you thinking of continuous functions?
yeah
its not true for differentiable functions
but this is clearly given since everything's smooth
but actually, we don't need that
smoothness in Euclidean spaces is defined by the existence of partials of all orders
and you get partials by fixing all but one variable and differentiating wrt to the one that's left
(and you can do that all orders if fixing all but one argument gives you a smooth function each)
14:35
thats the right definition because that agrees with f is differetiable, Df is differentiable, DDf is differentiable, ...
I have never thought about DDf and I don't think I want to
Why man? Hessians are nice. Symmetric for C^2. And also help generalize the second-derivative test for extremas.
yeah, I like Hessians
Hessian = mixed partials, DDf = no clue tbh
but bordered Hessians are the real shit
14:41
no clue tbh
useful for lagrange multipliers iirc
yeah, that's why I know them
you formulate sufficient second-order conditions for maximization on a smooth submanifold using the bordered Hessian
what you actually want is for the Hessian of the Lagrange function to be positive- or negative-definite when restricted to the tangent space
and you can check that by calculating minors of the bordered Hessian
@BalarkaSen Roushon asked me to read an intro paper on Lie Groupoids... And Thurston's notes on orbifolds.
Cool!
Teach that shit to me, I need to know Haefliger structures
w h a t
14:45
no way that's in the lie groupoid stuff
No clue. But that H-word appears thrice in this paper.
It's a guy's name
oh i misread orbifold as foliations
Thanks Mike.
idk what lie groupoids are
14:48
Yeah any time
I guess Haefliger structures were one of the first places that topological groupoids mattered to people
it makes sense that a k-dim foliation is classified by maps to something its not super clear to me what
germs of homeomorphisms R^n -> R^n preserving the k-dim plaques of the std foliation?
The Haefliger groupoid on $X$ is the groupoid of germs of maps $U \to V$ where $U, V \subset X$
and that germ stuff is not going to be a group bcuz youre not fixing anything
its flowing along the leaves
so groupoid, i guess
You bake in both the topology of $X$ and the germs of maps
And then you define "Gamma-structure" like you would for "G-bundle" in terms of cocycles, but apparently the theory for groupoids is much richer
sounds annoying to set up
14:52
paper looks short
oh this should be simple enough
Let $G$ be the groupoid of germs of diffeomorphisms of $\Bbb R^k$, then on a manifold with a $k$-dimensional foliation you should naturally have a $G$-valued cocycle
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