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16:00
1
Q: Statement about differential forms

studiosusIn a paper I'm reading (https://arxiv.org/pdf/1009.1175.pdf), one claims the following: Let $(M,\omega)$ be a $2n$-dimensional symplectic manifold. If $\mu$ is any $2$-form on $M$, then $$\omega^{n-1}\wedge\mu=0\Leftrightarrow \mu=0.$$ The implication $\Leftarrow$ is clear, but I have trouble ...

@BalarkaSen ^sanity check: is that comment right?
Because that'd imply that Guillemin claims something that's pretty clearly false in his paper :P
I am reading a paper in which it states that the terms of a series (its in Equation 1) are of the order 1/sqrt(m) for large m and hence the series is extremely slow to converge. But surely if the terms are of the order 1/sqrt(m) we have a p series with p=1/2 and hence the series shouldn't converge at all?!
is the m restricted to finite values?
The series I'm talking about is in Equation (1) of this paper - dii.unisi.it/~capolino/pdf%20publications/… - and the part about the slow convergence is right after Equation (3), with some more detail given after Equation (11).
@Secret It is an infinite series for m
maybe it's an alternating series ?
I don't like that o someone else is now using the name studiosus.
16:11
@MikeMiller Someone else?
Is there an example of an embedded submanifold of a smooth manifold which is not smooth?
@abenthy An embedded topological submanifold, or what?
Can't you just do a line with a cusp?
yes
an embedded topological, but not smooth, submanifold I mean.
or is every embedded topological submanifold of a smooth manifold smooth?
@Danu studiosus used to be the name of one of the best MSE contributors in topology.
The complex exp() in that series seemed to be alternating between + and -, and is symmetric wrt $\pm \infty$ thus I suspect it will converge because it is alternating at least in the imaginary direction
16:19
@abenthy You can always embed a topological manifold in some large R^N
That paper is terrifyingly bad.
What paper?
Morning, @PVAL, g'night, @MikeM. ... Wait, someone usurped studiosus's name?
The Gulleimin paper
or more accurately the paper written by his students.
16:21
I'm a long-time fan of Guillemin's. :)
I don't know why anyone could ever care about Poisson structures.
They show up naturally from physics, at least.
This studiosus has been around 6 months, @MikeM, so it's not a recent usurpation.
Maybe that's why the old one changed his name.
I've never seen an error that bad in a mathematical paper.
This is a paper thats primarily about the manipulation of differential forms, and they think thats true.
@MikeMiller I just found your helpful answer here math.stackexchange.com/a/1739784/88291 Do you maybe know any reference I can cite for this result instead of copying your argument?
16:26
There are classical papers on equivariant differential topology you can cite.
One by exactly that name I believe.
I wrote that answer in the generality of proper actions but in most cases you're really working with compact Lie groups anyway.
@abenthy If someone directed you to the right argument, you better say that as well as cite whatever original source you can find.
Yes sure.
I'm not sure I need to be thanked for something so classical.
But do as you please in any case.
I couldn't find the statement that the fixed point set is a smooth submanifold if the action is smooth and proper anywhere in the literature, but maybe i just didnt find it.
and the proof you give looks nice to me
16:31
Note that there are no fixed points on proper actions when the Lie group is noncompact. See the comment.
Oh right, i read that some time ago and forgot about it... so its a statement about actions of compact Lie groups, right?
Basically yeah.
@MikeMiller Oh
@PVAL-inactive So it's an actual mistake?
Is it worth it to call the attention of Guillemin to that error?
@Danu Yes, unless there are some hidden assumptions there.
No, you should contact the corresponding author instead.
@PVAL-inactive The way it is stated seems unambiguous...
@PVAL-inactive Ah, of course.
Maybe I will
There is no indicated corresponding author, however
16:38
Contact Pires. She posted it.
arxiv.org/abs/1009.1175 The corresponding author is indicated on the arxiv papge
@PVAL-inactive I didn't know how that stuff works. Thanks, also @Mike
Time to fly back to Munich today...
Safe travels @Danu
@Danu: It seems that the correct conclusion is that the 2-form $\mu$ must be orthogonal to the symplectic form. Certainly not 0.
17:02
Hey @TedShifrin could you help me understand this example ? I just want a sanity check
I don't understand how is this sequence defined ?
is it from right to left ?
