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12:21 AM
@ArnoldFernández Without computer, you can e.g. find the global minimum of x^8-x^5 and x^2-x separately (which is -15*cuberoot(25)/256 and -1/4 respectively, you can find it by differentiation), and show that sum of the two plus 1 is higher than zero. Therefore the global minimum of the original function must be positive too.
 
Whitot differentation?
 
 
1 hour later…
1:27 AM
I just read that every compact, connected 2-manifold can be covered with only 3 charts. Insane.
 
2:00 AM
@ArnoldFernández You can convert the function to the sum of squares (x^4-x/2)^2 + (x/2-1)^2 + x^2/2, which can't be negative. To show it cannot be zero, show that x/2-1 and x cannot be zero at the same time (which is trivial).
 
I'm confused by en.wikipedia.org/wiki/… when it says, "Sometimes, it is more convenient to deduct backwards, proving the statement for $n - 1$, given its validity for $n$. However, proving the validity of the statement for no single number suffices to establish the base case; instead, one needs to prove the statement for an infinite subset of the natural numbers."
I was trying to find out if mathematical induction can work by (using the ladder analogy) proving an arbitrary rung $r$, proving that an arbitrary rung $k$ above $r$ entails $k + 1$, and proving that an arbitrary rung $j$ below $r$ entails $j - 1$. Basically, sawing the (possibly bidirectionally infinite) ladder into two ladders such that $r$ is both the bottom of one and the top of the other. But I don't think that's what it's saying?
 
2:22 AM
@Bubbier how you get that idea?
 
2:50 AM
@Thorgott Why insane? Take the polygonal representation of surfaces; use the interior as one chart, and a chart containing the vertices and half of the edges for the second, and a chart containing the remaining half of the vertices third, or something like this. You can draw the picture for the torus or genus 2 guy without much difficulty
 
What area of mathematics are polytopes most commonly found in?
Is that something one would learn studying mathematics in undegrad or graduate school? or is that a niche topic?
 
3:18 AM
@robjohn it is a bit of complex!
and how did you derive that?
 
3:44 AM
@StanShunpike you'd see polytopes showing up in toric geometry
 
 
1 hour later…
4:58 AM
@Thorgott A modified version of Mike's atlas that I like is throwing away a wedge of circles from a genus g surface, which gives a chart, throwing away another distinct collection of wedge of circles, which gives the second chart - you now miss 2g points, which you join by a path and take a tubular nbhd
Three charts
The minimal number of R^n charts needed to cover is called the Lusternik-Schnirelmann category
(Or LSC - 1, there's some convention)
This number is still 3 for a non-orientable compact surface
Only 2 for S^2
 
5:15 AM
It's still 3 for an orientable surface of infinite genus.
 
5:30 AM
Take this 2D complex $X$, and consider folding it to a 2-simplex according to the folding scheme indicated. This gives a map $X \to \Delta^2$ which has 3 fold lines (the Z shape in the interior) and two cusp points (the two kinks of Z).
Taking a cone on this we obtain a simplicial map $\Delta^3 \cong CX \to \Delta^3$ from a subdivision of the 3-simplex to the 3-simplex which folds along a $C(\mathsf{Z})$, a fold surface consisting of two cuspidal lines that meet at a point $v$, the cone point of $CX$.
This is the local simplicial model of a swallowtail singularity
This provides a triangulation near the worst singularity of $f : \Bbb R^3 \to \Bbb R^3$, $f(x, y, z) = (x^4 + yx^2 + zx, y, z)$, say, and it's easy to extend this triangulation to a triangulation of the whole mapping $f$.
This is the Thom-Boardman singularity $\Sigma_{1, 1, 1}$ if I am not wrong
 
5:59 AM
How do you put a pciture?
 
6:41 AM
@Yuvraj I noticed a mistake. It might be more complicated, or possibly simpler. I am working through the correction.
 
