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01:05
What are non-obscure subrings of $\Bbb C$
wdym
do you just want examples of subrings of C or?
I was worried about computations like $H_n(X,A;\Bbb Q)$ coming up in the exam and now that I learned that this is just $H_n(X,A) \otimes \Bbb Q$ I want to milk this fact
But algebraic numbers, real numbers, rational numbers, integers are probably the only realistic examples
I don't think anyone cares for homology with coefficients different from Z,Z_p,Q,R in a concrete manner
(that's probably a wrong statement, but it's probably alright to pretend it isn't)
for all my purposes, probably
my main purpose is passing the exam with an acceptable grade so
are $\Bbb R$ coefficients much different to $\Bbb Q$ coefficients?
I'd expect this to be the "same" for all practical purposes
no, you're literally just replacing a Q-vector space by an R-vector space of the same respective dimension
01:15
nice
the only reason I even listed R as having relevancy is cause the singular cohomology with coefficients in R of a smooth manifold is canonically isomorphic to the de Rham cohomology
Finally attained my goal of learning deRham cohomology without putting in the effort to get comfy with differential forms
also, for lots of things, Q and Z_p coefficients are all one needs
e.g. "homology is 0" or "map induces iso" hold for Z coefficients (and hence all coefficients) iff they hold for both Q and Z_p coefficients
me rn
cohomology in a nutshell
@Thorgott ah nice fact thanks
pure algebra stonks
01:23
Now that I think of it, I think I saw the first fact already. It's basically just saying that the non torsion parts and the torsion parts are 0, right? Do I need a finiteness condition for that
01:34
For a finitely generated group, the result actually holds in each degree individually. If $G$ is finitely generated abelian and $G\otimes\mathbb{Q}=0$ and $G\otimes\mathbb{Z}_p=0$ for all primes $p$, then $G=0$. For we can write $G=\mathbb{Z}^r\oplus\bigoplus\mathbb{Z}_{p_i^{k_i}}$. Tensoring with $\mathbb{Q}$ kills torsion and gives $G\otimes\mathbb{Q}=\mathbb{Q}^r=0$, whence $r=0$, so $G=\bigoplus\mathbb{Z}_{p_i^{k_i}}$.
But now tensoring with $\mathbb{Z}_p$ kills $\mathbb{Z}_{q^k}$ for any prime $q\neq p$, so $G\otimes\mathbb{Z}_p=\bigoplus\mathbb{Z}_{p^{k_i}}=0$ (my indices suck, but w/
but I think for a not f.g. group, the result only remains true if you have the hypothesis in all degrees simultaneously and it's a homological argument with the Tor functor instead
but I haven't really thought about this
@user2103480 I would say that's a misrepresentation.
makes sense
@TedShifrin it surely is, I was mostly joking
Mostly?
well, it's a natural isomorphism, isn't it?
So what?
01:38
that means that I can reasonably compute deRham cohomology of some spaces with this method
the integrand is dual to the integree
I think I just made that word up
I give up.
Just claim 0 understanding of the concept and be honest.
I could do that but that wouldn't annoy anyone
of course knowing either per se doesn't help understanding the other, but I do think understanding why they are isomorphic generates insight
Does anyone have a good link of the derivation of the general solution to the classic wave equation, however with an extra d/dt term in it?
I’m only familiar with the classic one, i.e. with a single d^2/dt^2 term.