What do you mean by right to left? He drew the graph of the $n$th function.
He's defining a continuous function that has value $1$ at $a$ and is $0$ on $[a+1/n,b]$.
so this graph represent each nth function right ?
Yes, that's precisely what your notes say.
oh ok nvm I understand it now thank you
yeah
@MikeMiller I wonder if $f$ is a no-zero degree map from S^n\to M , where $M$ is a closed oriented $n_$ manifold, then how close the map $f$ goes to become an covering map?
In other word, is it true, that $f$ is homotopic to some covering map?
17:07
What if $M$ is simply connected, @Anubhav?
No just precompose with some self map of $S^n$ of degree $2$.
For nontrivial examples there are degree 2 maps $S^5 \to SU(3)/SO(3)$.
How about the squaring map $\Bbb CP^1\to\Bbb CP^1$?
That's exactly what PVAL said
Well, yes, he was precomposing. I'm just letting $M=S^2$. :P
Anyhow ... :)
17:15
Yes, I actually wanted to see some non-trivial example.
I forget how you construct that map. But it can be done.
What qualifies as a trivial vs. non-trivial example? Maps of degree $k$ from $S^n$ to $S^n$ are trivial?
@TedShifrin I didn't get your question?
You said you wanted to see some non-trivial example. What does non-trivial mean?
Ohh, I mean where $M$ is not-simply connected.
Sorry for not speaking out in the first time.
17:21
OK.
When M is not simply connected you just factor through the universal cover.
The interesting thing is when the codomain is not S^n. The example I gave is simply connected.
Mike, isn't $SU(3)/SO(3)$ simply-connected?
Oops. Too slow.
I'm trying to think of unitary frames on $\Bbb C^3$, but I don't yet see the map.
@MikeMiller yes, because in that case we have Hopf Degree theorem
Ok, use the Hurewicz theorem mod C, where C is finite groups. That says the image of pi_5 SU(3)/SO(3) in H_5 has finite index. In particular there is a map of nonzero degree.
Harder to see that it's 2. But in particular any simply connected rational homology sphere has a map of nonzero degree from a sphere.
Now i need to come up with an argument for Georges.
@MikeMiller what argument?
17:31
You can prove this using G&P degree.
Interesting: $SU(3)/SO(3)$ double covers $SU(3)/SU(2) \cong S^5$, so I don't get a map the right way.
Or maybe I'm being stoooopid again.
@TedShifrin That's nonsense. :)
Double covers of $S^5$ are disconnected. And the two groups $SO(3)$ and $SU(2)$ inside $SU(3)$ are unrelated: one is real matrices, and one is block diagonal matrices.
Our Lie group course definitely did not mention that.
@MikeMiller I didn;t get this, in what context you are saying this?
@Anubhav He claims you need to invoke homology. I'm sure that's not true. I'm trying to write a degree proof.
17:35
Yup, stooopid.
There's got to be a geometric way to see this
Ohh, yes, even there I wrote a comment... for finite pre image of a regular point+ the degree concept of G&P will implies the multiplicity.
This is coming from the Hopf bundle on $\Bbb CP^2$.
I'm currently taking a reading course with curriculum "whatever you want in chapter 4 in Hatcher." Any recommendations on the additional topics?
All of them.
I have found 4A-4G all useful at various times. 4H-4K I haven't found useful but I do found interesting.
@AndrewThompson you should read as much as you can digest from that chapter... you may skip a few proof.
17:37
4L is eminently useful.
There are other people in the course I have to consider as well. We will do Brown representability at least.
Why do you have to consider them?
LOL
@AndrewT: Follow in Mike's footsteps and be selfish. :)
Hello @shred
17:40
I'm having trouble making the argument work. maybe someone else can.
Well, they may have their own interests and/or needs. I laughed a bit when I saw Hatcher introducing pushouts in 4H. He should've done that in Chapter 0.
@GeorgesElencwajg I disagree. Consider a map $f: M \to X \to N$, where $M, N$ are oriented, $X$ noncompact; call the first map $f_1$, the second $f_2$. $f_2^{-1}(p) \cap f_1(M)$ is a finite set for generic $p$. Because $X$ is noncompact, you can find a proper map $[0,\infty) \to X$, where $0$ maps to one of the points and $X$.
2
Q: Is every vector bundle over an open subset of $\mathbb{R}^n$ flat?

