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12:01
hi
user306715
What is the definition of exterior derivative?
@BalarkaSen Hi
Hi, @Danu, @Steamy, @Krijn, chat in general
@YCNDM There are textbooks and materials on internet which define the exterior derivative. Why not read those?
@mago False for $f(z)=1/z$ on $\Omega=\Bbb R-\{0\}$. True whenever $\Omega$ is simply connected ("does not contain any holes").
12:14
Or alternatively you could say they have antiderivatives but locally
(Remember that the complex logarithm is multivalued; we cannot give it a consistent value throughout $\Bbb R-\{0\}$.)
user306715
I have seen two definitions: One of them has an extra term, $\omega ([X,Y])$. I do not know why it appears.
user306715
$d \omega (X,Y)=D_X(\omega (Y))-D_Y(\omega (X))- \omega([X,Y])$
@BalarkaSen do you know any Sanskrit?
@YNCDM You can explicitly take a form $\omega$ and check via computation that it appears (assuming you know the basis-wise definition of $d$). But otherwise I am not sure how to answer "I do not know why it appears". Notice also that $D_X \omega (Y) - D_Y \omega (X)$ is not a linear term; $\omega([X, Y])$ corrects that.
@skulll nope
12:23
@YCNDM This is not the definition of the general exterior derivative, that's just an identity for the exterior derivative of a one-form
@Danu You can extend that to a definition for k-forms though
It involves an ugly sum over the Lie brackets of n-1 of them
user306715
I have seen that as the definition. So what is the original definition?
@BalarkaSen yeah... but I feel like it's not "morally" the right thing you know
it doesn't tell you what's going on
:O "morality" from an ex-physics major? :P
joke^
True. Actually there are times where it's useful; eg Frobenius theorem is proved using that identity, but I agree; I don't like that formula very much
user306715
12:30
I have also seen the following definition:
$df(x_u,x_v)=\frac{\partial (f(x_v))}{\partial u}-\frac{\partial (f(x_u))}{\partial v}$
user306715
Why are they equivalent to each other?
What def does your book use?
user306715
I have seen both of them from two different books.
Ok, how about your prof?
@BalarkaSen It's definitely one of the most useful formulas... It's not called "Cartan's magic formula" for nothing ;D
(I always saw this as the main application of Cartan's formula)
user306715
12:33
I have no prof in this field.
Actually, that might not be an accurate statement
The magic formula is overall awesome :P
@YCNDM There are multiple definitions, but the one I like is defined basis-wise as $d(f dx_{i_1} \wedge \cdots \wedge dx_{i_k}) = df \wedge dx_{i_1} \wedge \cdots \wedge dx_{i_k}$ and for a 0-form $f$, $df = \sum_{i = 1}^n \partial f/\partial x_i dx_i$.
@BalarkaSen How is life?
user306715
So why are the above definitions equivalent to each other?
@Danu Hm, I thought Cartan's magic formula was the chain homotopy formula.
@YCNDM It's a computation; check it.
@YCNDM Also this is not a different definition from what you already said. Plug in $\partial/\partial u, \partial/\partial v$ for $X, Y$ in $d\omega(X, Y) = X\omega(Y) - Y\omega(X) - \omega([X, Y])$ and you get that formula
Because $[\partial/\partial u, \partial/\partial v] = 0$
@Krijn Not bad. What about you?
user306715
12:40
Thanks.
@BalarkaSen Working on my thesis but can' t get things right
How come?
Hey people, sorry for interrupting. I am not very active in math.stackexchange.com, and therefore I don't have privileges to comment. It's about this post
https://math.stackexchange.com/questions/1777975/interior-and-closure-of-l1-mathbbn-in-l-infty/1778043#1778043
The comment has a mistake there: where you read -y in B it should be -y in Y
can someone with privileges comment that please?
Well after five years I've noticed, mathematics is quite hard
4
True
So it's a mathematical trouble you're having?
12:45
Mostly getting through an article I can' t seem to grasp
But also some editorial problems
How to (sub)divide chapters, sections
What and what not to scrap
Delete, might be the better word there
@BalarkaSen Yeah, but you can use it to get that identity, using $da(X,Y)=((i_Xd)a)(Y)=(L_Xa-di_Xa)(Y)$
@Danu Ah...
Someone here with some knowledge of functional analysis or similar?
12:48
@BalarkaSen That's how I learned it :)
So Cartan's magic formula expresses $i_X$ as a chain homotopy from $L_X$ to $0$? Never thought about it like that, really.
