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00:00 - 18:0018:00 - 00:00

00:46
@PedroTamaroff Yes I have learned both
Taking my AP calculus BC exam this year
So that I can go multi next year
 
2 hours later…
02:40
Hello
Is $\int_{-\infty}^{\infty} e^{- \frac{x^4}{\alpha^4})$ equal to 1?
02:54
Is $\int_{-\infty}^{\infty} e^{-\frac{x^4}{\alpha^4}}dx$ equal to 1?
Wolfram should answer that for you
Hi PVAL
Hi
03:29
I'm just going to leave this here...
 
2 hours later…
04:59
Hi
There is a flux function F defined on R^m to M^{m \times n}
Can you tell me what M is?
hello @user19405892
I need help with a geometry question
okay
what is it?
here is the solution
i don't get how we can assume $A_0...A_{n-1}$ is convex
05:09
Draw picture
The only angle to worry about is A1A0A{n-1}
Rest all are < 180
oh right
Make two cases:
One in which this is <180
then it is convex
yes
automatically
case 2 is when ot is >180
*it is
ok
why can we ignore case 2
05:13
then you can extend the line say, A2A1 or A3A2 to intersect A{n-1}An
what does that mea
*mean
make a picture to see this
it could potentially intersect two segments right?
if it hits a vertex
also i don't see what this pronlongation so that it intersects shows
@zed111
The reason why the second case can be ignored is because say A2A1 intersects A{n-1}An
do we need to prolong it
?
05:20
that is not convex
yes i meant it to be concave
Make it for the second case: angle A0A6A5 > 180
hi @ForeverMozart.
Also internal angle A6A5A4 in the fig you made is > 180. It can't be
hi whats new
05:24
not much
I found a space with the following properties
connected
remove any point and get two components
@zed111 I can't understand it...
Hausdorff compactification of it with remainder [0,1]+[0,1]
but the compactificatin has no cut points!
Your figure is misleading since all the internal angles are not < 180 which is required by the question
Clearly the angle A6A5A4 is > 180
05:27
thats all I got
Ive been working on presentations
@zed111 better?
I need to take a shower so i'll be back in 15 min
Oh this looks okay sorry
05:28
i turn on the water
brb
then what
how can this case be disregarded
Now you have a convex polygon
whose one vertex is b/w A1 and A2 => consider it as new A0
*new A6
you can prolong because the condition (i) in the question still holds
i blow dry my hair
cause I have 70s hair
sort of like this guy google.com/…
05:44
is that shiny too? @For
@ForeverMozart
actually more like this
so stylish :)
hehe
@user19405892 I hope you are also done with scratching your hair... on this question
at least its not like this:
if I fail at math I can always open a nostalgia hair salon
 
