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00:49
What's the name of the function that's f(x) = 1 + 2 + ... x ?
01:08
triangle numbers
01:22
@Akiva Yeah, but I am not convinced degree won't contribute to # of connected components.
 
4 hours later…
05:01
I have a question which is so simple I don't really want to post it. Given a scheme X with global section s, suppose the stalk of s is zero in every residue field. Should s = 0? If so, why?
05:21
Nevermind, it's obvious when you look at it affine-locally.
 
2 hours later…
07:45
Cool. I got a facebook message from a friend that he had noticed my name mentioned in one of the talks at the conference he was at. So there are actually people out there who have heard of my work.
I have not researched for any poster. This poster seems to me when he/she posted. He/she got 5 likes and more than 3 upvotes in 2-3 minutes without having any attempt?

http://math.stackexchange.com/questions/1883140/an-integration-of-product-1-xn
08:51
@TobiasKildetoft Very nice. You're quickly gathering fame and money, then? :D
@BalarkaSen Possibly fame, but not much money yet (I am highly confident that this too will come soon).
Good. You owe us a treat when it comes. :P
@Semiclassical I just realized that the wave equation comes from the Hooke's law. I am sort of excited by this observation, but it's probably very trivial.
Actually I am not yet quite sure how to formulate the picture rigorously, but it should just be motion of a spring after you lift some force from it. I'll think about it a bit.
Hi @arctictern
09:08
hi
What's up?
watching the man from nowhere and mr robot
enjoying random fruity vodka cocktail
huh, never heard of those two
Nice description "We can also think of e as a roadmap for a gentle stroll through the Bruhat graph (with much pausing to admire the scenery)"
My internet connection is terrible, and chat is not very good at figuring out whether it managed to send a message.
Bad internet connection is annoying, yes
09:35
@akiva you cant escape the fact one from either arabic or hebrew plagiarized from the other i think hebrew is the older right ?
10:03
hey @rob
Huy
Huy
10:20
mine's been terrible too the last few weeks, I surely will change provider when I move flats
@Agawa001 hi
@robjohn how are days
@Agawa001 still around 24 hours...
@robjohn i believe they turned out shorter
even with short nights not as in the two poles
11:26
Hi I am trying to do a proof by contradiction for the statement "a set of vectors of size < dim(V) where V is the vector space are always linearly dependent", but it seems I can get a contradiction to arise
Consider the following set S={v1,v2,v3,v4} and S is a subset of V and dim(V)=3. Suppose S is linearly independent, then there exists li such that

l1v1+l2v2+l3v3+l4v4=0 implies li=0 for i=1,2,3,4

Now suppose we have a basis set {a1,a2,a3} of V. Then any vi=sum_j cij aj where cij not necessary all zero is in the reals (as a zero vector cannot form a basis set). Since it is a basis, therefore the vectors in them are linearly independent i.e. p1a1+p2a2+p3a3=0 implies pj=0 for j=1,2,3

Therefore
and then using the assumption I got 0=0, which does not lead to any contradiction
Typo: I cannot get a contradiction to arise
11:39
@Secret surely you mean >dim(V) ?
yeah, I am trying to prove a set S of vectors with size > dim(V) must be linearly dependent via proof by contradiction, but I cannot seemed to get a contradiction to arise
Oh ok (you wrote <dimV earlier)
The best I get is that the ls can be not all zero, but all ls=0 is still a solution, therefore I am not sure if I have already caused a contradiction
I'm gonna be busy for 30-ish mins, I'll be back later if no one has helped you
Huy
Huy
12:02
when does one use algebraic vs algebraical, topologic vs topological, geometric vs geometrical?
12:44
I just use algebraic, topological and geometric.
Huy
Huy
why? when does one add al ?
12:58
@Secret back
@Secret I haven't looked at your proof yet, but afaik the direct proof is much simpler (as opposed to a proof by contradiction)
Why chose a proof by contradiction ?
I kinda forgot the sketch of the direct proof, i.e. do I start with a basis set {v1,v2,v3} and show that v4=linear combination of v1 v2 v3?

