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2 hours later…
03:49
I want that book.
hopefully the fires are not impacting @leslietownes...
04:07
@robjohn ...and robjohn
and Ted
 
1 hour later…
05:11
@NirbhayKrishnan The key step is observing that $T_i=a^ib+a^{i-1}\left(\frac{b^i-1}{b-1}-1\right)$, after that it should be easy enough.
05:35
I spent months re-inventing the wheel
Let $\Delta: \mathcal{I} \to \mathcal{I}$ denote a $\Delta$-action, and define the slicing plane $\Sigma_{x_1} := \{ (x_1, x_2, x_3) \in \mathcal{I} \mid x_1 = 1/2 \}$ as the plane through which we partition $\mathcal{I}$. This plane intersects $\mathcal{I}_{\Gamma}$ and defines two subregions:

1. $\mathrm{Right~Half~Surface}: \mathcal I ^+:=\{ p \in \mathcal{I} \mid x_1 > 1/2 \}$
2. $\mathrm{Left~Half~Surface}: \mathcal I^{-}:=\{p\in \mathcal I \mid x_1<1/2\}.$



We define the twist map $\tau: \mathcal{I}^+ \to \mathcal{I}^+$ as a 90-degree rotation about the axis normal to $\Sigma_{x_1}
because this is basically a Dehn twist
05:48
And @robjohn of course. I think Ted is in a different state.
I'm okay everyone.
I'm surprised there are this many folks in the chat at this hour
reminds me of a time when we had a topology pow wow and then all of us returned 7 hours later to discuss more
after sleeping
does anyone know what "oud" is?
I have a candle that says "sandalwood & oud"
06:19
@HomesickIguana it's resin
 
2 hours later…
08:00
wow that is cool
never knew what that was
@LukasHeger I tried asking the same question on mathoverflow but I guess it didn't work there either. Honestly I'm about to throw in the towel on math.
They honestly think I'm trolling - i know that I am not. LOL
that is the disconnect
🤷
08:52
@copper.hat did he move from San Diego
 
1 hour later…
10:39
just realised this course I am taking is actually a galois theory course
the title of the course, though, is fields, modules and algebras
im in for a nice ass beating semester
11:03
@nickbros123 field theory is basically Galois theory
at least in the sense that when you study one, you study both
@SohamSaha yep i have got the same general term great :)
I like this book for field theory, I studied from it the bits that interested me
it was for real-closed fields, so things related to transcendental degree
11:26
@Jakobian nice. this book is also in the recommendations for the course (primary one being Dummit and Foote)
some people, I have noticed (in my class), have already figured out what they want to do research in and narrow down themselves to it already in undergrad
like, I know a guy obsessed with number theory, algebraic geometry, so he only really cares about that.
@nickbros123 that's good that they did
the sooner the better
interesting you advocate this. I am not sure for myself though
I really like analysis, my department is also analysis flavoured
but I dont think i have seen enough of stuff
to make a choice like that
11:42
it's like with choosing a university or what are you going to study there
the sooner the better
you haven't seen enough, most people didn't
you'll waste your time trying to, no?
it's not a time to be indecisive
12:07
@nickbros123 I'd suggest something you could try to learn that I found pretty interesting, but at the same time deep
take a look at Stochastic differential equations and diffusion processes by Ikeda and Watanabe
@Jakobian what is that something
probability theory
I used to think statistics was synonymous with probability theory
and you were wrong
and that is why I succeed :P
12:13
@Jakobian thank you very much. I actually will be doing probability theory the upcoming summer (come what may, rain or shine, but in india its mostly shine). Doing measure theory (little by little) in this semester to prepare myself a bit
@nickbros123 why not download the book I just mentioned? You can learn the gaps in your knowledge as you go
I feel like that's a good motivation
Is math sometimes never not well motivated? For example, the triangle. Wasn't that just a curiosity?
not what I was saying
yeah i was just asking a question independent of your statement lol
when you ask a question like this right after I have said something, it can be put into context that you are trying to ask something in relation to what I said
even if you didn't mean that, this is how it will appear to most people
so it's natural that, regardless of what you mean, I would clarify this
isn't that obvious
12:25
@Jakobian sure.