 
3 hours later…
9:45 AM
I appreciate the explanation even though I don't really get it
 
Do it for the torus, eh? Let $m_1, m_2$ be two distinct meridians, $\ell_1, \ell_2$ be two distinct longitudes. $U_i := T^2 \setminus (m_i \cup \ell_i)$, $i = 1, 2$ are both homeomorphic to $\Bbb R^2$, and $U_1 \cup U_2 = T^2 \setminus \{p_1, p_2\}$ where $p_1 = m_1 \cap \ell_2$, $p_2 = m_2 \cap \ell_1$
Let $\gamma$ be a smooth path joining $p_1, p_2$, and let $V$ be a $\varepsilon$-neighborhood of this path, which is gonna be homeomorphic to $\Bbb R^2$. $\{U_1, U_2, V\}$ is an open cover of $T^2$
 
10:06 AM
@Balarka I did my homework, around a month ago you mentioned that every compact metric space of dimension $n$ embeds into $\Bbb R^{2n+1}$. In fact compact is overkill, separable metrizable of dimension $n$ is enough. This is due to Menger–Nöbeling, the idea is that they all embed into the Nöbeling space, the subspace of $\Bbb R^{2n+1}$ with at most $n$ rational coordinates
 
Oh shoot
 
There's also some nonsense result that all strongly metrizable metric spaces of weight $\kappa$ and dimension $n$ embed into $\kappa^\omega\times N_n$ where $N_n$ is the Nöbeling space in $\Bbb R^{2n+1}$
 
what is weight
 
Where strongly metrizable means something weird like metrizable with a basis consisting of a countable union of star finite coverings or metrizable+completely paracompact
 
Ugh
 
10:15 AM
@BalarkaSen smallest cardinality of a base
 
Ah OK
 
Yeah that's just ugly
But I want to go through the proof for the separable metric case
 
Tell me the key ideas if you understand it
 
oh, I see, that makes sense
 
10:21 AM
Can you prove $T^2$ cannot be covered by two Euclidean charts
 
cutting along a meridian + longitude essentially undoes the gluing done when you construct the torus from a square
 
Yep
 
Oh no, the proof for the nice case is to do the general case, embedding into $\omega^\omega\times N_n$ (since separable implies second countable for metric spaces) and then showing that the embedding built in the proof of the general case is actually constant in the first coordinate in the special case
I need to find a different book that does only the special case lol
 
Lmao
 
10:34 AM
@Thorgott Follow-up (Challenging): Prove that there is a function $f : T^2 \to \Bbb R$ with exactly three critical points (Why is it a follow-up?)
There is a function with exactly 4, the height function on an upside down donut - classic Morse theory picture
You cannot improve to 2, by Reeb's theorem :)
 
Engelking has a much saner proof. Actually it seems that embedding into $\Bbb R^{2n+1}$ rather than this Nöbeling space is much easier and a BCT trick
 
Gotcha
 
It's lunchtime now but I think I can tell you more later
 
That'd be great!
Enjoy
 
Please I need help how to prove that $\lim_{x\to-\infty}x^n\exp(x)=0$
I need idea
 
10:46 AM
Is this vector field conservative ?
I tried to draw closed loop around center to see work done to reach initial point to again same point .
0
Q: vector field property using figure

maths student Is this vector field conservative ? I tried to draw closed loop around center to see work done to reach initial point to again same point .This is same as checking line integral along closed path is 0 or not.

 
11:14 AM
Still here? @Balarka
 
I thought I figured something out, but I just realized you wanted 3 critical points, not values..
urgh, I think messing around with projections isn't enough to do this
 
11:36 AM
Yeah it's quite hard
@Alessandro Yup
 
Ok so to prove that all separable metric spaces with $\dim X\leq n$ embed into $\Bbb R^{2n+1}$ we need three ingredients, one is easy, one is technical, one is needed to go from compact to separable
A function $f:X\to Y$ between metric spaces is called an $\varepsilon$-map if $\mathrm{diam}(f^{-1}(y))<\varepsilon$ for all $y\in Y$
So now let's assume that $X$ is compact so that $Y^X$ is a metric space with the metric induced by the sup norm. The easy ingredient is that for all $\varepsilon$ the set of $\varepsilon$-maps $X\to Y$ is open in $Y^X$
 
Ya OK
 
The technical ingredient is that if $\dim X\leq n$ and $H$ is an $n$-dimensional linear subspace of $Y=\Bbb R^{2n+1}$, then the set of $\varepsilon$-maps that miss $H$ is dense in $Y^X$
(We don't really care about $H$, we only care about the set of $\varepsilon$-maps being dense)
 