One reason I tried a proof by contradiction is I am trying to see "a set S of vectors with size > dim(V)" must lead to "linearly dependent" with no other possibility (e.g. is there exists a result that "linearly independent" such that "a set S of vectors with size > dim(V)" leads to "linearly independent"). Because if this is true then any assumption of other possibilities should lead to a contradiction thus disproving the existence of such possibilities
13:13
Oh for the direct proof you don't even need a basis
@Huy because "topologic" sounds weird.
Huy
Huy
who says that
ask any normal people
Huy
Huy
in German it's always algebraisch, topologisch, geometrisch
no complications
sorry I don't know any normal people
in german, though
13:21
@Secret Owait nvm :( give me a min
Indeed you need a basis but it's fairly simple
@Secret Have you seen matrices ?
yes i do
And the Rank–nullity theorem ?
@BalarkaSen hey
Suppose I have a smooth function $f:S^2\to M$, and I identify this with a function $f:\Bbb R^2\to M$ via stereographic projection from the north pole
If I give $\Bbb R^2$ the coordinates $(x,y)$, is there a reason why $\partial_xf=\partial_yf=0$ "at infinity"
13:31
@Secret Take a set {v1,...,v4} and the matrice A=[v1,...,v4] (the matrice whose columns are v1,...,v4) then its rank is less or equal to 3 by the rank-nullity theorem therefore the set is linearly dependant
You're restricting $f$ to $S^2 - p$ where $p$ is the north pole, and then composing with the homeomorphism $\Bbb R^2 \to S^2 - p$, that is to say?
@Hippalectryon By matrice do you mean matrix?
@0celo7 Ah yes my bad
@BalarkaSen Diffeomorphism, but yeah.
@0celo7 That's false in general, so I am not sure what you mean.
13:33
@BalarkaSen typo
I basically need $\partial_x f=\partial_yf=0$ "at the north pole"
Which is "at infinity" on the plane
Once $f$ is a function from a chart missing the north pole, I don't know what derivatives being 0 at north pole is supposed to mean.
You can probably put that point back by continuity
@Hippalectryon ok I understood the case where rank(A) < 3 (because then nullity(A) > 0 by rank nullity), but for the case where rank(A) = 3 would it cause a problem in that for the cases where rank(A) then the statement "a set of vectors of size > dim(V) where V is the vector space are always linearly dependent" will be false in general because there exists counterexamples in the form of matrices with rank 3?
@0celo7 That extends to the original map $f : S^2 \to M$. That may or may not have zero derivative on the north pole...
Soorry keep making that copy paste typo...
13:36
In that sense, it's false.
It's apparently supposed to have zero derivative, which is confusing me
Maybe your map is something specific.
No, it's general
@Secret I don't see the problem. When rank(A)=3 then by definition A has exactly three linearly independent columns
I don't know the context, so I can't help.
What you said so far is either vague or false.
13:38
You're right, it is vague.
But that's all I have
I might have to track down the paper they mention
OK.
I read a bit about framed cobordism from Milnor. Cool stuff.
Yup
I got back some motivation and started on Poincare-Hopf.
Now they invoke Riemann-Roch. I refuse to learn algebraic geometry, book
I have yet to decide if I want to follow Milnor's proof on that one or G-P's. I don't really like the Lefschetz fixed point theory business.
13:40
Milnor's proof is pretty sketchy at times, tbh
And it requires Morse theory
not so much Riemannian geometry
I take it back, you need geodesics
But nothing horrible like the variational theory
When rank(A)=3 then by definition A has exactly three linearly independent columns -> <insert a deduction or sentence> ->therefore since the set has 4 vectors, it must be linearly dependent

