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17:00
yes, @Semiclassic. Geodesics on any sphere are great circles.
The research I'm doing right now concerns Lie groups and algebras, and I kinda wish I hadn't been given the research since I only know the basic definition and some basic examples of Lie groups and algebras.
Eric got quiet — I guess that means he's pondering.
[Chemistry]
Today's progress in chemistry: One of the software technicians have reported back on the error and they said the current software is too old. I have just forwarded that reply to the computing cluster's help desk as they have the new version in the cluster, but it is not installed properly (the executable script is not present in the binary folder while it should)

so much for chemistry for 5 hours, I need to rest a bit with some maths
Don't know what totally geodesic means, though.
Though the S^2 is a bad mental example since it's presumably not an example of that.
17:02
Totally geodesic submanifold means that any geodesic starting tangent to that submanifold stays in the submanifold.
Spheres won't be good for a counterexample.
Am I right in thinking that exp in the case I sketched earlier would just give the sphere itself?
i remember working out an example to this before but im blanking now
you need to be thinking in higher dimensions than 2, Semiclassic.
Yes, well
Then I've got no hope of saying anything useful at all :P
Not an interesting question for a surface.
17:04
Ok, I got too many questions to ponder on
It's all your own fault, Balarka'.
lol
I don't mind it at all
Fixed point theory is a good way to find totally geodesic submanifolds :D
Right, @SteamyRoot
We want something that's not totally geodesic.
17:05
Would it be necessary to understand a decent amount of analysis before trying to understand Lie groups/algebras? (Namely, I'm asking, "Should I work through a lot of Rudin before worrying about them?")
Fixed point locus of isometry f such that f^2 = id => totally geodesic
I don't think this helps here though, because what Ted said
Not that much, @Fargle. There are algebraic, geometry, and analytic parts of this subject.
Hmm. I guess I'm just trying to understand the prerequisites overall.
Well, in that case, I know a lot of exampes, but they're way too specific, most likely.
17:05
I'm having a hard time even understanding the claim, though. But that's presumably b/c I am teh ignorant when it comes to Riemannian geometry.
Depends what aspect you're supposed to think about, @Fargle. I can't advise without lots more details.
@TedShifrin I can email you with relevant details.
@BalarkaSen Do you even need $f^2 = \operatorname{id}$ ?
$\exp(\Lambda)$ is generated by geodesics, but you want an example where one of those geodesics doesn't remain in $\exp(\Lambda)$? That doesn't seem like the right way to understand it.
17:07
@Semiclassic: The issue is geodesics starting somewhere other than $p$.
@SteamyRoot Ah, probably not.
No, actually you don't
easy to see that
One thing which is confusing me, I suspect, is notation.
Where is $p$ in $\exp(\Lambda)$? I presume it's implicit in there and I'm just not aware of it.
We were talking about $\exp_p(\Lambda)$, to be precise.
I said $\Lambda\subset T_pM$.
17:08
Fair.
Fair for you to query.
Okay. So one is looking for a case where $\exp_p(\Lambda)$ depends on the choice of $p$? (That doesn't seem quite right either but it seems closer.)
It almost always does. We want to understand the geometry of that surface away from $p$.
We want an example where not every geodesic of exp_p(Lambda) is also a geodesic of M
M being the ambient manifold
17:11
I think I can see why the surface case would be uninteresting, at least. Each exp_p would just give the entire surface?
That's differently stated, but I guess correct, Balarka'.
Right, Semiclassic.
you can also find an example where the shape tensor is nonvanishing
second fundamental form, you mean? yeah
so do you have an example?
yeah
not yet im still pondering
If I go to M=R^3, would the point be something like: If I pick a point on the z-axis, then the tangent vectors of the form $a\partial_x+b\partial_y$ would give a horizontal plane through the z-axis
17:14
it didnt take me this long last time hmm
Oh, great, the cluster have also mistyped one of the paths in the script, thus even if an alternate way to run that calculation is not possible. Guess I cannot do much chemistry calculations today ::goes back to read journal articles::
great so the whole chat is now thinking about this problem lol
(I am not complaining)
I still remember that when I taught the beginning manifolds/geometry grad class my first semester teaching at MIT, I put the question on the take-home final to show that sectional curvature was curvature of $\exp(\Lambda)$. My solution (which I handed out) was wrong, because it assumed that that would be a totally-geodesic surface. So this has become one of my favorite challenges.
