#point-set-topology
1 messages · Page 240 of 1
Okay maybe I did a really bad job at explaining yesterday. Let me make it clearer now. You already got it and tterra already answered but I kind of feel bad for just leaving you confused yesterday so I will make this super clear now.
Like you said, if $f:X \rightarrow Y$ is a continuous map of spaces (let's assume that they are path connected, i.e the base point doesn't matter) then the functor $\pi_1$ must assign a morphism to a morphism, just like tterra said. Morphisms are in this case continuous maps between two (based) spaces. We will define this "assignment" $\pi_(X) \rightarrow \pi_1(Y)$ by simply mapping the morphism into it's induced homomorphism, i.e $\pi_1(f) = f_$ where $f_[p] = [fp]$. We want to show that $\pi_1(f) \pi_1(g) = \pi_1(fg)$, i.e $f_g_ = (fg)*$. But this is not hard to check since $fg_(p) = f_([gp]) = [fgp] = (fg)_[p]$. We also want to show that $\pi_1(1) = 1$, i.e $1_* = 1$. This is also simple because $1_*[p] = [1p] = [p]$, so the induced homomorphism of 1 maps everything to itself so it is the identity.
I might have overdone, now it's all written out in baby steps lmao
f(X) -> Y
frick
Tokidoki ✓
looks good to me
pi_(X)
old notation of functions was literally f(X) \subset Y
the f: X \to Y thing started around the same time as category theory
i already got you once i'm not gonna go twice
holylocks 
CP^2 # CP^2 
i think
godlylocks


CATLOVE???
Imagine investing 100 dollars a year into emotes 
Imagine having :catlove:
geometry 

More like rigid topology
there's a reason symplectic is sometimes called "symplectic topology"
I have never seen any geometry so all I know about geometry is charts and integrals 
all symplectic manifolds of the same dimension are locally isomorphic
so there's really no local study of symplectic manifolds
it's all global 
that's a cool fact i think

it's easier to appreciate this fact if you've spent an ungodly amount of time doing riemannian geometry
where everything is local
eg curvature
integration 
all of math is integration
i was under the false impression they were the same thing
oh no

i guess to me "geometry" implies the existence of local invariants, like in riemannian geometry
brain rot


ultra is the funniest person on the server.