Ah so it's the same trick as the manifolds thing
 
But now we are done, let $X$ be compact with $\dim X\leq n$, for every $i$ consider the set $U_i$ of $1/i$-maps $X\to\Bbb R^{2n+1}$, by the previous two things every $U_i$ is open dense in $Y^X$, which is baire, so $\bigcap U_i$ is dense (in particular nonempty), but every element of the intersection is a continuous injection $X\to\Bbb R^{2n+1}$, hence an embedding
So not only there is an embedding $X\to\Bbb R^{2n+1}$, there's plenty of them, they form a dense $G_\delta$ set in the space of all continuous functions $X\to\Bbb R^{2n+1}$ (if $X$ is compact)
 
11:48 AM
Hm, not quite
Cool proof
 
To get the separable case there is a result saying that a separable metric space $X$ with $\dim X\leq n$ has a metrizable compactification $cX$ with $\dim cX\leq n$
@AlessandroCodenotti The hard part is showing this
The $n$-dimensional subspace thing is there to get embeddings into the Nöbeling space. If $N_n$ is the subspace of $\Bbb R^{2n+1}$ of points with at most $n$ rational coordinates then we can write $\Bbb R^{2n+1}\setminus N_n$ as a countable union of $n$-dimensional linear subspaces (those given by equations $x_{i_1}=q_1,\ldots,x_{i_{n+1}}=q_{n+1}$ for rational $q_j$) and use as $U_i$ the $1/i$-maps missing the $i$-th element in an enumeration of those linear subspaces
So $N_0$ is the space of irrational numbers, which is then universal for $0$-dim separable metric spaces. The Cantor space $2^{\Bbb N}$ is also known to be universal for $0$-dim separable spaces, and just like the Nöbeling spaces generalize the irrational there is also a family of higher dimensional universal spaces generalizing the Cantor space due to Menger
(That's where the Menger sponge comes from)
 
12:03 PM
lol
 
This will take nontrivial effort for me to understand. I get the outline you explained, though. Thanks!
Weierstrass preparation theorem seems like a technical result
I have been staring at a proof without getting anything out of it for last 2 hours
 
I got the impression that every result in several complex variables is a technical result
 
Skip Weierstrass and just prove Malgrange
 
that's what I am interested in but it seems that they borrow ideas from Weierstrass
maybe thats an illusion
 
Do you actually need Malgrange for something
 
12:14 PM
Apparently its crucial for classification of singularities of map-germs
 
Huh
I guess that makes sense
 
The algebra formulation of Malgrange preparation theorem is that if $f : (M, p) \to (N, q)$ is a smooth map-germ, $A$ is a finitely generated $C^\infty_p(M)$-module, then $A$, under basechange by $f$, is a finitely generated $C^\infty_q(N)$-module iff $A/\mathfrak{m}_q(N)A$ is a finite dimensional real vector space
 
weird
 
 
1 hour later…
1:43 PM
@Balarka can that 3 critical point function be Morse?
I'm wondering whether it's possible to build a torus by two handle attachments
 
Nope :)
Good question though
You're correct to wonder about what having 3 critical points would mean in the sense of handle attachments
 
I'm wondering what it means generally, one ought to be a global minimum, the second a global maximum and the third is ???
 
You know the Morse lemma, right?
 
@Balarka apparently the 2n+1 bound in the dim X=n comes out of the fact that the nerve of a cover with multiplicity n can be realized as a simplicial complex in $\Bbb R^{2n+1}$
 
@Alessandro That makes sense, actually. What is the homeomorphism, though?
 
1:57 PM
Which homeomorphism are you talking about?
 