02:03
wait no, I'm being stupid in some way, shape or form, but I'm not sure which
a module always injects into the product of its localizations
but the stronger form is not how it's stated in Hatcher, so something is fishy
ah, I figured the issue
Hatcher wants to state an iff. Vanishing of Q- and Z_p-homology does indeed imply vanishing of Z-homology in each degree individually. The converse obviously fails (see projective space), so if you want an iff, you have to make a statement in all degrees simultaneously.
you're putting in too much effort hahaha I'm satisfied with what you told me before
just had to rid me of my self-induced confusion and make sure I didn't exactly blabber anything wrong
also talking about topology here is distracting me from the fact that I'm failing to solve my actual topology homework
fair enough
@Thorgott what course is that?
it's called "Topologie II", but it's effectively algebraic topology without any homotopy theory, but with characteristic classes
??? what is your "Topologie I" then
My course is also "Topologie II" kek
Is that some Bonn-type snobbery
They start with "Elements of Geometry and Topology" which is basically topology I, then do Topologie I + II where they handle homology & cohomology in detail, and only then they continue with Algebraische Topologie I + II
02:22
Topologie I was point-set topology, smooth manifolds, vector bundles, de Rham cohomology, that type of stuff
@user2103480 coincidentally, the lecturer is from Bonn
@Thorgott doesnt smell like a coincidence.......
Intro to real analysis in Bonn, first sentence: "Let's start with a short recap of what tempered distributions are"
prerequisites: basic arithmetic
I mean, how do you plan on doing analysis if you don't know distribution theory??
literally doesn't make sense
Where/when did you learn all the homology stuff?
@Thorgott kids these days
I learned it in this lecture
I'm duly impressed
Quick maths
But wtf how many topics do you cover in this lecture
02:31
2+2 is 4, yet I'm currently unable to prove that H^2\otimes H^2->H^4 is surjective
We just did singular homology, then cellular homology, then cohomology and now characteristic classes. The lecture is pretty sparse in some aspects and we have skipped some things like e.g. Poincaré duality. But I've additionally supplied myself by reading a good amount of what's in ch.2/3 of Hatcher along the way.
Um, it isn't.
in a specific case, Ted
Well, you didn’t say that, did you?
I didn't, because it would've constituted extraneous typing effort that I wasn't willing to expend since it wouldn't have elevated the joke.
@TedShifrin he also only said that he is unable to prove it, not that it's correct!
02:38
also true
You Germans are particularly obnoxious tonight!
(though it should be correct)
@Thorgott googled it. weird syllabus. And all that in only one weekly lecture?
And you use homotopy groups to define (co)homology groups?
ah no, we didn't talk about homotopy groups at all
the syllabus on the webpage is mostly inaccurate
we did a spontaneous democratic voting on the syllabus in the first lecture
Oh okay. So it's more like the syllabus of the 2019 version?
02:43
dunno man, why would I know the 2019 syllabus
Where it was just fundamental groups, singular (co)homology
and poincare duality, but he said you skipped that
yeah, no Poincaré duality, also not even fundamental groups
homotopy theory-free zone
Probabilists are really business in comparison to topologists lol
(but it turns out I will have to know a lot about higher homotopy groups of spheres to understand the computation of the rational cobordism ring, so that's a temporary bummer)
Legend says one of our probability profs in cologne, who did his PhD in berlin, came into uni with a berghain t-shirt once
He always put some weird-ass emblems on exercise sheets
02:47
@Thorgott Talk me through this and I can comment on anything I know you need to know
@user2103480 lmao
@MikeMiller no, way too complicated (for me)
@Thorgott and they changed
is that Mozart
uni was really an entertaining affair if one paid attention to the details. Can't cope with the fact that it's over soon
@Thorgott no clue
03:06
oh shit, it's already 4am
I will now switch from detracting myself from my homework to pretending it's too late to solve it altogether
this is the right way of solving problems
mood
Instead of studying I'm now looking in awe at the types of probability theory used in population genetics
hey all. does the fundamental theorem of algebra say anything about functions containing trigonometric terms. for instance, $x^2 + 10 \cos(x)$
03:46
What is a polynomial? Hmm ...
04:18
Does anyone have any opinions on what the word "positive" should mean "by default" in this question?
2
Q: Why is the transpose of a density matrix positive and trace preserving?

heromanoWith density matrix $\rho=\sum_{a,b=0}^1\rho_{a,b}|a\rangle\langle b|$ and it's transpose $\rho^T=\sum_{a,b=0}^1\rho_{a,b}|b\rangle\langle a|$. How to confirm that $\rho^T$ is positive and trace preserving.