Bruce BartlettCan every smooth, real vector bundle over an open subset $U \subset \mathbb{R}^n$ be equipped with a flat connection? Intuitively I feel the answer is "yes", but I don't know how to prove this.

Somehow this should lead to a proof that $f_2f_1$ is degree zero.
Could someone please help me with a composite relation proof? Been stuck on it for a good few hours now.
17:41
@Anubhav The answer to that is no.
@TedShifrin can you explain me the answer.
Huh? @Anubhav What answer?
I didn;t understand the answer, why $TS^2$ is not flat?
Because the Euler characteristic comes from integrating the curvature.
Just ask your question, @shred.
ohk, and since $TS^2$ is deformation retract onto $S^2$.
Now I get it.
17:44
Not really. We're not thinking of a metric on $TS^2$. We're computing the Euler class of $S^2$ from the curvature of the connection on that bundle over $S^2$.
http://math.stackexchange.com/questions/1969608/problem-with-composite-relations
That's the link to the question. My main problem is I don't see how I can show that each relation is a function when the composition of $R_1\circ R_2=diagonal of X$ and $R_2\circ R_1= diagonal of Y$
@MikeMiller There aren't any non-trivial examples. Any degree k map factors through the universal cover.
@shred: Ugh, I hate math filled with so many symbols.
@TedShifrin I never encountered any of these kind of relation.
@ted I'm sorry!
17:47
@shred: OK, so let's stay calm and think. What do we need to know $R_i$ is a function? We need the vertical line test for its graph as a relation, right?
@ted I'm studying from Zorich's Analysis book and it's pretty heavy on the symbols.
@TedShifrin Maybe I should read your note, becasuse do Carmo didn't do much with vector bundle in his Riemannian geometry book
I was trained to write in English, fewer symbols :)
@Anubhav: My notes are undergraduate diff geo, nothing to help you.
But, yeah, you need to discuss connections on vector bundles or principal bundles, not just Riemannian geometry.
@TedShifrin then reffer me something.
I've completed the book of Do Carmo
and solved almost all problems
@ted Umm, let's see. For a relation to be a function every element in the domain needs to have a unique element in the range.
17:50
Milnor/Stasheff discuss this stuff briefly in an appendix in Characteristic Classes. There's Kobayashi-Nomizu. Books on complex geometry discuss it, because complex geometry uses this heavily.
Wells, Griffiths/Harris, etc.
@shred: Right. So if we had $(x,y_1)$ and $(x,y_2)\in R_1$, would that contradict one of your compositions?
@PVAL I know this. I said examples where the codomain isn't a sphere.
Any simply connected rational homology sphere is an example.
@TedShifrin I've read 1st 12 chapters of Milnor's book, now I'm thinking the I should first go through the appendix before starting Charn classes.
I don't like that book, honestly, but I'm a differential geometer, not a topologist. I would learn from Chern or Griffiths/Harris or other places ...
@MikeMiller For some reason I thought we were still assuming the manifold has universal cover a sphere.
Milnor's book is awful but it's the best place for a topologist to learn.
17:54
@shred: Are you drawing any pictures to help?
@MikeM: I put my non-topologist disavowal.
@TedShifrin personally I prefer the language of topology over geometry.
I do not think that book is awful.
Then you shouldn't talk to me, @Anubhav :P
bcz most of the time, while doing geometry, I lost inside heavy notations.
Don't take it as offence @TedShifrin
I think differential forms and moving frames make geometry much more geometric than the traditional approach, but most mathematicians avoid them.
17:56
good evening
I'm not offended, @Anubhav; I'm just saying my viewpoint disagrees with yours and my taste disagrees with yours, so you might not want advice from me.
Good morning, @Alessandro :P
Hi @Ted
@ted Does it contradict the definition? I'm not really sure. I've not been taught how to draw graphs for diagonals.
@PVAL I think a good book would have an actually readable section on obstruction theory, a discussion of G-bundles as well as vector bundles, a good discussion of classifying spaces and some discussion of curvature and geometry.
I also don't much like their writing.
@TedShifrin I dont have as much knowladge as you. You know the global picture of math way more than me, so taking advice from you is always he;pful.
17:58
The obstruction theory is probably the thing that upsets me most.
@MikeMiller I agree with you
@MikeMiller You're asking for the scope of the book to increase.
