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00:00 - 17:0017:00 - 00:00

17:00
Oh wow try a two-parameter perturbation
$z^3 + tx + sy$
The leminscate at $(t, s) = (1, 0)$ desingularizes in two ways if you move $s$ to be positive or negative respectively
This is incredibly rich
Looks like Thorgott's having lots of fun with Mathematica :)
Poor folks like us use desmos instead
Yeah, but I confess that now that I retired and no longer had access to Mathematica from the university, I gave in and paid money to own my own.
Ah, English.
lol
that is desmos
17:05
Next semester I'll get Matlab access hopefully
I hate Matlab. I found it so clunky and never got close to mastering it.
Have it in my course
Huh
I'm not even sure what Balarka's endgoal is, but this stuff looks cool
Gotta go shopping now, but I'll check in again later
I'm a man with no mission
Just demonstrating the fact that fold singularities are incredibly generic whereas holomorphic singularities are incredibly unstable
It's an old theorem that maps which are nonsingular everywhere except a 1-dimensional submanifold along which fold singularities occur form a stable generic subset of $C^\infty(\Bbb R^2, \Bbb R^2)$
this is one of the weirder series expansions I've seen:
$$h(x) = x^{1/2} - 1 + \frac12 x^{-1/4} - x^{-1}
\sum_{k=2}^\infty 2^{-k}(x^{-2^{-k}} - x^{-\frac32 2^{-k}})$$
17:17
I don't use software
first time I've seen a lacunary series show up as part of an actual answer
well
i guess it's not really lacunary. smaller and smaller exponents
@BalarkaSen How is that stable
Stable means open right
But why can't I just take the codimwnsion 1 subset, and instead of folding along it, first collapse a tubular Nbhd then good
Then fold
Is that a smooth homotopy?
Feel like I can make it smooth using a bump function trick.
Yeah, seems like it should work
17:22
Maybe that would start from something with an e^(-1/x^2) singularity along the codim 1 guy?
Which wouldn't be a fold
Ah, possibly
@BalarkaSen Consider the graph of the map f, let's say it's a self map. Then the fold singularities are presumably transverse intersections of the graph with the diagonal?
That would explain why the folding submanifolds still make sense after perturbation
Oh, if they were transverse they'd be isolated f.p. lol.
But there should be something you're using here
I sort of buy it now
It's transverse in the sense that if you look at the space of jets they're the ones with rank 1 singularities
Rank 1 is the top stratum of the singular substratified space of M_{2x2}(R)
So yes, you can prove it by transversality
Ok.
So you get stability of fold sets and this is enough to convince me stability in general
Just to write it down: A map $f : \Bbb R^2 \to \Bbb R^2$ gives rise to a holonomic section of the jet bundle $J^1(\Bbb R^2, \Bbb R^2) \to \Bbb R^2$, with fibers $M_{2 \times 2}(\Bbb R)$, and the singular matrices fiberwise forms a stratified subset $S$ of $J^1(\Bbb R^2, \Bbb R^2)$. By Thom transversality you can homotope the section $j^1 f : \Bbb R^2 \to J^1(\Bbb R^2, \Bbb R^2)$ a tiny bit so that it's 1) transverse to $S$ and 2) still holonomic
17:41
$J^1(\Bbb R^2 \times \Bbb R^2) = \Bbb R^2 \times \Bbb R^2 \times M_{2 \times 2}(\Bbb R)$ is an $8$-dimensional space, and $S$ is cut out by $\det = 0$ fiberwise so that it's $7$-dimensional. The section has dimension $2$
So they intersect in a codimension $\codim j^1 f + \codim S = 6 + 1 = 7$ dimensional subset, i.e., a dimension $1$ stratified subset.
So maps $f : \Bbb R^2 \to \Bbb R^2$ with folds and cusps as singularities (the singularity set is Whitney stratified with 1-stratum of folds and 0-stratum of cusps) forms a stable generic family by transversality.
The cusps are somehow not a problem if everything is oriented, but I dunno how to do this bit.
google doesn't give me a satisfying answer: what's a fold singularity?