I am not sure if I overthink this, but somehow I felt I am missing a step in the logical flow
This Ricci flow book randomly invoked Morse theory on the path space
my face kinda looked like :S
Maybe it won't hurt to learn all of that but given the amount of prereqs it seems better to learn the apparently easier proof from G-P first.
13:42
yeah
Grr, I don't feel like reading Lefschetz fixed point theory.
@Secret By definition of the rank, if a matrix has exactly $n$ linearly independent vectors then it has a rank of n
I need more motivation for that.
why not?
also holy crap look at the time
If {v1,v2,v3,v4} was a linearly independent set then rank(A)=4
13:43
I am not sure. Maybe because studying fixed points for maps between manifolds doesn't excite me as much, but I am to blame for that, if any.
To fully understand this section it seems I need Shoen & Yau's book on Harmonic Maps
I am not ready for that
rip
Hi @JuanFran
hi @BalarkaSen
@BalarkaSen they use complex algebraic geometry and harmonic map theory to prove a sphere theorem
"rip" is then even more applicable
13:45
@Hippalectryon ok I thinnk I see it now, thanks
oh and the Hurewicz theorem
whatever that is
@Secret :-)
@0celo7 what is so surprising about this?
complex AG has very strong methods
I don't know anything about it
@0celo7 if $\pi_k = 0$ for all $k < n$, then $\pi_n \cong H_n$.
13:47
cf. Hatcher, I assume?
well, given $n > 1$.
Yep.
it's all in there
Something I find annoying about these sphere theorem things is that they always give the pinching constants as decimals
i think you Need an abelianization for n=1
0.87 seems really random
Yes, @Juan.
13:48
but it's probably the solution of $\tanh \pi x=\sin 2\pi x$ or something weird
$H_1$ is always isomorphic to $\pi_1^{ab}$.
very true. it might be this Statement to which the book is referring to
idk
i guess there are more theorems called "Hurewicz thm"
huh, odd, because this is the easiest version of the theorem
This proof is pretty crazy. They use existence theorems from harmonic theory, some AG theorem on complex line bundles, Poincare duality, universal coefficient theorem, Hurewicz theorem, morse theory
h cobordism
What is le theorem
13:52
true it is the easiest version, but it is very basic and useful
sounds like a good one, given the amount of machinery they use
@JuanFran sure, fundamental stuff are useful
so how do these things interact
i wanna see that proof
but I don't think it's worth giving it the name "Hurewicz theorem". it's just what homology is.
Let $(M,g)$ be a compact, simply connected Riem. manifold with dim $n\ge 4$. Suppose that $\mathrm{Riem}(\zeta,\eta,\bar\zeta,\bar\eta)>0$ for all $p\in M$ and all lin. indep. vectors $\zeta,\eta\in T_p^\Bbb CM$ satisfying $g(\zeta,\zeta)=g(\zeta,\eta)=g(\eta,\eta)=0$. Then $M$ is homeomorphic to $S^n$.
By Riem(...) do you mean curvature?
13:54
Riemann tensor
Yes.
Cool. Sounds like a nice theorem.
You use Morse theory to show that it's $(n-1)$-connected.
actually i don't find it surprising that a proof uses poincare duality and UCT. arguably these are the most useful general theorems
in particular, UCT just gives base change
Do we know something analogous for diffeomorphism?
13:55
so important in Algebra in general
Hey all
@BalarkaSen Yes.
Hi @Krijn
That's the point of this book, actually.
13:56
Let $(M,g)$ be a compact Riem. manifold of dimension $n\ge 4$ which is strictly $1/4$ pinched in the pointwise sense. Then $M$ is diffeomorphic to a spherical space form.
I don't know what "strictly 1/4 pinched" and "spherical space form" means, admittedly
Well, neither do I know what any of Riemannian geometry means, so...
Strictly $1/4$ pinched means the sectional curvature is in $(1/4,1]$ at each point
then there's a result about weak pinching, which is just $[1/4,1]$.
$\partial_t g(t)=-2\mathrm{Ric}_{g(t)}$
Such a simple PDE
simple?
highly non trivial!
14:05
Looks simple
true dat
but Ric, Riem, etc are quite nontrivial
I know
I've studied general relativity intensively
nice
i never bothered too, i guess lack of time
and if you understand the math behind it already it is probably less interesting
i guess most people start learning differential geometry because they want to learn general relativity, and not conversly
If you know Lorentzian geometry already, then you're a weird person :P
Lorentzian is so much different than Riemannian
For instance, there is no distance function to be obtained from the metric
true, but you can make up a generalization of both (just a general Framework, of course the results are different)
14:10
If you define the distance as an inf, you always get 0
If you define it as a sup, you generally get infinity
Studying when the distance function blows up is interesting
is it physically relevant?
Then there is the Geroch theorem, which is probably one of the coolest theorems
i mean what does it mean in physics
that this happens?
@JuanFran Eh
Our universe is thought to be pretty well-behaved
There is a conjecture which states the universe is globally hyperbolic
Which is a very boring topology
when i look up geroch's Splitting theorem
they mention "cauchy surfaces"
not sure how they made up that terminology :D
but it looks like a very nice theorem
14:14
It's from PDE theory
basically sayinig that space time is a sort of fibre bundle
i see
The usual way of thinking about it is that spacetime has a global time function
well PDE's is not something i know a great deal about
and that allows you to split it into a "time" and "space" in a topological sense
@JuanFran Basically, if you know the metric and its derivatives on a Cauchy surface + boundary conditions, you can solve the Einstein equations
well that is something i actually find very interesting
it is the sort of physics i can understand (i.e. maths :D )
14:16
+ stuff about matter fields
@JuanFran there are 3 kinds of GR books
books for physicists
books for mathematical physicists
books for mathematicians
My favorite book of all time falls in the first category.
which one? dirac's ?
The third category is pretty dry, honestly.
@JuanFran Zee's
hmm some Problem with the third category is
14:18
10
A: Getting started self-studying general relativity