You need to embed $X$ in $\Bbb R^{2n+1}$
 
@AlessandroCodenotti it's here, any element of the intersection will do
 
So far I can see a Lipschitz map to the nerve by squishing stuff in the open sets to points and edges and faces etc, which embeds in $\Bbb R^{2n+1}$
 
The thing is that functions in the intersection are $1/i$-maps for every $i$, so they must be injective, and continuous injection from compact to Hausdorff is an embedding
 
I didn't see the nerve in the outline you wrote
 
2:01 PM
that's only for non-degenerate critical points though, right
 
@Thorgott Ah but you were trying to decide if the function can be Morse, right?
 
though I guess the third one could be non-degenerate and the global min/max degenerate
 
@BalarkaSen No that comes up to prove the technical bit
 
I see
 
To prove it you use that map, but you need to argue that you can place the vertices of the simplices close enough to get an $\varepsilon$-map
 
2:02 PM
@BalarkaSen Surely that's relevant for constructing these 1/i-maps
yeah
 
And you also argue that you can place them in a way that misses an $n$-dimensional linear subspace apparently
 
I didn't pay too much attention because I didn't understand it, but makes sense
I only vaguely get it anyway
 
What's the convex hull of the twisted cubic
 
I haven't read all the details, it's a longish proof relying on a bunch of previous lemmas, so I'm still working my way through it
 
@MikeMiller Twisted cubic is what you get if you blowup $y^2 = x^3$ at the origin. So the image of everything in the inside of that curve by the inverse (well-defined away from origin), right
That might give a geometric way of understanding why segments with distinct pairs of endpoints are disjoint
The endpoints always have different direction data or something
 
2:14 PM
Hmm, I guess it comes down to whether one can glue together two spheres to get a torus (and that shouldn't be possible)
 
@robjohn any improvement?
 
@Thorgott This is in reference to if you can cover it by 2 R^2's?
 
@Yuvraj it turns out that the weights are the reciprocals of what I had before. Just checking to make sure.
 
@robjohn it will be very kind if you can help me in understanding it's derivation , once you have finished?
 
Eh, I confused things. It's in reference to handle attachments. I start with a 0-cell and since a graph can't be a 2-manifold, there's gotta be a 2-cell involved. The first attachment can be done in only one way in either case. So it comes down to a) can we glue a disk along the boundary to a circle to get a torus or b) can we glue a disk along its boundary to another disk to get a torus.
 
2:24 PM
@Thorgott I'm confused about your setup. You have a function $f : T^2 \to \Bbb R$, $f$ has three critical points?
Each critical point contributes to a handle/cell - so you should be playing around with three handles/cells
Assuming $f$ is Morse and trying to get a contradiction from there, that is to say
 
isn't the first attachment just the 0-cell
no wait
this is nonsense
 
No that's correct. A Morse critical point of index k corresponds to a k-cell.
For k = 0 (i.e., the minimum) you add a 0-cell
(The standard height function T^2 -> R has four critical points, of index 0 (min), index 1 (first saddle), index 1 (second saddle), index 2 (maximum) - which thus says there's a CW structure on T^2 with a 0-cell, two 1-cells and a single 2-cell. That's correct!)
This naive analysis does not say how the cells are attached, but you indeed can get a T^2 from attaching two 1-cells to a 0-cell (only way to do this here - gives you $S^1 \vee S^1$) and attaching a 2-cell to this $S^1 \vee S^1$ - you don't know what this attaching map is from naive analysis but you know gluing by $aba^{-1}b^{-1}$ gives $T^2$
Agreed?
 
agreed except I'm not sure what you mean by "gluing by $aba^{-1}b^{-1}$". Is this in terms of fundamental groups?
 
Exactly, that describes how the 2-cell is glued to $S^1 \vee S^1$ completely. The 2-cell is a disk, whose boundary is a circle, so it must be glued to $S^1\vee S^1$ by some map $S^1 \to S^1 \vee S^1$. In fact, (fact:) homotopic maps give homotopy equivalence CW complexes upon attachment, so it suffices to specify the homotopy class of this map, an element of $\pi_1(S^1_a \vee S^1_b) = \langle a, b \rangle$, the free group on two generators. I claim this element is $aba^{-1}b^{-1}$
This can be seen from the square identification picture, because $S^1_a$ is the image of one edge of the square and $S^1_b$ is the image of the adjacent edge.
The 2-cell is the interior of the square, which is thus attached to $S^1_a \vee S^1_b$ by exactly the gluing scheme of the square, which is $aba^{-1}b^{-1}$
 
2:46 PM
oh wow, that sounds like a great picture
 
Thorgott, a function $f$ doesn’t have any local maxima and minima, then can I say the function is monotonous ?
 
