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12:03 AM
Actually what if we let $b=a$?
Nope that won't do anything
Uh, let $c=a-b$
Then we have $z(a,b) - z(b,a-b) + z(a+b,a-b) = 0$
$c=a+b$?
$z(a,b) - z(b,a+b) + z(a+b,a+b) - z(a+b,a+2b)$
Okay one thing I'd like to see is what's $z(a,-a)$
So let $a=c=-b$ in the cocycle condition
Okay that just gives commutativity... maybe if we let $c=0$?
Nope
 
12:19 AM
Whatever I'll take commutativity for now, how to get an inverse
So given $[a][b]$ we want $[c][d]$ such that $[a+c+z(b,d)][b+d] = [0][0]$
We know $b=-d$
So if we let $c = -a-z(b,-b)$ we're good
Oh no wait that doesn't make sense, does it
Fuck
Oh no actually I think it might be fine
YEAH
Dank
Okay back to commutativity
Fuckin hell
OH THIS MOTHERFUCKER
Okay okay
$z(a,b) - z(b,c) + z(a+b,c) - z(a,b+c) = 0$
$z(b,a) - z(a,c) + z(a+b,c) - z(b,a+c) = 0$
Subtract, you get
$z(a,b) - z(b,a) - z(b,c) + z(a,c) - z(a,b+c) + z(b,a+c) = 0$
Oh no
This doesn't work as planned
 
12:50 AM
rip with a capital b
 
I'll just black box this for now and figure it out later
Now coboundaries
 
1:12 AM
Alrighty. First G-P exercise.
A smooth function on $\Bbb R^k \subset \Bbb R^l$ is a function $f : \Bbb R^k \to \Bbb R^n$ such that for every point $x \in \Bbb R^k$, there is an open set $U \subset \Bbb R^l$ and a smooth function $F : U \to \Bbb R^m$ such that $F|_{U \cap \Bbb R^k} = f$. But $F$ restricted in this way is essentially just the first $k$ coordinates of $F$, and this is clearly smooth in the usual sense in $\Bbb R^k$, as it has continuous partial derivatives of all orders.
Conversely, suppose $f$ is a smooth map on $\Bbb R^k$ itself. Then the map $f \times \text{id} : \Bbb R^k \times \Bbb R^{l-k} \to \Bbb R^l$ is smooth (again, having continuous partial derivatives of all orders), and so for each point $x \in \Bbb R^k$, the whole space constitutes a nbhd on which you have a smooth function that restricts to $f$. So $f$ is smooth on $\Bbb R^k$ considered as a subset of $\Bbb R^l$.
I feel like I might be missing something somewhere here.
 
@BalarkaSen Do you know much about triangulated categories?
 
2 seems easier. Let $f : X \to \Bbb R^m$ be smooth, and let $x \in Z$. There is a nbhd $U$ at $x$ such that a smooth map $F : U \to \Bbb R^k$ exists where $F|_{U \cap X} = f_U$. But then $F|_{U \cap Z} = f_{U \cap Z}$, so that $f|_Z$ is a smooth map.
lots of typos in that but I think the sense of it is clear
 
1:45 AM
3 is giving me some trouble
I'm not sure how to "glue" the information of the smooth maps
 
Which text @Fargle?
 
Guillemin-Pollack.
I think I have something here tho
The problem asks to show that for $X,Y,Z$ subsets of Euclidean spaces, if $f : X\to Y$ and $g:Y\to Z$ are smooth, then their composition is smooth
So let $x \in X$; there is a nbhd $U$ such that there's a smooth function $F : U \to \Bbb R^m$ (the ambient space of $Y$) yadda yadda.
There is also a nbhd $V$ of $f(x)$ such that there's a smooth function $G : V \to \Bbb R^l$ (the ambient space of $Z$) yadda yadda yadda.
$f$ is smooth, hence continuous--that means $f^{-1}(V)$ is open, and $F|_{U \cap f^{-1}(V)}$ is smooth. Furthermore, this restriction can now be composed with $G$ to give a nbhd $U \cap f^{-1}(V)$ of $x$ such that there's a smooth map $G \circ F|_{U \cap f^{-1}(V)}$ for which $(G \circ F|_{stuff})|_{stuff \cap X} = (g \circ f)|_{stuff \cap X}$.
 
