« first day (3844 days earlier)      last day (1469 days later) » 
00:00 - 19:0019:00 - 00:00

00:00
but ok, with the previous computations, it's clear that this is gonna be transversal to the zero section iff that bottom half is non-degenerate, so that works out
I've talked about this before here and on main (you can search for that phrase). The derivative of a section of a vector bundle is well-defined at a zero of the section without any connection needed on the vector bundle.
00:16
that's the "in general, we need a Riemannian metric to define the Hessian, but at a critical point, we can always do it" point, yes?
the pushforward of the tangent space through the zero section provides a canonical splitting of the tangent spaces of a vector bundle along the zero section
so you have an intrinsic canonical splitting into horizontal and vertical component there
and in this particular case and in coordinates, the vertical projection precisely gives me the part of that matrix that consists of the mixed partials
explicitly in this case, we have $T_{(p,0)}T^{\ast}M\cong T_pM\oplus T_p^{\ast}M$ (image of pushforward of zero section and kernel of pushforward of projection) and the composition $T_pM\rightarrow T_{(p,0)}T^{\ast}M\rightarrow T_p^{\ast}M$, the first map being the differential of $df$ and the second being vertical projection describes a bilinear map $T_pM\times T_pM\rightarrow\mathbb{R}$, which is the Hessian at the critical point
great, I never got this point before, but I think now I do
thanks @Ted
I didn't do much.
00:33
you told me all I needed to figure out the rest
00:47
So apparently an open smooth $n$-manifold $M$ can be embedded in $\mathbb{R}^{2n-1}$. Roughly, I know that $M$ deformation retracts onto an $n-1$-dimensional submanifold $N$, strong Whitney tells me that $N$ embeds in $\mathbb{R}^{2n-2}$ and I would guess/hope that if we then take a tubular neighborhood of $N$ in $\mathbb{R}^{2n-1}$, this will be diffeomorphic to $M$. Is anything remotely close to that true?
Sounds good to me.
01:24
@MikeMiller @Thorgott do you have some easy introductory exercises for getting a feel for local homology
01:37
I don't know if there is all that much to say about local homology. Understand in which sense it is local. Compute it for a smooth manifold relative any point and for any cone relative the cone point.
It came up mainly for justifying degree computations by local degrees and that's been meh for me. My basic intuition atm is via excision, i.e. $H_n(M, M \setminus \{x\}) \simeq H_k(D^n, D^n \setminus \{ x \}$
In a manifold. And it now seems simpler than before lol, maybe the knowledge starts to solidify a little bit
About time though, exam is on the first of march and I genuinely thought it was exactly three weeks away. Then I realized there is no 30th february
Your brains: ugly and wrinkly
My brain: smooth and beautiful
What is the analogue of Lebesgue measure in the complex plane?
I don't think you will ever have to realistically calculate local degrees for a non-differentiable map
Is it just the same one as the one in $\mathbb{R}^2$?
for a differentiable map, the local degree at a point is the sign of its determinant
@Clarinetist yes, the analogue of the Lebesgue measure is in fact the Lebesgue measure itself
01:50
And incidentally, the fourier transform is also the same, to revisit what we went over yesterday
At least the part in the exponential is just x_1*Im(z) + x_2*Re(z)
So here's a theorem I was presented:

Let $f$ be a Borel measurable function on $[a, b]$. Then there exist continuous functions $f_n$ on $[a, b]$ with $\lim f_n(x) = f(x)$ for all $x \in [a, b] \setminus E$, where $E$ has Lebesgue measure zero.

Especially with the interval, I'm struggling to understand what the complex-function analogue of this theorem would be.
Uhh fourier transform only if density. I meant characteristic function, but should be the same by viewing Im(X) and Re(X) as random variables and then substituting to get a double integral, if these things have a joint density (which is the same as a density for X itself)
you don't actually need to exclude a measure 0 set
anyway, the natural analogue of an interval is a rectangle
but I'm kinda sure the domain can be any measurable subset and the result will still be true
probably true for the Borel sigma-algebra on any paracompact topological space, but I'm not thinking much
Hi, I have a problem about smoothness of moment generating functions on arbitrary open sets. Someone suggested an answer, but it does not have generality and I am still stuck at it. Can anyone take a look? Thanks. math.stackexchange.com/q/4018712/792125
1
Q: Prove that MGF defined on an open set is infinitely differentiable

MikeI am doing an exercise in the book "Applied Stochastic Analysis" by E-Li-Vanden-Eijnden, and I meet this problem (on Page 26): (Exercise 1.19) Prove that if the moment generating function $M_X(t)$ can be defined on an open set $U$, then $M_X(t)\in C^{\infty}(U)$. Here is my approach: Use Taylor...