A monotonous function is boring
 
Really?
So, my above conclusion is true?
 
I'm doubtful of that tbh
 
2:55 PM
About Balaraka’s joke or my statement?
 
I feel there should be a counterexample, but it would be really ugly
 
@BalarkaSen If I were a rude man I would have flagged it by saying “you have called me a joke” :-)
 
Lmao
That's not what the gif is saying
Hilarious
 
@Thorgott So, what special property the function $f$ have ? (Given that it doesn’t have any local maxima and minima)
 
It's the joke_over_you.gif going over you
 
2:57 PM
@BalarkaSen LOL
 
oh wait, the Dirichlet function works as counterexample
 
Balaraka did you study Loney’s Elements of Coordiante Geometey ?
 
wait nvm
urgh, this is ugly
$f(x)=x$ if $x$ rational and $f(x)=1-x$ if $x$ is irrational
 
Just consider a piecewise function which goes up, stays constant in $[-1, 1]$, dips down
 
Well, my problem is that it is written that “solutions to Laplace’s Eqaution results in a function that have no local maxima and minima”
 
3:00 PM
that has a lot of local minima/maxima
we're not specifying them to be strict
 
Local max/min means strict local max/min to me. Knight needs to clarify
 
What is strict maxima/minima ? Maixima/minima are the places where derivative is zero
 
Lol, i give up
 
uhhhhhhhhhhhhhhhhhhhhhhhhh
no
that is not what a maximum/minimum is in any sensible way of thinking about it
however, the statement that a differentiable function R->R with non-zero derivative everywhere is monotonous is true
cause the derivative has to have constant sign by Darboux
no local minima/maxima + continuous also implies monotonous on connected domains
 
3:17 PM
@Balarka if $M$ is a compact smooth manifold, what does $C^\infty(M,\Bbb R)$ look like as a subspace of $C(M,\Bbb R)$?
 
Like you Dense
 
Right, by Weierstrass
Is it $G_\delta$ though?
I'm wondering whether Whitney embedding also gives a result similar to the dimension $\leq n$ embedding, meaning is there some result of the form "the set of smooth embeddings $M\to\Bbb R$ is dense/G_\delta/somewhat big in $C^\infty(M,\Bbb R)$"
 
Nah I don't think it's $G_\delta$
I think $C^1$ already isn't. $C^1(M,\Bbb R)$ should be already $\prod^0_3$ in the Borel hierarchy as a subspace of $C(M,\Bbb R)$
 
3:33 PM
Is there any compuationally efficient invertable mapping form {1, 1, 2, 1, 2, 3, 1, 2, 3, 4, .....} to {1, 2, 3, 4, 5, 6, ...}?
You can think of it as mapping a triangular matrix to it's the memory efficient form.
I need a fast way to compute the [i][j] index in the matrix from an element's linear memory location.
The matrix is stored as a[0][0],a[1][0], a[1][1], a[2][0], ... linearly. Assume it's a lower triangular matrix.
computational efficiency order: additions > multiplication >>> division = modulus
 
You should really write in your first thing {(1,1), (2,1), (2,2), (3,1), (3,2), (3,3), (4,1), ...}, otherwise who knows how to distinguish between all the different things you call "1"? In this notation, your map is (m,n) -> (m-1)(m-2)/2 + n.
How large are your matrices?
To go from k to the corresponding (m,n), you first need to identify the largest triangular number $T_{m-1}$ less than $k$, at which poinst $n = k - T_{m-1}$
A pretty hackish approach (I know nothing about computational algebra) would be to store a list (m, (m-1)(m-2)/2) --- then you could compare k to the triangular numbers on this list, and you've already stored the information of what m corresponds to that triangular number
 
@AlessandroCodenotti Huh how do you prove this? I have no clue
 
@AlessandroCodenotti If $N$ is a smooth manifold and $\dim N > 2\dim M$, then the space of smooth embeddings is dense in $C^\infty(M,N)$
Of course embeddings aren't dense in $C^\infty(M,\Bbb R)$ for $\dim M > 0$ --- there are no embeddings for dimension at least 2, and in dimension 1 you would be saying "maps with f' > 0 are dense in all maps", which is preposterous
 
Yeah sorry, $\Bbb R$ was supposed to be $\Bbb R^{2n+1}$
 
@MikeMiller They aren't matrices actually. I just rephrased my actual problem as a matrix storage problem thinking it would be easier to understand. I am writing a GPU program for performing non-max suppression. I have an array of boxes and I need to compute intersection area of every pair of boxes. Intersection area of two boxes is commutative. So I need to compute n(n - 1)/2 areas only. To do this I need to map linear thread ids to two box ids.
 