5 hours later…
10:47
Can someone send a link to the Mathematics stackexchange question that discusses this picture: curiosamathematica.tumblr.com/post/55356261770/…
I have seen it before here, but I can't remember what to search for.
11:00
@MatsGranvik This exact picture ? Or coud it be another image of the spiral zeta ?
@Hippalectryon Yes thanks! Exactly.
@Hippalectryon I now tried to bookmark the question you sent me. Turns out I already had it bookmarked in my browser. Silly me.
Haha :-)
11:16
Hi. I have started with Counting and was trying to understand the concept of choosing. If I flip a fair coin 50 times, I have 2^50 outcomes. Now if I want to know how many ways can I get 5 heads and 45 tails?
I came up with 2^50_C_5 ways of selecting 5 element subsets, and multiply that by 50! because there are 50 places to put those coins
Is this correct?
@TusharTyagi 2^50C5 is just the number of ways to get 5 elements in 2^50... which is not what we're looking for, since were getting 5 elements in 50
There are (way) more than 5 outcomes out of the 2^50 that have exactly 5 heads
Will that 50! multiplication help?
Overall I was thinking 2^50C5 x 50!
I don't think so. One correct way to do it would be as follows : for the first heads you have 50C1 ways, for the second you have 49C1, ... for the 5th you have 46C1, so overall you have 50*49*48*47*46/2^50 chances
Hmm. Your numerator is equal to 50C5 x 5!
That's 5 elements subsets out of 50 places.
Well of course :P we're selecting 5 elements out of 50
So the answer is 50C5/2^50
11:29
Sorry noob here, so that will mean picking 5 places out of the given 50 and fill them with heads
Haha, yeah :P
Yep, since once the heads are filled, the tails are automatically filled too
Yeah, now I get it. As you said, 2^50C5 will be wrong, we cannot pick just 5 out of all the outcomes, but we can pick 5 out of 50 tosses
5 places that is.
Thanks a lot :8
:)
No problem :D
11:49
Having a bit of trouble understanding why "we can replace $x^n$" in this proof.
12:43
I am thinking of writing another blog post, this time about some of the strengths of higher representation theory and categorification, highlighted by some examples. Not sure how much interest there would be though.
@TobiasKildetoft Blog posts are always welcomed though :-) even if there's not much interest right now, it could help many people in the future
@Hippalectryon True, but with the blog having been basically dead for a while, I am hesitant to put a bunch of effort into writing for it.
I mean, most of the comments in my last blog post were just advertisers trying to boost their search hits
:/
I liked your last blog post though :P
Glad to hear it
12:50
I need help with something simple in projective geometry
I am reading coxeter and it says in the introduction to the book that an isosceles triangle doesn't belong to the projective plane
why is that?
@user19405892 That sounds like a very weird statement
let me give you more context sorry
it was an exercise that said "Which of the following belong to the projective plane: (i) a parallelogram (ii) an isosceles triangle (iii) a triangle and its medians"
Still a very weird question. I mean, these are things that belong to the plane naturally. The projective plane is something else.
yes but doesn't the triangle belong to the projective plane in general? why wouldn't an isosceles triangle? projective geometry only uses the straightedge
@user19405892 I have no idea what you mean by that last part. The projective plane is defined in a certain way, which does not involve a straightedge
12:56
oh
nor does it use the compass?
@TobiasKildetoft pastebin.com/SaT7D88C that 'exercise' comes right after the intro of the book. Maybe it hasn't been properly defined yet.
@Hippalectryon ah yes that's what i thought, but that shouldn't change the answer to the question?
@Hippalectryon Ahh, I have never studied projective stuff like that. I don't really see the point of doing these things the way they were introduced so long ago
@user19405892 The idea is that in the projective plane, we can no longer really measure lengths, so a triangle being isosceles does not make sense
@TobiasKildetoft Ah, i see now. But technically the triangle still exists though right?
@user19405892 Sure, triangles exist, but we cannot distinguish which ones are isosceles
13:01
not everything in the euclidean plane is constructible using ruler and compass but is everything in the projective plane constructible using compass?
@user19405892 The compass is enough in Euclidian geometry
you can't construct an angle of 42Ëš in the euclidean plane
@Hippalectryon Well, for those things that could also be constructed with rules and compass. Not everything can be constructed with those.
Ah, yeah indeed, that's what I meant
i think i am confused what they mean when they say projective geometry uses only the compass
because not everything in the euclidean plane is constructible
is the same true in projective geometry?
13:06
>.> I haven't really done any projective geometry so I'm gonna avoid saying false stuff haha
I have just read the intro of the book you mentioned and the wiki page
I have never done any of that "construct using..." stuff.
"the geometry of the straigghtedge at first seems to have very little in connection with the familiar derivation of the name geometry as 'earth measurement'"
i have no idea what that means
doesn't it seem to have a lot of connection?
 
1 hour later…
14:18
hi
is angle, side and height a congruence
hhh
hhh
14:49
Can someone explain why each $x\in\mathbb Z$ has a multiplicative inverse $x^{-1}$?

The division is not defined in the ring. So for example what is the multiplicative inverse of $5$ such that $5*5^{-1}=1$?

Is the fact that $\mathbb Z$ is a ring explained with rational integers? Even though we cannot divide, we can define inverse elements with rational integers (https://en.wikipedia.org/wiki/Integer)?
hhh
hhh
15:08
Moved question here.
Hi. I'm trying to prove that $\displaystyle\lim_{(x,y) \to (0,0)}xy=0$. So I need to show that for every $\varepsilon>0$ there is a $\delta>0$ such that $|xy|< \varepsilon$ whenever $\sqrt{x^2+y^2}<\delta$. Can anyone please give me a hint as to what to do next?
hhh
hhh
Can someone explain $6=2\cdot 3=(1+\sqrt{-1})(1-\sqrt{-5})$ in the extension $\mathbb Z[\sqrt{-5}]$?
Huy
Huy
@MikeMiller: in the image I sent you, I sometimes use different notation for the same thing ($\| \cdot \|_{H^k} = \| \cdot \|_k$ for example). I was just too lazy yet to go over the document and make all notation "well-defined"
15:26
hi
hhh
hhh
28
Q: Why is $\mathbb{Z}[\sqrt{-n}], n\ge 3$ not a UFD?