02:09
@Mike in the taylor expansion, I think this should be o(t)/t
@user2103480 Personally, I find the Taylor expansion argument not a rigoruous one. Do you have other approaches to prove that? Note the open set is arbitrary.
Say we have a ring $A$ and its field of fractions $K$. Say we have a guy, $a/b \in K$ such that $a/b \notin A$. $A$ is integrally closed.

Does it follow that $a/b$ is *not* integral over $A$? Kind of fumbling definitions here I think
Because if it were integral, then $A$ being integrally closed would mean that $a/b$ had to be in $A$?
that's what integrally closed means, isn't it?
yeah I think so- I just haven't internalized the definition.
Really dumb because it's not that complicated. thanks though
02:35
@Mike Hm I think I just used the wrong taylor formula. But now I get a not so nice expression e^tX = 1 + tX + o(tX)(tX) which doesnt align with your expression either
why not just differentiate under the integral?
It's maybe not the best approach since you have to control the tX terms there
what's there to control
though tbf doing Taylor is just like manually re-proving differentiation under the integral, so it's not like this is a conceptually all too different approach
Oh I didnt mean yours
I meant the taylor expansion
Differentiating unter the integral should be fine, but you gotta show that the derivatives have a common integrable majorant
One might also try the ol' switcheroo to get a power series locally, but gotta be careful about the necessary conditions being fulfilled
yeah, but it's monotonous in $t$, so you just bound by the max. value of $t$
(we can always restrict to a bounded domain since smoothness is local of course)
02:49
@user2103480 Nah, you have uniform convergence on compacts. Sometimes you don’t need Lebesgue s****.
Hmm, I guess I didn't look. I assumed this was Taylor/Laurent.
@TedShifrin this is a random variable, no? What exactly converges here
@Thorgott still gotta argue that X exp(t_0X) is integrable
And so on
I think using fubini locally to make this into a power series with coefficients being the moments and radius of convergence given by openness should be a good approach
ok, you got me there
but, like, small values of X don't make an issue, but for large values of X, you can bound X above by exp(t_0*epsilon*X) for epsilon as small as you like (by making X larger) and then the product is bounded above by exp(t_0(1+epsilon)X), which is integrable by hypothesis if we chose epsilon small enough
Hahaha there surely is a way to use that approach
of course I first choose epsilon appropriately and then a cut-off for X to get a uniform bound, but this should work
Might be tedious, might even have an elegant, quick solution
But I will better go to bed instead of thinking about completing the argumenr
02:59
I think this is complete enough
details are left to the reader as an exercise
Good night!
Can we move the discussion to my post? I think your epsilon-approach is interesting, can you go to my post and write an answer if you are willing to?@Thorgott
03:01
Suppose I have three complex random variables $Z_1, Z_2, Z_3$ and can demonstrate that $Z_3$ can be completely determined by $Z_1, Z_2$. In such a case, $Z_1, Z_2, Z_3$ are dependent random variables.

Now, suppose I have three complex random variables which are dependent as explained above. Does this mean that $\text{Re}(Z_1)$, $\text{Re}(Z_2)$, and $\text{Re}(Z_3)$ are real-valued dependent random variables?
sorry, but I'm about to follow user suit and go to sleep as well
 
1 hour later…
04:05
I figure this out, anyway. Thanks for the help.
123
123
04:43
Hello Guys..
05:24
@Clarinetist By dependent, do you mean not independent?
Dependent could be interpreted in a different way.
 