I hope you didn't mind me calling you an "ex-physics major?"
I don't really care what you say about me..
@Danu Yeah, that's my usual intuition for it
I like what you said; never realized that formula is a corollary of Cartan
@BalarkaSen Is it a useful intuition for anything specific?
I never really encountered any use for chain homotopies besides pretty technical stuff so far, that's why I'm asking
Why is my pdf suddenly rotated in TexMaker and how do it turn it back
12:54
Do you know why they made the math mods' office a private room all of a sudden? @Danu
you switch to TeXStudio, which is the updated version of TeXMaker ;) @Krijn
@skullpatrol No idea and even if I knew I probably wouldn't say :P
@Danu :(
Never mind, I asked this in the functional analysis chat.
I'm now pretty weirded out @BalarkaSen. What does the presence of a chain homotopy from $L_X$ to $0$ tell us? That any Lie derivative is null-cohomologous?!
@skullpatrol I was pondering to ask it on meta.
12:59
^that might be a good idea
Nah @quid not that important pal.
@Danu I am not sure if it's formally useful for anything, but say you integrate $\mathcal{L}_X = i \circ d + d \circ i$ over a small loop $\gamma$, you get $\int_\gamma \mathcal{L}_X \omega = \int_\gamma i_X d\omega$. Think about $\int_\gamma \mathcal{L}_X \omega$ like "$X(\int_\gamma \omega)$"
Well, it's a pretty strange thing to happen.
Let them have their privacy in peace.
So, uh, you're computing a little change in the integral $\int_\gamma \omega$ as you flow along $X$
13:03
We can make our own room called The Echo Room @quid :-D
or Echo Chamber even.
Sure, extra rooms are a dime a dozen.
@Danu Yeah
@BalarkaSen I feel like I didn't know that... But maybe I did? Not sure
hi yall
how do I find a generator of Z/50 *
How do I know it is cyclic in first place?
13:07
I'm still confused @Balarka. If $\omega=L_X\alpha$ then it's not automatically a coboundary, is it? What about the $i_X d\alpha$ term?
is it by trial and error? because that can take long time since its order is 20
Right, @BalarkaSen, $\alpha$ is closed by assumption.
@KasmirKhaan $50 = 2 \cdot 5^2$
sorry, my internet is being bad
right, $i_X d\alpha$ vanishes
@SteamyRoot I found the elements but my question was how can we find if it is cyclic or not in an easy way, without rising all elemets to power 20
13:16
How do you mean, you "found the elements"?
The elements in Z/50 *
other notation is U_50
the elements such that gcd(50,k) = 1
@SteamyRoot
@Danu I guess "$X(\int_\gamma \omega)$" $= \int_\gamma i_X d\omega$ is like differentiation under the integral sign :P
{1,3,7,9,11,13,17,19,21,....49}
So maybe my supreme conclusion is that Cartan's magic formula is differentiation under the integral sign.
lol
13:20
Hi @Semiclassical
hi pal
any good math today?
@BalarkaSen I should probably know what Cartan's magic formula is, sigh
What you want to use is that, if $n = p_1^{e_1} p_2^{e_2} \cdots p_k^{e_k}$, then $(\mathbb{Z}_n)^* = (\mathbb{Z}_{p_1^{e_1}})^* \times (\mathbb{Z}_{p_2^{e_2}})^* \times \cdots \times (\mathbb{Z}_{p_k^{e_k}})^*$
something something interior product / exterior derivative / Lie derivative
How goes your TA situation?
13:22
I think Ted likes to say it's like an infinitisimal version of Stokes' theorem but I'm having trouble remembering why
@SteamyRoot Euler phi function right? but my question was how do we know it can be generated by any element ? ie cyclic
@Semiclassical yeah it says $\mathcal{L}_X \omega = i_X d\omega + d(i_X\omega)$
It got resolved.
Sup semi
13:23
hi @KasmirKhaan
@BalarkaSen Neat.
Excellent.
My main problem with Cartan is that, of the three operations there, I only know how to use $d$ fluently
@KasmirKhaan If you calculate what group $\mathbb{Z}_{50}$ is isomorphic to, you'll know whether it's cyclic...
$\iota_X$ I know at a manipulation level but not intuition
and $\mathcal{L}$? nope
@SteamyRoot hmm so without isomorphism it cnt be done in an easy way ?_
13:24
I never gave interior product much thought. Lie derivative is cool.
What do you mean?