@Thorgott Fold a piece of paper
Couldn't have put it better myself. It's essentially any singularity which locally looks like folding a piece of paper along a line, like $f(x, y) = (x, y^2)$
Aka locally your map is modeled on $M \times I \to M \times I$, given by $(m, t) \mapsto (m, t^2)$. I'd use $|t|$ if it were smooth
They also call Morse-type singularities fold in higher dimensions, $f : \Bbb R^m \times \Bbb R^n \to \Bbb R^m \times \Bbb R$, $f(x, y) = (x, y_1^2 + \cdots + y_k^2 - y_{k+1}^2 - \cdots - y_n^2)$
Morse along one factor
The cusps are like the Cerf-type singularities, appearing where two fold-lines meet tangentially
$f : \Bbb R^m \times \Bbb R^n \times \Bbb R \to \Bbb R^m \times \Bbb R$, $f(x, y, z) = (x, z^3 - 3yz + y_1^2 + \cdots + y_k^2 - y_{k+1}^2 - \cdots - y_n^2)$
I should eventually learn to see how handle-cancellation happens geometrically
18:16
I can see how $(x,y)\mapsto(x,|y|)$ would look like folding a piece of paper (along the $x$-axis), but $(x,y)\mapsto(x,y^2)$ does involve some stretching too.
hmm. trying to find a function $f(x)$ which behaves like $x$ for small $x$ and like $\sqrt{x}-1$ for large $x$
@Thorgott Yeah it's just doing it smoothly.
the best so far is $\sqrt{1+2x}-1$ which works for small $x$ but behaves like $\sqrt{2x}-1$ for large $x$
I agree there's some stretch. You cannot fold a piece of paper in real life smoothly
If it was made of rubber you could, by the $y^2$ trick
Hm
also, it should be a smooth monotonic function
18:21
If you project it parallely to your plane of vision, the set of singular points looks like this:
so $1/(1/x-1/(\sqrt{x}-1))$ doesn't work despite having the right asymptotics
I wonder how it'd modify the immersion if I tried to cancel a pair of cusps on the diagram
Hmm, ok. And how is the notion of "locally looks like" captured here? Composition with a diffeomorphism?
that looks trefoil-y
@Thorgott Yeah, I say two maps $f, g : \Bbb R^2 \to \Bbb R^2$ looks the same if there are diffeomorphisms $\phi, \psi : \Bbb R^2 \to \Bbb R^2$ such that $\phi \circ f = g \circ \psi$
Basically "after reparamatrization on both domain and codomain", $f$ and $g$ match
@Semiclassical It's really a planar diagram though
18:27
so equivalent up to composition with diffs?
@BalarkaSen ah
I wouldn't say that, I'd just say equivalent upto change of coordinates
fair enough
"there exists $\phi$ such that $f = g \circ \phi$" or "there exists $\phi$ such that $f = \phi \circ g \circ \phi^{-1}$" are all different notions
The latter is known as smooth conjugacy
"or equivalent as dynamical systems"
oh, nice. I've seen that concept before
the former, I dunno if it has a name, but you could study stuff like that. You're only allowing reparametrizations on the domain basically, so it captures topology of the map
18:30
vis a vis logistic map versus tent-map
or whichever conjugacy it is
yeah
Hmmmm
Ok, makes sense. Can maps be classified up to locally looking like one another by the behavior of their rank? In the case of constant rank, I know this to be true.
This looks suspiciously like the swallowtail singularity
That's like cancelling two cusps right
I never actually understood the swallowtail catastrophe, but I guess I see the point now
@Thorgott For maps between 2-manifolds, yes. But in higher dimension this gets much, much harder
You can have different singularities of the same rank, interacting with each other. The whole setup is known as the Thom-Boardman hierarchy.
I don't understand it well
Huh, sounds cool
18:48
$\frac{\ln(x)\ln(y)}{\ln(1-x)\ln(1-y)}=1 $
is it possible to solve for $y$?