🥴

is it correct if i say that a free group on a set X is the same (in the sense that it's isomorphic) as the free product of $\abs{X}$ copies of Z ?
chrisply
Yes
so free groups are just a special case of free products ?
Yeah
ok ty i just needed a sanity check since i'm not that comfortable with the material
Can someone help me with this ?
Let be $X$ a compact space and ${C_n}{n \in \mathbb{N}}$ a subsequence of closed not empty subsets of $X$. If $C{n+1} \subset C_n$ for every $n \in \mathbb{N}$, show that $\bigcap_{n\in\mathbb{n}}C_n \not = \varnothing$.
galois.theory
Given that the notion of „closed space“ does not make sense in topology, you need to give a little more context
metric spaces?
Your terminology is a bit off, since that's just a sequence not a subsequence. But I think I understand. Are you familiar with the finite intersection property characterization of compactness?
yes
(ah, compact makes more sense)
Try to show your family of closed set satisfies the FIP
Then you can use that characterization
I'm sorry I do not speak much English and I translated it with many errors
It's okay
Do you understand what I am suggesting you try though?
If you can show the collect ${ C_n: n \in \bN }$ satisfies the finite intersection property (and because the $C_n$'s are closed and the space is compact), then the intersection is nonempty.
Lunasong the Supergay
Oh! i've got it, thank you very much
👍
In the context of complex manifolds, how precisely would one define a complex-valued differential form (i.e. some structure such that dz=dx+idy makes sense)?
I am remembering that instead of Ω(M) we can consider Ω(M,V) for arbitrary vector spaces (like e.g. a Lie algebra 𝖌), but I'm not quite sure how the construction would look like. I mean we probably want a DGA such that pullback becomes a morphism of DGAs.
My guess would be something like Ωⁿ(M, V) = ℝ-multilinear (n arguments) antisymmetric maps →V, and then one could define iω as (X_1, …, X_n) ↦ ω(iX_1, …, iX_n), where multiplication i in this context is a bundle homomorphism TM→TM
Motivation: I want to „understand“ complex integration literally in terms of of differential forms
Ah, okay, The pdf from Wilhelm Schlag does that in Chapter 6, but not in “general”, only over Riemann surfaces.
dz just seems to be the differential of the function z: (x,y)↦x+iy, U→ℂ for an open U in our MF
looking at the material again i realized that i really dont understand what's going on at all. The free group on n generators is defined to be the free product of Z n times. And the general free Group over a set M is defined to be the free product of copies of Z indexed by M. Now that means that for finite sets M which have let's say m Elements there really is no difference between the free group over M and the free group on m generators, right ? I also don't see how the two definitions of a free group are compatible. One definition your words consist of elements in an arbitrary set M and in the other one your words are just integers concatenated ?? What would be an isomorphism between these two?
You just identify the generator (1) of each copy of Z with an element in the basis of the free group
You can think of each integer as a power of the generator
That's exactly your homomorphism. You send each element of M to a generator of a copy of Z then extend by the universal property
Then m^k will be sent to k for example
well that actually sounds plausible 
The key is that each 1 in each copy of Z is different
Since the underlying set of the free product is a disjoint union
so since it is built upon a disjoint union it really shouldn't make a difference whether you take the free group over {1, ..., n} or another set M with the same cardinality, right?
Free groups over bases with the same cardinality are always isomorphic. The free product of some copies of Z though isn't exactly the same. It's almost purely notational though (Exponentiation becomes multiplication etc.)
So instead of i^k you have k*1_i =k_i
(Where 1_i, k_i are elements of the i-th copy of Z in the free product, and i is the i-th element of the free group over {1,2,..,n})
I mean if you wanna think of it being indexed over [n] when it's finite that might make it easier
I hope i'm making sense
yeah i think it does make sense
thanks for your help. I think especially what the copies of Z mean made it click for me (and looking at it now it does seem kind of natural even)
Tbh the universal property is one thing, but, for me personally the point where I got really comfortable with F(X) was when I learned about universal algebra and had to deal with term algebras all the time.
I feel like the explicit description is easier and more approachable than this convo makes it out to be
And the concept of generators and relations that arises from it is indispensable
Oh, yeah, generators and relations might be the best approach to it.
well that's kind of a cok-y statement
Is that true? So each rule is just a homomorphism between free groups? What does is an example for D_n
I just googled the universal property of free groups. The normalizer of the subgroup generated by {a^n,b^2,baba} is the image of f?
So we let X be our set of letters and
g:X->G implies there is a unique group homomorphism
f:F(X)->G where f is an extension of g.
In this case g acts as the function that maps the relations to the freegroupp of generators of D_n?
What can you do with this information though?
Oh ok I thought that recontextualizing it might have atleast one other theorem attached to it
It is (in my opinion) pretty rare for a more abstract characterization to give more theorems than a concrete construction
What do you mean by categorical presentation?
I do not think this message bleongs here 
I think you mean normal closure, not normaliser
What is the difference?
Adding elements that are fixed under conjugation to those elemtns?
a categorical presentation of something would characterize it by a universal property which can be explained only in the language of category theory, i.e. using arrows, objects, composition, etc. For example the tensor product has a universal bilinear mapping property, the localization of a commutative ring at a multiplicative subset has a universal property. The characterization usually characterizes the object in question up to a unique isomorphism. On the other hand the existence of such an object might be given by a set-theoretic construction where one specifies what elements are in the set, what the addition and multiplication laws are, when two elements are considered equal, etc.
Normaliser N of H<G is the largest subgroup of G such that H is normal in N. Normal closure of H is the smallest normal subgroup containing H
Smallest and largest being w.r.t inclusion
Oh ok thats what I thought, thank you so much!
So the object D_n, dihedral groups of order n has a categorical presentation?
I dont remember exactly how to verify is something is a category
If I remember correctly a category is a class of Objects, Arrows such that there is an identity arrow and composition is allowed
So objects would be groups D_n, but im not sure what the arrows would be
@cedar pebble Can you help me with this problem in Szamuely?
I know that the genus of Y has to be n/2 + 1
Mhm
So what you have to do is 1) produce a transitive action of Dn on a set of 2n elements, then 2) compute the cycle decomposition when you go around a small loop around a puncture at a ramification point
Take say the right action of Dn on itself
If you compute the cycle decomposition you should see the branching you want
yes
wait have you not been reading the version with the errata?
and yes this book has a lot of atrocious mistakes but it keeps you on your toes and it's good practice
no
its terrible
I have been reading this book with the errata
Still spent several hours on this problem
on an incorrect problem
Okay
I see that the commutator is just sigma^2
And this partitions the fiber into 4 sets of n/2 cycles
How do I contruct the cover now ?