3:46 PM
@MikeMiller But this answers it, do you have a reference where I can read about this?
 
I'm sorry to tell you these words are mostly meaningless to me. :) Does my comment help you in your situation at all? (I'm not even sure if it would be an efficient approach in the matrix case.)
@AlessandroCodenotti Hirsch, but I could also just explain without much difficulty
 
If you want to and have the time do so I'll be very happy to listen
 
Open dense, I should have said
 
@MikeMiller I need a fast inverse computation. Need to go from (m - 1)(m - 2)/2 + n to (m, n). You can lay it out in any fashion: {(1, 2), (2, 2), (3, 1)...}. I need a one-to-one mapping from every pair of boxes to a linear index. I need a really fast way to compute (m, n) from the linear index.
 
Got it, very clear. Thanks.
I assume "list off the triangular numbers ahead of time and check which is smaller than (m-1)(m-2)/2 + n" is an awful idea, then.
 
3:50 PM
@Alessandro A modification of the argument here will prove it
I didn't realize that was your question, I got thrown off by $\Bbb R$
 
@BalarkaSen Yeah that made no sense, sorry
Uh a long answer, let me read it
 
No don't read it
@AlessandroCodenotti A smooth immersion is a map $f: M \to N$ so that $Df: M \to f^*T^*N$ has no zeroes; a smooth embedding is a smooth immersion so that $(f,f): M \times M \to N \times N$ misses the diagonal.

As soon as $\dim N \geq 2\dim M$, the first is equivalent to: "$Df$ is transverse to the zero section". As soon as $\dim N > 2\dim M$, the second is equivalent to: "$f \times f$ is transverse to the diagonal."
 
Let me define it formally. S = {1, 2, 3, 4, ..., N} is an index set. I need a one-to-one function that maps every pair of indices in S to another index set Q = {1, 2, 3, ...., N(N - 1)/2}. That is, I need a function f : (m, n) -> k where m, n belongs to S and k belongs to Q. Ideally, m != n but it's ok if m = n (these happen relatively less often).
 
@BalarkaSen let's do $X=C([0,1],\Bbb R)$. The trick is that a function $f\in X$ is $C^1$ iff for all rational $\varepsilon >0$ there are intervals $I_0,\ldots, I_{n-1}$ such that for all $j<n$ and for all $a,b,c,d\in I_j\cap\Bbb Q$, $|(f(a)-f(b))/(a-b)-((f(c)-f(d))/(c-d)|<\varepsilon$
 
Transversality conditions are open and dense conditions by the usual arguments, so in these dimension regimes, the properties of being a smooth immersion or smooth embedding are open dense properties
 
3:53 PM
@MikeMiller You need immersions are dense before this, but that can also be achieved
This is the summary of my argument in the answer
Ah you dealt with immersions being dense
 
I am being a bit sloppy because $Df$ depends on $f$ and is not an arbitrary map
 
You need 1-jet prolongation of $f$, mapping to the jet space
 
But the usual arguments still go through
 
So if $A_{j,\varepsilon}$ is the set of $f\in X$ for which that inequality holds for all $a,b,c,d$ in $I_j$, it turns out that $A_{j,\varepsilon}$ is closed and $$C^1=\bigcap_{\varepsilon\in\Bbb Q^+}\bigcup_{n\in\Bbb N}\bigcup_{I_0,\ldots,I_{n-1}}\bigcap_{j<n}A_{j,\varepsilon}$$
 
Gotcha
Wait no what's wrong with the outline I presented
 
3:54 PM
That was awful to type, it's an example in Kechris
 
This shows that $C^1([0,1])$ is $\prod^0_3$ in $C([0,1])$, I don't know how to show it's not already a simpler set
 
honestly what's right with the outline I presented
 
I was referring to you being sloppy with $Df$. You need to move $Df$ around somewhere; I am saying you should move in in the jet space
It's essentially correct
 
Hm I'm not very familiar with transversality, but I see the idea, thanks!
 
