« first day (3108 days earlier)      last day (2208 days later) » 

00:00
Though I prefer the interval factor first.
Oh, gotcha. You're starting with an arbitrary one. Sorry.
Yeah, yeah, I'm rusty.
OK, I'm caught up. Now you can finish after the dentist. :P
No need to be sorry.
LOL, no need to be hyper-solicitous, either :P
Yeah, seems right.
Anyway, you cap off the boundary components and have a simply connected closed 3-manifold.
In other words (Perelman) you have S^3.
Now you just need to delete the balls.
Oh, I see.
00:04
Ok, I'm gone. T^2 is harder.
Thanks :P
It's a surgery argument (like one I have in a post about 3manifolds with fundamental group Z).
I got a textbook
Same
Eh I guess "I got" suggests recent so I can't make that joke
:/
what textbook? lol
lol what joke?
i really need to stop saying lol. I do it too much irl...
00:19
you say lol in spoken language?
yeah lol.
heya Dair.
i have problems.
@TedShifrin Hey! I believe you can confirm is say lol in real life?
I don't usually, no.
ok. nvm. haha.
@Ted The weather has been crazy today.
@Dair it's a joke I make sometimes. If someone starts a story saying "So the other day I was taking a walk" I immediately interject and say "same".
Yeah, Dair.
And yeah sometimes I say "lol" in real life but it's rare
00:25
it just rolls of the tongue so well. And it's less cacophonous than haha.
if u say lol in real life ur a nerd don’t at me
Do you say "lol" or L-O-L ?
@Ted "lol"
I don't actually spell it out.
I know no one (else) who does that.
I was about to say... Until you corrected your message
00:27
I also say it as "lol"
I also do that with "lmao"
luh-mao
L'Mao
Yeah definitely I feel it.
that one is way worse
next you'll say Lao-Tzu.
00:28
next you'll be saying raful.
too bad there isn't really a good way to wtf except for spelling it out...
It's like a french cat: "Le Mow."
@ÉricoMeloSilva You seem to be greatly troubled by this.
En français on dit "miauler" ...
im not troubled by anything lol
well, except for your GR pset...
:P
00:32
insulted is a better word tbh
Gotcha, Ted
Miauler sounds like some sort of bastardization of Mahler
not if you pronounce it in French :)
Miauler's Symphonie Fantastique.
It looks like it'd be closer to "moo-lay"
00:36
that's Berlioz, Dair :P
ohhh yeah.
didn't Mahler make like that depressed version of Frera Jacque?
i forget how to spell it lol.
wait lmao i should know this.
Yes, Mahler 1st symphony has that.
Frère Jacques
except creepy af
and Beriloz has the massive Eb clarinet part.
Berlioz has serious brass stuff
Eb clarinet part is super rare. nobody likes the Eb clarinet.
00:40
@TedShifrin what is the physical significance of the laplacian?
divergence of the gradient
It measures how much the value at the center of a sphere differs from the average values on shrinking spheres centered at that point.
is there like an "integral" formulation?
khan calls them "formal definitions" which I disagree with
what do you call a derivative that is not truthful
@TedShifrin and hence governs heat flow :)
Green's identities are the answer to that, Leaky.
Did the dentist pull any teeth, @MikeM?
00:50
No, but I have to come back. :(
Story of my life ....
dentist
I know one of those
0
Q: How do I prove the $f:X\to I$ by $f(x)=\min\{f_i(x_{\beta}):i=1,2,...,n\}$ is continuous.

Unknown x How do I prove that $f:X\to I$ by $f(x)=\min\{f_i(x_{\beta}):i=1,2,...,n\}$ is continuous. My attempt:- Minimum of two continuous real-valued functions are continuous. $$f_i \circ \pi_{\beta_i}: X\to I$$ be continuous function.So, $f(x)$ can be re-defined as $f(x)=\min\{f_i(x_{\beta_i}):...

