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04:32
@MikeMiller Thanks!
user116211
Is there any difference between $\sum_{ij}$ and $\sum_i\sum_j\;?$
05:00
Hi
What is the meaning of a surface being "closed"
It means it doesn't have a "boundary".
In my textbook, it says "If the surface is closed, then the boundary curve is empty and the surface integral is 0"
closed like a sphere is closed?
Yeah, sphere is closed.
but the surface integral through a sphere is not always 0
A surface integral on a sphere is always $0$, by Stokes' theorem.
Why do you think it isn't?
05:03
but
because like in Divergence theorem, surface integral over sphere is not 0
Can you give me an example?
I am losing context here, surely you mean you are integrating a gradient of something on the sphere?
wait actually, I think that only happens is F = curl(A) for some A
Right that's how I interpreted it.
Your book says that, right? Because I agree it's not true that all surface integrals over the sphere is 0.
yep, i just didn't read the sentence before about it
OK, great.
05:10
suppose F = del(f) for some f, so it has a vector potential, and is conservative. Then does that still apply?
the thing about the surface integral over a sphere being = 0
You're integrating F over the sphere?
yeah
Um, no, it need not be true, I don't think.
so just because F = del(f) for some f, it does not necessarily follow that F=curl(A) for some A
No, definitely not.
05:17
ok great. Thanks!
06:07
Hi, @Huy.
Huy
Huy
morning @BalarkaSen
what's up?
Huy
Huy
@BalarkaSen: about to teach, just revising stuff for graduation exams
you?
not much, about to start doing math again.
Huy
Huy
good, have you been cooking in the meantime?
06:18
yeah, i can boil water now
Huy
Huy
very good. soon you'll be ready to mix water and syrup.
@Huy can you teach me the quasi isometry proof
Huy
Huy
@MikeMiller: maybe later, the question I asked last week was related to the proof. I need to work on a few parts for a bit before I'm convinced
@MikeMiller: the proof in F&M contains a lot of statements without proof or reference, and some intuitively make sense and some don't, but most aren't that easy to prove (at least for me)
06:39
@Huy what would mixing water and syrup accomplish though?
fair enough
 
3 hours later…
09:52
Hi @Kari
Hey, @BalarkaSen!
How's it going?
It's ok. Not doing much math this week.
How about you?
Hi!
Its about polynomials
10:10
https://www.youtube.com/watch?v=gpM_rnQBCr0
I wonder how can one construct a proof that the symmetric way that this ad shows will ensure it took the least number of steps to completely exchange all business cards for n people?
11:02
I don't suppose anyone has CARAT installed?
11:16
@robjohn Cool news! I developed a new master theorem that will appear in my second book. I think a powerful master theorem (one piece) is enough for a single book.
(stuff unseen before in no environment because it wasn't invented - my estimate is that a master theorem can be used to easily write 5-10 books (300-400 pages) each one)
I love them.
Theoretically, you can use them indefinitely, I mean you can write infinitely many books, but after a while the stuff you get looks too ugly for a potential reader.
But, yes, theoretically you can write infinitely many books using each one. Limitless potential!
11:38
@Semiclassical btw, almost forgot to ask you if you slayed that limit I gave you some days ago, the easier version.
Preparing for a trip. Back later if possible.
11:53
Hi!
Can someone help me with this question? http://math.stackexchange.com/questions/1790284/finding-the-prime-factors
Its about number theory (related to prime factorization)
@Henry Do you know Euler's totient funtion? (it is not strictly needed here, but it will make things a bit simpler)
12:14
Does anyone see a simple proof for math.stackexchange.com/questions/1790290/… . I feel it is meant to be obvious
but sadly it's not obvious to me
sry I never really thought seriously about probability theory
@JuanFran no problem
I think it's going to be very simple for someone :)
Hello again @JuanFran.
12:37
what is the operation called on two matrices A and B where you take the inner product of the concatenation of the columns of A and the concatenation of the columns of B?
12:51
@felipa $A^TB$?
@AkivaWeinberger thanks!!