I would have been able to participate in this discussion but I knew nothing about algebraic geometry
17:15
@Semiclassic: In a flat space, you just get linear spaces, essentially, yeah.
This isn't algebraic geometry at all, Secret.
Riemannian geometry.
ah ok then
In that case I can see why different p's and Lambda's would give different exp(Lambda).
Two parallel planes won't intersect etc.
Well, in general, you can't even compare $\Lambda$s at different points!
But I feel like this is missing the point somewhat.
Yeah.
I think I don't have the toolkit (either analytically or in terms of known examples) to see why a geodesic of $\exp_p(\Lambda)$ would fail to be a geodesic of the ambient space.
17:21
Well, as I said, of course the ones going through $p$ are just fine.
maybe you could use a product
In my R^3 example, is that point that any geodesic in R^3 (i.e. a straight line) intersects a horizontal plane either as a point, as a line in the plane, or nothing.
No, the $\Bbb R^3$ example isn't an example. Nor are things in spheres or any other space of constant curvature.
No, I'm not trying to say R^3 is an example.
I'm trying to figure out what it means that R^3 is not an example.
Though even on those terms I think what I was saying didn't make sense.
17:25
Any straight line starting tangent to your surface (anywhere) stays in the surface.
I think in R^3 the reasoning would be that, if I pick two points on a given horizontal plane, then the straight line between them is a geodesic for both the plane and for R^3 overall.
Shrug. Same thing.
Thanks, @Ted. Looks like I can no longer tacitly avoid using your book. >_>
Mmkay. Just trying to put it in my terms.
Sorry, @Fargle :)
17:27
Haha, no big deal. I do like your book. I'm just very scattered.
$\exp_p(\Lambda)$ is the set of all geodesic at $p$ of the $2-$plane $\Lambda \subset T_pM$ and we want to find an $M$ such that $\exp_p(\Lambda)$ don't form geodesics of $M$ but do in $\Lambda$ at $p$?
I am not trying to solve the problem so much as understand it in the first place :P
Secret. That's sorta muddled. The question is: if you pick $q\in\exp_p(\Lambda)$, $q\ne p$, must geodesics starting tangent to the surface $\exp_p(\Lambda)$ at $q$ stay in that surface? Or, as Balarka said, must the geodesics through $q$ in the surface coincide with geodesics in the ambient manifold?
As I said earlier, alas, my toolkit of relevant examples is narrow as heck.
You're not alone. This is a non-obvious question, I think. Presumably @EricSilva has an example now.
17:40
I am thinking about how to make geodesics in $\Lambda$ away from $p$ to "diverge like crazy"...
(assume I understood correclty) here, only those geodesics through p will coincide with the manifold M. Now to figure out what M is
@Ted shouldn't there be such a plane in any manifold of nonconstant curvature
Are the only geodesics on a torus the horizontal and vertical circles?
Definitely not
i think there's a theorem of Cartan to the effect of: if there's a totally geodesic submanifold tangent to every $\sigma \subset T_{p}M$ then $M$ is constant curvature
lol suuuuuper no
@TedShifrin I never caught that subtlety before
17:43
in which case there are loads of examples
@Secret You have geodesics spiralling across the torus, or wavy lines contained in an annulus on the surface
ah I was suspecting about the spirals, but I never though of the wavy annulus ones
and also geodesics that converge to parallel circles...
@Ted Can you change the metric to third order to force the existence of totally geodesic submanifolds?
Trying to find a manifold with very wavy geodesics...:
17:53
EricS: yes, and I think you'll find that result on one of my homework assignments :P
I doubt it, @MikeM.
yeah last time i did this i thought of products immediately, they're usually good for this kind of counterexample
Is it possible to find a manifold whoose geodesic behaves like $\sin(\frac{1}{x})$ (made continuous by specifying f(0)=0$)?
ah i think it's not hard to show that theorem just playing with jacobi fields
@EricSilva: See problem 4 on assignment 3 from my Riemannian geometry homeworks.
ah i see
18:02
Sorry I had to afk for a while
so, did we figure it out?