3:56 PM
beautiful formula
 
@AlessandroCodenotti Ahhh I see this is great
That's a nice trick
I don't know how to show it's not somewhere below the Baire hierarchy either
 
Those kind of arguments are often trying to replace the condition that defines your set with countably many uglier conditions
 
Yeah
I have used these tricks before in trying to investigate points where a function is not continuous, never farther up the Baire hierarchy though
This is nice
 
I've seen such things pop up in measure theory
 
Right that's also a classic example, instead of saying "$f$ is continuous at $x$" you have the countably many conditions "$f$ has oscillation below $1/n$ for every $n$ at $x$"
To get continuity on a $G_\delta$
 
4:01 PM
Where in the B heirarchy do open dense sets lie
 
they are the lowest level, $\Sigma^0_1$
$\Sigma^0_1$ is open, $\Pi^0_\xi$ is complement of sets in $\Sigma^0_\xi$, $\Sigma^0_\xi$ is sets $X$ which can be written as a countable union of sets $X_i\in\Pi^0_{\beta_i}$, where $\beta_i<\xi$ for all $i$.
 
you can also express convergence that way
from there it follows that the set of points where a sequence of measurable functions converges is measurable
 
So for example $\Sigma^0_1$ is open sets, $\Pi^0_1$ is closed sets, $\Sigma^0_2$ is $F_\sigma$ sets, $\Pi^0_2$ is $G_\delta$ sets
 
How do I write a cartesian product which doesn't have reflexive elements in set notation? I have an index set S. I need the set that consists of all pairs from S but not (a, a) elements.
 
it also appears in the proof of LLN
 
4:05 PM
Oh and $\xi$ goes up to $\omega_1$
In Polish spaces that is
@Thorgott LLN?
 
@Thorgott Yeah that's another B hierarchy but a different B - Borel instead of Baire
 
the set of tuples of the form $(a,a)$ is usually called the diagonal of that product and denoted $\Delta_S$, so what you want can be called $(S\times S)\setminus\Delta_S$ @Yashas
@Alessandro law of large numbers
 
Oh, weird
@AlessandroCodenotti something similar should also work for $C^2$ right? Write more "nested incremental ratios" to approximate the second derivative
 
@Yashas Well, what I was suggesting was a perfectly well-defined function, just not one given in terms of addition and multiplication etc. A perhaps faster approach than previous is that you know that $m$ is either $\lfloor \sqrt{2k} \rfloor$ plus one or plus two. Then you can check which it is by actually computing m(m-1)/2.
 
It's essentially just $\{\omega\colon\lim_{n\rightarrow\infty}\frac{1}{n}\sum_{i=1}^nX_i(\omega)=0\}=\bigcap_{m\ge1}\bigcup_{N\ge1}\bigcap_{n\ge N}\{\omega\colon\left\vert\frac{1}{n}\sum_{i=1}^nX_i(\omega)\right\vert\le\frac{1}{m}\}$
 
4:11 PM
Yeah convergence in probability should be written explicitly like that
 
then you can complement and apply Borel-Cantelli to the inner two expressions
well, depending on how many finite moments you presuppose
the most general case requires more technicalities
 
SLLN is pretty terrible to prove
You go to like fourth moment, and then truncate shit
 
if you suppose finite fourth moment, it's not bad
 
I never understood the truncation trick I think
No I am not supposing anything
 
you should suppose finite first moment
cause that's an iff
 
4:14 PM
Expectation is finite, otherwise the statement is nonsense :P But in general you truncate so that everything has finite fourth moment
See here, section 2
 
right
 
Never understood that
Horrible estimates
 
I've looked at the general case once, but I never fully grokked it
 
@MikeMiller Turns out that is a difficult problem and people write papers on it :D
 
it was the definitive indication for me that i will never be able to do probability
 
4:18 PM
probability is weird
 
I don't understand how people estimate man
How do you do that
 
reminds me, did you ever end up taking a look at the Janson-Suen inequality
 
Oh fuck yes
 
that was some real "how do people estimate"
 
it's like LLN for weakly dependent RVs, or am i misremembering?
 