 
2 hours later…
3:43 AM
Alright, number 4:
(a) The function is clearly smooth on its domain. Its inverse is $y \mapsto \frac{ay}{a^2 + \|y\|^2}, also clearly smooth. Bada bing bada boom.
(b) Given $x \in X$, $U$ nbhd of $x$ gets mapped by $\phi$ to $V$. There is a ball $B$ in $V$ containing $f(x)$ since $V$ is open, and this pulls back to an open set containing $x$--since $\phi$ is a diffeomorphism, we conclude that $\phi^{-1}(B)$, a nbhd of $x$, is diffeomorphic to a ball $B$, which is diffeomorphic to $\Bbb R^k$.
Oops, didn't even check the TeX. That's $y \mapsto \frac{ay}{a^2 + \|y\|^2}$
 
@Alex Vaguely
 
 
6 hours later…
9:37 AM
@Alessadro u done w exam
 
I have an algebraic number theory presentation to give next Friday
that'll also be my last exam
 
ahh
cool
 
(I should also finish writing my thesis at some point)
 
is your thesis on lagic
 
yeah, model theory to be precise
 
9:44 AM
very cool
 
I want to focus on model theory and set theory during my master
 
I know nothing about that particular discipline of mathematics
I should, someday, learn something about it
 
LoL looks like the modules handbook for next year was written by a mathematician
 
LOL
 
How is it going with interviews and stuff by the way? When will you know where you're going to study next year?
 
9:54 AM
I have the interview on 21st
I think I will know by a few days after that if I'm going to get in
 
What about the other place (or places? I remember only two) you applied to?
 
I applied to two, I got in one of them, of which I will be taking the interview
I didn't get in the other
 
Ah, I see, that sucks
 
Eh its ok
 
I don't really know much about it but the Indian admissions sound crazy
 
9:58 AM
It has been driving me quite insane for the last few months. But I have sort of stopped caring now
Whatever shall happen will happen
 
10:10 AM
I see, good luck!
 
thanks
 
 
3 hours later…
12:53 PM
OK, I'm going to rant about function spaces and technicalities about the topology on function spaces and how classical result follows from such conversations
 
spicy
 
The only reasonable function spaces are Banach, all else is garbage
 
That is correct, they will be Banach.
 
Good, so it's not too bad
 
1:08 PM
$M^m, N^n$ be smooth manifolds. Denote $C^k(M, N)$ to be the space of $C^k$-functions from $M$ to $N$ and $C^\infty(M, N) = \bigcap C^k(M, N)$ consists of smooth maps from $M$ to $N$ (so they are $C^k$ for all $k = 1, 2, \cdots$).
Denote by $\mathscr{G}(M, N) = \bigcap \mathscr{G}_p(M, N)$ to be the space of germs of functions, where $\mathscr{G}_p(M, N) := \{f \in C^\infty(U, N) : p \subset U \subset M \text{is open}\}/\sim$ where $f \sim g$ if say $f$, $g$ are defined on some neighborhoods $U$ and $V$ of $p$, and $f|_W = g|_W$ for some smaller open set $W \subset U \cap V$ containing $p$.
Now we can start putting topologies on these objects.
The topology on $J^k(M, N)$ comes from pulling back the topology (and also the smooth structure) by the local trivializations of $p^k$, where $J^k(\Bbb R^m, \Bbb R^n)$, which is a space of tuples of polynomials, is given the Euclidean topology on the coefficients of the polynomials.
There is a natural morphism $C^k(M, N) \to J^k(M, N)$ by sending a $C^k$ function $f : M \to N$ to it's $k$-th order Taylor polynomial in the $k$-jet space, which let us denote as $J^k f$. This is the "k-jet prolongation/extension of $f$"
We define the weak Whitney topology on $C^k(M, N)$ by setting the basic open sets up as $\mathcal{V}(K, U) = \{f \in C^\infty(M, N) : J^k f(K) \subset U\}$ for any compact set $K \subset M$ and open subset $U \subset J^k(M, N)$.
If $M$ is noncompact, a better choice is the strong Whitney topology, where the basic open sets are $\mathcal{V}(\{K_i\}, \{U_i\}) = \{f \in C^\infty(M, N) : J^k f(K_i) \subset U_i\, \forall i\}$ where $\{K_i\}$ is a family of compact subsets of $M$ and $\{U_i\}$ is a locally finite atlas on $J^k(M, N)$.
If $M$ and $N$ are closed manifolds, then as proved in this paper, $C^k(M, N)$ under the (weak or strong, they agree if $M$ is compact) Whitney topology forms a Banach manifold.
 