0celo7This list is extensive, but not exhaustive. I am aware that there are more standard GR books out there such as Hartle and Schutz, but I don’t think these are worth mentioning. Books with stars are, in my opinion, “must have” books. (I) denotes introductory, (IA) denotes advanced introductory, i.e...

I have a list of books I think are good
that when i would look at their mathematical discussions, i would probably get very mad
Why
i like maths the bourbaki style
elegant, neat, coordinate free
but an interesting list you got there
In differential geometry coordinate cannot be avoided, period
it seems like no one reads the only GR book i own
i.e. dirac's :D
14:20
@JuanFran The third category is written by mathematicians.
it is very short
what you mean by that? it cannot be avoided?
There are things which cannot be proven without coordinates in differential geometry
obviously you cannot do calculations without them
give me an example!
For instance, I'd be very surprised if you can show that the dimension of the tangent space is the dimension of the manifold without coordinates
thats probably true
14:22
:D
but this is because the dimension of a manifold
is basically defined via coordinates
You can probably define it via homology or something stupid
yeah via H_n(X,X-{x},Z)
but only for closed manifolds
There you go
which is Kind of sad
14:24
How about showing that geodesics always exist, locally
You need coordinates to write down the geodesic equation in a chart
true
well the very nature of a manifold gives you coordinates
so you cannot avoid it entirely
but when you can, i find it preferable
I don't see any shame in using coordinate for proofs
how would you define the tangent space?
me neither, but i just don't find it appealing
Oh, the tangent space is easy to define without coordinates
It's the vector space of derivations of germs of functions
But you need coordinates to show that this is spanned by the partial derivatives
yeah, i was just interested which definitiion you would give me
i mean you can also define it via coordinates
14:27
I like the algebraic one
pretty ugly and cumbersome
@JuanFran Yeah
me too
it actually works for any locally ringed space :D
But that's how Hirsch does (coordinates) it because it's the one that works on $C^r$ manifolds, $r<\infty$.
The algebraic definition fails in the non-smooth case
Which is probably my favorite factoid of all time
it also Fails for complex manifolds i think
14:29
I doubt that
The complex tangent space is the complexified tangent space of the underlying real manifold
I think
let me find a reference
what are we talking about
I'm right, according to Jost
i think there is one Definition of tangent space
which Fails for complex manfiolds
In my mind, the complex tangent space is the complexified real tangent space
So as long as the manifold is smooth, the algebraic definition works
14:32
yeah, i think the Definition i had in mind is a derivations of C^infty(M) at that points
I don't understand the craze about coordinate freeness. Whenever coordinates are elegant, use them. Whenever coordinate free things are elegant, use them. Done.
@JuanFran I think that fails hard for C^k manifolds, no?
when are coordinates elegant?
I already told him that, @BalarkaSen
you were quite right about that @0celo7
14:34
actually i admitted it before :D
@JuanFran Elegant for understanding, not for conciseness. I understand differential forms better coordinate-wise than sections of the exterior product bundle.
i said the Definition works for any locally ringed space
and of course a complex manifold is a locally ringed space
The most physicist proof of all time right there
i understand them as the exterior Algebra over the 1 forms :D
@JuanFran That completely subsumes the geometric content for me.
14:36
well the geometric content is contained in the 1 forms
covector fields
Depends on what you mean by that.
sections of the cotangent bundle
No, I mean, what do you mean by "geometric content"?
surely covector fields have a very vivid geometric intepretation?
or not?
Sure, but I am asking: what does differential form mean to you?
What do you mean when you say "geometric content"?
14:38
something i have a geometric picture of. vector fields are just functions assigning arrows
in the most primitive sense