It's the Hilbert Schmidt inner product apparently
Is anyone here familiar with maximum likelihood estimation?
Huy
Huy
you should be
don't you do that to get an estimator for the mean, variance, etc. ?
13:06
I will hopefully take statistics in my school this year.
Huy
Huy
I don't think you'll like it
well, hopefully I'll prove you wrong. :)
Huy
Huy
:)
13:19
hi @BalarkaSen sorry I was AFK
No worries.
@felipa Well, the trace of that, probably
(Sum of diagonal elements)
13:53
Hello @BalarkaSen
How are things
Hi @AliCaglayan
@AliCaglayan It's alright, still learning math. How about you?
@BalarkaSen Yes. Studying for exams
Then university
Good luck with the exams.
Thank you very much
@BalarkaSen Perhaps you would be interested in this
Have you ever seen diracs belt?
13:59
The demonstation that Su(2) double covers So(3)
In mathematics and physics, the plate trick, also known as Dirac's string trick, the belt trick, Balinese cup trick, is any of several demonstrations of the mathematical theorem that SU(2) (which double-covers SO(3)) is simply connected. To say that SU(2) double-covers SO(3) essentially means that the unit quaternions represent the group of rotations twice over. == The trick == One way of doing the trick is to rest a small plate flat on the palm, then perform two rotations of one's hand while keeping the plate upright, ending in the original position. The hand makes one rotation passing over it...
I have seen it.
I stumbled upon it yesterday I found it very interesting
Although more classically it's used as a demonstration of fundamental group of RP^2 being Z/2.
I guess its rare to get a demonstation in algebra
That SU(2) double covers SO(3) is not really an algebra fact.
14:02
@TobiasKildetoft Thanks! I've solved it.
@BalarkaSen I read about coming from Lie algebras
Here is a small problem for anyone interested. Given a matrix that can be written as $\left [\gcd(i, j)\right]_{ij}$ component wise, what is it's determinant?
I mean SU(2) is the group of unit quaternions, which is the 3-sphere. That double covers RP^3, which is precisely what SO(3) is.
@BalarkaSen That is a simple way to think about it
I suppose this double cover preserves the group structure though, so perhaps there is more to it than just the topology.
I submit that Sp(1) is the group of unit quaternions and SU(2) is the group of 2x2 special unitary matrices.
14:06
Well, they are isomorphic, aren't they?
Yep.
But so is the multiplicative group of positive reals and the additive group of all reals, e.g.
One doesn't use the notation for one to refer to the other. Pet peeve of mine when everyone calls SU(2) unit quaternions.
@Ali Why would you want to think about it in a complicated way? The simpler the better. But I am talking about the picture, I do understand that it might be more than just a map between the topological spaces.
@anon Fair enough.
Why is thinking of the unit quaternions as Sp(1) more preferable than SU(2)? Just curious, I do not know these groups too well.
Well, two distinct questions here. One is of notation. From the outset, Sp(1) and SU(2) refer to different things. They happen to be isomorphic. So one could in principle identify them. Which is the second question: under what circumstances is it a good idea to identify them? For the purpose of having the double cover of SO(3), I think it's a lot easier and more direct to just think about Sp(1) than SU(2).
A lot more people know about SU(2) than quaternions though which is I suspect part of the reason they do that.
"For the purpose of ... I think it's easier and more direct to just think about Sp(1) than SU(2)" I was asking why you think that, actually.
One can prove Sp(1) double covers SO(3) using basic geometrical properties of the cross product. How would you do it for SU(2)?
(Also, do you know why they're isomorphic?)
@AliCaglayan Sp(1) or SU(2) is the universal covering group of SO(3). u.c.g. can be constructed explicitly as the group of endpoint-preserving-homotopy-classes of paths emanating from the identity. a path in SO(3) from the identity is essentially a continuous family of rotations, which is actually more akin to our intuitive mental picture of what a rotation is than an actual rotation. (a single rotation has only a before and after, and no in between.)