@Ultradark It's probably a good idea that everyone in chat knows at least one dentist.
So, $f(x)$ can be re-defined as $f(x)=\min\{f_i(x_{\beta_i}):i=1,2,...,n\}=\min\{f_i\circ \pi_{\beta_i}(x):i=1,2,...,n\}$.
Is it necessory to redefine the function like this?
00:55
@MikeMiller heat flow best flow lets go
$f(x)=\min\{f_i(x_{\beta_i}):i=1,2,...,n\}$ Can I appy the result 'Minimum of continuous real valued function is continuous directly here?
Hey want to read that Ricci flow on surfaces paper together later? Month from now maybe?
@N.Maneesh: Note that your title makes no sense. You need the subscript on the $\beta$.
okay. I have corrected it.
The tricky part here is that you have a function of $x$, not just of the finitely many $\beta_i$. But it's not very tricky.
00:58
@TedShifrin What about my argument? Is there any mistake?
Think about the product topology. If you have $X = \prod X_\alpha$ and you fix one $\alpha$ and set $f(x) = g(x_\alpha)$, if $g$ is continuous, does it follow that $f$ is?
I haven't read it.
I think I'm going to try to read Kirby-Siebenmann.
Yeah, your argument is right, @N.Maneesh. Once you know the min of two continuous functions is continuous, it's just induction to get $n$.
@TedShifrin Thank you very much. :)
heat check, get wrecked, ricci flow cruisin on the manifold. top down, windows low, can't stop, modular flow over the space of lattices, you already know
6
01:52
The mathematics of emptiness:
$\varnothing = \text{class}(\varnothing) = \text{object}(\varnothing) = 0 < \text{null}$
But for some reason, I felt zero is less empty than the emptyset
Meanwhile, null is much less empty than zero because zero is a subset of null objects, which includes any object not necessary zero such that given some relation, it evaluates to zero
A common example are nilpotent elements in algebra where there exists some nonzero $\epsilon$ such that $\epsilon^2=0$, another example are null vectors in inner product spaces
interesting
02:12
For most who are untrained in the perception of emptiness, all notions of emptiness, such as nonexistence, nothingness, phantom, ghost, vacancy, hollow, emptiness, blank, conceal, unseen, hidden, subtle, counterfactual (ok this one is not), etc. look the same and considered to be the same equivalence class of nothingness
But the reality is, there are different shades of nothing, and they are all different
Back to maths, no matter how many times an empty set is partitioned, (can be rigorusly done by letting a partition function $\pi_i$ and $i \in I$ where $I$ is some index set, and then put elements under $\pi_i$ into the ith equivalence class) the resulting sets are always empty
02:49
@TedShifrin very nice video youtube.com/watch?v=ez1rWBPznEc
Let $f:\Bbb R\to\Bbb R$ be such that $f''$ is continuous on $\Bbb R$ and $f(0)=1, f'(0)=0, f''(0)=-1$. The $\displaystyle{\lim_{x\to\infty}\left(f\left(\frac{\sqrt2}{x}\right)\right)^x}$ is .....

I did this using particular function $1-\frac{x^2}2$, but how to do generally?
 
3 hours later…
05:52
Hello!! How can we calculate the supremum of $-\frac{2}{9x^{\frac{4}{3}}}$ ? I got stuck right now.
Apparently xkcd wrote another book
hmm?
Marystar: Isn't the supremum of that just the asymptotic value?
06:08
@AkivaWeinberger, hi. Will you please let me know why does this happen: This here says that line integral over scalar field is a special case of line integral over vector field, but while line integral over vector field changes sign when path reversed, this says that line integral over scalar field is independent of path direction!!
If we have a line integral over a vector field, but the vectors are all tangent to the path of integration, then it's the same as the line integral over the scalar field of their magnitudes
If you reverse the direction of the path then the vectors are no longer tangent to the path of integration
Er, I guess we need "tangent and pointing in the same direction"
and so if it points oppositely it counts as negative
@Silent
ok! thank you very much for that modification
@AkivaWeinberger, so modification is needed in math.se answer, right?