123
123
04:48
Hello Guys..
 
2 hours later…
06:27
Any hints for Question 3...
07:26
Got it!
07:54
@TedShifrin Isn't it a chain of islands in the Pacific Ocean?
 
2 hours later…
09:45
hello everyone
can anyone help me with this?
We need to find the rank of the matrix:

\begin{bmatrix}
0&c_{1}&-b_{1}&a_{2}\\
-c_{1}&0&a_{1}&b_{2}\\
b_{1}&-a_{1}&0&c_{2}\\
-a_{2}&-b_{2}&-c_{2}&0
\end{bmatrix}

Where all $a_{i},b_{i},c_{i}$ are non zero.

The only thing I could observe was the given matrix is *skew-symmetric*, and the determinant is $(a_{1}a_{2}+b_{1}b_{2}+c_{1}c_{2})^2.$However I could not proceed any further than that. The rank is ofcourse = the number of non zero rows in the row echelon form of the matrix, but taking that route seems to be too tedious , and I believe the purpose of giving a skew symmetric matrix was
10:36
@Astyx thanks
by the way do u have any different approach other than thus
I got this one but still if anyone have one more way to look upon the problem I would be happy
11:35
@JackRod is the point of this to get people to work out a youtube video problem for which you already have the solution?
11:53
In Question 4 the no. of solutions will be 2..?(acc to me ), but answer given is 1.
@Rover won't there be 3? one positive, then the negative of that, and then 0
(In principle values )..
@Rover the principal values go from $-\frac\pi2$ to $\frac\pi2$
Yes, ok x= -1,1,0..?
@Rover yes
what I meant was the principal value if arcsin was in that range.
12:03
Ok
So it seems answer given is wrong..
Ans should be 3. For x=1(2Tan^-1(1)=pi/2,5pi/4(not in principle value ) and similar for x=-1 and one solution x=0 .
Am I right ..?( To change the answer)
12:33
Good morning
Example of a function that has $\mathrm{Re}(z)=0$ and $\mathrm{Re}(z)=1$ as a natural boundary, and is analytic only in $(0,1)?$
A modular function, has a natural boundary and is on the upper half plane
12:51
@satan29 The rank of a matrix $M$ is the largest integer $n$ such that an $n\times n$ submatrix of $M$ is invertible (resp has maximal rank, resp has nonzero determinant)
so here "determinants of the third order" refer to the determinants of the $3\times 3$ submatrices
 
2 hours later…
14:38
@Astyx but there will be so many submtarices
how can we claim that all of them will have determinant=0?
read Astyx' message again, it already answers that
i did not understand "resp" in the context...respectively?
still no clue
which part is unclear?
14:53
How is it that in my matrix, all 3x3 submatrices have zero determinant
what would happens if one had non-zero determinant
No clue
you just have to quote verbatim from Astyx' comment
I really am lost, his statement made no use of what my particular matrix was
yes, because it explains the general relationship between rank and determinants of submatrices
15:10
right.
So how is it, that in my matrix, ALL submatrices have zero determinant? I cant seem to find any reference to this in his message
15:26
I have to say I am completely lost when it comes to elliptic functions.
15:45
🧐
@satan29 There are 16 such determinants, and since the matrix is very symmetric you can compute them all
hmm actually it might take some work now that I look closer
16:05
ok it works
you need to use the fact that $a_1a_2 + b_1b_2 + c_1c_2 =0$
And things cancel out nicely
hint: the determinant of a submatrix not on the diagonal can be factored by one of the terms
Thanks a lot @Astyx , I think I can make some headway now
glad to help
Is the integral $$\int_{0}^{2\pi}\int_{0}^{2\pi}\left[\cos(nx + y)\right]^p\text{ d}x\text{ d}y$$
a well-known value, where $p$ is an arbitrary integer, and $n \geq 1$ is an integer?