Danielle Intal I'm considering the ring $\mathbb{Z}[\sqrt{-n}]$, where $n\ge 3$ and square free. I want to see why it's not a UFD. I defined a norm for the ring by $|a+b\sqrt{-n}|=a^2+nb^2$. Using this I was able to show that $2$, $\sqrt{-n}$ and $1+\sqrt{-n}$ are all irreducible. Is there someway to concl...

@Huy what image did you send me
hhh
hhh
Thing for my own question, probably useful.
Huy
Huy
@MikeMiller: email
(morning)
@Huy: A supreme pedant would say you mean "compactly supported smooth function" everywhere. Luckily, I'm not one.
Huy
Huy
15:29
@MikeMiller: it's not perfectly rigorous yet, just quickly written down
@Huy: how are your manifold Sobolev spaces defined? Are they just "Do the thing but on charts and add 'em up"?
Huy
Huy
@MikeMiller: basically, but I also wrote it down on the upper right, did you see that or is it unclear?
Sorry, yes, I missed it. I'm a little slow this morning.
In which case I agree. Once you have it in $\Bbb R^n$ it should be a formal exercise.
Huy
Huy
@MikeMiller: so what I wrote down for it makes sense? and the step that fails in general is switching order of limit and sum to make the sequence Cauchy?
(for the compact manifold case, I mean)
Hrm, the step that fails in general should be a uniformity problem, maybe
In that case the sum is a finite sum but doesn't have bounds independent of the function (you're summing over charts covering the support of $f$, but there can be arbitrarily many of them)
Something like this
Huy
Huy
15:43
urm
why is the sum still finite in general?
@DanielFischer In this answer (which is sort of related to what we were talking about yesterday), you state that the integral over the large semicircle vanishes because $|\sin (\mu z)|$ grows exponentially as $\text{Im} (z) \to \infty$. Are you implicitly using the proof of Jordan's lemma here?
@Huy: You're summing over a locally finite cover, presumably, and your input is not a function, but a compactly supported function. A compactly supported function hits only finitely many elements in a locally finite cover.
Huy
Huy
right
15:58
hi
i need some help on a geometry probelm
i don't get why we can reduce it to the convex case
anyone have any idea?
@Huy sorry for being slow this morning.
16:13
@RandomVariable Yes.
@DanielFischer Can you help with my question?
Huy
Huy
@MikeMiller why are you saying this twice?
@user19405892 Geometry is too complicated for me, I do that only if necessary.
@DanielFischer Do you mean geometry in general or this question?
I think that Daniel Fischer said implicitly that he did not want to do geometry :) @user19405892
16:28
@user19405892 Geometry in general. I didn't even look closely at the question. I saw it has angles and such …
@DanielFischer Hello, a consequence of Morera's theorem is that when a sequence of holomorphic function $f_n$ converges uniformly to $f$ then $f$ is holomorphic then. So when we are ( juste as an example) on the open disc $D(0,1)$ we can write Cauchy's formula for $f$ around a disc $D(0,r)$ for $r<1$, but if we have only uniformly convergence on the circle $bD(0,1)$, it doesn't follow necessarily that $f$ is holomorphic on the hole disc right ?
@JeSuis We're assuming that the $f_n$ are continuous on the closed disk and holomorphic in the interior, aren't we? Use the maximum modulus principle on $f_n - f_m$.
@DanielFischer badly stated sorry, I take a sequence of holomorphic function $(f_n):D\to \Bbb{C}$ where $D$ is the open unit disc, we assume that $f_n$ converges uniformly to $g$ on any circle $\Gamma_r$ centered at $0$ of radius $r<1$. Does it follows that we have uniformly convergence on the closed disc $\overline{D}(0,r)$?
@JeSuis Yes, maximum modulus principle.
16:44
Someone should prove that $C(\phi) = 0$ for all $\phi$.
@DanielFischer to $f_n-f_m$?
@JeSuis Yup.
@DanielFischer I just saw it yesterday, so let's see if I can do it :D. As $f_n$ is holomorphic on $D(0,r)$ and continuous on $\overline{D(0,r)}$, and non constant (assuming that the constant case is trivial). Then for $f_n-f_m$ we have for all $z\in D(0,r) \Vert (f_n-f_m)(z)\Vert\le \sup_{\Gamma_r}\Vert f_n-f_m\Vert$ and now we the uniform convergence right ?
17:07
But we can only conclude on the open disc, not the interior.
morning
@MikeMiller that's a neat problem
i'm curious how that would read if one works in terms of $z=x+i y$
Not very helpfully, I don't think. I tried some examples in polar coordinates but didn't get far.
17:16
hrm. unfortunate
Note that this is a group of symplectomorphisms, which helps us a bit, since there's quite a bit of study on that.
i'm forgetting what that means in this context.
preserves the area form?
Yes