The answer in math.se says exactly what I just said
(Note that $r$ is the path)
06:36
@AkivaWeinberger I am sorry, but i can't figure out how $\cos \theta=-1$ possibility says "tangent and pointing in the same direction"
If it's $-1$ then it's pointing in the opposite direction and counts negative
(and $\theta=180^\circ$)
So, if we reverse path, then line integral on scalar field be negative, right?
Zee
Zee
07:05
Who knows
@Zee I still think that reversing path reverses sign even in scalar integral, i took path parallel to x axis and tried both directions, and sign seems to reverse!
@Silent No, it should stay the same
for a scalar field
07:21
Here blue arrows represent f, while red arrows are path's direction. Please explain how does line integral does not change.
@AkivaWeinberger
(Maybe i need to provide more info, but f(x,y)=(1,0) is what in my mind, and (t,0) is original-first path.)
Hi chat.
08:29
@Silent You've drawn a line integral of a vector field though
Note that in our recipe for converting a line integral of a scalar field into a line integral of a vector field, the vector field depends both on the original scalar field and the path
omg! let me think about that. thanks for pin pointing that.
Apparently you can't loop a song in Spotify even if you paid?
Yes you can
@LeakyNun Put the song into its own playlist, then turn loop on
or just double click the repeat button
08:41
Oh nice, I didn't know about that
A little $1$ appears
@ÍgjøgnumMeg no I can't do that with the new update
Hmm that's weird
on phone version?
ok I found the button it's hidden in the 3 dots menu
yes phone
Yeah
I've just seen that lol, weird
wonder why they'd bother moving that
08:44
The Spotify team isn't the brightest
09:32
The Simons Center at Stony Brook
@Secret What are these different shades of nothingness?
Do you mean in reality, or in logic, or what?
yesterday, by Rudi_Birnbaum
@AkivaWeinberger Fourier-Transformation
@Rudi_Birnbaum Found this
10:03
This is also a neat image
@Rudi_Birnbaum Go here jcrystal.com/steffenweber and click on "Fourier Tr." on the left
Heh:
Markings on the Penrose rhombs that enforce the matching rules
(with the result that these tiles can tile the plan, but they cannot do so periodically)
(and they can tile the plane in a locally unique way, in the sense of, if you have two infinite tilings with these shapes, any finite piece of one can be found infinitely many times in the other)
10:44
@user616128 nah forget that, its metaphysics and possibly not even wrong
11:08
Whoa:
how come this is a fractal. I thought quasicrystals have fixed sizes?
Oh my god there's a whole gallery of these GIFs
and here
11:27
Whoa indeed
@Akiva I like the fast ones
This one is messing with my head a little bit: i.imgur.com/8GpZL.gif
Pentagonal tilings are so weird. The fact that you can almost do it uniformly actually gives rise to some arguably more interesting patterns than uniform tilings would.
11:45
This one appears to be a tiling of equilateral triangles in disguise, if those flashing green lines are a reliable indication: biorobots.case.edu/personnel/adh/quasicrystal/examples/…
What the hell did I just watch:
(If you do watch this, I would recommend not having the sound on, maybe having some other music on instead)
(Not a fan of the music)
It's not even music, I'd say. Just discordant noise.
@Secret It's made in a different way from the Penrose tiling
It's made from superimposing waves, I think
Not 100% sure how they got it to be self-similar but I think it was in a similar way to auditory illusions like the Shepard's tone
(Fun fact: the sound equivalent of "visualize" is "audiate")
I see
@Rithaniel Well most neoclassical music sounds like that, nothing very surprising
Is that what this is? (I still wouldn't call it music, though that also begs the questions of how I define music.)