@Jakobian I see what you are saying yeah
how can I make this to not show up in my chat list
hm. It disappeared now
12:54
@Jakobian you know anything about this by chance? math.stackexchange.com/questions/5021145/…
@Thorgott homogeneous spaces?
If $X$ is homogeneous and $x, y\in X$ then there is a homeomorphism $f:X\to X$ such that $f(x) = y$, so that $X\setminus \{x\}$ and $X\setminus\{y\}$ are homeomorphic
yeah, it's sufficient, but not always necessary
sure, but isn't homogenity the reason of OP's question
13:11
@Jakobian the banner at the top of the page with upcoming events is annoying; plus the name of the events seems made by a 3 years old. Did you manage to remove it?
all the examples they know are probably homogeneous, but it's still an interesting question IMO
I think the sufficient condition for the converse in my comment can be improved by a lot
@SineoftheTime no
@Thorgott David Gao provided example of $\omega_1$ which is not homogeneous
and I believe any ordinal $\omega_\alpha$ should work
in this question you want to look at what, the group of homeomorphisms of course
homogenity says that for any $x, y\in X$ there is $f\in H(X)$ such that $f(x) = y$
sure, but ordinal spaces are still decently ugly depending on how you look at them
this questions asks about slightly distinct property, that if $x, y\in X$ then $X\setminus \{x\}$ and $X\setminus\{y\}$ are homeomorphic
for a concrete question, I wonder if there is any counter-example that is non-compact, LCH and connected
13:17
@Thorgott what? Ordinal spaces are very nice
as I said, matter of perspective
you never saw an ugly space
as for this, maybe $[0, 1)\times \omega_2\setminus \{(0, 0)\}$ with lexicographic order works, the longer line
this doesn't work
isn't it homogeneous?
maybe something like long circle
@Thorgott long line would be, but I used $\omega_2$ and not $\omega_1$
but this doesn't work because it doesn't have the homeomorphism property
so I think you want to wrap it around like a circle
@Jakobian and why is that not homogeneous?
13:25
@Thorgott because $(0, \omega_1)$ is a point where this space is not first countable
urgh, ok
perhaps it's not so easy to get a sufficient converse in the non-compact case
I have an idea like this
take an open shape homeomorphic to the circle, and puncture it in countably many places
add closed intervals, countably many
maybe I should draw this
the green dots are holes, the red is where there's no boundary, blue is where there is boundary (but not on the edge)
oh maybe the gaps being so large won't make it homeomorphic when we remove the points from blue ones
so perhaps just puncture the x-axis by countably many points
no matter which point you delete from this, it should still be homeomorphic to itself
in $\mathbb{R}^2$, locally compact, path-connected
Explicitly by a formula, say, $\mathbb{R}\times [0, \infty)\setminus (\mathbb{Z}\times \mathbb{N}_0)$
(where $\mathbb{N}_0$ is natural numbers with zero)
is it clear that satisfies the property?
it's clearly a manifold with non-empty boundary and thus not homogeneous
which property
13:40
that the point complements are all homeomorphic
but I suppose you can just wiggle everything and it checks out
well intuitively it does, since if you remove a point from above the x-axis then you can move it upwards
and the rearange those points
and if you remove one from the x-axis then you mess with that area of your space
formal proof - that would be a chore
yeah, I mean, away from the $x$-axis we are homogeneous anyway
removing a point from the $x$-axis is the critical case, but you should be able to just rearrange the nearby punctures above the $x$-axis
@Jakobian yeah I agree
@Thorgott yeah I think you can just move the x-axis back in place, and then rearange the points above so they get in their original place
I think if you have the half-plane, and remove discrete closed infinite countable set from both the upper plane and the x-axis, then that's always this space
yeah, that has to be true
I believe you can have some kind of dendrite without a point as well
ah no how would that work
I can't think of anything 1-dimensional
For subsets of the real line, of course nothing works if we want it to be connected
but I was thinking about 1-dimensional subsets of the plane
 
2 hours later…
15:37
Who is cleo?