It appears that if $p$ is odd, the integral is $0$. I've not figured out what the even pattern is yet.
16:21
You can linearize $\cos^p$
What does that mean?
Write as a sum of trigonometric functions
This sounds like Fourier stuff
Using $\cos x = (e^{ix}+e^{-ix})/2$
it isn't
Wait a sec
Okay, that looks like a good idea, but what do you do with $(e^{ix} + e^{-ix})^p$?
16:23
You expand and it should give you terms like $\cos kx$
A linear combination of those at least
You should work those out yourself if you have never done it, but here' the general result
Sorry, more specifically... so you get $(e^{i(nx+y)} + e^{-i(nx+y)})^p$ and then you rewrite that as $(2\cos(i(nx + y)) + \sin(i(nx+y)) + \sin(-i(nx+y)))^p$, so at the end, using $\sin(x) = -\sin(x)$, this appears to be $2^p\cos^p(i(nx+y))$ if I did it right
Whoops
Those $i$s should not be in there
but basically, you end up with $2^p\cos^p(nx+y)$
No that's the wrong idea, we made the exponentials appear to use the fact that $(e^{ix})^k = e^{ikx}$
I think he's looking for the keyword "Binomial theorem"
I literally typed that in the message I was going to send :)
Oh, so the binomial theorem applies to complex numbers? Learned something new today
16:28
it's purely algebraic
$(a+b)^n=\sum{n\choose k} a^kb^{n-k}$ in any commutative ring
So, just based on my rusty algebra from 10+ years ago, my guess is you could probably extend that to general field...
Ah, thanks
You're smashing the expression with a+b repeatedly and using some binomial identities
even in a commutative rig
Okay, so let's use the binomial theorem... you would get
$$(e^{i(nx+y)} + e^{-i(nx+y)})^p = \sum_{k=0}^{p}\binom{p}{k}e^{ik(nx+y)}e^{-i(p-k)(nx+y)}$$
and then we want to integrate this with respect to $x$ and then with respect to $y$...
@Clarinetist You could do this, but I believe it's easier if you regroup exponentials together to form trig functions again
16:38
@Astyx Right, so it looks like in the summation, I get $\binom{p}{k}e^{in(2k-p)x}e^{in(2k-p)y}$... so I assume we then convert these to the complex $\cos + i \sin$ forms
I think you can put everything in the same exponential
So then we get $\binom{p}{k}e^{in(2k-p)(x+y)}$
And then you should try to find identities of the form $e^{ia}+e^{-ia}$
(your n is not in the right place)
Let me try this again
Hmm
$ik(nx+y) - i(p-k)(nx+y) = ik(nx+y) - ip(nx+y) + ik(nx+y) = 2ik(nx+y) - ip(nx+y) = (2ik + ip)(nx+y)$, ah, there we go
and so we end up with $i(2k+p)(nx+y)$
16:45
Whoops, thanks
So then we end up with $$\sum_{k=0}^{p}\binom{p}{k}e^{i(2k-p)(nx+y)}$$
Now here I'm stuck. So you said to make use of identities of the form $e^{ia} + e^{-ia}$. How does that work here?
split the sum in 2
Separating the $x$ and the $y$?
Or alternatively take twice the sum, but make the index of one um go from p to 0
no, in terms of k
We want to use that ${n\choose k} = {n\choose n-k}$
$$\Huge{TESTING}$$
Hmm, I'm not seeing what you're trying to explain here.
16:51
What happens when you replace k by n-k in the sum?
