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8:02 PM
Surely using so many explicit indices makes everything much worse.
I'd write x in R^k and y in R^{n-k} so that points in R^n are written (x,y).
 
Yes, @MikeM, I do that also, but I was trying to fit in with the notation of the posted question. Being a good Chern student, I also use index ranges: $\alpha$ for the submanifold and $\mu$ for the normal space.
I follow your suggestion, in fact, and write the implicit function theorem with $\partial \mathbf f/\partial\mathbf y$ (both in book and in lectures).
 
Oh, I agree that you should match the notation of the question. I just think the author of that book has chosen obscuring notation.
Google says it's O'Neill, Semi-Riemannian Geometry. So of course he uses indices.
 
Well, not that I don't agree, but note that Guillemin & Pollack don't do what you and I recommend. I'm not remembering about Hirsch.
I don't think Spivak does, either, in his magnum opus.
 
Yes. When I teach out of GP I suggest people do what I say here, too. :)
A variable for each thing going on, not necessarily each number
 
If I'm following a textbook, I generally try to adopt its notation just to make it easier on students, but maybe I should have followed your advice on this one. As I say, when I wrote my book, I did it right. (And I always hated Buck's Advanced Calculus because he wrote everything out explicitly in components, never used any vector notation. Ugh.)
Yes, and while we're ranting, all books and all teachers should try students to choose $x\in X$ and $y\in Y$ and let letter choices guide what's living where. I'm stunned by how many do it randomly.
 
8:11 PM
I was shocked when 1/4 of students said "Let U be a closed set" on a midterm!
 
LOL. Yes, I do not allow that.
 
They parsed this as just "variable for a set"
 
Well, who are you and I to say $U$ has to denote an open?
 
I tend to match notation when I think there will be a serious issue for the students otherwise. I match notation every time I teach calculus, say, and 99% of the time I match notation linear algebra. (The textbook I'm using has absolutely atrocious notation for change-of-coordinates, so I modified it.) In more advanced classes I give a dictionary between notation but do not make as much effort to match.
 
We're back to leslie's symbol-pushing. If you're pushing symbols consistently, who cares what they are?
 
8:12 PM
But we are social creatures, and I might have trouble following the symbols.
 
That's your problem.
 
Well, U rotated resembles C, which stands for closed right ?
 
As long as I'm being presumptuous, see my comment here.
@Astyx: But damn you, you rotated negatively.
 
I know nothing about MC but I understand the OP's question.
 
Oh, I guess that's OK, because you're starting with C and rotating positively.
 
8:14 PM
The multivariate Cauchy formula requires integrating on a polytorus right?
 
Yes, I understand OP's question, too, but if you actually want to do geometry with these homogeneous spaces, MC is essential. As opposed to pushing symbols.
 
I would be tempted to tell him that he should delete his question and work very hard to understand those identifications himself.
 
It's obvious but I never thought about it
 
Yes, @Astyx.
That's why it's about holomorphic $n$-forms :P
 
I had done very little multivariate complex analysis, and always assumed it went circle -> sphere -> hypersphere
But it turns out the product of circles is not a sphere
 
8:15 PM
@MikeM: It also comes back to my pet peeve that books don't talk about the tangent bundle as an explicited associated bundle (associated to the adjoint rep). Indeed, that OP seems not to know what the tangent bundle is.
@Astyx: There are different analogues of a residue in higher dimension. But if you're working with a complete intersection, then the polytorus you're observing is what shows up.
 
Agree, though I worked that out myself as a boy and have understood it in that language ever since.
I think I remember having conversations with. you about this a half decade ago.
 
It becomes much harder to visualize
 
Yeah. I was never taught it. I only figured it out when I taught grad diff geo at UGA (the third quarter of it!).
I worked with Stiefel manifolds and frame bundles very comfortably, but never thought much about associated vector bundles.
Well, @Astyx, you're not going to visualize higher dimensional varieties, anyhow :P
 
@Astyx criminal
 
It's very clear what it means for a singularity to be in a circle in $\Bbb C^1$. I have no clue how to think about it being in a polytorus in $\Bbb C^2$
 
8:22 PM
Well, think it as arising as the intersection of two curves (intersecting transversely) in $\Bbb C^2$. For example, $f(x,y)=xy=0$. Take tubular neighborhoods of the two component curves and intersect.
I'm using "curve" in the algebraic sense (i.e., one-dimensional complex submanifold).
 
right
 
Can I ask math questions in here instead of posting a question in an effort to have a conversation about it? If so: If we have a function from R to R, x= x^2 what would we say about the image of the interval of [-1,1) ? would we say the it doesn't exist because the inverse function function of -1 doesn't exist in the reals.
Or would we only list the real part of it?
 
You mean $f(x)=x^2$. And you mean inverse image, which has almost nothing to do with an inverse function.
Call it preimage if you're going to think of inverse functions.
 