1:28 PM
In the immortal words of one of my analysis professors, "That's good. draws smiley face on the board We like that."
 
The topology on $C^\infty(M, N)$ is given by the "limit topology" coming from the $C^k$ Whitney topologies. Namely, we have inclusion maps $C^\infty(M, N) \hookrightarrow C^k(M, N)$ for all $k$. Give $C^\infty(M, N)$ the topology given by union of the topologies of $C^k(M, N)$ under these inclusion maps.
Alternatively just add "for all $k$" in each of the definitions above.
Here's a classical result in differential topology. First a definition: If $M, N$ are two closed smooth manifolds and $W \subset N$ is a submanifold then a smooth map $f : M \to N$ is said to be transverse to $W$ if $df_p(T_p M) + T_{f(p)} W = T_{f(p)} N$ for all $p \in M$. (If $f(p)$ lies outside of $W$, then this is vacuously satisfied). We say $f \pitchfork W$.
Theorem: If $f : M \to N$ is so that $f \pitchfork W$, then for any smooth homotopy $h_t : M \to N$ of $f$ for $t \in [0, 1]$, there is an $\epsilon$ such that for all $t < \epsilon$, $h_t \pitchfork W$. Transverse maps are stable under perturbation.
Here's a proof sketch using these technical topology on function spaces business. Consider the subspace $\mathscr{R} \subset J^1(M, N)$ of $1$-jets $(x, f(x), L(x))$ where $f : U_x \to N$ is a function defined near some chart around $x \in M$ and $L\in \text{Hom}(T_x M, T_{f(x)} N)$ is a linear map, such that this 1-jet is transverse to $W$, ie, $L(T_x M) + T_{f(x)} W = T_{f(x)} N$, then
$\mathscr{R}$ is a closed subset of $J^1(M, N)$. This is easy to see; say $(x_i, f_i(x_i), L_i(x_i))$ is a sequence of 1-jets in $\mathscr{R}$ converging to $(x, f(x), L(x))$. Then $L_i(T_{x_i} M) + T_{f_i(x_i)} W = T_{f_i(x_i)} N$ for all $i$.
But by choosing a smooth path $\gamma$ containing $x_i$ for all $i > n$ for some large enough $n$, and trivializing $TM|_{\gamma}$, we can realize this situation as a sequence of subspaces $(P_i, Q_i)$ of $\Bbb R^n$ such that $P_i \pitchfork Q_i$ for all $i$ and $P_i \to P$ and $Q_i \to Q$, but that of course implies $P \pitchfork Q$ because transversality of subspaces of a vector space is clearly stable.
That wasn't correct, I got confuzzled. The complement $\mathscr{R}^c$ is a closed subset of $J^1(M, N)$, consisting of 1-jets $(x, f(x), L(x))$ such that $L(T_x M) + T_{f(x)} W \neq T_{f(x)} N$. Replace all the $=$'s in the last three messages by $\neq$. It is easy to construct a sequence of transverse subspaces of $\Bbb R^3$ which converges to non-transverse subspaces (take a 2-plane and a line in $\Bbb R^3$, and at each stage reduce the "angle" between them to $1/n$)
Non-transversality is a closed condition on linear subspaces.
 
1:51 PM
what's the idea behind transversality
 
To clear the confusion: I'll state it. The complement $\mathscr{R}^c$ consisting of 1-jets not transverse to $W$ is a closed subset of $J^1(M, N)$.
@Fargle Guillemin-Pollack. It's all there :)
 