Well, let's see. Let $t = n - k$, then since $k$ goes from $0$ to $p$, we have that $t$ goes from $n$ to $n-p$... so we would end up with $\sum_{t=n-p}^{n}\binom{n-p}{n}$ with the exponential in the summation... I have a feeling this is not what you intended
Oh sorry, I meant p-k, not n-k
Oh, k. So let's let $t = p - k$. Then we have that $k$ goes from $0$ to $p$, so that $t$ goes from $p$ to $0$, and we have $k = p - t$ so that $2k = 2p - 2t$ and $2k - p = p - 2t$, hence we have$$\sum_{t=0}^{p}\binom{p}{p-t}e^{i(p-2t)(nx+y)}$$ assuming I did the binomial coefficient right
Seems correct so far. Do you agree that this is the same sum as with k? also you can simplify that binomial coefficient
Right, per the identity you gave, we have $\binom{p}{p-t} = \binom{p}{t}$
17:02
@MaryStar: did you see the animation of the oblate spheroid?
@Astyx So yes, I'd agree they're the same sum, but how does this help me translate to trig functions? I suppose... Oh, I see what's going on here. Pull out a negative from $(p-2t)$...
right
Then the sum is the half of twice the sum, invert one, regroup the terms, make \cos appear
So then you basically get... what is this...
$$2(e^{i(nx+y)} + e^{-i(nx+y)})^p = \sum_{k=0}^{p}\binom{p}{k}\left[e^{i(2k-p)(nx+y)} + e^{-i(2k-p)(nx+y)} \right]$$
Great
So from there I believe you got it?
And divide by $2$, you get...
$$(e^{i(nx+y)} + e^{-i(nx+y)})^p = \sum_{k=0}^{p}\binom{p}{k}\cos((2k-p)(nx+y))$$
And then divide by $2^p$, you get...
$$(\cos(nx+y))^p = \dfrac{1}{2^p}\sum_{k=0}^{p}\binom{p}{k}\cos((2k-p)(nx+y))$$
@Astyx Does this look right?
17:10
yes
Wow. Where do you learn this stuff?
(I didn't check the details but you're on the right track)
By dealing with trig functions for long enough I guess?
So for the double integral of this over $[0, 2\pi] \times [0, 2\pi]$, I assume we're probably going to want to use the addition identity on the right-hand side
Whenever you want to integrate powers of cos/sin you prefer to do this because it's easy to integrate linear trig function
Well, thank you so much for being patient with me on this
I hopefully have enough to go on at this point
17:19
glad to help
ok so I didn't look at this stuff for a few days and it leaked out of my head a little bit
Salut, @Astyx. Howdy, @Clarinet, @BigS
salut!
Hey there @TedShifrin
Writing up a big ole question atm
As in writing up the solution?
17:28
Nah, to ask here
@Astyx So let's say I wanted to integrate something like $(e^{i(nx_1 + y_1)})^p(e^{i(mx_2 + y_2)})^q$ over the same domain in 4-space (i.e., $[0, 2\pi]$ each variable). Would this approach make sense?
"this approach" meaning the one I provided earlier
Looks boring.
where $p, q$ are integers
17:29
Still boring. ;)
well, yes, but in this particular instance you're able to separate the integral in two
Luckily, we know a rule for $(e^a)^b$.
Right, so you would write this as $$e^{i[(nx_1 + y_1)p + (mx_2 + y_2)q]}$$
@TedShifrin Feeling listless this morning?
@robjohn Are you going to quote Lucy Ricardo and the Vitameatavegamin ad? :D
17:32
@TedShifrin Don't tempt me...
or rather
Every time you say "listless" I think of that.
I'm sure we can come up with some lists, though.
What would be most useful, @Clarinet if you wanted to integrate, say, first with respect to $y_1$?
@TedShifrin Right, so you could split this
$$e^{inpx_1}e^{ipy_1}e^{mqx_2}e^{qy_2}$$
There you go.
and I imagine Fubini works over complex functions...
or something like that
17:34
Of course.
Most of integration theory is done with $\Bbb C$-valued functions, in fact. You just don't notice.
Whoops, forgot the $i$s
$$e^{inpx_1}e^{ipy_1}e^{imqx_2}e^{iqy_2}$$
Yeah, but you only care about one particular factor here.