I don't know. Did "we"?
@Secret: You don't mean what you wrote there with $\sin(1/x)$.
@EricSilva Oh cool
But remember you have to have geodesics in every direction at every point, and things vary smoothly.
@Balarka': That's the theorem whose proof is the exercise I mentioned above.
O smooth, right, then geodesic which "shape like" a continuous version of $\sin(\frac{1}{x})$ is not possible since it is not differentiable at $x=0$
18:05
Ah, I asked MM, @Ted. He says the complex hyperbolic plane works.
You meant $x\sin(1/x)$ or some $x^k\sin(1/x)$, but ... yeah, smooth.
Anything not of constant curvature will work :)
You just need to figure out an explicit example.
Right, I wanted a visual example. He says if I exp project a 2-plane which is not totally real or a complex 1-dimensional subspace, then I get something that isn't totally geodesic.
Though of course it's very interesting that literally anything works
The same should work in $\Bbb CP^2$.
We know what the geodesics are, etc.
Ah, good point
I suspect a torus is not going to work. Even though it has regions of positive cuvature, regions of zero curvature and regions of negative curvature, in each region where the curvature are of the same sign, it is constant
18:09
Both Eric and I had the idea that you should think about a simple product (that is not constant curvature).
the first place my mind went to prove the theorem was to use $J'' + R_{J, \dot{\gamma}}\dot{\gamma} = 0$ and then Schur's theorem
cool theorem tho
Not so, @Secret. I really don't understand.
EricS: I have never been a Jacobi field person :P
More evidence that I'm NOT a Riemannian geometer.
i think the jacobi equation is p cool
Sure thing.
18:10
Sturm comparison, etc.
@Secret: But totally NOT constant anything.
I am very content with CP^n as an example. Thanks all, for all the very interesting facts
i like to keep $S^{2} \times S^{1}$ and $S^{2} \times S^{2}$ high on my list of possible counters to things
@Eric I am not sure if I understand the geodesics of either very well
Nah, for the first, I do. It's covered by S^2 x R
$S^1 \times S^1$ is the flat torus, thus should have zero gaussian curvature everywhere?
What I always wonder when I see "Jacobi field" is why it's called that.
18:13
I can cheat for $S^2\times S^2$ and write it as $\tilde G(2,4)$, so it's a symmetric space.
OHHH, right
$S^{2} \times S^{2}$ has a totally geodesic torus @Balarka so that's cool
@Secret: Depends on the metric!! If you are thinking of it in $\Bbb R^2\times\Bbb R^2$ in the obvious way, then, yes, flat.
Presumably because Jacobi thought of them in terms of varying geodesics, @Semiclassic.
I assumed it was cause they satisfy the Jacobi equation but that might not be true
18:14
Mostly I wonder about the prehistory of Riemannian geometry.
well, why is the Jacobi equation called that?
good question
How do you find the range of $f(x)=\log_e \sqrt(4-x^2)$. I am getting $\R$ but the correct answer is $(-\infty,\log_e 2]$.
I see, yes, I tend to think of it as being embedded in $\Bbb{R}^4$
i am not usually confident that things are named after the right people
18:15
Spivak addresses some of it, Semiclassic. After all, he includes translations of Riemann, etc.
True, Eric.
Hmm, nice.
@EricSilva I'll bite you for not knowing the history
Well, Secret, most of us think of it in $\Bbb R^3$. :)
Yeah, Arnold's principle and all that.
^^
18:15
heya @Danu !
Hi Ted
Wow, Danu and Manu ...
hi skull
@Balarka tbf when i say we should know history i mean more history of ideas than i do history of who named things what
I mostly wonder to what extent classical mechanics served as a historical motivation/inspiration for Riemannian geometry.
18:16
@Eric i know i was pulling your leg :P
i am aware
why so serious
Thinking of geodesics in terms of the energy functional, sure, Semiclassic.
@TedShifrin Who's Manu?
I'm not sure if that was the first approach.
Manu Schiller just entered, @Danu.