2 hours later…
06:55
In finding shortest distance between the skew lines , how the shortest distance that is PQ will be the projection of AB .Can anyone help visualise...
07:29
How do I know the musical isomorphism will give me a global smooth vector field as the preimage of a one form. By riez representation I get that the map is surjective and locally I do have a smooth vector field. But how do I know this vector field can be defined globally?
08:00
If $A$ be a commutative ring and $x\in A$ is a nonzero element and $a\subset A$ is an ideal, then $Ax/Ix$ is free over $A/I$ by a generator $\overline{x}$ which is an image of $x$ under $Ax\to Ax/Ix$. Then the operation would be $(a_1+I)\in A/I$, $(a_2x+Ix)\in Ax/Ix$, $(a_1+I)(a_2x+Ix) = (a_1a_2x+Ix)$?
 
6 hours later…
14:23
@StudySmarterNotHarder Hey mate, text me when you are here :d
14:43
$\textcloserevepsilon$
$\closerevepsilon$
$\revepsilon$
$\closeepsilon$
@AkivaWeinberger estas haciendo un corazon?
@LeakyNun Did you just learn some spanish and wanted to test it on him?
yo y el hablamos espanol
recommendations on self-teaching set theory?
14:47
@John_Krampf what's your background
@LeakyNun PhD in Math, but I never had a course in set theory, I studied Functional Analysis and Differential Equations
@SayanChattopadhyay What's your definition of the musical isomorphism? I think this should be true by definition.
@John_Krampf Jech set theory
@LeakyNun Thank you
@John_Krampf why do you want to study set theory?
14:49
@LeakyNun I want to understand what is meant by "The Constructible Universe" what is in the constructible Universe, and what is outside the constructible universe
fair enough
yeah that's inside Jech
@LeakyNun Nice, thank you
that requires ordinal numbers
which is also inside Jech
@LeakyNun Thank you. Also there is something else I was hoping to maybe learn one day. I had a logician friend who drew me a rough picture of it one day. Where you have a "logical system" that is "inside" another logical system like a 2d space embedded inside a 3d space, and then you talk about what statements are provable in the 2d space vs what statements are provable in the 3d space. Is that also in there?
(and if so then what part?)
that sounds like model theory to me
which is like everywhere inside the book
something like "inner model" may be what you seek
@John_Krampf
14:56
Thank you :)
I have another question, I never took a logic course either but a few years ago I studied a few introductory chapters on propositional and 1st order logic on my own. Is there a connection between that and set theory?
a lot
that's why like usually logic courses have both 1st order logic and set theory
it's like studying ODEs and PDEs i guess
Do you have a recommended text for Logic as well?
I think it's closely related to model theory
so like you'll find it inside as well
Nice, thank you
I think Kunen's book is better for self studying. Jech is the best reference for sure though
15:09
Hello!!
Why does the vector sum $\vec{a}+\vec{b}$ not always the length $a+b$, i.e why does in general hold that $|\vec{a}+\vec{b}|\neq a+b$ ?
And when does the equality hold?
@AlessandroCodenotti Thank you I will check it out
Hello guys
Hope you are doing well.
I got a question for you.
It's here:
@MaryStar draw a picture
0
Q: What is the point of having a unit vector $\hat{\phi}$ in the cylindrical or polar coordinates?

CardinalAs we know in the cylindrical (or polar) coordinate system we have: $$\hat{\rho} = \cos{\phi} \hat{x} + \sin{\phi} \hat{x}$$ $$\hat{\phi} = -\sin{\phi} \hat{x} + \cos{\phi} \hat{y}$$ Now lets consider a given point $\mathcal{P}$ in the cylindrical coordinate as $\left(\alpha, \beta, 0\right)$. Us...