@cedar pebble 
Do I have to use some covering spaces = transitive pi-1 sets equivalence thing?
this
so maybe an analogous situation that is clarifying that I took a whole course on
to specify a cover of P^1 minus points a_0,...,a_n you need to specify generators \gamma_0,...,\gamma_n with the condition \gamma_0...\gamma_n=1
this is what the picture looks like around the 4 branch points
This is kinda fun 

Hello, reading the following article (http://www.doiserbia.nb.rs/img/doi/0350-1302/2011/0350-13021103049I.pdf) I have trouble understanding lemma 2.3, only in the part that says that it is easy to show that the sets \mathcal{A} and \mathcal{B} it defines are closed. We work on the Vietoris topology over 2^X, and in the first case you could see that the set \mathcal{A} is the Vietoric of C and I think that C is closed, but I don't think this argument is correct. So I hope you can help me understand why those 2 sets are closed in the ordered arc. Thanks!
is it true that for a variety, every local ring is regular <=> every local ring at closed point is regular ?
Okay so this is the exercise that I am working with:
Show that for a space X, the following three conditions are equivalent:
(a) Every map S^1 -> X is homotopic to a constant map, with image a point.
(b) Every map S^1 -> X extends to a map D^2 -> X.
(c) pi_1(X, x_0) = for all x_0 in X.
I know that (a) and (c) are equivalent since Max explained to me that the elements in pi_1(X, x_0) could be regarded as homotopy classes of maps S^1 -> X instead of maps I -> X. Now I am stuck on proving that (b) and (c) are equivalent. Let [f] be in pi_1(X). Then f: S^1 -> X and this can by assumption be extended to a map g: D^2 -> X. But now what? What can I do with this map? I think that I am supposed to use a theorem that involves some sort of relation between a map and the extended version of that map, but I can't think of such a theorem. I can't either figure out a homotopy between g and a constant map right away. The book has not proved any results involving D^2 that will help me I think. The only theorem involving D^2 is the Brouwers fixed point theorem, but I doubt that it will help me here. Any hints?
Are you sure that you know that (a) and (c) are equivalent 
Because if you regard loops as circles, their homotopies would have to fix the base point, but in (a) there is no mention of fixing the base point
What you said only gives (c) → (a)
Hmm okay let me think over this again
For what you said about D^2: If f is homotopic to f', and g is homotopic to g', and the compositions gf and g'f' make sense, then gf is homotopic to g'f'
Okay I will take that as a hint. I will try to fix (a) <=> (c) now lmao
I'm still kind of confused. Doesn't this work?: If pi_1(X, x_0) is trivial for all x_0 in X, then the loop f: I -> X is homotopic to c (the constant map). This loop can be based at every x since pi(X) is trivial for all x_0 in X. This f can be seen as a map from S^1 to X and so this map is also homotopic to c. Since x (the basepoint) can be whatever it wants to be, then every map S^1 -> X is also homotopic to c.
I think the logic is a little awkward here but it’s the correct idea
Yeah (c) → (a) this works
The map S^1 -> X comes with a basepoint in the sense that we think of S^1 as equipped with a basepoint and the basepoint in X is determined by wherever the first one is sent
The other one is a bit trickier because you might have nullhomotopies that don't fix the base point
Then of course your logic plays out nicely
omg I was supposed to show the other direction smh lmao
btw don't try to do (a) → (c) directly 
Hmm why not?
Hes saying that (b) might be helpful
Honestly b is like
Ugh
I could give a talk
Just on the importance of (b)