4:21 PM
it was like a version of Chernoff for dependent RVs
 
gotcha
 
with a bunch of super weird hypothesis that I'm forgetting
something about dependency graphs
 
Lmao
its coming back now
There was that weird shit wait
Lovasz local lemma
 
I did work through the proof fully, but, as you are witnessing now, I didn't retain much of it
 
WTF
 
4:22 PM
Thorgott why you gotta give him PTSD attacks like that
 
@Thorgott that happens to me, that's why i gave up on probability
 
it's in my nature to make you all suffer
I am now equipped to say something more about the categorical construction from yesterday
 
Probability is a very efficient and effective way to reach that goal
So is category theory lol
I'm leaving. (I actually needed to leave anyway, the timing is just a fitting coincidence)
 
i remember pictures, i can't remember $\Bbb P(|S_n/n - \mu| \geq \varepsilon) \leq \Bbb E(|X|^2/n \Bbb{1}_{|X| \leq M})/(\epsilon/2)^2 + \Bbb E(M \Bbb 1_{|X| > M})$
 
haha see you
 
4:25 PM
Cya @Alessandro
 
I wlll say something about colax-slice 2-categories some day
that bound looks familiar
I think you use this to prove Weierstrass approximation probabilistically or sth
 
Weierstrass approximation follows from LLN type things yeah
LLN for $f(X)$ where $X$ is binomial or something
 
yeah, that gives the Bernstein polynomial in expectation iirc
we had to work that out as homework once in my probability course, it wasn't too bad
 
yeah
something man
Research leading to these inequalities was motivated by a ground-breaking proof of B. Bollobás [a2], who, in order to estimate the chromatic number of a random graph, used martingales (cf. also Graph colouring; Graph, random; Martingale) to show that the probability of not containing a large clique is very small. Bollobás presented his proof at the opening day of the "Third Conference on Random Graphs (Poznań, July 1987)" . By the end of the meeting S. Janson found a proof of inequality (a1) based on Laplace transforms (cf. also Laplace transform), while T. Łuczak proved a related, less exp
These nutcases
 
I think you need that trunctuation trick in proving CLT too
The CLT proof I learned was smart, but simultaneously horrible
 
4:29 PM
CLT is actually fine
 
I should learn how to do it using Fourier transforms
 
It's just Fourier theory yeah
 
@Yashas Are any of the algorithms comprehensible to someone without much knowledge of computational math? It's an interesting question
 
probabilistic graph theory is a really weird topic, but it's pretty cool in some ways
 
5:00 PM
@MikeMiller Not really. I looked at a bunch of papers. They suggest something similar to the sqrt method you suggested. Most of the paper deals with hacky solutions for fast sqrt computation and placing work items in blocks of threads. Barely any math. It's all computer science.
 
Fair enough. Glad you were able to find something, though.
 
This is one but it requires some rudimentary understanding of CUDA (or GPU programming in general) to make sense out of it.
 
I'm confused @Balarka, surely $C^1([0,1])$ is completely metrizable, by the norm $\|f\|=\|f\|_\infty+\|f'\|_\infty$, right?
 
{(X,y)|X not equal to 0} is connected , open and simply connected or not ?
 
^draw a picture
 
5:14 PM
failed again :-(
 
How to say 4" x 9/2" x 8ft? Can anyone offer some insight?
 
If x = [2;3>
 
If I want to say that on phone, how would I say that?
 
5:20 PM
(x^3+4)/(2x-1)=?
Sorry, I don't speack English
 
Ohh
No problem :)
 
@DecapitatedSoul 4 inches by 4 and a half inches by 8 feet
 
@TobiasKildetoft, Thank you so much. :)
 
5:40 PM
If x = [2;3>
(x^3+4)/(2x-1)=?
 
@WhyWhatWhereWhenHow Where are you brother? Long time no see :-)
Give us a come back
 
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