no it isn't
15:19
I'll appreciate if you discuss your takes.
I suppose it's just a pure mathematical definition and there is no actual point in it !! :sweating: :embarrassed:
The point it that it makes computations easier
If you deal with gravitational motion for instance, using cartesian coordinates is a nightmare because the forces are radial
I didn't say the whole cylindrical system is pointless
I meant, only the $\rho$ direction does the job
having a unit vector for $\phi$ does not make sense to me
No, because ${d\over dt} \vec u_r = \dot\theta \vec u_\theta$
or something like that
So when you study motion, you're bound to deal with both radial and tangent vectors
it must also be said that you don't always have rotational symmetry in cylindrical coordinates
What I see is, any point on the X-Y plane can be completely described by the "\rho" unit vector
15:26
an occasional situation in electromagnetism, for instance, is that you have translational symmetry along the z-axis but not rotational
@Cardinal a lot of problems are like that, but it's hardly universal
What do you mean, it is not universal? It works for all the points on the X-Y plane
I mean, either \phi or \rho
the rule of thumb is to use the coordinates that are most appropriate for different symmetries of your problems. Studying the motion of an object subject to gravity on the earth surface is easily done in cartesian coordinates (you get a parabola). Studying the movement of planets in space is easily done in spherical coordinates (or in cylindrical when you have only 2 planets). Studying the electromagnetic field around an infinite straight wire is better done in cylindrical coordinates
one is redundant in general
for specifying where a point is, yes. for specifying in what direction it might be moving, no
Hmm, for X-Y plane, I would say I don't agree with you
15:29
@Astyx to amplify that last one: magnetic field around a straight wire in the presence of a uniform electric field
Yes, I am teaching Emag to the Undergrads
Literally this semester LoL
And for studying spherical cow in a vacuum, you'd rather use spherical coordinates :)
well, suppose you have circular motion $v=(x,y)=(\cos\theta,\sin\theta)$
then $dv/dt = (-\sin\theta,\cos\theta)$
I see what you are saying.
now, you could say that that's just $(x,y)$ with a different $\theta$. but you don't want to do that
because you're already using theta for one thing
also, to be clear on the example I have in mind
15:31
from the vector analysis though, I would say you only need the coordinates and either one would do the job.
B-field of a wire is a good example. if you're looking at a point $\hat{\rho}$, then the field at that point is in the $\hat{\theta}$ direction (or phi, depending on your coordinates)
@Semiclassical I believe this is the crux
I think both of $rho$ and $phi$ directions are not actually unit vectors if we look at them carefully, because they are not unique they are dependable on x and y.
I mean, they are just a definition to make things read better
I think I now could fathom what is the idea behind in such definitions.
I mean, they just created to make them for sake of mathematical tractability
What's your definition of a unit vector ?
they're point-dependent, sure
15:37
I meant unique unit vectors (my bad)
but they still have unit length and are vectors, so...
eh.
they're unique at each point in space
that's all one needs for them to be useful
if you give me a point in space, i can tell you what the basis vectors are. if I pick a different point, it's a different basis
I don't know, I can say z is a unique direction but I could not say that for "rho" since it depends on x and y
maybe "stand alone" is a better terminology than unique
i mean, you could equally well say that "up" on the earth isn't a unique direction because it matters where you are on the earth
"up" is a different direction at the north pole vs. south pole if you look at the Earth from the moon
OK, my discussion is a bit philosophical than technical.
but if i'm standing at either pole and I toss a ball upwards, then the direction the ball falls is the same in my frame of reference
15:40
I mean, x y z are genuine, the rest of systms for the three-dimensional space are fake
:embarrassed:
i don't think 'fake' is the right word. 'relative', perhaps
there's an absolute meaning to the x,y,z directions, but there's only a relative meaning to the rho,phi directions
I see, meanwhile, this relativeness also exists with respect to phi and rho in my opinion.
@Semiclassical Thank you, yes.
I don't completely agree with this
15:43
to be clear, when i say "relative" I'm meaning in the same way that a physicist talks about reference frames
You believe the x,y,z coordinates are natural because you can move left/right/up/down on the earth's surface
Perhaps, in some geometry using "phi" unit vector instead of "rho" unit vector would make the mathematical expressions less lengthy