I guess my problem was that I didn't realize f^k(x_1, ..., x_m) can be defined on much larger set than just W, even though f^k is defined by inverting (x_1, ..., x_m) on W
let me see if that makes sense
 
8:38 PM
You are restricting the chart to the submanifold but the chart is more global.
 
not the inverse image, the image is given as [-1,1) thus the output of the function is [-1,0)
 
@TedShifrin the fact that $f^{-1}(\{x\})$ exists for a given $x$ even if $f^{-1}(x)$ doesn't is sorta weird to me. i get why the notation works like that, to be clear
 
sorry [-1,1)
 
but notationally it sorta makes me frown
erk
 
Just do what I said and use the chart to put you in Euclidean space to start with .
 
8:39 PM
Any function g on R^k extends to a function on R^n by f(x_1, ..., x_n) = g(x_1, ..., x_k).
You're just not using the extra variables since they aren't important.
I maintain this author's notation makes things worse.
 
What you're saying doesn't make sense, @OneColdRuben.
 
This is a function from the reals to the reals. I cant imagine how that makes any
This is why i thought is just DNE
 
Yes, from reals to reals. The image means we evaluate on the points in $[-1,1)$ and end up with $[0,1]$.
 
So it is saying what interval gives the image [-1,1)
 
The preimage means we ask what $x$ values give us $f(x)\in [-1,1)$.
You are talking about preimage or inverse image, as I said, then.
Nobody says you have to hit every point in there. You just want everything that lands in there.
 
8:43 PM
Well i am telling you the image so yes we are saying the same thing backward from eachother.
 
Ahh, I haven't seen this before, but it makes perfect sense. This captures the intuition I was trying to get at before, but I wasn't able to make it precise. Since bundles over the circle are either trivial or trivial + Möbius, this illustrates why the Möbius band is the quintessential example of non-orientability once again. Of course, if you don't have these loops, fix an orientation at one point and just transfer it to any other point via arbitrary path (the pullback bundle on the interval is trivial, so an orientation of one fiber unambiguously determines an orientation of the others) a
 
I'm using the language correctly.
 
And i am a fool.
 
It is not saying that the image has to be all of that interval. It's important to understand.
 
Thus the questions, to be less foolish.
 
8:46 PM
@Thorgott Mike is nicely making “no orientation-reversing loop” more tangible with the bundle. I like it.
 
So it is only the interval that covers most of the image given.
 
It might not be an interval. It might be unions of intervals.
 
@Thorgott Your dragging buys you a map $[0,1] \times D^n \to M$, and taking df_{t,0} gives a bundle iso from [0,1] x R^n to pullback bundle of TM along [0,1] x {0}. Since when you glue this up you get the non-trivial bundle, df_{0,0} and df_{1,0} must be oriented differently.
This can probably be phrased more elegantly.
 
You want all $x$ so that $f(x)$ is in the desired set. Try $(0,1)$.
 
Why would you need to specify that a function from R to R could ne a union of intervals?
 
8:49 PM
Damn. Where did I say that?
 
:57239892
 
Using language carefully is the first thing you have to do.
 
Oops.
 
I never changed your function.
What $x$ map to the interval $(0,1)$?
 
It would be [0,1) -> [-1,1) so the answer is [-1,0)
 
8:52 PM
also, Thorgott, consider the homomorphism w: pi_1(M) -> Z/2 given by w(gamma) = 1 for gamma an orientation reversing loop and 0 otherwise.
1) Notice that ker(w) is the subgroup corresponding to the oriented double cover. 2) Homomorphisms pi_1 X -> A correspond bijectively to cohomology classes H^1(X; A). w now corresponds to a class called w_1(M), the second Stiefel Whitney class. 3) Elements in H^1(M; Z/2) correspond bijectively to real line bundles. w corresponds to the real line bundle "det(TM)", whose transition functions are the determinants of those of TM.
In terms of the oriented double cover M' it's the bundle M' x_{Z/2} R, with Z/2 acting by negation on R
 
I have no idea what you just said. For what values of $x$ is $x^2$ in the interval $(0,1j$?
 
But I find that weird. because nothing goes to -1 using the function F(x) = x^2
 
I like how all of this matches up so cleanly. If you have Poincare duality these also correspond to a closed codimension 1 submanifold S --- the zero set of a transverse section of det(TM), for which w(gamma) = #(gamma cap S)
And this is the divisor picture of line bundles you learn in complex geometry
 
@MikeMiller Ah nice. You're saying the differentials constitute the clutching function $S^0\rightarrow\mathbb{R}^n$ for a non-trivial $S^1$-bundle, so must be reversely oriented.
 
F( [-1,1) ) = [0,1) but that is only a subset of [-1,1), using the function F(x) = x^2
 
8:57 PM
uh, GL(n)*
 
Yup
 
sorry corrected
F( (-1,1) ) = [0,1) but that is only a subset of [-1,1), using the function F(x) = x^2 so we are saying that only a sub set is still the correct answer for the question about the preimage of [-1,1) of F(x)=x^2 in an function defined from R to R.
 