Ping me when you get it and I’ll send you a generalization of it for you to prove
Okay great, thanks! Btw, does a -> b, b-> c and c->a sound like a good idea in this case?
Yep that is what I have in mind
I'm not that comfortable with these equivalent multiple things questions
They need to form a strongly connected directed graph 😌
The idea is that implication is a transitive relation. So you prove a bunch of implications, you automatically prove their transitive closure
Which means all finite sequences of those implications are done 
Ive seen some hilarious bad ones
With parts a-h or whatever
And proven in like the worlds most complicated graphs
The truly woke do like
We prove a->b and then that b+c->d and finally that…
how would one describe homeomorphism vs homotopy equivalent geometrically/visually? For example it's always said that you can stretch and bend, but not tear or glue something with a homeomorphism. Can this be made more rigorous? For me it makes sense if you think of continuity in terms of neighborhoods. Since that just means that things that are supposed to be at somewhere the same place stay at the same place relative to each other (or formally it preserves the topology) But how would one, on a intuitive level argue that you can't fill out a shape (like S^1 is homotopy equivalent to S^1 x D^2 (a filled out torus) but not homeomorphic ) with homemorphisms ? I just don't see how this sort of "filling out" shapes violates the definition of continuity?
I think that the only way to build this intuition is to see a lot of examples and understand the rigorous reasons
unless you are asking for a proof that S^1 x D^2 isn't homeomorphic to S^1
One suffices 🙂
you need a different contradiction
but it still works
donut with small bite
or a small air hole
could one say that S^1 x S^1 is a deformation retract of torus with one point removed and then maybe something with fundamental groups ?
Oh its simpler than that
S^1-pt is contractible
whereas no matter what point you remove from S^1 x D^2
it won't be
that means the homotopy equivalence can't be a homeomorphism
anyway yeah working through a lot of examples
is how you get intuition for when two spaces are homotopy equivalent
and homeomorphic
how do you see that? isn't that essentially through fundamental groups?
That's one method
a space X is contractible iff every map Y->X is contractible
so it suffices to find one nontrivial loop
no need for the full pi1
hmm ye true
Okay I think that I finally proved it lmao. First $(a) \implies (b)$: first notice that the circle can be expressed as $e^{i v}$ where $v$ is some angle and that $D^2$ can be expressed as $ae^{iv}$ where $a \in I = [0, 1]$. Let $f: S^1 \to X$. Let $h_t: S^1 \to X$ be a homotopy so that $h_1 = f$ and $h_0$ is the constant map. Then $g: D^2 \to X$ defined by $g(te^{iv}) = h_t(e^{iv})$ is the desired extended map since the restriction to the circle is $g(1e^{iv})$ and when $t=1$, $h_1 = f$.
Lets do $(b) \implies (c)$. Let $[f] \in \pi_1(X)$. We will show that this is homotopic to the constant map. By assumption, this map extends to a map $g: D^2 \to X$. Since $D^2$ is path connected, there is a deformation retraction $h_t$ that "deformation retracts" to a single point $x_0$. Now $gh_t: D^2 \to X$ induced a homotopy $g \cong g(x_0)$. So $g|{S^1} h_t: S^1 \to X$ induces a homotopy between $g|{S^1} = f$ and a constant map.
and I already did c->a
Tokidoki ✓
and composition and restrictions "preserve" continuity so the associated map is still continuous after all the manipulation
looks good to me even though you are breaking my heart with all the explicit maps and stuff ❤️
:catlove:
what do you mean by explicit maps and stuff?
Is that something that I should ignore?
keep doing what you're doing, just for the sake of annoying max
oh i just mean
/s
my proof would go like this
Quotient topology universal property? 
actually no i'd probably do the same basic thing
it works well
I realized my proofs would only make sense if i could draw pictures lol
A nullhomotopy is a continuous map from S^1 x [0,1] to this space such that S^1 x {1} is constant, so it factors through (S^1 x [0,1])/(S^1 x {1}) ≈ D²
Yes
Thats what I had in mind
But written like that idk if its simpler
I would ditch the e^ix stuff
I’d just say
Yeah that part just makes me not wanna read it 
Let S1 be a unit circle and u a vector, then the points of the disk D^2 can be written at tu for t in [0,1] blah blah
yeah that's true lmao