@आर्यभट्ट an user that existed on math.se famous for solutions to questions about integrals without explaining them
I think math.se banned cleo, and it made a lot of people disappear from the site, or something like that
16:13
@XanderHenderson Will you sponsor my paper for ArXiv?
hi chat. so why do we define the geometric genus only for smooth (complete) varieties over $k$? as long as $X$ is a proper $k$-scheme, we have that $\Omega_{X/k}$ is coherent, using the description of finitely presented $A$-algebras for the module of differentials $\Omega_{B/A}$. so $H^0(\Omega_{X/k}, X)$ is a finitely generated $k$-vector space and $g(X):=h^0(\Omega_{X/k}, X)$ still makes sense.
16:31
you're right. but iirc the focus on smooth complete varieties is because $\Omega_{X/k}$ behaves more predictably as a locally free sheaf. Also $g(X)$ aligns better with geometric intuition and other invariants like Hodge numbers and the canonical divisor. And I think that singularities make $g(X)$ harder to interpret geometrically
You might use alternative invariants like arithmetic genus for non complete varieties.
16:47
@HomesickIguana No. I don't know you, and I don't know your work. I'm also pretty sure that I don't know the general area of your work, and I don't have the time to get caught up.
@HomesickIguana properness is ok for me. but i'm wondering why the smoothness hypothesis is necessary, as the geometric genus would still be well defined. well, guess i just have to accept
17:03
@XanderHenderson hmm... why are they asking you this all the time
@Jakobian No idea. I'm not even sure that I could sponsor someone.
what does it mean to sponsor someone on ArXiv anyway? I thought the service is free?
@Jakobian arXiv doesn't allow just anyone to upload a paper. In order to upload your first paper, you need to be endorsed by someone who is "trusted" by arXiv.
I am not exactly sure how they establish "trust". I think that anyone who has already submitted a paper to arXiv can endorse a new author, but I am not certain of that. In any event, I don't think that I have an arXiv account, so despite the fact that I have a couple of papers on arXiv, I am not sure that I could endorse anyone else.
ah, I see. Interesting, since people still go there to post their proofs of RH and Collatz conjecture
Greetings.
@SineoftheTime would you like to play another chess match one of these days?
17:19
my h-index must be in the pico range
@XanderHenderson You need to be registered as an author of some amount of papers in a category (like math.RT) in the last five years to be able to endorse a paper in which this category is primary.
@VladimirLysikov Well, then, I'm useless. I am not sure that I ever created an arXiv account, and my papers are all more than five years old.
and even if they weren't, I'm pretty sure they're listed under a different category
@Thorgott almost certainly
17:59
In Folland's text, specifically on product measures, he defines "the" product measure $\mu\times\nu$ to be the restriction of the outer measure induced by the premeasure $\pi(E)=\sum_1^n\mu(A_j)\nu(B_j)$ on the algebra $\mathcal{A}$ of finite disjoint union of rectangles (indeed, he uses the word 'the' when saying "We call this measure the product of $\mu$ and $\nu$ and denote it by $\mu\times\nu$.").
Someone told me once that by $\mu\times\nu$, Folland denotes a unique measure (the restriction of the outer measure from Carathéodory's extension theorem).Maybe unique is not the right word here, but if I remember correctly, this is what I was told once. Folland goes on to say if $\mu,\nu$ are $\sigma$-finite, $\mu\times\nu$ is the unique measure with the property $\mu\times\nu(A\times B)=\mu(A)\nu(B)$. Has someone read this part and has the same doubts concerning the notation $\mu\times\nu$?
I guess by his last remark, $\mu\times\nu$ is not always a unique measure on the product $\sigma$-algebra.
I don't understand the concern, $\mu\times\nu$ is an explicitly defined thing.