:^|
nah you right
 
Anyhow, so $\mathscr{R}$ is an open subset of $J^1(M, N)$. But that means the set $\mathscr{T} = \{f \in C^\infty(M, N) : J^1 f(M) \subset \mathscr{R}\}$ is an open subset of $C^\infty(M, N)$, as the weak $C^\infty$ topology consists of union of weak $C^k$ topologies for all $1 \leq k \leq \infty$. But $\mathscr{T}$ is exactly the set of smooth functions $f : M \to N$ such that $f \pitchfork W$, by definition of $\mathscr{R}$.
So the set of smooth functions transverse to $W$, which let's call $C^\infty_{\pitchfork W}(M, N) \subset C^\infty(M, N)$ is an open subset. By the paper sited above, $C^\infty(M, N)$ is a Banach manifold, hence for any $f \in C^\infty_{\pitchfork W}(M, N)$ we can choose a Banach chart $\mathscr{U} \subset C^\infty_{\pitchfork W}(M, N)$ containing $f$.
If $h_t$ is a smooth homotopy of $h_0 = f$, then there exists an $\epsilon > 0$ such that for all $t < \epsilon$, $h_t$ are all contained inside the Banach chart $\mathscr{U}$. Therefore $h_t$ for all $t < \epsilon$ are also transverse to $W$, as desired.
@BalarkaSen Correction: No, some $k$ where $1 \leq k \leq \infty$. It's the union of all the topologies.
@MikeMiller Do you want to check if this proof of the stability theorem works :3
@Fargle I was writing so was trying to hold off an exposition on transversality. Linearly, it's easy to describe: If $V_1, V_2 \subset W$ are two subspaces of a vector space, they are said to be transverse if $V_1 + V_2 = W$. Simple as that.
 
2:07 PM
I see
 
If a thing cuts another thing by slicing
Not tangentially
For manifolds, it's an easy follow-up of the linear definition. $N_1, N_2 \subset M$ two submanifolds are transverse if for any $p \in N_1 \cap N_2$, $T_p N_1 + T_p N_2 = T_p M$.
The x-axis and the y-axis in $\Bbb R^2$ are transverse, but $y = x^2$ and the x-axis are not.
 
oh that makes perfect sense
nice example
 
Yup it's a very intuitive thing
 
seems like it extends easily enough too--e.g. $S^2$ and a coordinate axis are transverse, but $S^2$ and a tangent line are not
 
Careful
 
2:15 PM
oh
yeah
I see the problem
 
What is the problem? State it.
 
Alright I still believe the first part of the sentence I said
 
The problem is that you haven't stated where they are transverse inside of
 
The normal line plus the tangent plane make 3-space
ah right
they're transverse as submanifolds of $\Bbb R^3$
 
Correct, they are transverse in $\Bbb R^3$
Not in $\Bbb R^4$ though
 
2:18 PM
right
plane plus line $\neq$ 4 dim
 
2 + 1 $\neq$ 4 quick maffs
 
that property is a uckas
 
lmao
 
alright, so under your latter formulation, it looks like transverse manifolds have to add up to at least the dimension of the space
 
Indeed
 
2:21 PM
I guess my question now is, where is that sum of tangent planes taking place? Inside of $\Bbb R^n$, the ambient space of the manifold $M$?
 
No, inside $T_p M$.
$N_1, N_2$ are submanifolds of $M$
 
Oh right right
 
If $p \in N_1 \cap N_2$, then $T_p N_1, T_p N_2 \subset T_p M$ are subspaces
 
So for example, two (non-parallel) planes are transverse in $\Bbb R^3$ as well
 
Yes.
 
2:22 PM
I just wanted to make sure there wasn't a more rigid condition there I didn't see
 
"Transversality of manifolds" is a meaningless term. Transversality is an adjective of submanifolds (well, you can slightly generalize it to maps and submanifolds, but whatever)
 
In the same way you wouldn't call a group normal
 
Yep
Here's the magic of transversality. If $N_1, N_2 \subset M$ are transverse submanifolds, $N_1 \cap N_2$ is also a submanifold of $M$, with $\text{codim} \, N_1 \cap N_2 = \text{codim}\, N_1 + \text{codim} \, N_2$.
 
So what does it mean to say a map is transverse to a submanifold--how does that translate into this definition?
Oh I buy that
 
@Fargle There's no hurry to learn that stuff.
 
2:25 PM
Fair enough
 
It's all in G-P, you can read at your leisure. Really one should understand it for submanifolds first.
 
(that probably sounds a bit dejected but nah srsly, fair enough--I trust your judgment)
 
Yeah I just don't want to rewrite Guillemin-Pollack in this chat while you already have the book, is my standpoint :P
 
I think I've done enough of the first section's exercises to feel justified in moving on
 
Better to talk about ideas togather
 
2:26 PM
yee
 
Non-transverse submanifolds can have totally bad intersection
You can find two submanifolds of $\Bbb R^2$ intersecting at a Cantor set.
 
>:c
 
@BalarkaSen what
 
that's just disgusting
 
Even a fat Cantor set
 
2:28 PM
intervals are just cantor sets in progress
 
That's the kind of bullshit you expect from real analysis, not geometry!
 