In turns that for paths in SO(3), rotating 360 degrees around an axis is distinct from not rotating it, but 720 degrees isn't. If one affixes an object to an unmoving environment using, say, belts, one can interpret the twisting of the belt as encoding a memory of how the object was rotated, and hence the trick.
14:18
I don't know how to construct a map SU(2) --> SO(3) directly. I usually just show SU(2) is isomorphic to the group of unit quaternions (which is easy, just write down the matrices for 1, i, j, k) and construct the map by making the unit quaternions act on $\Bbb R^3$ by rotations. I think the last bit requires some work.
You conjugate span(i,j,k) by unit quaternions to get rotations. :-) I've written about the geometry in a number of answers under arctic tern.
Can anyone suggest me some book to study analytic NT?
@anon I'll have a look at those answers.
Thanks.
14:21
Wow! Looks Good. Thanks a lot!! @robjohn
Does it cover Dirchlet Convolution?
@robjohn
Nice question from a middle school test
People from a city speak either French or English. If 64% speak French and 58% English, how many speak both languages?
I received tons of wrong answers (unfortunately).
@robjohn Whoa Shafarevich wrote an analytic number theory book.
That's pretty cool.
@Henry It doesn't do much with convolution,
Oh.
That could be in either an algebraic or analytic NT book
14:30
Still a good book though
it is
No Problem, I'll find it elsewhere :)
I've been told that convolution is analytic NT
Also, does inclusion - exclusion come in NT? I thought it was combinatorics.
Combinatorial flavor of number theory, yes.
Mostly used in sieve theory.
Someone used Inclusion Exclusion to solve this NT problem brilliant.org/problems/exploring-divisor-function-4
Can someone tell me how inclusion exclusion is used here?
@Henry @BalarkaSen is our expert in NT problems
14:38
I do not know number theory.
In particular, I won't be able to help.
@AliCaglayan Oh, I just remembered. There's a cute "application" of the belt trick which can be used to demonstrate a constructive proof of the sphere eversion theorem. You might want to look into that, there's a youtube video of it somewhere. It's incredibly cute.
Not to mention surprising.
@BalarkaSen What is it called?
Eh, maybe it's not quite the belt trick but it looked a lot like it. In any case, it's worth watching.
@Ali "How to Turn a Sphere Inside Out".
@BalarkaSen Oh yeah I have watched that.
Ah, ok.
@BalarkaSen Yeah it was an argument with turning numbers
14:47
Um, no, winding numbers can be used to show why it fails for the circle.
There is no homotopy-through-immersions of the identity and the antipodal map from the circle to R^2. Because these have different winding numbers.
14:59
I have posted an elementary set theory question on MSE, I'm having a difficulty proving it. Can anyone please help? math.stackexchange.com/questions/1790497/show-that-aa-geq-2n-1
15:12
can someone tell me how to solve this $\frac{d^2x}{dt^2} = -(\frac{k}{m})x$
this is simple harmonic motion
yep
the answer is $x=A\sin\left(\sqrt{\frac km}t-\theta_0\right)$
how do you get that solution
well, firstly, do you know that $\frac{d^2x}{dt^2}=v\frac{dv}{dx}$?
15:14
@user1618033: good morning
yes
what do you get when you use that substitution?
if you integrate with respect to $dx$ on the right side you get $-\frac{kx^2}{2m}$
@robjohn Hi (here is 18:15 :D)
which isn't sinusoidal
15:15
but the left hand side becomes $\frac12v^2$
you're missing a constant also
so $\frac{v^2}{2} = -\frac{kx^2}{2m} + C$
how is that turned into a sine/cosine function?
Express that, with $v$ being subject
what do you mean subject?