@BalarkaSen the answer being yes there's a classification no it's much worse than rank
hahah
yeah
Damn this stuff is so beautiful why is this branch dead
I hate mathematicians
19:11
@BalarkaSen Sociology
Not enough problems to build a community of grad students around
If you can't do that a field dissipates
Makes sense
19:32
Define $f : \Bbb{Z}/(q_1\cdots q_r)^* \to \Bbb{Z}/(q_1 \cdots q_{r-1})^*$ by $f(x) = x^2$ is surjective right?
where $q_i$ are the first odd primes
or any odd primes
@Ultradark
@JinLong
19:48
@shi I have no idea
20:12
What are the unknown knowns
Who knows
goodbit
the answer to that question I asked above is $y=1-x$ lol
$\frac{\ln(x)\ln(y)}{\ln(1-x)\ln(1-y)}=1$
$\frac{\ln(x)\ln(y)}{\ln(1-x)\ln(1-y)}=2$
not sure how to solve for this though
It's almost as if the 2 wreaks havoc on the distribution of prime numbers
20:34
a @Balarka: With McCrory and Varley I wrote several papers largely on singularity theory. I don't remember if I sent you copies of all. I know I sent one or two.
@TedShifrin Yeah you sent me one about singularities of Gauss maps on hypersurfaces.
OK, you can find all sorts of versal unfolding stuff in there :P
There were ultimately 4 papers, I think, plus one monster one that never got written.
@BalarkaSen play?
Not now @Leaky
@TedShifrin I first learnt about Nash blowups from your paper, I think
Wow I am staring at your paper right now, this looks so good
here's a recent talk by grant sanderson (3blue1brown) at mit if anyone's interested
20:45
@loch next time you should delete the fbclid parameter :P
@Balarka: The Gauss map for surfaces in $\Bbb P^3$ was first; the big one you have, I think, was for threefolds in $\Bbb P^4$. Then there are some on theta divisors.
oh
let me try again
Yeah it's about threefolds in $\Bbb P^4$
@loch halp i'm jetlagged
The one for $\Bbb P^3$ is a good warmup.
20:47
@LeakyNun you're in hk?
@Leaky, are you back home?
i see
im arriving hk on 26
nice
@loch what's the main point of the video?
ok i dont think i'll be doxxed with this link
20:49
nice
I'll doxx u
it's about story telling
pls
boo
ask 3b1b to make a video on catastrophe theory
go be a patreon
What the hell is that?
20:54
@JinLong catastrophe theory
its singularity theory taken over by cranks
What does this image represent?
this was popular back in the day
catastrophe theory
Good poster
20:54
René Thom had all sorts of essays to popularize this stuff.
Interesting.
Thom said he switched to catastrophe theory because he couldn't understand what people were doing with Thom spectra
its in some interview
he was like I give up
cant keep up with these homotopy theorists
I didn't read that, but I believe it.
Here is a puzzle for you
You live on an island in which everyone wears a hat, either blue or red.
@TedShifrin I borrowed a book by Arnold which discusses applications of singularity theory in contemporary science. It's a very thin book called "Catastrophe Theory"
It's very good
20:58
If you read Arnold to get the ideas, and not the details, he's wonderful.
In McCrory's and my paper on surfaces in $\Bbb P^3$, we spent five pages proving something Arnold totally handwaved in an earlier paper.
Hahah
amazing
He just asserted "generically," and never justified it remotely.
You've misplaced your hat. Everyone is staring at you. It's clear you're not welcome.
The horde of hatted people begin to approach you, chanting "no hat. No hat. No hat".
You walk backwards as they chase you towards the edge of the island. The water does not stop them.
wonders if he stepped into a Trump rally with hats
This sounds like the humanity test in Blade Runner.
20:59
As you begin to drown you ask: "what did I do to deserve this?"
That's it.
nice puzzle
very puzzling indeed
Oh, I missed the introduction.
@MikeMiller Clearly, the answer is he misplaced his hat
@JinLong I wasn't trying to channel Voight Kampff but I see your point
This doesn't seem quite like the colored dot puzzle.
21:01
@MikeMiller what were you trying to do?
Someone mentioned 3b1b so I was just trying to suggest a math puzzle
But everyone knows the usual hat game so I figured it's better to try something new
I forgot "Here is a puzzle for you" is what he starts with
You left out the "puzzle" part tho
Nah check 2 minutes before the start
I just had to write the puzzle bro
Everyone's ganging up on me for providing content
It's very funny if I imagine it said in 3B1B voice
21:04
Maybe don't introduce it with "here's a puzzle for you"
@BalarkaSen 2-day correspondence?