11:55
I look at the zoom-in GIF and then I look somewhere else and it looks like wherever I'm looking at is shrinking away
(The opposite for some zoom-out GIFs)
It's so weird
Who needs drugs
Alright, homework question: "If $N$ is a normal subgroup of $G$, show that $G/N$ is abelian if and only if $N$ contains the commutator subgroup of $G$." I'm having some difficulty coming up with a good approach to this. (I think I need to have that if $n\in gN$ then $n^{-1}\in gN$ as well, but I can't figure out how to show that either.)
hey anyone know anything about binary search?
@Rithaniel How have you had the commutator subgroup defined?
It's the subgroup generated by commutators of any two elements in the parent group.
Ok, so what does it mean for a subgroup to contain this?
12:07
It must contain all commutators of any two elements in the parent group. I assume we have to use this to show that $(gh)N=(hg)N$
Right. What does that equality mean in terms of certain elements being in $N$?
Oh, I think I see. On one side you have $(hg)1$ and on the other you have $(gh)[h,g]$
hi chat
@Rithaniel No, just use the standard result about when two cosets are equal
They have non-trivial intersection?
12:13
No, in terms of something to do with their representatives. I.e. $xN = yN$ iff "something to do with $x$ and $y$ and $N$"
Well, I know that if $xN\bigcap yN\neq \emptyset$, then $xN=yN$
I am looking for the one that does not involve cosets in the end
I might not have learned that one yet.
$xN = yN$ iff $y^{-1}x\in N$
(I refuse to believe you have not learned that btw)
12:16
Yeah, haven't learned that one yet.
what terrible text does not include that one before going into quotients by the commutator?
Well, I don't know what text we're using, I've been going off the class notes. We've mostly been touching on the notion of cosets forming a partition on the group in lecture.
Anyway, prove the statement I wrote (it is pretty easy given the ones you already know), then use that.
Alright, it seems much more straight forward with that.
Thank you for the help.
An applet that generates quasiperiodic tilings by taking slices of higher-dimensional, periodic tilings
@Rithaniel Why is this a normal subgroup?
12:24
What do you mean? Why does it need to be a normal subgroup or what makes a particular subgroup normal?
A subgroup $N$ of $G$ is normal if $gN=Ng$ for all $g\in G$
Unrelated, it actually puzzles me on whether the notion of Lebesgue measure actually have an intuitive counterpart. Because that fact that the ordering of points in an uncountable set can change the value of the measure is something that does not really have a real life counterpart (how often does one saw something that basically change its length or area or mass or whatever purely because of how it is arranged in space)
In other words, if $h\in N$ then $ghg^{-1}$ is also in $N$
Yes, I'm familiar with that. (Also, the n=4 tiling on that gregegan applet is cool)
So why is $a(bcb^{-1}c^{-1})a^{-1}$ a product of commutators
Oh I figured it out
12:29
@AkivaWeinberger It is actually a lot easier to write up that the image of a commutator under any homomorphism is again a commutator.
$a[b,c]a^{-1}=[a,b][b,ac]$
@AkivaWeinberger unnecessarily complicated. It is also just $[aba^{-1},aca^{-1}]$.
$=[aba^{-1},aca^{-1}]$
Ohh
Ohh I get you, $f([a,b])=[f(a),f(b)]$
and then let $f(x):=axa^{-1}$
Right yeah that's much simpler
How to get 1D quasiperiodicity from 2D periodicity:
(Note that the diagonal line isn't being cut by the grid lines it intersects, but rather by the projections of nearby grid points onto it)
(so that there are only two lengths of segments that it is cut into)
(If it were cut by the grid lines, the result would be the same as just superimposing two periodic 1D lattices of different sizes.)
12:50
I'm not sure how this was generated but it doesn't look like periodic lattices rotated and superimposed on each other so I assume it is actually based on Penrose somehow
Or maybe it's from superimposed plane waves again
is there notation like big-O to indicate that terms do not depend on a given symbol?