It has a certain property and that property may or may not uniquely determine it, but that's neither here nor there.
@psie I think we already went over this and even had some example of non-uniqueness
yes, that's how I'd phrase it too; $\mu\times\nu$ is a specific measure. I believe one can't restrict the outer measure induced by the premeasure and obtain (again) another measure. So it's a distinct object.
what's of concern here is the definition of product measures
Folland defines them that way, while someone else might define it as any measure satisfying the given property
@Jakobian yes, possibly. Currently I'm reading a text where the product measure is not constructed through Carathéodory's extension theorem, but through a $\pi$-$\lambda$ argument.
18:14
huh. Interesting
$\pi$-$\lambda$ is a tool to check if something is a $\sigma$-algebra, so not sure how that would be applied
@Jakobian it has a corollary by which you can check uniqueness of measures
18:28
I want to prove that $f:[a, b) \to \mathbb R$ is uniformly continuous on $\mathbb R$ $\implies$ $\lim_{x \to b} f(x)$ exists.
I have the following lemma available:
Let $f : [a,b) \to \mathbb R$ be a function. If for every monotonically increasing $(x_n)_{n \in \mathbb N}$ with limit $b$ the sequence $f(x_n)$ in $\mathbb R$ converges, then the limits match and $\lim_{x\to b} f(x)$ exists.
So if we can show the premise, this should immediately follow. Any ideas?
Somewhat related, he also talked about what it requires to post on arXiv.
18:45
@ILikeMathematics hint: a uniformly continuous function takes a Cauchy sequence to a Cauchy sequence
19:12
@ILikeMathematics This follows from theorems about completions. Interval $[a, b]$ is the completion of $[a, b)$, and so any uniformly continuous function $f:[a, b)\to \mathbb{R}$ extends to $\tilde{f}:[a, b]\to\mathbb{R}$
19:54
@Thorgott I must say, the discussion about when $X$ is Alexandroff extension of $X\setminus\{x\}$ was pretty interesting
"Alexandroff extension is functorial with respect to homeomorphisms (more generally proper maps) so homeomorphism $X\setminus \{x\}\cong X\setminus \{y\}$ extends to $X\cong X$"
what does functorial mean in this case?
If you mean that it's a functor then isn't this not really saying much
the latter seems to be part of checking if it is a functor (or er, that it makes sense to define it)
but yeah, it should be pretty clear that a homeomorphism extends to homeomorphism of Alexandroff extensions in a pretty obvious way
 
1 hour later…
21:17
@Jakobian a proper map $f\colon X\rightarrow Y$ induces a continuous map $f^+\colon X^+\rightarrow Y^+$ that maps $x\mapsto f(x)$ and $\infty\mapsto\infty$, and this construction is compatible with identities and composition
21:55
@leslietownes something for you. I had some ideas but I pass
22:05
@Almanzoris ok I can next week
23:01
jakobian: good idea. similar to what robert israel is doing here: math.stackexchange.com/questions/1227253/a-dense-subspace-of-l2 (it doesn't seem to matter that n is an integer, only that it is a sequence going to +oo)
the other solution in that exercise shows another idea, which is to somehow go through holomorphic functions. i don't immediately see how to get it to uniform approximation, but the 1/(z-a)'s are clearly dense in H^2(the disc) by the argument given there (the 1/(z-a) represents evaluation at 1/a, or -1/a, or some scaled version of that)
there are a lot of pretty baroque reuslts in approximation in C[0,1], patterned on simple classical results for polynomials like the muntz-szasz theorem. this exercise doesn't seem to invoke anything near that level of substance because it doesn't care about how the sequence goes to infinity, and the lot of the conditions you see in polynomial or rational approximation absolutely do care about stuff like that. that is where they shoot off into outer space.