But if you were not in control of your motion and all you could do is observe the universe from a given point, you'd more likely use the spherical coordinates
@Astyx No, I say that because they constitute the spherical and cylindrical systems
What do you mean by that ?
15:45
well, it should be noted: If I move in the (x,y) plane, changing my definitions of rho,phi along the way in the expected manner
then the rho,phi directions may rotate but they'll always remain orthogonal
the $\rho$ vector is always "radially from my point of view". The $\phi$ vector is always "going to the left from my point of view"
@Astyx I mean, rho does not represent a unique dimension of the space on its own.
a single unique dimension
Compared to x and y and z, which all three do.
then again, it depends what you call a dimension
something something parallel transport
@Astyx No, a dimension of space is a singular entity. I suppose it could not have two constituents.
15:54
it does depend who you ask
and the context
I believe in GR you don't have parallel transport, so x,y,z are no longer sufficient coordinates
hmm, i don't know, by definition rho depends on x and y not the other way around. even any radial line from the origin would have two unique dimensions of the tangible space
to amplify the point I was making: suppose I'm holding a sign pointing East (+x) while standing at the point (1,0)
It was a good chat guys, thanks. I have to go. I wish you a good rest of day. take care.
then at that point I would say that the sign points radially away from from the origin, so the sign points in the $\hat{r}$ direction
you too
16:01
but if I walk north from that point, the sign's direction as specified in cylindrical coordinates will change.
it'll still be a unit vector, but it won't be a unit vector in cylindrical coordinates anymore
and that'll also be true if i walk around the circle
modular forms are on the upper half plane
if you could rotate the x-axis to become vertical would this be some other thing?
Hi guys could anyone explain how this answer math.stackexchange.com/questions/193258/… shows that we have a basis for the cotangent space, this is a very basic question on manifolds.
@Thorgott Do we maybe not get the equality when it is $\vec{b}=-\vec{a}$ ?
no, then the sum is 0
@Thorgott I dont really have an idea
16:13
have you drawn a picture?
@Thorgott Ahhh is this related to triangular inequality?
But how do we justify that? Just that the distance a and b is greater that that of a+b ?
And we get the equality if the vector are colinear, right? @Thorgott
@geocalc33 not really. things would look different but the theory would be the same
@Flows. it calculates that the given set of vectors is the dual basis to the given basis on the tangent space
16:16
I realise that this is how you show such a thing
but
@MaryStar no, $\vec{a}$ and $-\vec{a}$ are collinear too, there's one more condition
@Clarinetist Hm, maybe dependent, but at the least I wouldn't expect that the real parts alone determine the real part of the dependent variable. What you're describing is random variables $Z_1 = (X_1,Y_1), Z_2 = (X_2,Y_2)$ and $Z_3 = (X_3,Y_3)$ with $Z_3$ measurable with respect to the sigma algebra generated by $Z_1$ and $Z_2$. This is equivalent to $Z_3 = f(Z_1,Z_2)$ for some measurable function (between the right spaces)
@Thorgott They have to be collinear and they have to have they same direction?
@user2103480 they obviously don't, take $Z_1,Z_2$ purely imaginary
@MaryStar yes
surely you just need to show that a cogtangent basis element_i acting on a tangent space basis element_j = $\delta_{i,j}$
16:18
@Thorgott well f*** you too
Ok! And how do we justify that the equality does not hold in general? Do we justify that using the graph? @Thorgott
lmao but yeh right, thanks
@Flows. Can you clearly and concisely explain what your question is, without reference to something else? That will help me understand what you need.
@user2103480 ♥
16:19
@MikeMiller Hi im just confused by this answer math.stackexchange.com/questions/193258/…
@Flows. that's what the answer does
@MaryStar well, you just visually determined precisely which conditions are necessary for the equality to hold. surely you can come up yourself with two vectors not satisfying this condition and then calculate their respective lenghts.
"Without reference to something else". You should be able to isolate exactly what the issue is. I don't really want to spend the time trying to understand someone else's notation.
I have to go now though.
they write (dx_i)_p ( \frac{ \partial }{ \partial x_j } ) (f) which reads cotangent acting on tangent acting on function
@Thorgott Well it is just that if you have a riemannian manifold $(M,g)$ then the map is $g^{*} : \mathfrak{X}(M) \to \Omega^1(M)$, where you take $X$ to $g(X,\cdot)$. How does just this ensure that the inverse is a smooth globally defined vector field?