On a surface, a symplectic form is the same as a volume/area form
perhaps foolishly, the moment i hear 'symplectic' i hear 'phase space'
so i wonder what an interpretation in terms of classical mechanics would be
@DanielFischer Is the fact that $\left| \sin (\mu z) \right|$ remains bounded on the portions of the contour near the real axis as $R \to \infty$ enough to conclude that the integral vanishes along those arcs as $R \to \infty$? What's bothering me is the fact that $\frac{z}{z^{2}+a^{2}} \sim \frac{1}{z}$ as $|z| \to \infty.$ What's happening to the length of those arcs as $R \to \infty$?
17:19
e.g. thinking of the area form as $dx\,dp$
It's the canonical example of a symplectic manifold, but you're thinking too rigidly. We're on a very small symplectic manifold - a small open subset of the usual phase space $\Bbb R^2$ of a particle on a line.
Classical dynamics usually moves outside a disc, methinks.
hmm.
well, if you start with a harmonic oscillator potential $H=x^2+p^2$, then the phase space is foliated into concentric circles by different choices of energy $H=E$. so if you set a maximum positive energy $E_{max}$, then that'd give you $D^2$.
and more generally it'll be diffeomorphic to $D^2$ if you pick a potential $V(x)$ with a single global minimum and then pick energy to be sufficiently close to that minimum.
not convinced that's the right way to think of that, mind
@DanielFischer I meant that $\left| \csc (\mu z) \right|$ remains bounded.
OK, yeah, it's an old theorem that this group is perfect.
the one of interest in that problem?
17:28
Yeah. I can find it mostly in fancy language.
So the homomorphism has to be zero, since it's a map to an abelian group. But that makes one wonder "Can I prove it's zero without invoking big machines?"
(In particular, the proof that the group is simple, or the proof that it's perfect, are longer than I would be willing to write on that post.)
what i'm forgetting right now is the meaning of such a symplectomorphism in classical mechanics.
Coordinate change that infinitesimally preserves the dynamics.
right. there's a name for that, in physics, and i'm forgetting it
17:31
Well, eh, maybe not quite.
For instance, given a Hamiltonian vector field, its flow preserves the symplectic form.
time evolution preserves phase space, yeah
that's just Liouville's theorem in classical mechanics, if memory serves
@Hippalectryon Salut!
"phase space density" is the right phrase, though
In any case, I find it unlikely philosophical perspectives will help. If it has a straightforward solution, it should be from clever symbol-pushing.
Since, after all, that's how $C$ is defined.
admittedly, the change of perspective more for my own curiosity than to supply any proof.
ahah, found it. in classical mechanics, it's called a canonical transformation.
though, actually, i can't remember if that's the right scope. i.e. every canonical transformation counts as a symplectomorphism, but i don't remember if the reverse is true
17:41
Presumably canonical transformations are elements of the linear group of symplectomorphisms.
can you clarify that?
They're presumably in particular linear transformations.
this answer on Physics.SE gives definitions from two textbooks (the first being the one i used in grad school)
and Spivak's definition seems to be "canonical transformation = symplectomorphism"
canonical transformation that simplify the hamiltonians ?
I used the first definition which was used in goldstein
Spivak's Definition: A transformation $f:\mathcal{P}→\mathcal{P}$ on phase space is canonical provided it preserves the symplectic form.
17:50
gotcha
so i'd say there's no need to restrict to the linear group here
@JeSuis o/
@MikeMiller amusingly, while you were editing your answer, i noticed this bit on wiki's page on symplectomorphisms (link)
which references Banyaga. namely, "Groups of Hamiltonian diffeomorphisms are simple, by a theorem of Banyaga."
not sure that's quite the same as what you're referencing, but the two definitely seem linked
I was referencing a related (easier) theorem.
17:57
Simple implies perfect.
Well, I guess simple implies perfect or cyclic of prime order. But it should come as no surprise that diffeomorphism groups are not cyclic of prime order...
I thought a canonical transformation preserved the contact structure.
@Hippalectryon comment ça va ? alors bientôt les concours ?
@TedShifrin hello
I guess it depends whether we're doing contact manifolds or symplectic manifolds.
Bonjour, @JeSuis et @Hippa.
@TedShifrin yeah, and classical mechanics is the latter.
17:59
@JeSuis oui :( ça va sinon
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