Just think of $X=Y=\Bbb R$ and what's the easiest relation that's not a function (that you know from high school)? @shred
I like the fact that it isn't Steenrod at least.
That's true.
17:59
I liked Steenrod, @PVAL, so we disagree.
I think I might have had I been taught by people who use that language.
I have yet to give the paper a careful look but I've been thinking about yesterday's problem @Ted, a poset could have some infinite descending chains and also some minimal elements, so the fact that we can't extract a minimal basis from the rational balls one does not necessarily imply that there are no minimal basis at all
It just felt completely at odds with much of the stuff I've read.
@Alessandro: I thought we got to start with a basis for the topology. We're only starting with the topology?
Like I think it was probably a much better book nearer to when it was published.
18:01
@PVAL: Steenrod (and Chern) preceded the Bourbaki-ing of mathematics. For that I am grateful.
And if I'm not mistaken the fact that countably generated $\sigma$-algebras have minimal generating set is not enough to conclude the existence of a minimal basis for the usual topology on $\mathbb{R}$
@ted $xRx^2$?
Mathematics has not successfully been Bourbaki'd.
Ah, right, @Alessandro, I forgot we had switched to $\sigma$-algebras.
@shred, right. Now use that and its inverse relation and write down the compositions.
my first comment was about topologies though, what I meant is that it's possible that there is no minimal basis which is a subset of the rational balls basis, but there could be other basis from which a minimal one can be extracted
18:03
@Alessandro: I would still bet you $10 that that can't be true. :P
I still think you would win that bet, but I'm still looking for a proof :P @Ted
Good. I'm glad you are :)
@TedShifrin :/
@ted so we have $xR_1x^2$ and $x^2R_2x$?
I think bringing up the Bourbaki in a pedagogical discussion is basically equivalent to bringing up Hitler in a political discussion.
5
18:09
lol
LOL
You mean equivalent to bringing up Trump?
@shred: Yes. I guess the domain of $R_2$ is just non-negative reals, but proceed.
@TedShifrin Is there a difference?
@ted so that would mean the composition $R_2 \circ R_1 = X \rightarrow X$?
Yes, @shred, and $R_1\circ R_2\colon Y\to Y$, where $Y$ is nonnegatives.
Again, let's not draw parallels between WW2 Germany and the current state in the US! It takes away from the gravity of that war.
18:15
You take away from the gravity of the current situation in US politics. It's hardly a triviality.
American society (but, frankly, most of European, as well) is now at violently toxic levels.
Danu, did you see my postscript on that symplectic form thing?
@PVAL: In all honesty, I don't think Bourbaki is anywhere in that league. It's very much against my style, but I am not revolted by Bourbaki and have even read the occasional passage.
I have to cite Bourbaki.
@ted so two elements from the domain of $R_1$ map to one element in the domain of $R_2$ but those elements get mapped to only one element for the inverse relation?
No, the inverse relation has both as values, @shred.
$1R_21$ and $1R_2(-1)$.
@ted Ah, I see. So $x^2R_2x={(x,-x)\inX}$?
18:23
@shred: What you wrote doesn't make sense, but I think you're on the right track.
@MikeMiller compared to WW2? How US centric and absurd
Which composition are you looking at, @shred?
@TedShifrin no, sorry
@ted not really up to grips with all this notation. I was meaning that the inverse relation is the set of ordered pairs of negative and positive $x$ in the set X which is the domain of $R_1$.
I'm on my phone
18:25
I pinged you up there. I believe the right statement is that $\mu$ has to be orthogonal to the symplectic form.
Yeah,at least if you have a Hodge star I know it for sure
@Shred: So tell me this. $1 R_1\circ R_2 ?$ and $1 R_2\circ R_1 ?$?
Does $2^\omega$ usually denote the set of binary sequences?
Time to board! Bye guyZzz
That's fine, @Alessandro. I prefer to write $\{0,1\}^\omega$ for clarity. What you're writing is an ordinal, I guess, giving the cardinality.
Bye @Danu.
18:30
I'm asking because I found it in the $\sigma$-algebras paper and the next sentence is "If $X=2^\omega$ and $B$ is it's natural Borel structure" but I'm at a loss about what that natural Borel $\sigma$-algebra is supposed to be
@ted Is it $1 R_1\circ R_2 1$ and $1 R_2\circ R_1 1$?