which doesnt make senes
16:22
@Thorgott incidentally, constant 0 RV are trivially independent so this also solves the other question
@Flows. Presumably their initial definition of cotangent space is different from yours. If you ignore the $f$, can you make sense of it? There are a lot of slightly different definitions flying around.
@SayanChattopadhyay I don't understand. This is an operation you do pointwise. There is no issue with well-definedness.
At each tangent space $(g^*X)$ is the one-form with $(g^*X)_p(v) = g(X_p, v)$.
To specify a 1-form you specify what it does to tangent vectors at each point (it is an element of a dual space). So we have just done so.
The only difficulty is smoothness, which is a computation checked in coordinates.
@Semiclassical can you imagine this vertically oriented modular form?
Right but given a one form by riez, on each tangent space I have a vector $v$ such that $g_p(v,\cdot) = \omega_p$. To show smoothness I did a local computation as you said, but I was not given any credits claiming that a local computation does not show global smoothness
ok what
smoothness is a local condition
Precisely, I am being asked to use sections, and I do not see how that removes any local calculation, because even if I want to show smoothness of a section, I have to do that locally as well
16:28
Sorry, I don't really follow. "Blah is smooth" is defined on charts. That's the definition!
Unless you've defined a "smooth 1-form" to be one so that $\alpha(X)$ is a smooth function for any smooth vector field $X$.
That's equivalent to the standard (local) definition, by a (local) computation.
Came across a paper which defined a Riemannian metric (on GL(n)) by writing something like $\langle \dot A,\dot A\rangle_A = ...$. Does this actually fully define the metric?
Yes, any norm that satisfies the parallelogram law determines an inner product via 1/2 [N(x+y) - N(x) - N(y)].
Oh!
I forgot about the parallelogram law.
Thanks Mike!
Kind of cute, I guess.
Yeah I do not get it either. I do not understand what the instructor has in mind
I mean check back to definitions or results so far
It's possible they just want you to check smoothness by the above
Which ought to be clear if you already know $g(X,Y)$ is a smooth function for any smooth $X, Y$
OK Now I really have to go
16:34
@Flows. There's a subtle point here, namely that $dx_i$ really means two different things. On one hand, $x_i\colon M\rightarrow\mathbb{R}$ is a smooth function, so we can form it's differential at the point $p$, which is a linear map $dx_i\vert_p\colon T_pM\rightarrow T_{x_i(p)}\mathbb{R}$ (I'm using $T$ to denote the tangent spaces). On the other hand, we want $dx_i$ to be a cotangent vector, i.e. a linear map $T_pM\rightarrow\mathbb{R}$. These two ideas are related by the fact that we have a canonical identification of a tangent space $T_{x_i(p)}\mathbb{R}$ of $\mathbb{R}$ with $\mathbb{R
I was trying to depict this ^
123
123
16:55
Hi All...
hello
Hi uno dos tres
I made 4 cents last year
gotta start somewhere
17:13
Helllloooooo!
My first time in a chat room
I am trying right now to do some stuff in Grimm's conjecture
So far I have that if n=p is a prime, then n+p can be written as a product of primes
Not just any product though
It contains at least two distinct primes that divide p+i
Not n+p, p+i.
17:34
@geocalc33 no but i dont' do modular forms
but it's like doing $x+i y$ vs. $i(x+iy)=-y+i x$. Things change but in a way that's entirely uninteresting
one could rewrite things but there's usually no reason to
in the same way that it's more typical to label horizontal motion as $x$. you could label it differently, but you shouldn't expect that to change anything substantial
@user2103480 I agree with your statement.
17:56
$\nlessgtr$
$\lessgtr$
$\not\lessgtr$
18:09
@TedShifrin I only really realized while teaching this sem that the usual Gaussian elimination algorithm endeavors to give a canonical basis for a subspace presented as a kernel, and that the corresponding column operations endeavor to give canonical bases for subspaces presented as an image.
$\changenotsign\not\lessgtr$
$\not\neq$
Oh wow \not\neg is identical to \neg
$\not \neg$ $\neg$
huh?
neq I meant
\not\neq
$\not\neq$ $\neq$
Not for me
The \not is too far right
the first one looks thicker?
18:25
For me the only difference is the diagonal is a bit thicker, yeah
18:51
It has to do with how they choose to rasterize at different scales
Zoom in and they are indistinguishable
Not sure if there is a nice way of doing this, but I have a symplectic matrix $X$ and a positive definite $A$. I want to find a symmetric positive definite symplectic matrix $Y$ such that $XAX^\top = YAY^\top$.
00:00 - 19:0019:00 - 00:00

« first day (3844 days earlier)      last day (1469 days later) »