Well, $v=...$
oh
$v = \sqrt{-\frac{kx^2}{m}+C}$
15:18
now, note that $v=\frac{dx}{dt}$
$\int dx = \int {\sqrt{-\frac{kx^2}{m}+C}~dt}$
like so?
not so fast
take the reciprocal of both sides
$\frac{dt}{dx} = \sqrt{-\frac{m}{kx^2} + C}$
and then you can go ahead
remember that you try to group terms with the same variable
so, $x$ and $dx$ on one side, $t$ and $dt$ on the other side
oh I see, then solve for $x$ at the very end
15:21
yep
oh, you forgot to take the reciprocal of the right hand side
oh, you took it wrongly
oh
remember there's a $C$ there
I thought $\frac{1}{C} = C$
like it's a constant regardless
but $\frac1{x+C}$ is not $\frac1x+C$
@robjohn I got some fantastic result today, but I had to work for it a pretty long time.
15:24
oh
that would be an integral of the form $\int\frac{dx}{\sqrt{a^2-x^2}}$
which means trigonometric substitution (or Euler-substitution)
I guess in this case it would be useful to keep the $C$ as $\frac{1}{C}$
not really
@user1618033 That's great! I am home today, but I have a lot of things to take care of here.
$\frac{dx}{dt}=\sqrt{C-\frac{kx^2}m}$
$\frac{dt}{dx}=\frac1{\sqrt{C-\frac{kx^2}m}}$
15:25
@user1618033 I will try to take a look at the problem you sent
oh .. lol
@robjohn you refer to the limit I sent to you? If, yes then that is great. One more thing, try also the variant without the zeta expresson in front, it is very nice.
@kennyL Isn't there another way to represent this harmonic motion? I feel like there could be a more general periodic function that one could construct
The limit is $0$, but this is less important. For the version I sent to you, the limit is $1$. Mathematica goes crazy after a while and gives wrong results.
@Obliv using the formula above?
13 mins ago, by Kenny Lau
the answer is $x=A\sin\left(\sqrt{\frac km}t-\theta_0\right)$
15:27
@user1618033 Can you post the question here, I like limits.
instead of $\sin$ couldn't we use $f(x+P) = f(x)$? i read this is a general definition for periodic functions here en.wikipedia.org/wiki/Periodic_function
@Henry That one not really now (I have some plans with it).
@robjohn it's nice to notice some things there for the simpler version without zeta in front.
@user1618033 Oh ok. No problem :)
@Obliv I believe it must be $\sin$, because that's what solving that integral gives
@Henry :D
15:31
hmm for a respectfully notable room as mathematics, that is too much few chatters to be in
or maybe it is summer !
hence holidays
@robjohn btw, someone contacted me these days showing some interest for buying my book project. The thing is that I wouldn't accept any offer ever, no matter what. This is not a business.
It was unexpected though.
@Agawa001 Maybe you can help me. Can you tell how is Inclusion Exclusion used here?
Or you @user1618033
@Henry I'm not into these problems for a long while, although I admit they are cool. When I return to this stuff, I'll let you know.
@Henry if noone from the members rowed right there to the margin could help you, how would u expect from me to do me poor math thing ?
@Henry Maybe you like this inequality
If $P$ degree$>2$ and $P'$ has all real roots, then

$$\frac{\displaystyle \int_a^b \frac{1}{P'(x)}\ dx}{\displaystyle \int_a^b \frac{1}{P''(x)}\ dx}>\frac{P'(b)-P'(a)}{P(b)-P(a)}$$
15:39
look there is some heavy-reputed members as robjohn who are more dignified, just ask dot ask to ask @Henry
Can anyone help me find the explicit formula for the recursive series $(k+1)a_{k+1} = 2a_{k-1}$
@user1618033 Do you know a Latex rendering website?
@Henry Read the description of this chatroom
@NoahHarris all the even terms are skipped?
also, what is the initial term?
Haha! Thanks @KennyLau
$a_0 = 1$
15:42
So all the odd terms are skipped?
Oh, but I don't want to install, I want online Latex renderer...