Nah mane
That's too long
I'll play eventually
But instead, more accurately, describe it as "here's a bit of nonsensical content that is not at all a puzzle"
what is it with you
@LeakyNun is that chess?
21:05
he's triggered because he wanted a genuine puzzle
I'm leaving before the riot/fight breaks out. BBIAB.
I have this weird notion that when someone presents a puzzle, I expect it to be an actual puzzle.
Bizarre I know.
If $\mathbb{P}$ is a probability measure, $X$ a random variable and $x$ an arbitrary realization of $X$, does it ever make sense to write $\mathbb{P}(X)$ or $\mathbb{P}(x)$? If yes, what would these notations more precisely mean (in terms of measure theory)? Note that I know that $\mathbb{P}(X=x)$ is an abbreviation for something else (which I don't want to write here)!
@MikeMiller that's what happens when we're out of proofs for twin primes
21:06
lol
@nbro $\mathbb P(X=x)$
@loch We should move on to triplet primes
Prove that there are infinitely many triples (p, p+2, p+4) with all three terms prime
as a wise man once said
Sep 2 '14 at 18:34, by Karl Kronenfeld
The conjecture relating to the number of twin primes is too difficult though, so I stick to prime twins
according to Dirichlet's theorem there are arbitrarily long arithmetic sequences in the set of primes
Of course you get TWO copies of the twin prime conjecture as a corollary
@LeakyNun Yes, I've edited my comment to include that I know I can do that. However, in statistics, we often see $P(X)$ or $P(x), so I am wondering what those expressions would more precisely mean.
21:08
OH lmao
One from (p, p+2) and one from (p+2,p+4)
Sep 2 '14 at 18:37, by Karl Kronenfeld
@PedroTamaroff I am working with EnjoysMath
@ShineOnYouCrazyDiamond You have been doing this for a long time aren't you
what are prime twins?
For example, in this blog post https://blog.tensorflow.org/2019/03/regression-with-probabilistic-layers-in.html, the authors wrote that $Q(w)$ is a probability distribution. Is $Q(w)$ a probability measure, cdf, or what? If it's a probability measure, what does $Q(w)$ exactly mean?
Read a book on probability dude
5
21:10
@nbro can you quote?
I would like to note that I am very familiar with machine learning and probability concepts. I just would like to have a more rigorous (measure-theoretic) explanation of this notation and terminology.
where did they say that Q(w) is a probability distribution?
> layer uses a variational posterior Q(w) over the weights to represent the uncertainty in their values. This layer regularizes Q(w) to be close to the prior distribution P(w)
P(w) is thus a distribution, so Q(w) must also be a distribution.
Are they referring to probability measures, cdfs, or what?
it's a distribution
lol
Is this your explanation? It's a distribution? This is written in the article.
21:13
it's a random variable
lol
A distribution or random variable? And, when you say "distribution", are you referring to a probability measure?
You're acting very high and mighty for someone who refuses to read a book
9
@MikeMiller I will read maybe in the future, but definitely not now (I don't have time for that now). I've already read books on probability in the past. And what? You forgot stuff after 1 week. Everyone forgets. That's part of the plasticity of our brain!
Why does this chat exist? If you're not willing to answer, just ignore my messages or questions.
is the distribution the random variable? they feel kinda different for me
You're the mathematician (not me) :) I studied computer science and AI.
21:17
a distribution is characterized by a measurable function from a probability space to R, how about this
but is it the function?
@MikeMiller I don't know about this
it feels like a philosophical question
The random variable induces a probability measure. The random variable is the measurable function.
@LeakyNun there is no loss of information in saying a distribution is a probability measure. dont respond if you dont know definitively
a random variable is said to follow a distribution if the induced measure is that distribution
'aight
@nbro i am not a statistician** , but my guess is that for the formulas in the link they're referring to the corresponding density functions
@loch However, in that article, they are talking about "variational inference". All variational inference is about approximating a usually called "distribution" (the posterior) with another "distribution"
21:31
yes but when densities exist they're "the same thing"! (meaning from a pdf you can get your cdf / your measure etc.)
What if they don't exist? Or when wouldn't they exist?