23:22
I was wondering: at first sight, does this surface look regular to you guys?
spoiler it is not: I couldn't draw it so I checked all the requirements and found out that the normal vector $\mathbf{\phi}_u \times \mathbf{\phi}_v$ is not non-zero in the interior of $K$
lmao, if only I'd been able to draw it from the getgo I wouldn't have wasted all this time checking all the requirements (fun fact it satisfies 2 out of 3 of the latter)
this more general form may help you recognize what kind of surface it is a part of, and why the equations have the form they do math.stackexchange.com/questions/1578756/…
these folks even drew a picture web.maths.unsw.edu.au/~rsw/Torus/index.php
well that explains it, on my part, I must admit I've never encountered the parametrization of a torus :)
now it makes sense
oh wait
now that I think about it it also looks familiar to the parametrization of the moebius strip I've seen in my book
@leslietownes as a person of my age would say: this is absolute fire
the moebius strip parametrization components are in fact similar, but $K = [0,2\pi] \times [-1,1]$ so the second parameter is not an angle
23:37
the picture in the second link suggests thinking of the formula for g(u,w) as a vector sum of two things, a formula that sweeps out a circle in the xy plane of radius R_1 (here 2) that sweeps out the center of the donut that the torus is the surface of, and then a formula that sweeps out a circle in a plane containing the z-axis
if you sort of think that through symbolically you do get that gibberish
@leslietownes that's a neat way of constructing it indeed
and yeah if you let things twist around the origin you get a moebius strip type formula, all of this mysteriously paired cos sin stuff is reflecting rotational symmetry or near symmetry about the origin
I see
someone who thinks in pictures can say this all in like 20 seconds while drawing it perfectly at the same time, and make it look easy
and then you go home and stare at your notes and think ".. what"
yeah I wish I could do that :P
maybe a differential geometer, or whatever they are called
23:41
it should be a regular surface though. at any given point the "x_u" and "x_v" will be a little tangent vectors pointing along their respective directions and their cross product should be a nonzero thing that points normal to the surface of the donut
lots of opportunities to make sign errors or errors with trig identities here, that is probably what is going wrong if something is going wrong
the normal is $[(2+\cos u) \cos u \cos w, -(2+\cos u)\cos u \sin w, -(2+\cos u)\sin u]$ which clearly is zero at some point in $(0,2\pi) \times (0,\pi/2)$
that expression isn't "clearly" anything :)
but if you compute its length there's a lot of squaring and a lot of opportunities for sin^2 + cos^2 = 1 to make it look different from how it looks now
oh wait maybe no :)
cos and sin are never both 0
no ok it is regular then, but the normal vector clearly can't be continuous from the picture
wait, I must check in the interior of $K$, so maybe the picture is misleading
why can't the normal vector be continuous from the picture? you could probably draw it by hand anywhere, except maybe on the absolute edge where there isn't enough "surface" for the normal to make sense
but that's just a result of the parameter restrictions they made in the problem (and is not present on the interior of the parameter space)
no yeah I thought the edges were the problem
23:52
if you let that 0,pi/2 parameter run over some larger a,b you just get a bigger or smaller slice of donut, or if you let it run over all R you get the whole thing
but then again one can probably extended even to the edges so that it attaches smoothly
@leslietownes Yeah you're correct, it is indeed continuous
yes, if you let it run over all of R you no maybe no longer have what your book would describe as a regular coordinate patch for a different reason - different pairs of parameter values can map to the same point in R^3
but the normal vectors you'd compute (using the same formula as above, for different angles u, v) would actually coincide for different choices of parameter mapping to the same point of R^3, so even then you have a well defined normal :)
that maybe doesn't happen in the moebius strip case
what you said above is that the normal vector does not depend upon the choice of pairs of parameters?
for choices of parameters that represent the same point
it obviously depends on the choice of parameter, but if you allowed yourself negative angles or whatever you'd find that the normal you'd get corresponding to the parameters (u,v) = (0, 0) would be the same as the normal you'd get corresponding to the parameters (u,v) = (-6 pi, 0)
so in this case it doesn't matter which parameter values you choose to represent a point of R^3, the normal you get using those values will be the same

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