But toki here’s my better theorem
You've seen quotient topology in munkres right? 
Let f:X —> Y be continuous. Let CX denote Xx[0,1]/~ where ~ collapses the copy of X at time 1 to a point
i will let max write the thing out first before I ask my question
Show that f is contractible iff it extends to a map CX->Y over the inclusion at time 0
Ok don't look at my argument now 
Then explain why this generalized (b)
Hmm okay I will write this down and try it out
but what does "factors through" mean?
and the S^1/blablabla thing that you wrote moldi?
Oh okay
Yeah forget about factors through for now 
Bonus points if you can explain this result using only vague geometric language
Okay I will look at the thing that moldi wrote earlier later when I've tried this "exercise" thing, but I have one more question
When solving this exercise, I used the argument that D^2 is path connected so that it deformation retracts to a single point. Why is path connectedness needed for this?
I understand it intuitively, but not formally
Not all path connected spaces deformation retract to a point
and I just snatched this fact from Hatcher lmao
S^1 doesn't
The better way to see this might be to use the extension to construct an explicit null homotopy
Wait did I misunderstand what you were saying 
In Hatcher he says that "all path connected spaces deformation retract to a single point" while talking about a counter example that not all retracts are deformation retracts. But why is path connectedness needed?
This is my question. Ignore the thing that I wrote, I might have used a bad langauge there
Wait
That is just wrong lol
Thats
Or something like that wait
Not true
Yeah hahaha
I was losing it for a second thank u moldi
I was like have I forgotten the defn of a def retract
Because deformation retractions preserve fundamental group in particular
So that would mean S¹ has trivial fundamental group
Okay here: "but a space that deformation retracts onto a single point must be path connected"
Yes
Yeah that is the part that I was reading. But why is path connectedness needed?


Yeah I thought about this while doing the other exercise and I think that it has something to do with that H: X x I is continuous. But I can't find a map from I to X that is continous
Try to track points as you deformation retract the space to a point
Like just track the motion of one random point
yeah that becomes a path from the random point to the deformation retraction point
But how can you see it using only homotopy?
Wdym
Homotopies are continuous in t
Huh
The proposition in the book
The family h_t actually represents a continuous map h from X x [0,1] to Y
Thats not super relevant this is straightforward
the maps f_t as hatcher writes them are continuous in t
So in particular
$t\mapsto f_t(x)$ is a path
Karen
Thats ur hint
Isn't that the full solution 
no
I mean
Anything counts as a full solution
To a sufficiently lazy grader
But this wasn’t obvious to toki so I’m gonna make him write it out
Fair lol
Pls delete
But yeah more point is just like
You dont need any lemma or anything
Its just definitions
Sorry for messing up the exercise
No ur fine
Okay I think that I see it now lmao. So H: X x I -> Y defined by H(x, t) = h_t(x) is continuous by definition. So f: I -> X defined by f(t) = h_t(x) for some x in X is continuous. f(0) is the identity so it equals x and f(1) is x_0 so we get a path there
Just to be extra pedantic how do I use this to get a path from arbitrary x_1 to x_2
Oh
Well if I have a path from x_1 to x_0, then I can have a path from x_0 to x_2. THis is a equivalence relation to there is a path from x_1 to x_2
or using the pasting lemma or something like that
to construct a path from x_1 to x_2
Just reverse the second path 🙂
Boom
This of course leads one to construct the fundamental groupoid
That’s a joke don’t worry about that it’s lame
Okay anyway, thank you all so much! I will tackle the "better theorem" sooner today since I have to go now
Sooner today or later today? 
sooner today? 
Later today I mean sorry