and differential forms are just induced by them via natural algebraic constructions
basically my Definition makes this clear
OK, I do not see how that is a useful geometric interpretation. But each to his own, maybe you think algebraically.
Naturally thinking algebraically is totally fine.
so how is the coordinate stuff more useful as a geometric Interpretation?
i mean you think of a differential forms assinging to each point some mulitlinear alternating map
how is that different from what you say?
in your geometric interpretation
you can*
I think of differential forms as something which eats infinitesimally small parallelograms and spits out their signed area :) This is also easy to see from the section definition, but only becomes apparent - I repeat, to me - when I look at it via coordinates.
The coordinate-free definition is a nice and concise packaging of that to me.
i see, yeah well i think our interpretations are quite similar
i just stated them more fancily
in the most primitive way i would say
differential forms is what you integrate over :D
not very convincing, but it is essential
@JuanFran Which distinguishes our thinking style, I think :)
Yes, that you can integrate over them becomes apparent to me from the parallelogram thing I said.
14:44
might be very well
i think what is nice about my interpretations (and this is what i just noticed now) is how it puts the focus on vector fields
oftentimes students find differential forms harder to understand than vector fields
i basically say vector fields+natural algebraic construction = differential forms
i guess these students just have Problems with natural algebraic construction :P
Tensor fields are precisely parametrized version of "infinitisimally small parallelograms" :)
so to speak yeah
Mathwise, given $n$ vector fields $X_1, \cdots, X_n$ on $M$, at each point $X_1(p), \cdots, X_n(p)$ span a parallelogram at $T_p M$.
haha did you star my message?
you know 3 references, but how does the proof work? - 2d ago by Juan Fran ▼
:D
14:51
ok ok, i just thought. it somehow appeared on the board
i recently had an amusing discussion
with someone claiming that number theory is "by far" the hardest subject in math
turned out he did a phd in number theory, expected
not sure why people always think their own subject is the hardest
To make themselves look smarty
mostly this is just due to ignorance about other subjects
god forbid krijn!
@JuanFran Probably it's true.
From some point of view.
well it seems that every subject is the hardest
"Hardest" is probably a wrong choice of word. "Vast" or some such would have been more appropriate.
14:54
from some pov
imo both the hardest and most interconnected subject is algerbaic geometry :D
but i might be wrong haha
@BalarkaSen what the hell
Oh
Never mind
@JuanFran they do?
15:00
assign to each vector it's length (a number in general)
what are you referring to?
For higher forms what Balarka said makes sense
But I've never had a feeling for covectors
but you have a feeling for the dual space?
Not geometrically
it is just a vector field
in a parallel universe :D
15:05
it's easier to visualize covectors than the whole dual space
What's a covector
ELI5
a thing which assigns a number to a vector.
yikes i should get back to studying
procrastinating for too long
@BalarkaSen so?
Is that supposed to be a geometric interpretation?
The only one I've heard is the "egg crate" one
Which is terrible
15:38
vote for reopen this question math.stackexchange.com/questions/1883064/…
@BalarkaSen help me
Not even a please?
@0celo7 I was in a hurry at that time, so missed it
yes please vote for re-open that qes
15:55
@Agawa001 It's not plagiarism. They both evolved from a common ancestor.
 
2 hours later…
17:54
Guys, I'm doing calculus (or analysis, I don't know which) and I've encountered the "Cauchy Criterion"
And whenever there's a problem based on it, my profs use the "contractive criterion" to solve the problem instead
And I've seldom been able to come up with solution, using the statement of the Cauchy criterion, for such problems, myself.
So, do you know of some problems, solutions or links where the cauchy criterion can be directly used to examine convergence?
Or is it totally useless?
Thanks in advance

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