Using the formula I just gave you, it's really easy...
one way is to rise all elements to power 20
interior product satisfies $i_X \omega(X_1,\ldots,X_n)=\omega(X,X_1,\ldots,X_n)$?
Well, have fun with that :^)
13:25
@SteamyRoot $\Bbb Z_{50}^\times$
right.
but while I can write that down, I don't have an intuition for what it says
@BalarkaSen Hahaha
@anon Thanks for clarifying things =p
with $d$ I can say "oh, it's basically a coordinate-independent way of expressing div/grad/curl"
Hi, why I can't read @SteamyRoot
13:27
but with $i_X$ I only have the formal meaning of it.
I don't see his commenter
@Semiclassical yeah I don't really understand what interior product does. but $\mathcal{L}_X \omega$ is literally $d/dt \phi_t^* \omega|_{t = 0}$
modulo a sign perhaps
eh, and that doesn't mean much to me since I haven't ever absorbed the 'tangent vectors = equivalence classes of curves' notion
or whatever it's supposed to be
Sorry, but why I can't read @SteamyRoot
I don't know why you can't read...?
13:30
@Semiclassical why do you want to think about tangent vectors like that?
I literally think about tangents as tangents
@Dattier check your ignore user list
isn't that what $\phi_t$ is supposed to be communicating here?
but I'm probably misremembering
oh it's the flow corresponding to $X$
@skullpatrol Thanks
13:31
np
any vector field on a compact manifold gives rise to a 1-parameter group of diffeomorphisms "tangent to $X$"
hi guys
Heh, I was ignored? :P
@BalarkaSen Seems to be the only way to efficiently compute differentials n stuff to me
Not sure you're familiar with it
but say you have a red black tree
13:32
@SteamyRoot maybe a mistake of me
each leaf is red
Accidents happen :P
and I wonder if the sibling of each leaf is also a leaf
The main place in physics where I think Lie derivatives show up is in the symplectic manifold formulation of Hamiltonian mechanics.
which would make sense---Hamiltonian flow and all that
(question about graph theory/computer science)
13:34
hah, I just checked my copy of Arnold and he doesn't call it "Cartan's magic formula"
he calls it the 'homotopy formula'
Cartan's magic formula is something I saw in symplectic geometry
He relegates it to a problem, though he may use it again later.
he also seems to avoid using the phrase "Lie derivative"
he acknowledges it, but he first labels it as "$L_X$ is the differentiation operator in the direction of the field $X$."
Guys can you please clarify something for me ?
I am trying to find the geneators of U_50
the order of U_50 = 20
<a^k> = < a^gcd (20,k) >
{1,3,7,9,11,13,17,19 }
Those must be the power of what?
@Semiclassical right, that's what it is
He also terms it as the "fisherman's derivative"
"the flow carries all possible differential-geometric objects past the fisherman, and the fisherman sits there and differentiates them."
13:47
nice visual
The exercise he gives for that has the following hint. "We denote by $H$ the "homotopy operator" associating to a $k$-chain $\gamma:\sigma\to M$ the $(k+1)-$chain $H\gamma:(I\times \sigma)\to M$ according to the formula $(H\gamma)(t,x)=g^t \gamma(x)$ (where $I=[0,1])$." ($\{g^t\}$ is the phase flow of the field $X$.)
"Then $g^1\gamma-\gamma = \partial(H\gamma)+H(\partial \gamma)$."
So that maybe means something to you, even if it doesn't mean anything to me. :P @BalarkaSen
right, he's explaining chain homotopy
Would you @Semiclassical consider
A. P. French's physics textbooks as outdated for today's undergrads?
never read it
so could not say either way
13:54
<3^k> = < 3^gcd(20,k) >
Why does gcd (20,k ) have to be k < 20
@Semiclassical I have explained the chain homotopy formula here (from the topological point of view) if you ever want to read it.
What textbook did you use in your first year at uni?
good question. i'm not sure i remember now, tbh
that would've been back in 2006
we currently use Mazur in the version of intro physics which physics majors take
13:59
I see.
@BalarkaSen not going to try to understand that right now, but i can see a bit of what's going on
in that the LHS of what Arnold asks you to prove tells you about how the chain $\gamma$ changes in one second of time evolution, and the chain homotopy stuff is telling you how that prism subdivision works
you can tell I understand this very precisely :P
different contexts; same formula
right.