18:17
@Semiclassical Hint: Ask on History of Science and Mathematics!
whooooaaaaa
I can visualise the tesseract, the pentachoron, $S^1 \times S^1$, $S^2 \times [0,1]$, Klein bottle, $S^3$ and $T^3$ as close as possible to it in $\Bbb{R}^4$, but there's a lot of mathematics and geometry I still don't understand, and I expect to have those gaps all filled in once I get into differential geometry
EricS: Such utterances are so informative.
The real question is: Why are there no tennis matches today :(
18:18
i was informing you all of my delighted surprise
What I have in mind is the dimensionality of phase spaces in classical mechanics.
Because Wimbledon always gives the lawns a rest on the middle Sunday. (Unless there have been massive rain backups.)
@TedShifrin So it turns out the Riemann surfaces course is kinda... ehh... We're not even going to do Riemann-Roch :\
Bah, @Danu. I fail him.
@Balarka i default serious bc internet unseriousness is hard to read
18:19
I mean, if you've got a particle confined to the surface of a sphere, the configuration space is 2D but the phase space is 4D. So just by thinking in that way it seems like one is forced to go to spaces of higher dimension than 3.
How do you find the range of $f(x)=\log_e \sqrt(4-x^2)$. I am getting $\mathbb{R}$ but the correct answer is $(-\infty,\log_e 2]$.
No RR, and no surfaces associated to algebraic functions
@Danu good question
That leaves us with the torus and the sphere :D
This is what happens when someone too removed from algebraic geometry teaches it, @Danu.
18:19
I even tried to sneak in an exercise showing that any oriented surface will do but it was veto'd :P
It's like people who teach undergraduate curves and surfaces and don't get to Gauss Bonnet. Makes me so angry.
omg why would you ever do that
(Or multivariable calc and don't get to Green's/Stokes's, etc.)
Everybody will be left with the feeling of: Why did I do this?!
Because people don't plan or time things right, and they may or may not be experts on the material.
18:20
Most other 4D shapes, I cannot visualise or draw their projections without incuring significant error
By the way, Ted, I have finally come to appreciate the Weierstrass P :D
Ah, cool, @Danu.
I have done so many exercises on that this semester
The only negative feedback I got on the student evaluations was a one-sentence critique saying "Less Weierstrass P".
gauss-bonnet and theorema egregium are like my must do theorems i think
I usually did it in the regular part of complex analysis and then reintroduced it during Riemann surfaces.
18:21
@MrAP think where log will be undefined
@JyrkiLahtonen welcome
I'm just saying, Eric. There are lots of badly constructed/taught courses out there.
so sad :(
The problem in this case was really that the teacher didn't know the theory himself
It's not hard for him but he had no overview at all before starting... No plan
@Danu: One of the best courses I ever taught was a year-long applied math course back in 1986-87. I learned over half of it as I taught the course. But I guess I worked a lot harder at it than the average university prof bothers to.
18:22
He was just reading the material from the book a few weeks before teaching it
@TedShifrin Hmm.. Maybe.
You are probably way more into teaching than most, yeah.
Yes, but I was also excited to learn that stuff and teach it well. ... Surely reading the table of contents or preface should give someone perspective on the Riemann surfaces course. Or talking to colleagues ...
we should have a riemann surfaces course here
but alas
I think I was probably among those who learned most this time :)
Well, if you're going to have probabilists teaching complex analysis ... :)
I found this super amazing complex analysis book (2 volumes) by Freitag
18:25
I think they recently used that at UGA.
when i take the grad complex course it will be a geometric measure theorist teaching it
I don't know the book.
I really like it. It sorta does Riemann surfaces but completely without "technology" so no sheaves and stuff
Very classical... I like it
Sounds like the kind of book I'd appreciate.
It does applications to number theory, also.
18:26
I remember when one of our analysts complained back in the 80s the first time I taught graduate complex analysis that I wasn't competent to teach it.
Um, complex geometer? Really? ... :D
I'm finding reasons to be interested in number theory/algebra recently. That's good becuase I probably have to spend time learning algebraic geometry...
Well, so does Stein/Stakarchi, Danu. Meh.
@TedShifrin Yikes
Also hey everyone!