Let's say we got $C_f := k[x,y]/(f)$ where $f$ an irreducible poly in $k[x,y]$, and $k$ alg. closed. Say we want factor the ideal $(x-a)$ explicitly as a product of prime ideals (I think this was building up to the fact that we can only do that when our noetherian domain of dimension 1 is a Dedekind domain).

We write $f(a,y) := c \Pi_{i=1}^s (y-b_i)^{e_i}$ (with $b_i \neq b_j$ whenever $i \neq j$) so that $f(x,y) = (x-a)g(x,y) + c \Pi_{i=1}^s (y-b_i)^{e_i}$ with $g(x,y) \in k[x,y]$ and $M_i := (x-a , y-b_i)$ would be the maximal ideals of $C_f$ that contain $(x-a)$.
So let's integrate this over 4-space
$$\int_{0}^{2\pi}e^{inpx_1}\text{ d}x_1 \cdot \int_{0}^{2\pi}e^{ipy_1}\text{ d}y_1 \cdot \int_{0}^{2\pi}e^{imqx_2}\text{ d}x_2 \cdot \int_{0}^{2\pi}e^{iqy_2}\text{ d}y_2$$
@TedShifrin muggles don't see nothin', do they?
17:38
Naively, I would think that this would result in
$$\dfrac{1}{inp}(e^{2\pi i} - 1) \cdot \dfrac{1}{ip}(e^{2\pi i} - 1) \cdot \dfrac{1}{imq}(e^{2\pi i} - 1) \cdot \dfrac{1}{iq}(e^{2 \pi i} - 1)$$
but of course, you're talking to someone who's never taken a course on complex variables
@robjohn is in a very whisper-loudly-in-an-aside mood today :P
You lost exponents @Clarinet. The FTC has nothing to do with complex analysis.
What you need to know is that whenever $p$ is an integer, $e^{2\pi i p} = 1$. But this doesn't work for non-integers, of course.
@TedShifrin Hi, here's a random observation. Suppose $X$ is a stratified space with two strata, and you chip off a little piece out of the bottom stratum
$$\dfrac{1}{inp}(e^{2\pi inp} - 1) \cdot \dfrac{1}{ip}(e^{2\pi ip} - 1) \cdot \dfrac{1}{imq}(e^{2\pi imq} - 1) \cdot \dfrac{1}{iq}(e^{2 \pi iq} - 1)$$
Hopefully this is right...
17:41
@Balarka: So the lower stratum isn't just points?
@Clarinet: You actually only need to evaluate one of those and see it is $0$.
No
Could be any dimension
Right, that entire thing is $0$... hmm.
I guess you'll tell me what "chip off" means.
Often in Fourier analysis there's a conjugation that appears somewhere? @ Clarinet
Say the normal link at any point of the bottom stratum is $A$, then chipping out a little neighborhood of a closed disk on the bottom stratum is tantamount to chipping off $(A \times D^n) \cup_{A \times \partial D^n} (C(A) \times \partial D^n)$
I.e., the inner product is defined by integrating $f\bar g$, not $fg$. @Clarinet
17:43
@robjohn tfw I am a muggle
And @BigSocks loves to mug for the camera, too.
hops around, mugging
I have a mug of chai that I'm drinking currently
This one isn't a Fourier problem, thankfully. But if this is true... this must mean that complex random variables to some powers, when multiplied, have moments equal to $0$ if we assume $x_1, y_1, x_2, y_2$ are uniformly distributed in $[0, 2\pi]$...
17:45
So, where are you going, @Balarka? What if we take the simplest example and do $xy=0$ in $\Bbb A^3$?
@BigSocks Breakfast this morning was cinnamon raisin bread, cheese, and chai (from Trader Joe's)
@Clarinet: You're talking only about $e^{iX}$, not general complex random variables.
@robjohn what kind of cheese? I wish I had chai from Trader Joe's. (it's my favorite, but there's no Trader Joe's here)
So here is a picture. $L, S$ are the two strata, of dimension $m > n$ and $n$ respectively.