That's why geometers and topologists invented transversality
Transverse intersection is always nice
You go think about non-transverse nonsense, analysts
 
Sounds like a great solution to me
 
I really liked doing the exercise for stereographic projection
 
@Fargle Did you work out the bump function?
That's probably all you need to do from section 1
 
2:30 PM
oh I need to do that?
shit
 
Yeah those will be essential throughout GP
 
I worked out that the $e$ thing is smooth--that's a classic example of a smooth non-analytic function
 
Yup
 
but that functional equation scared the bejesus out of me
 
Good work
It looks scary, but isn't afair
 
3:00 PM
Okay I've finally convinced myself it's zero outside $(a,b)$
 
Nice
 
3:11 PM
but why the gosh dang heck do it gotta be positive
oh is there a typo in my edition
oh, yep, just found Ted's errata
 
Check here
snip
 
yeah so it had $g(x) = f(x-a)g(b-x)$
and, like, no
I'm not doing that
but $g(x) := f(x-a)f(b-x)$? ez
Alright, so a function that's $1$ in the ball of radius $a$, $0$ outside the ball of radius $b$, and in between in the in between: Let $g^*(x) = f(\|x\| - a)f(b - \|x\|)$. Then define $h$ as before but as a quotient of line integrals of $g^*$.
Or I guess alternatively just compose $h$ with the magnitude function.
Oh no that gives me something inside out
oops
oh I guess I can just do some $1 - h$ business
 
3:45 PM
oh snap, tangent space is well-defined
 
@Balarka In class we defined the tangent space of an abstract smooth manifold at a point $p$ as the space of derivations on the germs of smooth functions at $p$, but I find this definition a bit unsatisfactory because it's using the smooth structure while it looks like a $C^1$ manifold should be enough to define tangent spaces
 
It doesn't!
 
How is the tangent space of a $C^k$ manifold, $1\leq k<\infty$ defined?
 
You can't do the same derivations definition
You'll get an infinite dimensional vector space if you do that for $C^k$ with $k < \infty$
@Alessandro Let me recall the point. So the definition is that, the tangent space of a $C^\infty$ manifold $M$ at $p$ is the space of linear functionals $\mathcal{G}^\infty_p(M) \to \Bbb R$ on the space of smooth germs at $p$, which satisfy the Leibniz rule (these are derivations), yes?
 
@BalarkaSen I'm not even sure how do that for $C^k$ manifolds, "germs of smooth functions at $p$" doesn't seem to work at all here
@BalarkaSen Right
 
3:57 PM
You can look at germs of $C^k$ functions at $p$.
So $A_k = \text{Der}(\mathcal{G}_p^k(M), \Bbb R)$
If $k = \infty$, we know $A_\infty = T_p M$.
 
So the problem, if I recall correctly, is that $A_k$ is infinite dimensional for $k < \infty$.
Let's see. I think the issue stems from the fact that $\mathcal{G}^k_p(M)$ is not a Noetherian ring for finite $k$.
Yeah, of course it isn't.
 
Hmmmm, I'm looking at the proof that the derivations in $A_\infty$ induced by a chart in $p$ are a basis that we did in the $C^\infty$ case and I can't pinpoint where smoothness is used and being $C^k$ isn't enough
 
You still get an injective map $T_p M \to A_k$ by using a tangent vector as a differential operator, like if $X \in T_p M$ then the differential operator is $X(f) = D_X f$, directional derivative of a germ at $p$ along $X$.
But this would not be surjective
How do you prove surjectivity? That every derivation appears as a tangent vector?
You need the soupled up Taylor expansion for that (every smooth germ $f$ can be written as, in local coordinates $(x_1, \cdots, x_n$), $f = f(0) + \sum_{i = 1}^n x_i g_i$ for smooth germs $g_i$), and for $k$ finite you reduce the regularity of $g_i$ to $C^{k-1}$, which fuckducks the proof
 
That's what we did, but it seems to me that $g_i$ is still $C^k$, wait a minute I'll check it again
 
4:09 PM
$g_i$ are the partial derivatives of $f$
 
Ah, right
ok I'm convinced now
 
So the key point is $\infty - 1 = \infty$
:3
 
quick maths
 
Now here is the real point, which is really algebraic of nature
 
$\infty = \infty + 196883$
deep fact about monster group or something
 
4:11 PM
So we need a completely different construction in the $k<\infty$ case?
 