18:27
i think im not gonna have a mathy day today
If I don't actually find any PhD positions I'm gonig to work my ass off on algebraic geometry stuff in the coming months.
Keep me posted on news, Danu.
0
Q: Tangential proof regarding the Collatz Conjecture formula.

TyphonLet us start with the set: $\{1\}$. Every iteration replace every element $x$ in the set with two elements $2x$ and $\frac {x-1}{3}$. Conjecture: The sum of every element of the set formed by the Nth iteration is $2^N$. I was just messing around with reversal of the Collatz Conjecture and ...

@EricSilva Same here! Got up at 7:30 to play tennis, arrive at the courts at 9, started raining. Moved tennis to 12:30, went to play squash 11:15-12:15 then played tennis 12:30-2:30
Haven't managed to be productive since getting home :\
Rain again, Danu? Geez ...
18:28
Yeah, it's been super unlucky: Every day but Sunday seems fine!
LOL
I thought I was the only jinx.
i just have a migraine
I lost that tournament match btw Ted
but the guy is now a training partner of mine
Sorry if it's my fault for asking you questions, Eric :)
and I beat him for the first time today!
18:29
nah i woke up with it
aww, well that's a cool result, Danu.
6-3 7-5, came back from 1-4 in the second
I gotta wonder how the tennis player with the knee injury is faring.
usually it helps to cook good food but i have no groceries
But that probably won't be clear for quite a while.
18:29
She has more doctors to see in the US, last I heard, Semiclassic.
Well, go get some and cook, Eric.
I have a fractured finger. I am coming up with impressive stories to tell about it's origin.
Makes sense.
Had an epic point serving at 4-5, 15-30 down. He managed to come to the net and I handed him a smash, but then hit a forehand winner down the line, on the run. That really swung the momentum in my favor!
Not to mention ITS origin, Balarka'.
@BalarkaSen does it hurt?
18:30
that's the plan @Ted
...would've been two set points down had I lost that point.
A deadly fist fight with a neobourgeois on Hegelian dialectics is my current story
...
Danu, no one can accuse you of lack of self-confidence :)
the truth?
18:30
@TedShifrin Well... That's just in tennis ;)
@Balarka i broke my finger free climbing a cliff once
i didnt realize until i was writing an essay the next day
@EricSilva bad or minor?
relatively minor
oh ok
"The thesis was his smug face, the antithesis was my fist, and the synthesis was a broken finger."
8
18:31
currently dealing with a radial neck fracture in the e;box
Gold
Thanks for supplying me with this
it doesnt hurt except when i do something I shouldn't and then that's literally the equivalent of my body slapping me in the back of the head for being an idiot
im out
bye chat
Bye, Eric. Save me some food :)
18:33
OK, I'm going out to lunch with a friend. See y'all anon. Oh, haven't seen tern in a while!
see ya, skull
Bye geometers
@AkivaWeinberger scroll up to see a neat number theory question I posted
Given $f(x)=\frac{x}{3}-\frac{1}{3}$ $$f^n(x)=\frac{x}{3^n}-\sum_{k=1}^n\frac{1}{3^n}=\frac{x}{3^n}-\frac{\frac{1}{3}‌​}{1-\frac{1}{3}}=\frac{x}{3^n}-\frac{1}{2}$$
Given $g(x)=2x$ $$g^m(x)=2^m x$$
Any cross term has the form: $(f^n \circ g^n) (x)$ or $(g^m \circ f^n) (x)$
@Typhon It's in a random order
It shuffles every time you load the page
Back to algebra finally
Woo algebra
18:40
By which I mean dynamics because holy crap this problem
@Daminark Way to ruin my excitement :(
I mean also algebra
Dynamics has a different vibe than I thought it would
$(f^n \circ g^m) (1)= \frac{2^m1}{3^n}-\frac{1}{2}$

$(g^n \circ f^m) (1) = \frac{2^m1}{3^n}-2^{m-1}$
There are a few main examples we're looking at, the automorphisms of the torus, solenoid (which I don't really get), horseshoe which is apparently conjugate to symbolic dynamics and shifting, and rotations of the circle
18:43
symbolic dynamics are neat
"automorphisms of the torus" ?