17:47
@TedShifrin Ah, I agree
$A$ is the normal link of $S$ in $L$, drawn in blue.
$D^n \subset S$ is a closed chart.
@BigSocks Gouda, Havarti, Swiss, and Cheddar.
Seems like most probability books avoid any discussion of complex random variables for some reason
I chip out a closed neighborhood of the stratified space $S \cup L$ containing $D^n$; this is gonna look like $D^n \times C(A)$.
@robjohn now that is a well balanced cheese breakfast
17:48
Once I remove it, it leaves off a boundary, which is $(A \times D^n) \cup_{A \times \partial D^{n-1}} (C(A) \times \partial D^{n-1})$.
So I like my example, because the link is more interesting @Balarka.
$xy = 0$ in $\Bbb C^3$ or $\Bbb C^2$?
$\Bbb C^3$.
Two transverse planes intersecting along a line.
Well for $\Bbb C^3$ the picture is the same as $\Bbb C^2$ (where link is Hopf around origin) $\times \Bbb C$, I suppose.
Yes, but you weren't going to allow a $0$-dimensional stratum. But, yes, product. To warm up.
17:50
So normal link is Hopf
Yeah
Got why you did that now
0
Q: Group acting properly on $\Bbb R^2$ and restriction of a covering map, part $2$

MathloverThis post comes out from another question in the comment box of this answer. Let $G$ be a free group with countable-infinitely many generators acting on $\Bbb R^2$ properly, and $H\subsetneqq G$ be an infinite cyclic subgroup of $G$. Let $p:\Bbb R^2\to \Bbb R^2/H$ be the orbit map, i.e., a coveri...

Any help?
So I guess if you chip off a little closed disk $D = D(0; R) \subset \Bbb C$ (and all the normal junk around it) from the singular stratum, you cut out $D \times C(S^1 \sqcup S^1)$ basically, which leaves off a boundary that is two copies $S^1 \times D^2 \times \{i\}$ with a double cone filling in every pair $S^1 \times \{x\} \times \{0, 1\}$ for all $x \in \partial D^2$.
$C(S^1 \sqcup S^1)$ = Double Cone
The cone on the link should (at least up to homotopy) just be a neighborhood of our piece of stratum.
Yeah, the topological type (not upto homotopy) is (piece of stratum) x cone(link)
Aha, I see what's going on. It's like, initially you had the constant family of a pair of hyperplanes in $\Bbb C^2$ which kept intersecting at $0$ transversely. Now you do some kind of stratified surgery at the origin such that in a little neighborhood it looks like the family which is a pair of transverse hyperplanes in $\Bbb C^2$, then became the family $xy = 1$ (by the homotopy $xy = t$, $0 \leq t \leq 1$), and then back to transversely intersecting hyperplanes again
This is the AG picture
You desingularize and resingularize quickly
This is like the Milnor fiber game for smoothing isolated singularities.
18:01
Oh, really? It's about time I learn it, ugh
Except the family is mostly the cone, not going from hyperboloid of one sheet to cone to hyperboloid of two sheets
I learned it early on because of Griffiths's work tying it into curvature integrals and integral geometry.
(Remembered this picture from elsewhere, in a different context)
Your example and the Milnor fiber comment is very interesting because that means my chipping operation is hopefully algebraically meaningful. I am trying to do something which only happens upto chipping, and I was wondering how much you lose.
So the differential geometry question is to compare the integral of curvature on a neighborhood in the smoothing with the integral of curvature on a neighborhood of the singular thing. There is a defect, which you can interpret in terms of Gauss maps.
Yeah, I'm not enough of a topologist to intuit your chipping :)
@TedShifrin Ah, this is cool.
Linda Ness and Gary Kennedy wrote papers on these things back in the late 70s, early 80s.
18:05
This is the Ness of Kempf-Ness?
Cool!!
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