I would write $\{0,1\}^{\Bbb N}$ for binary sequences. The symbol $\omega$ connotes ordinals, and in ordinal arithmetic $2^\omega=\omega$ holds, which is not the set of binary sequences.
For which one of them do you also get $1 R\circ R (-1)$?
Hi, tern. So you're totally agreeing with me. Yippee :)
But if you want to stick your head in the sand, keep it there where I can't hear you.
18:32
@ted $1 R_2\circ R_1 (-1)$ I believe.
@shred: $1 R_1 1$ and $1 R_1 (-1)$, but $(\pm 1)R_2 1$ only. Right?
So $1 R_2\circ R_1 1$ only.
(It helps me to draw $y=x^2$ and $x=y^2$ :))
Ah, I should learn how to read, what exactly is meant with $2^\omega$ is defined a few pages earlier
@ted but according to the definition of a functional relation in my book, it says that the elements of the range must be unique
@Alessandro if it's power set of w, then that's already a sigma-algebra. that it?
But remember that we're trying to understand what goes wrong if we do not start with a functional relation, @shred.
18:38
The fact that I've found a definition does not mean I understand it yet :P, give me a moment @arctic they're defining it as a particular case of a product between Borel spaces
@ted looking at our relations we map from two elements to one, but on the composite we are mapping back to only one element.
Not so, @shred. Let's look at $R_1\circ R_2$.
Start with $1$. Where does it go?
Oh, hell. I have my R's labelled wrong for our discussion.
Sorry.
@ted so $x^2 R_2 x$ goes from 1 to 1 and then $x R_1 x^2$ maps from 1 to 1?
@ted it's okay. I've spent long enough on this problem, don't mind spending more haha.
I'm sorry. I messed up the indices. Let's do $R_2\circ R_1$. $1R_1 1$ and $1 R_2 (\pm 1)$, so ....
(What I said far above was using the switched indices. Sorry.)
That's fine @ted I appreciate all the help I can get
18:44
So you were absolutely correct. You have $1 R_2\circ R_1 1$ and $1 R_2\circ R_1 (-1)$. So you do not get just the diagonal for the graph of $R_2\circ R_1$.
@ted because the diagonal would only map 1 to itself, yes?
Yes. The diagonal relation is just $x R x$.
So this composite relation does not give us the diagonal. So this implies that if we have a composite relation which gives us the diagonal, the first relation and second relations would have unique elements in the range for every element in the domain?
Right.
Easiest way to prove this is to do the contradiction argument we just did the example of. You think you can do it?
So the first part of my proof to show that $R_1$ and $R_2$ are functional relations is complete?
18:51
Well, you have to write a general argument. Suppose $x R_i y$ and $x R_i y'$. Show that $y=y'$ must follow.
(Do $R_1$ for concreteness. Choose the right composition. Say an analogous argument works for $R_2$.)
Just trying to arrange all of this in my head, sorry if I am a bit slow to respond
I recommend doing concrete examples often in learning mathematics.
This is a new topic for me and I should have started with it when I started the section tbh
started with concrete examples I mean
Yes, even if your teacher doesn't, you should!
My teacher is the book here. Self-studying this :P
And you're teaching me too ofc :)
18:58
Ah. I don't know what book you have, but I like to recommend Kevin Houston's How to Think Like a Mathematician.
I'm using Zorich's Mathematical Analysis I. I had no trouble in the last section's exercises. I managed to push through, but this section is giving me trouble.
The proofs in analysis get logically quite complicated — layers of quantifiers. Have you done some proofs in linear algebra and/or abstract algebra?
I've done a few proofs with groups. Very elementary though.
My personal recommendation is to do some linear algebra proofs (and abstract algebra proofs, if possible) before trying to learn analysis.
I've noticed that. As soon as I started I was bombarded with logical quantifiers.
19:03
Yuppers.
The ones in linear algebra are a lot more straightforward, the ones I've encountered so far at least.
Right, usually just one quantifier, not two or three.
I've been using Vinberg's A Course in Algebra. I don't know if you've heard of it?
I remember the look of resignation on my professor's face as he was about to negate the triple quantifier in the definition of uniform continuity for a proof...
19:04
Yup. That's one of the standard ones. Or equivalence of continuity definitions.
he actually said that writing the negation correctly was the hardest part of the proof and he was right
What I observed is that most of the students in my Honors multivariable course were smart enough that they caught on quickly. But I remember spending an hour on this when I taught advanced calculus back 30 years ago.