9:14 PM
1) is clear. Let me think about 2). The first Stiefel-Whitney class of a line bundle should be the same as the mod 2 Euler class. So that is the cohomology class that takes a homology class, pushes it forward via zero section to the tangent bundle, then takes a representative transversal to the zero section and counts intersections mod 2, right?
So what you're saying is that an oriented loop generically intersects an even number of times, but an unoriented one an odd number of times. Looking at the standard pictures of the trivial and the Möbius bundle over a circle and the obvious sections
 
Sure, that's the perspective I wrote down below "If you have Poincare duality..."
I probably would not have defined w_1 the way you did but it's probably standard. It's also probably not how I would prove the relevant claim. I would prove the relevant claim in RP^n for large n, since every line bundle on an n-dim CW complex is pulled back from the tautological bundle on RP^n.
 
truth is I just don't know a good definition of Stiefel-Whitney classes, so I defaulted to using the Euler class
I'm still not really versed in the intersection viewpoint, but this all sounds very reasonable
how does the correspondence between H^1 and line bundles work? I don't think I've seen that before
 
Do you know the relation to EM spaces?
Actually, since this is H^1, I can skip down to knowing how K(G,1)'s work
You know that <X, K(G,1)> = Hom(pi_1 X, G), right?
So H^1(X; A) = <X, K(A,1)> = Hom(pi_1 X, A). But also, for A = Z/2, K(Z/2, 1) = RP^inf, and <X, RP^inf> = line bundles over X
 
9:38 PM
ah, interesting
that's a nice unified perspective on why orientable <=> w_1=0 <=> det(TM) trivial
 
@MikeMiller what does EM mean here, out of curiousity?
 
Eilenberg-MacLane
 
eilenberg maclane
 
sniped
 
kk
google assumes em spaces means typography
which, tbf, would usually be the right answer
 
9:41 PM
but man, there's way too many equivalent ways of characterizing orientability
I can probably give at least 10 equivalent definitions of orientability and explain why they're equivalent, but I still don't feel like I get the essence. Truly <insert von Neumann quote here>
 
if u twist is differnet
2
 
10:06 PM
@Ted ha!
I haven't really gotten past the third word.
 
an integer not divisible by 3, must be (3n)-1 or (3n)-2, right?
 
@10Replies yes
 
do I need to prove this?
 
I guess that depends on the course and the instructor
 
I'm writing a proof for proving that if n can't be evenly divided by 3, then n squared-1 must be divisible by 3
 
10:10 PM
I'd accept that, the $3n-1$ or $3n-2$ part, without proof if I were teaching that class.
 
ok, thanks :)
 
However, if there is doubt, including a proof wouldn't hurt.
 
what would that proof look like?
I don't think I'll include it, but I'm curious
 
@Thorgott >flag as inappropriate
To rub it in like this.......
 
@10Replies that depends on what you are assumed to know
 
10:15 PM
How do I find that out
 
Time to finish this job. Let's do a more general scenario for simplicity: if $M,N$ are manifolds with boundary and $f\colon\partial M\rightarrow\partial N$ is a diffeomorphism, $M\cup_fN$ can be made a smooth manifold without boundary so that the canonical inclusions are embeddings. If $M,N$ are oriented and $f$ is orientation-reversing, $M\cup_fN$ can be oriented compatibly with $M,N$. I claim the diffeomorphism type of $M\cup_fN$ only depends on the isotopy type of $f$, so let $f,g$ be isotopic. Then $gf^{-1}$ is isotopic to the identity on $\partial N$ and can be extended to a diffeotopy
I'm explicitly relying on the fact that the smooth structure on $M\cup_fN$ is unique up to diffeomorphism, which is not obvious from the construction, but whatever
 
@10Replies you could start by looking at division by $3$ and noting that the remainder has to be at least $0$ and less than $3$
 
I guess I should figure out why CP^2#CP^2 and CP^2#\overline{CP^2} are different for completeness sake
 
That leaves $0,1,2$
 
One is as old or as young as one chooses to be @robjohn........I've chosen my fixed age as 28. (there may be lot's of variation in that choice, but I'm sticking to it :) )
 
10:30 PM
@dc3rd It is interesting that I did not get pinged by the @robjohn there. Perhaps it has to do with the dots after it.
 
@Thorgott Hm? I think it's clear enough, you construct an atlas (which depends on f, but no additional choices)
Well done, IMO going through this is very very instructive
 
the construction I have in mind works by choosing collars
I guess you should be able to construct an atlas completely explicitly, but it seems very annoying
 
10:48 PM
I'm guessing that is probably what it is, which would be odd.....
 
11:25 PM
@Semiclassical if I have the positions and velocities of particles in a fluid under some hamiltonian dynamics at hand, what is the stress tensor?
 
11:46 PM
@robjohn Oh, now I get why you ha!ed me.
 
35? Give me a break!
Of course, I wonder what the average is here.
 
In chat or on MSE?
 

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