I’m gonna turn your next question into an exercise if u dont fix that attitude
i’ve got a student who is trying to learn about the basics of manifolds. they have some mathematical maturity but not a lot of background beyond basic analysis. can anyone recommend a resource for exercises?
i’m looking for practice with the general definition of a manifold, tangent spaces, smooth functions on a manifold, and other basic things of that nature
spivak (the little one, not the massive 5 volume set
)
well maybe only for the super basic manfold stuff
honestly that’s ok I honestly forgot about that book
although i would like something that would help someone understand general smooth manifolds, not just submanifolds of R^n
but i’ll look at it again and see if there’s anything in there I can recommend
hadn’t heard of this one, this is actually great since they’re learning this for a physics related project
Okay so I'm back now and it's quite late but I still want to give this a shot today. But what does "extends to a map ... over the inclusion at time 0 mean?
It is the "over the inclusion at time 0" thing that I don't understand
Karen
Then you have a triangle
X —> Y
|
|
V
CX
And an extension is a map CX->Y
Making it commute
Okay I see. And the inclusion is from X to CX right?
Yes
Okay great! Thank you!
Hint: draw CX for some easy spaces X
Okay wait wait. What does it mean for a function to be contractible? Hatcher only defined what a contractible space is
Like homotopic to a constant map?
But that is nullhomotopic lmao
Okay great!
Okay I think that I got something going on. This is very handway lmao but I think that this still works. So let's prove the implication $\implies$ first. Let $f$ be the map that is homotopic to the constant map, $c$. Then there is a homotopy $h_t: X \to Y$ such that $h_0 = f$ and $h_1 = c$. Now $CX = (X \times I)/ \sim$ where $\sim$ means "take the last $Xx{1}$ and map that to one point". If we for a second replace $X$ with $S^1$, then $S^1 \times I$ is a cylinder. Then $CS^1$ is a cylinder with a "sharp edge/point" at the top and that point is no longer a circle. Hence $CX = (X \times [0, 1)) \cup {a}$ where $a$ is the point at the top. Now define $$g(x, y) = \begin{cases} h_t(x) t \in [0, 1) \ g(a, 1) t=1\end{cases}.$$ This is a map from $CX$ to $Y$ and we see that $gi(x) = g(x, 0) = f(x)$ so the diagram commutes. This is the first implication.
The second one is very similar to the other argument I had. Let $f: X \to Y$ that extends to $g: CX \to Y$. If we again replace $CX$ with $CS^1$ then we see that $CS^1$ is a deformation retraction of a single point. Let $h_t$ denote this deformation. Then $gh_t: CX \to Y$ induced a homotopy between $g$ and a constant loop. Then restrict $g$ so that it becomes $f$ and then we have our desired nullhomotopy.
Tokidoki ✓
why not? the vol 1 exercises were where I first encountered some neat concepts like the hole in a hole in a hole etc
I mean it's a comprehensive introduction, so one naturally shouldn't be scared by the volume of it
Plus old typesetting and lots of space
You don't have the required permissions to ban members here!
that's okay, latex hates you too @pearl holly
I mean regarding your question, I share your sentiment, the whole nullhomotopy and homotopy equivalence thing kinda confused me for a while as well
although I was too lazy to read backlog in order to provide more detailed insight :[
And this is indeed a generalized "version" of the previous exercise since, like I said before, S¹ X [0, 1]/~ is a sharp cylinder at the top and then if I project it down like the steorographic thing that you (Max) gave me as an exercise before (or if I simply "unbend" it like playdoo), then this is homeomorphic to D²
perfectly done!
Oh wow great! I thought that something there would be wrong lmao