Absitively, @Alessandro.
I just learned a new word!
You should never learn words from me, @Alessandro :)
19:07
negating quantifiers is easy
negating implications is less easy
"easy" for people who go to grad school in math, not "easy" for average or below-average students of proof mathematics
Newbie here
don't make the mistake of assuming everyone is at or above your level of competence or intelligence
@shred: Take a look at that Houston book if you can.
And try to look at a proof-oriented linear algebra course.
It's on the online library I have access to. I can check it out now.
cool ... I wonder if my books are available in that library :P
19:09
Let me have a look
Why is it that when you quotient out the center of a compact Lie algebra you get a semi-simple remainder, but for a non-compact Lie algebra you have to use solvable ideals and not the center again?
Agh, I don't remember enough to answer that, @bolbteppa. Maybe ask @arctictern?
@ted There are a few articles with your name on it. But I don't see if there are any books. Might have to look deeper in the system. The library has a terrible search engine.
Really really interesting to see how using solvable ideals in lie algebras seems to be motivated by the failure of the center
iunno. a little jarred by the word "remainder" used to mean "quotient" though :P
19:13
OK, @shred. There is a proof-oriented linear algebra book (coauthor Adams) if you can find it without having to spend horrid numbers of dollars.
haha
I nearly referred to quotienting as 'throwing away'
@bolbteppa: If @TobiasKildetoft shows up, you might ask him.
A comment of his on a deleted question motivated this!
All the more reason, then :)
I'm going to have lunch. See you all later on !
Good luck, @shred!
buon appetito @Ted!
19:15
@ted thanks. Have a good lunch :)
Grazie, @Alessandro.
I'm having trouble seeing the intuition behind the definition of $B$ in the product below. If $B$ is a $\sigma$-algebra and $B\subseteq X$ we call call the pair $(X,B)$ a Borel space.

If $\{X_\alpha,B_\alpha\}_{\alpha\in\Delta}$ is a sequence of Borel spaces we define their product as the pair $(X,B)$ where $X=\bigotimes\limits_{\alpha\in\Delta} X_\alpha$ and $B=\sigma\{A_\alpha\times\bigotimes\limits_{\beta\neq\alpha}X_\beta:A_\alpha\in B_\alpha,\alpha\in\Delta\}$
It seems to me that we're picking only an element from every $B_\alpha$ but that can't be correct
19:31
Hey guys, are there classes or examples of nonassociative algebra that has this rock paper scissors like property. More generally, if an algebraic structure display such property, is there any special names for the elements that participate in said rock paper scissors property?
Going to head off for a bit. Good luck with sorting out your problems everyone. :)
19:50
0
Q: In differential equations, do we ever use the assumption that the integration variance C is a constant?

TheGreatDuckIndefinite Integrals vary by constant values. This is a fact. In differential equations, these C values end up being mixed around all over the place. My issue (or rather my question) is based on the fact that some integral/derivative pairs change what C is and even make them into functions of th...

can anyone answer this?
even a naive answer would be good to some degree
It's still got a while but it would suck to waste a bounty when the question clearly seems... useful to others.
@TheGreatDuck I have no idea what you're asking.
@arctictern the various "cn's" we write in the general solution to a differential equation are obviously constants, but do we ever take advantage of that fact during the solution process
@TheGreatDuck if you integrate more than once, you may end up using that fact.
seems super weird to put a large bounty on this
in general, would our solutions to differential equations change in form completely if the nature of c was a different function, or would it just be a substitution
@arctictern it's actually a pretty important question, believe it or not.
@TheGreatDuck if you replace a constant C with something that's not constant you almost surely are no longer talking about a solution to the question
19:55
@arctictern there are integrals that treat certain types of functions as constants
@TheGreatDuck what makes you say so?
@arctictern what makes me say what?
@TheGreatDuck sure, if you're integrating a function of one variable with respect to a second independent variable, then it is constant (with respect to the second variable)
@TheGreatDuck "it's actually a pertty important question" (the thing I specifically replied to - see the gray arrows in front of our comments)
@arctictern no... I mean there are alternate definitions of the integral that treat certain functions as constants
@TheGreatDuck how so?