Yeah, they should be I think
They're zero anyway
@Henry You don't need to install
just a bookmark
it's a javascript code
@kennyL I see why. The $\sin$ function is a specific periodic function. If the equation was not $F = -kx$ and instead something that produces a periodic function like the first image here en.wikipedia.org/wiki/Periodic_function then sin wouldn't be the solution to such an integral
so $a_2=\frac{2}{2}=1$
15:44
I don't know of any equations that would produce such a periodic function and I can't imagine how getting the solution would be though
@KennyLau you became regular here? see how this place is useful but it is just summer holidays, so you r ought to wait another 2 or 3 months
$a_4=\frac{2a_2}{4}=\frac12$
$a_{k+2}=\frac{2a_k}{k+2}$
$a_k=\frac2ka_{k-2}$
$a_2=\frac22$
$a_4=\frac24\frac22$
$a_6=\frac26\frac24\frac22$
@NoahHarris Can you see it now?
@KennyLau That's magic!
Latex has now appeared!
Thanks.
@user1618033 I have noted your question. Seems interesting. I'll solve it in home later.
gtg, bye everyone.
15:50
@Henry You'll try you mean. :-)
uh I see $\frac{2^{n/2}}{n!!}$
Some tutoring sesion here. Later.
yes @NoahHarris
yikes.
single dollar sign to make it in-line
15:50
Yeah
"Mean", funny. I'll first try Mean value theorem :D @user1618033
Well, that's not nothing. But don't think that's what I was supposed to get
well
I can make it better
For reference this is what I'm trying to do: math.stackexchange.com/questions/1789074/…
sure, I can do that
$n!!=2\times4\times\cdots\times n=2^{n/2}(n/2)!$
15:57
@MikeMiller I'm trying to get back to math. Where should I start? Guillemin-Pollack chapter 1? If there's anything specific you'd want me to do before that, I'd have a try too.
Oooh. That looks helpful, thanks @KennyLau
@NoahHarris bonus question: how do you convert $n!!$ where $n$ is odd?
I want to start by reading some manifold theory as we planned to do.
@anon I'm not sure I agree it's that much more direct. you have an action of $SU(2)$ on $\Bbb C^2$; projectivize to get a linear action on $S^2$; extend over rays to get an element of $SO(3)$. I guess you could complain that there's work to be done in seeing that the thing you get in the end is an element of $SO(3)$
@BalarkaSen I gave you those linear algebra problems, but there's not really any serious need to do them - they tie in to some geometry, but geometry we're not ready for yet. G&P ch1 is not a bad idea. You know ch3, so you might as well do 1-3 and the exercises.
I think you already know what's in ch1 but it's harmless to go through again anyway.
In fact I suspect you're already aware of quite a lot of it. There's no harm in not doing stuff you already know how to do.
Alright, great, I'll start on GP 1-3 for now and occasionally think about those lin. alg. problem you gave. I'll ping you with the solutions of (what I think are) hard and interesting exercises from GP if you want too, if that's ok to you?
16:05
Yup
There are some fundamentals worth learning, but once we're done with those we can figure out where you want to go with all this
@MikeMiller I guess, but I suppose I need to do the exercises to get comfortable with it. I also usually try to learn things by heart: e.g., I can probably prove all the theorems that are in Hatcher, except perhaps Poincare duality, so I'd want to give it a read.
Well, Hatcher minus appendices and chapter 4
@MikeMiller Alright. I should also note that I probably won't be able to get things done super-fast as in what happened with differential forms from Ted's book, since I have not-so-pressing school work (school hasn't really started and won't start anytime soon, but I want to get ahead a bit).
I hope that's ok. I promise that I won't take a decade to learn it though.
I am skeptical. But sure.
I mean, in contrast to what happened with multivariable calc.
Multivariable was fast?
Well, apparently I took too much time to learn it than was needed. I am just saying even though I go slow on G-P, I promise that won't happen.
16:16
Oh, ok.
16:38
Hi @TedShifrin!
hi @Balarka
Did you finish all the Stokes's Theorem stuff?
You haven't been here for quite a long time!
@TedShifrin Yeah.
I've been back once or twice. About to disappear again for 2+ weeks.
Aw. Are you on a trip again?
16:40
About to be.
@MikeM: If I stopped to edit everyone's spelling and grammar, I'd never read any math.
Ah. Happy journey.