I still find it weird that Arnold doesn't really seem to use Cartan's magic formula at all in his text
on an entirely unrelated note: f*** seasonal allergies ugh
i took my allergy med two hours ago, and I can still feel the effect of said allergies
14:13
@Semiclassical can you help me with my abstract algebra exercice?
the U(50) one?
Its not about that number but the concept
I found out that 3 generates U50
I know this formula
<a^k > = < a^gcd (n,k)>
tbh, to the extent that I know anything about this is because of google-fu
where the order of a = n
14:15
Ill show u where i was stuck
I'm not hearing a question yet.
ok
<3^k > = < 3^gcd (20,k) >
so why do we take all the k's that are relativly prime to 20 and less than 20
the less than 20 part I did not get
<3^(k+20)>=<3^k>
What modulus are we working on ? 20 or 50 ?
This is what comfusing me
3^(k+20) = 3^k mod 50
because 3^20 = 1 mod 50 no?
14:17
oh right order of 3 is 20
so 3^20 = e
so the residue (3^k mod 50) only actually depends on the residue (k mod 20)
by residue you mean modulus?
no, residue
3^k mod 50 is a residue, 50 is the modulus
Ah we call that remainder =p
Okay so if I understood it correctly
residue, remainder
14:19
given any U_i
not much difference even at the level of the popular meanings of the words
first we try to find a generator
then from that generator call it a
<a^k > = <a^(gcd(n,k) > where n is the order of a
Let $f_1,...,f_n$ be $n$ continuous functions in a interval $[a,b]$
the set gcd( n,k ) are the exponents we rise a to
to get all the generators
Is that right?
in $[a,b]$ I define $b(x) = \min(f_1(x),f_2(x),\ldots,f_n(x))$
14:21
Thanks alot guys ! :)
@KasmirKhaan wait, no
the other generators will be a^k where k is coprime to n
when k is coprime to n, <a^k>=<a^gcd(n,k)>=<a^1>=<a>, so a^k will also be a generator
If $A_j = b^{-1}(B_j)$ where $B_j = \left\{ x : b(x) = f_j(x) \right\}$
what can I say about $A_j$?
@anon yes that was i meant , in case of U50 , order of it is 20, and 3 is a generator
so we rise 3 to phi (20)
to get all geneators
assuming $B_j \neq \emptyset$, can I say $\mu(A_j) \neq 0$?
@anon because in this case gcd(20,3) = 1
14:23
@user8469759 if $B_j$ is a set of $x$-values then why are you taking $b^{-1}$ of it? wouldn't you take $b^{-1}$ of a set of values in the range of $b$, not in the domain of $b$?
sorry
I meant to write the counter image
Let me start over
yeah, I'm asking you why you're taking the preimage of a set of domain values. don't we normally take preimages of sets of range values?
I wrote it wrong...
I meant $A_j = \left\{ x : b(x) = f_j(x) \right\}$
so counter image of $b$ when $b = f_j$
can I say the lebesgue measure of $A_j$ is not 0?
you can assume $A_j$ is not empty
so for all $j$ there's an $x \in [a,b]$ where $b(x) = f_j(x)$
14:29
Suppose $\alpha\in A_j$. Let $i$ be a different index. Then $f_i(x)-f_j(x)>0$ when $x=\alpha$. Since $f_i,f_j$ are continuous, this must hold in some $\epsilon_i$ interval around $\alpha$. Then $A_j$ must have size at least $\min\limits_{i\ne j}\epsilon_i$.
can we work in another way instead
$f_1,\ldots f_j$
are continuous
(assume from $[a,b] \to Y \subset \mathbb{R}$)
since they're continuous they're measurable
can I use some measure theory argument for the same conclusion?
I guess the argument would be kind of the same
Let $A_j = \left\{ x : b(x) = f_j(x) \right\}$
by definition we have
$A_j = \left\{x : f_j(x) - f_i(x) > 0, i \neq j \right\} = \left\{x : g_{ji}(x) > 0, i \neq j \right\}$
hence $A_j = \bigcap_{i\neq j} g_{ji}([0,\infty))$
because each $f_i$ is continuous so are $g_{ji}$
we have $[0,\infty)$ measurable, so the counter image for each $i\neq j $ is measurable
and finite intersection is also measurable
because $A_j$ is open in $\mathbb{R}$ its measure must be $\neq 0$
is this argument correct?
anyway it should actually be $A_j = \bigcap_{i\neq j } g_{ji}((0,\infty))$
I mean opensets in $\mathbb{R}$ have as basis openintervals $(a,b)$ with $a < b$ so the measure should be not 0
does this work?

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