19:57
they hold certain function forms constant
which in general, means that the "c" is now some arbitrary function type dependent on x
if you're going to be mysterious and not tell me what you're referring to I'm not sure what the point of talking is
im not being mysterious
it's a general case
there is no particular alteration worth mentioning
well good luck then
maybe someone out there will know what you're talking about
but they all have in common that c changes to a type of function (linear, quadratic, piecewise constant, etc.)
so the question boils down to
"aside from the integration do we ever assume c is a constant in our algebraic steps"
we assume it's constant, obviously
but do we ever use that assumption when finding the general solution
@arctictern now does that make sense?
it's an integration theory thing
distort the definition of the integral and see what follows
(granted, integration theory is more heavy handed on how we integrate)
wondering if there's a nice way to see that $$\det\left(\sum_{g\in G}\rho_V(g)X_g\right) $$ is an irreducible polynomial in the formal variables $\{X_g:g\in G\}$, where $G$ is a finite group and $\rho_V$ an irrep
20:04
whoa
i think that is something beyond my reasoning
:p
$$\int f(x,y,z,\cdots) dx = F(x) + C(y,z,\cdots)$$
no way can C be a function of x
@arctictern would you like to have a look at my rock paper scissors algebra question?
@Secret can you define "rock paper scissors property"? in the image you posted, it seems x is the usual group operation, but I don't understand + or its relationship to RPS
Ok, basically in the + cayley table (which is commutative) there's this interesting property where a+1=a, b+a=b, 1+b=1
as I understand it, in the rock paper scissors game, we have the set {r,p,s}, and the binary function outputs the winner of a round. but that implies every element is idempotent, unlike in your structure
20:18
So it's kinda like a literal rock paper scissors where one element absorbs another and together this absorbing property form a cycle
@Secret so it's the usual RPS structure but with squares of elements replaced by their superiors?
you'd have to decide how you want to generalize RPS to multiple hand gestures. also, is there any relationship between + and x in that structure?
I think so, the square of each element absorbs the corresponding nonsquared versions.

The only relationship between + and x is that distributive law holds as usual, only the + associativity is broken in all 27 except the listed 9 cases
Also, x forms our usual cyclic group of 3 elements
if you think RPS corresponds to quaternions, there could be an analogue for octonions. take the fano plane mnemonic - every two elements a,b is in some kind of cycle a,b,c with a third element c and we have "local" rock paper scissors. then you'd need to figure out what to do with squares though, as elements don't have unique superiors.
Sorry mistake, I mean, the double of an element absorbs the undoubled one, not squares. Let me flesh that out more clearly...
you seem to have a symmetric bilinear map $\phi:\Bbb Z_3\times\Bbb Z_3\to\Bbb Z_3$ satisfying the two properties $\phi(a,b)\in\{a,b\}$ and $\phi(\phi(a,a),a)=\phi(a,a)$.
20:28
yeah
So I guess it is kind of similar to quaternions, except that to get the next element, you only need one element instead of 2
The "generating equations"(a better term is needed) seemed to be the following:
1+1=a
a+a=b
b+b=1
The equations that give the RPS looking behaviour, and also the symmetric bilinear map you pointed above are
a+1=a
b+a=b
1+b=1
@Secret you're familiar with the cycle mnemonic for remembering i,j,k's multiplication table? I am using that as a model for which wins over which in rps.
Well, in physics we have the levi citiva symbol to do the bookkeeping for us because we use it daily in angular momentum calculations
The only thing I am known to get wrong is the sign
ij=k, jk=i, ki=j
suppose we take the oriented fano plane mnemonic for octonions and label them 1-7. there's now the Z/7Z operation, and then we can define a rock-paper-scissors operation for a,b by simply picking out the directed line that a,b are a part of and using the usual rock-paper-scissors operation.
not sure if distributivity will hold for any choice of 1-7 labelling though
I guess your $\phi$ has the additional property that if $\phi(a,b)=b$ and $\phi(b,c)=c$ then $\phi(c,a)=a$. this implies the "cycles have length 3" I guess.
yeah, that's what I noticed when I try to map where the elements gone in that triangle diagram in the slide, except the "cycle" is not the notion of cycle as that in cyclic groups, but a cycle formed by this interesting RPS like behaviour
meanwhile carrying out the fano plane suggestion to see what I get
20:59
the basic equation is

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