@MikeM: It's pretty clear I'm the one who got the quotient topology wrong. Sloppy mental miscue on my part.
I already don't do any math, so no harm.
@TedShifrin Well... I agreed with you. :)
Clearly points are closed in the leaf space. Now I'm trying to decide what the correct example (if any) might be where there can be dense points.
Anyhow, makes me more pleased with my charges. And glad I can be irresponsible and retired :)
Maybe you were thinking of torus foliations.
16:45
@TedShifrin Speaking of Stokes' theorem, interpretation of Stokes' theorem (at least the 3d version) using flux (i.e., using the Hodge dual of the forms) is much more clear, I agree now.
You mean solid torus, @MikeM? Somehow I doubt it.
No, @Ted, irrational lines.
I agree the Euclidean case is probably unsalvageable.
Namely, integrating (summing up) the divergence ("things flowing out of small nbhds around points") you get the flux along the boundary surface ("amount of thing which flows out of the surface").
Oh, surely points aren't closed in that case.
Right, @Balarka: That's the physicists' "proof" that I was suggesting to you for Green's Theorem (but you can do it for work just as for flux).
yes, in that case the leaf space is uncountable indiscrete
16:48
Ah, I see.
I gather I've missed more contentiousness from our favorite chatter who keeps changing names.
Did you do the exercise 8.5.22, @Balarka? That's actually a very important concept for modern geometry.
And you saw 8.7.7, 8.7.9, 8.7.12?
The standard version of the Green's theorem might be a bit unintuitive as stated, but thinking of curl as "the amount of thing some small ball rotates around it's axis when placed at a point under the action of the vector field", it becomes "small swirlies add up to big swirly on the boundary" which should be intuitive because one can think of swirls in opposite direction cancels out like this:
Sure, of course.
there's probably some nasty foliation of higher-dim Euclidean space, since I'm pretty sure your Haefliger-Reeb theorem comes from Poincare-Bendixson theory, which doesn't really generalize
Right, @MikeM. I actually am not sure I've ever thought about this.
And all my books that might be interesting to look at for this are long given away.
16:53
it's not in candel-conlon
in hunting for it, by the way, found the charming result: "if $M$ is compact and has finite fundamental group, it has no real analytic codim 1 foliation"
Hmm ... Does that come from lamination theory or something?
@TedShifrin Yep, but I didn't do 8.7.12. I liked Milnor's proof of hairy balls.
Pedro recently ran into that Milnor proof somewhere and posted it on his blog, I think.
You had inquired about 8.7.12 earlier. That's why I mentioned it.
What about 8.5.22 and calibrations, @Balarka?
guys if I'm to prove that if $x$ is an element of the group $G$, then $\{x^n~|~n\in \mathbb{Z}\}$ is a subgroup of $G$, how am I sure that $G$ is closed under exponents?
What do you mean by "closed under exponents," @Obliv?
16:57
@TedShifrin Hmm, I looked, that I didn't do. Is that the proof of the minimal surface equation using forms you mentioned earlier?
@Ted: It's reduction to Poincare-Bendixson (pulling back the foliation to a singular foliation on a well-chosen disc) and then some holonomy analysis; the contradiction comes because they get that the holonomy is (germinally) trivial on one side of the curve but not the other
which is nonsense if you're real analytic
Yes @Balarka
like that $x^n \in G$ @tedS
Ah, very cool, @MikeM.
Are you asking why all the elements $x^n$ actually belong to the whole group $G$, @Obliv? I do not understand.
Oh cool then I have to do it! I noted it down.
16:58
you have calibrations in your book? very cool...
I'm asking that based on the information given is it a valid assumption that $x^n \in G$?
It's a powerful argument, @Balarka. They appear in an exercise only, @MikeM.
seems hard to do a whole lot with them at this point though, but I guess that's the minimal surface equation you mentioned
Yes, @Obliv, because $G$ is closed under multiplication and inverse to start with.
You need to show that $H=\{x^n\}$ is non-empty and closed under multiplication and inverse.
are all groups closed under multiplication?

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