As in, of the fundamental group of the torus?
he means self-diffeomorphisms
automorphisms in the DIFF category
Think of the torus as $\mathbb{R}^2/\mathbb{Z}^2$
Though by that I mostly mean "it's neat that numbers in the Cantor set = numbers that don't need 1 when written in base 3."
Literally a quotient group
18:45
Ew, diffeomorphisms
I'll stick with homeomorphisms :3
Then if you have an integer matrix, you get an induced action on the torus
@Secret You evaluated the finite sum like an infinite one
Now, if we ask that it's got determinant 1, it becomes an automorphism of the torus
which is why it fails at $n=0$
ooooooops....
18:45
@Daminark Well, yeah, that integer matrix will just be the automorphism of the fundamental group of the torus, no?
Also, shouldn't determinant -1 be allowed too?
Oh right, yeah
@SteamyRoot homeomorphisms are yuckier than diffeomorphisms. but it seems Daminark means group automorphisms of the torus
And I mean, I guess that is true as well, but we're looking at the torus itself as a group also
Induced by automorphisms of its fundamental group, much as we aren't quite framing it in those terms
Though we're considering those that are called hyperbolic toral automorphisms
@Steamy I don't get it. There are distinct automorphisms of T^2 which induce the same thing in pi_1
Meaning, we don't want any eigenvalues on the unit circle. This has the effect of making them real if we ask $|\det(A)| = 1$
18:47
why do you want to identify it with anything happening on pi_1?
hi chat from me too
And also apparently the eigenvectors have irrational angles?
but still, computing those don't really help because $f$ and $g$ don't commute thus $fffffgggg$ differs from $ffggggfff$, and to compute the sum in typhoon's question, you need to summ up all possible strings of f and g. Otherwise, some clever number theory stuff is needed which I don't know
A lot of stuff will be the same up to homotopy
18:48
You don't want to do that
Restricting to the fundamental group means you merge a lot of those homotopy-equivalent stuff
Also, calculations on the fundamental group are easier :P
Anyway, so what happens is that you can take a point $x$ and define $W^u(x) = \{x + tv_{\lambda} \mod 1 | t\in\mathbb{R}\}$
Unless you want to study the mapping class group, which is an entirely different topic
@Steamy Yes, but utterly useless in dynamical contexts
Where $v_{\lambda}$ is the eigenvector associated with eigenvalue $\lambda > 1$, the other one being $v_{1/\lambda}$
If $f$ is a self-map of the torus, and $f_*$ is the induced automorphism on the fundamental group, then the number of $f_*$-twisted conjugacy classes is a lower bound for the number of fixed points of $f$ :D
18:50
This starts to sound like KAM theorem stuff
@Balarka I think the fact that we're not framing it in terms of fundamental groups is that the book doesn't want to assume you know any algebraic topology background? It may very well be possible that, as is often the case, weird shit connects fields
MCG(T^2) on the other hand (which is homeomorphisms of T^2 upto isotopy) turns out to be isomorphic to Aut(pi_1(T^2)) = SL2(Z), yeah
GL_2(Z)
@Daminark Well, it's not terribly useful to identify homotopic diffeomorphisms if you want to study the dynamics of a map like Steamy said
That's not relevant to the kind of business you want to do
In general maps with interesting dynamical properties tend to get dumb if you perturb it a little
For reference, KAM is this: en.wikipedia.org/wiki/…
18:55
I think I'll just table the torus problem though, even when not braindead (or at least not due to sleep) this isn't registering well with me at all
I'm guessing you'll learn about Anosov diffeomorphisms and Arnold's Cat Map, if you're already working on the torus?
Potentially
Right now, we're doing topological dynamics, so stuff like transitivity, mixing, expansiveness, entropy, etc
@SteamyRoot Oh yeah right. I meant the orientable MCG I guess
This Wednesday I'm gonna give a lecture on applications of topological recurrence to Ramsey theory
Especially this one theorem called van der Waerden
For each finite progression $\mathbb{Z} = \bigcup_{k=1}^m S_k$, one of the sets $S_k$ contains arbitrarily long finite arithmetic progressions
So that's something to look forward to for sure

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