@student It is customary to include the symbols that something does depend on, rather than the other way around.
13:07
@TobiasKildetoft Yes, but sometimes, you want to say that there are terms in an expression you don't care about. When you complete a square, say, and the term you add is irrelevant for the discussion.
@student "don't care about" is not a mathematical thing, so it should be written only in words and not in symbols
@TobiasKildetoft I don't write my papers in prose
then you are doing it wrong (unless you mean you write them in verse, in which case, awesome!).
A rhyming proof would be an incredible feat.
Map $\Bbb R^n\to M$
Derivative everywhere
It's a manifold
13:17
Consider the cantor set defined in the following way: if $C_0 = [0,1]$ and $C_n = \frac{C_{n-1}}{3} \cup ( \frac{2}{3} + \frac{C_{n-1}}{3})$, then $C := \bigcap_{n=1}^\infty C_n$ is defined to be the cantor set. Question: from this way of defining the cantor set, how does one show that $\{C_{n}\}_{n \in \Bbb{N}}$ forms a decreasing sequence of sets? I tried induction, but I had some trouble.
Showing that $C_2 \subseteq C_1$ is not hard (this is my base case), but the actual inductive step isn't obvious.
If you write $x\in C_n$ in base 3 you'll see why
@TobiasKildetoft My point was that there is notation for a reason, when of course you could always write your theorems and proofs without. A symbol akin to $O(n)$ would make it so that one can write $x^2 + 2xy = (x+y)^2 + \ldots$ without having to repeat each and every time that the other expressions do not depend on $x$ (but are not constant, or O(1) or something).
But I take it that there is no widely used thing I wasn't aware of
How does one do that? Also, is induction not needed?
@student The difference is that big O has a precise mathematical meaning. What you are looking for does not, so it has no common notation.
You can write any $x\in [0;1]$ as $x=0.a_1a_2\dots = \sum{a_i\over 3^i}$ where the $a_i are 1,2 or 3
The same way you can do it in base 10
Then by induction you find something that characterizes the $C_n$
And that demonstrates inclusion
13:24
Oh, I see. Thanks for the hints.
Where you asked specifically that the $C_n$ form a decreasing sequence of sets ?
Otherwise remember that $C = \bigcap_{n=1}^\infty\left(\bigcap_{k=1}^n C_k\right)$
Oh...so $C$ doesn't equal $\bigcap_{n=1}^\infty C_n$? It equals that double intersection?
Both are the same thing
But it's obvious that the second is an intersection of decreasing sets
Ooh, very nice! Thanks
13:42
Weird: a connection between the Penrose tiling and the Koch snowflake, though I don't think the author realizes this
14:05
Are the elementary row operations in Gaussian elimination vector space isomorphisms?
Yeah, as all of them are invertible matrices
Cool thanks!
14:40
> That’s how I created the image above.
> Now that I am able to visualize five dimensional space in my head, I’ve noticed that I get a lot of weird looks from priests and small children.
15:06
Well, you can kinda made out the envelope of a penteract in those penrose tilings
In five-dimensional geometry, a 5-cube is a name for a five-dimensional hypercube with 32 vertices, 80 edges, 80 square faces, 40 cubic cells, and 10 tesseract 4-faces. It is represented by Schläfli symbol {4,3,3,3} or {4,33}, constructed as 3 tesseracts, {4,3,3}, around each cubic ridge. It can be called a penteract, a portmanteau of tesseract (the 4-cube) and pente for five (dimensions) in Greek. It can also be called a regular deca-5-tope or decateron, being a 5-dimensional polytope constructed from 10 regular facets. == Related polytopes == It is a part of an infinite hypercube family. The...
Note the similarities between this and some of the patterns in penrose tilings
nCm
nCm
Is that the font of mathjax changed?
$\alpha, \beta$ looks different for me...