$\mathcal{G}^k_p(M)$ are really in bijection with $k$-order Taylor polynomials with remainder in $x_1, \cdots, x_n$ at $p$ for some choice of local coordinates $(x_1, \cdots, x_n)$ at $p$. That remainder term, however, can be totally irregular and is an element of $\mathcal{G}^0_p(M)$, the space of continuous germs at $p$.
So there is this kind of decomposition "$\mathcal{G}^k_p(M) = P(k, n) \bigoplus \mathcal{G}_p^0(M)$" (I don't know if this is the correct algebraic description)
And when you pass to derivations, intuitively, you get a contribution from $\text{Der}(\mathcal{G}^0_p(M), \Bbb R)$ which is a massive ass space
There are no $C^0$ tangent spaces
 
I see, that makes sense
 
That's why $C^k$ derivations fail. The remainder term is bollocks
@AlessandroCodenotti Yeah, but the cool thing is that if a manifold has a $C^k$ structure for $0 < k < \infty$, it has a $C^\infty$ structure
 
That's a bit annoying
@BalarkaSen what
 
Yup
 
4:18 PM
I kinda have to run away very soon but I'll think about what a smooth structure on the unit cube looks like <.<
Where very soon is right now! Bye and thanks for your help!
 
That does not obviously have a $C^1$ structure (It does if you think of it as a disk, in which case, clearly a C^infty manifold)
Bye
 
 
6 hours later…
9:52 PM
@BalarkaSen I am trying to recover Hatcher's proof that $\text{Diff}(S^2 \times S^1) \simeq O(2) \times O(3) \times \Omega SO(3)$ without re-reading his paper. Maybe you can help me. Here are the thoughts I have so far.
1) $\text{Diff}(S^2 \times S^1)$ acts transitively on $\text{Emb}^{[S]}_{fr}(S^2, S^2 \times S^1)$, the space of framed embeddings of $S^2$ into $S^2 \times S^1$ whose homology class is a fixed generator $S$ of $H_2(S^2 \times S^1)$. I think this can be proved using the orientation-reversing diffeomorphism on $S^1$ (so the framing is in the 'standard' direction), and then an argument involving isotopy extension theorem, passing back and forth between $S^2 \times \Bbb R$.
Its fiber is (essentially) $\text{Diff}(S^2 \times [0,1], \partial)$.
I think that $\text{Emb}^{[S]}_{fr}(S^2, S^2 \times S^1)$ should have the homotopy type of $O(2) \times O(3)$ but I don't know how to prove that yet. I guess it should, again, work carefully in the infinite cover, maybe using straight-line homotopies or something.
(The $O(3)$ parameterizes embeddings with the same image.)
$\text{Diff}(S^2 \times [0,1], \partial)$ acts transitively on $\text{Fol}_{S^2}(S^2 \times [0,1], \partial)$, the space of foliations of $S^2 \times [0,1]$ by copies of $S^2$, so that this is the standard foliation on the end. I think this statement is the theorem that there are no interesting foliations by $S^2$, which is in the CC book. However, I furthermore believe that space is contractible. Maybe we should try to prove this by carefully understanding the previous proof?
If that's true, note that the fiber above the standard foliation is precisely the space of diffeomorphisms of $S^2 \times [0,1]$ that preserve the $S^2$ leaves. After using the contractibility of $\text{Diff}([0,1], \partial)$, this is just the space of 1-parameter families of diffeomorphisms of $S^2$: that is, $\Omega SO(3)$.
So we have two jobs left: understand the space of foliations, and the space of 2-spheres.
Maybe I am working too hard, and I should have started by showing that the space of foliations by 2-spheres on $S^2 \times S^1$ is contractible. That seems right.
 
10:23 PM
Yeah, if $\text{Fol}_{S^2}(S^2 \times S^1)$ is contractible, we know that it is acted on transitively by the diffeomorphism group, and its fiber is $\text{Diff}(S^1) \times L\text{Diff}(S^2)$, the free loop space; using that the free loop space of a group splits as the group times the based loop space, and the known calculations of these, we get that the fiber is $O(2) \times O(3) \times \Omega SO(3)$.
I guess this should somehow reduce to Hatcher's theorem on diffeomorphisms of the 3-ball though.
 

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