Singular distributions are the issue
i dont think people care about such high generality so it's not something one has to worry about (KL divergence makes sense in general though - according to my googling skillz)

last time thorgott gave you examples where they don't exist already!
Eg cantor disturbution
Also cases where it’s a mixture of discrete and continuous, tho thorgott already covered that
its a theorem that every distribution can be written as a sum of an absolutely continuous part (has a density) and a singular distribution
this is known as the Lebesgue decomposition theorem
21:42
If you’ve got a continuous cdf, then I think it has a density? I could be making too strong a statement tho
Nah that's not true
@Semiclassical i think that's your counterexample :0)
the issue is that they're continuous but not absolutely continuous
21:43
Wait, Cantor is continuous?
Radon--Nikodym requires absolute continuity
Cantor function is continuous yeah
continuity occurs iff singletons have measure zero
absolutely continuity occurs iff Lebesgue-null sets have measure zero
How much smoothness do you need, then? Or is that the wrong question
21:44
Cantor set has Lebesgue measure 0
@Semiclassical if the cdf is of bounded variation then it has a pdf
wiki says:
for a compact interval,

continuously differentiable ⊆ Lipschitz continuous ⊆ absolutely continuous ⊆ bounded variation ⊆ differentiable almost everywhere
ah so what i said is not true
something more is needed
i forget what
21:46
On the other hand, being continuously differentiable suffices
the "Luzin N property"
wiki says $x \sin(1/x)$ is also a counter-example
so there goes your smoothness a.e. assumptions
well the cantor function is smooth a.e. isnt it
oh well
but this is even smooth except on a singleton lol
feels stronger
21:50
@Semiclassical yes because then you can differentiate the cdf and the derivative is integrable with integral the cdf :p
which then is your pdf
the key point here is that you only want the derivative to be integrable not continuous so continuous a.e. is sufficient so Lipschitz continuity is also sufficient because that's equivalent to C^1 a.e.
And tbh that covers most of the practical cases
In most practical cases the cdf will be C^1 minus a few points, so yeah
except if you for some reason decided to take the sum of $X_i$ where $X_i \sim U(0,2^{-i})$
its CDF has a name that escapes my memory
21:54
Ugh
the word "practical" has a meaning!
it starts with F
Mar 29 at 16:37, by Semiclassical
@akiva lots of values of the Fabius function here: https://arxiv.org/pdf/1609.07999.pdf
there you go
anyway nobody actually cares about these wild stuff. regularity is only an important phenomenon in probability when you start thinking about brownian motions
what happens in brownian motions?
with probability 1 the paths are nowhere differentiable
but they are holder continuous i think
i am not sure
21:59
Yeah, this all falls under the heading of “pathological” for me
And I have a hard time getting too interested in it, simply because it’s typically so remote from practice
wait why is brownian motion not practical
it's literally physics
all falls under is too strong, yeah
brownian motion, and stochastic systems in general, are a big exception
i have to learn something about them, someday
same
I know it at the physics level, to an extent
but when I start seeing Ito calculus I know I'm out of my depth
Hahaha
probabilists love Ito
this stuff is too hardcore for me
22:05
who is Ito
Itô calculus, named after Kiyoshi Itô, extends the methods of calculus to stochastic processes such as Brownian motion (see Wiener process). It has important applications in mathematical finance and stochastic differential equations. The central concept is the Itô stochastic integral, a stochastic generalization of the Riemann–Stieltjes integral in analysis. The integrands and the integrators are now stochastic processes: Y t = ∫ 0 t...
technically, I've worked on stochastic calculus stuff
but the work I did was predicated on an approximation method which immediately got rid of explicit stochasticity
("weak noise approximation")
22:20
oh yeah, I remember when a friend told me about one of his assignments last semester and said he has to solve a "stochastic differential equation". I replied "you what?" and I think that's where the conversation ended.
22:36
@Semiclassical Yes, that's right, he had provided an example, even though I hadn't fully understood it
lmao
@BalarkaSen ^
23:11
Why is there no implicit integration
say I have an expression I can't put in explicit form. Then there's no way to integrate it?
If you're talking about indefinite integration, then that exists and it's called solving a differential equation
I have an expression that I can't put in explicit form
I'm trying to figure out how to integrate it definitely
I wonder if it's impossible to represent the function explicitly
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