15:23
hello
i have the family $B_r=\{(x,y)\in \mathbb{R}^2, (x-3)^2+y^2<r^2\}$ is $\mathbb{R}^2=\bigcup_{r>0}B_r$ ?
In the world of algebraic groups, a connected algebraic group $G$ is simply connected if every isogeny $G' \to G$, with $G'$ connected, is an isomorphism. This is independent of the field $K$ over which $G$ is defined, right? So its a property of $G$ over the algebraic closure of $K$, right?
Does any form of \sum_ {n=1}^{\inf} \left (\frac{1}{(kn+1)^{2}} \right ) exists, where k is an integer ? (For example, k=2 we can get a form from basel problem)
If I’m using Lagrange multipliers, with the constraint being $G(x,y,z)=0$ what stops me from just saying $\lambda=0$ when equating the partial derivatives?
15:45
@JakeRose Do you get all the solutions?
0
Q: Analogy between metric space completion and algebraic closure

Kenny LauI've noticed some similarities between the story of completing a metric space and taking algebraic closure of a field. My question is whether these two stories can be generalized. Metric space Fix a metric space $(X, d_X)$. Consider isometries from it to other metric spaces (i.e. the under cate...

@MikeMiller I’m not sure
do an example?
what I don’t understand is, I have $G=0$ so why can I say $\lambda =0$
im trying one now
@JakeRose I do not understand this sentence.
I am a little confused as to how you think Lagrange multipliers go. Will you tell me how you think you're supposed to use it?
15:56
Say you want to find the extrema of some function $F(x,y,z)$ given the constraint $G(x,y,z)=0$ it can be shown that this is equivalent to finding the extrema if $F-\lambda G$. I.e. when $\nabla F = \lambda \nabla G$. So, $\partial_i F= \partial_iG$. The problem is, as $G=0$ then would $\partial_iG=0$ also?
sorry about the mistakes there
Huh?? You are misunderstanding the formula $G = 0$. It does not mean the constraint is identically zero for any x,y,z.
A common one is $G(x,y,z) = x^2+y^2+z^2 - 1$.
$G(x,y,z) = 0$ describes the set of points on the unit sphere.
But the gradient of $G$ is $(2x,2y,2z)$. That's not zero anywhere on the unit sphere.
That's almost always what will happen in practice.
Ohh yeah
wow
that was dumb
im sorry I even wasted your time with it
@JakeRose Don't be - the double question marks were just for emphasis
If I can offer a moral: always try an example! (if you are not sure what example to try, grab one from your book's exercise section.)
The sphere is a particularly good fella to cut your teeth on.
@BalarkaSen r
I was a bit confused by this question. I can take the vector field on S^2 with one +2 index zero, and flow along that to get a smooth S^1-action, no? The cardinality of the fixed point set is 1.
The right statement is obvious from Poincare-Hopf. Every S^1-action is determined by it's tangent field at identity
I suppose by "isolated" they mean "isolated and transverse fixed points"
If it preserves the AC structure maybe transversality happens. I don't know about that. I thought index wasn't allowed to be negative, that's all
16:08
I don't think the flow you have in mind has all orbits closed
Sure, why not? Take S^2 in R^3, take the tangent plane at a point, and consider planes transverse to that tangent plane cutting the S^2 into circles at various angles
I believe the following is true. Given a compact group G acting on a smooth manifold M, suppose G preserves the submanifold S. Then there is a diffeomorphism between the neighborhood and the normal bundle taking the action to its linearization.
I think the issue is about global periodicity in your example
Naturally a vf gets a $\Bbb R$ action. To descent to a circle action, there should be a constant $c$ so that the time-$c$ flow is the identity
I see, I was worried about it a little. I'm still not convinced you can't parametrize the smaller circles by larger time scales so that it's uniformly periodic
Maybe because the smaller circles keep shrinking
I think in your example we should have orbits with period in an interval
You'll get singularity at the fixed point
16:13
I feel like I noticed something similar when I once tried to construct circle actions on higher genus surfaces
But not sure
The relevance of saying "the set of periods includes $(a,b)$" is that we can't possibly choose a single real that is an integer multiple of all of these
Sounds right. Interesting that I never thought about this.
My linearization claim above says: if x is a fixed point of the circle action, then a neighborhood looks like S^1 acting on R^2
Probably by the standard action, unless your circle action has stabilizer
Right.
I should have thought of that. Just follows from usual G-equivariant tubular neighborhood theorem
You average out to find a G-invariant metric, then use exponential
(G compact is important: otherwise you run into my kind of example)
Well, I think there is value in ignoring that. In the case you described about planes intersectimg the sphere there was clearly something interesting going on, all orbits being circles but not a global circle action
So it is better to understand what is going on than to handwave the issue away with a bigger theorem
Actually, I now realize that in your example, the orbits are $\Bbb R$! Because the north pole is a fixed point.
Ah, heh
16:19
So then, ok, foliations by circles: do those come from circle actions?
I think the answer is yes in 2D and 3D - it's a big theorem in 3D but I forget how it goes in 2D
I think so. Take the tangent field of the foliation, away from the singular points. That integrates by Frobenius theorem
But it's false in 4D I believe, Bob Edwards came up with the idea and Sullivan a counterexample
Now you have to see how singular foliations by circles at singularities look like
The linear map from $\Bbb R^5$ to itself defined by $(x_0,x_1,x_2,x_3,x_4)\mapsto(x_1,x_2,x_3,x_4,x_0)$ rotates a unique plane by 72 degrees, another plane by 144 degrees, and keeps a line fixed
Somehow the circles have too many possible periods
16:21
I think that first plane is the one spanned by $(\cos(0),\cos(72^\circ),\dots,\cos(288^\circ))$ and $(\sin(0),\sin(72^\circ),\dots,\sin(288^\circ))$
but I'm not sure
Are those two vectors perpendicular?
I think they are
Ah, yeah, they are. That's neat
Can you do something to that vector field so that the flow actually becomes a circle action? Blowup S^2 at the zero, maybe?
RP^2 has nonzero Euler characteristic so actual blowup wouldn't work, of course
Idk
Oh, actually, I think I should've given those two vectors in the other order, so that the plane is oriented the right way. Otherwise it's actually a $-72^\circ$ rotation
@BalarkaSen See: Edwards, Millet, Sullivan, foliations with all leaves compact
Thanks!
In other words, let $i:=(\cos(72n^\circ))_n$ and $1:=(\sin(72n^\circ))_n$
16:26
The crucial point here is that the picture I had in mind was not a singular foliation. I didn't realize that.
Stuff limits to singular stuff in a very regular fashion in singular foliations
Yes, I didn't realize either.
Thanks for the paper, I'd need to read it
Ciao for now!
Would it be accurate to say that $\mathbb{Z}[i]$ can represent the vertices of a square tiling of the complex plane and $\mathbb{Z}[\omega ]$ can represent the vertices of an equilateral triangle tiling of the complex plane?
16:36
Is there a corresponding system for the vertices of a hexagonal tiling? Can you generalize this to any potential tiling, even a non-uniform one? (Or would that be more a question which needs research to answer?)
@Rithaniel A hex tiling would not be closed under addition
Ah darn.
@Secret What do you mean by asymptotic value?
You could get it as a subset of the Eisenstein integers though I think
Yeah, that's what I was thinking, initially, but if it's not a proper ring, then it's less interesting.
16:42
@AkivaWeinberger I get dizzy when I try to visualize 4D...
(I should point out that that's a quote, taken from the link)
16:56
@AkivaWeinberger IKR. But (I think that) some people do actually have a grasp of what's happening in those dimensions and I find this bizarre

« first day (3108 days earlier)      last day (2208 days later) »