Anyway, thank you so much for the help and for the exercises! I will go to sleep now since I'm kind of tired. Bye!
i think the big ones require a bit more background than little spivak (eg point set topology) but i could be wrong
i guess i wanted to specify i meant the little one, and not necessarily to disqualify the big one
I still vividly remember learning a ton about DiffGeo from that first volume even though I didn't formally know about topology yet
But that was more interested, nonlinear reading as opposed to conscientious word-for-word study
And I was studying physics back then so my judgement was clearly pretty terrible
S1 is not a retract of D2 and if someone gave a retraction r:D2->S1 with r(x)=x/|x| they would be wrong because r^-1(r(B(0))) is not open in D2? I feel like im explaining it wrong.
Where B is a open ball around 0
i mean r(x) isnt even defined on D2, the origin that is
However if you do D2- {0} then this would be a retract
So in the argument all I need to say is that r is not well defined so it cant be continuous
r isnt defined* would be more correct
Well defined is something more specific
Usually
I thought well defined meant it is defined over the entire function
So x=y means f(x)=f(y)
Yes
Sorry I meant domain
Thats different from what you said though
the issue is that you haven’t told me what r(0) even should be or might be
You literally haven’t defined it
max can you summarize your talk on the importance of proving that a loop is nullhomotopic iff it extends along the inclusion S^1 -> D^2
what's the short version lol
Its a shockingly useful intuition in my experience, generalizes to cones, and is the first time a lot of people are introduced to extension problems that matter
It also sort of parallels the visual intuition of homology in an interesting way
Ie a generation is trivial if it’s a boundary
Generator* fuck autocorrect
Idk I just think it’s neat haha
generator of?
Pi n
How is S1 x I/ S1 x {1} a quotient topology?
I thought you need a map X->X/~ and a equivalence relation ~
Would it be S1 x I -> S1 x I/~ where a~b iff a=b?
The equivalence relation is that all points in S1x1 are the same
And all other points are unchanged
I have to add the or a=b part to include the "all other points unchanged"
This is a very common construction
Where you have a space C
X not C
And a subset A of X
You write X/A
For “X with A smushed to a single point”
It isnt proper to think of it as X-A U {*} where * is equivalence class of points in A?
No
That gives the wrong topology in general
Take the following example
Let D be the unit disk in R^2
And let X be the 1/2 radius disk
Then D/X is homeomorphic to D (exercise)
But D-X U * is not
At least with the normal topology
As a set the two are the same but the quotient specifies the topology, and if you write the union people will assume your mean the disjoint topological union
q:D->D/~ where a~b iff a=b or |a|,|b|<1/2, q is continuous and D/~=D/X
A is open in D/X iff q^-1(A) open in D
The goal is to have a map f:D/X->D that is continuous from here
And then im thinking I can show f^-1 is continuous
Im thinking I can make f a function that takes the equivalence class made from |a|,|b|<1/2 to the origin
And it takes all the other points and and somehow stretches it to the origin continuously
Thats the right idea
I was thinking f:D/X->D with f({*})=0 and f(x)=1/2(1+x) for x!={*}
Nah
I ran into a problem i thinks
I guess I should write it in terms of e^itheta
You can come back to this later haha
I think I get the idea
similar to how quotient groups take cosets and treat them as elements, quotient topologies take equivalence classes of points and treat them as open sets
It just threw me off seeing S1 x I/ S1 x {1} instead of S1 x I/~ and then seeing the definition of ~
Oh lol
I think I understand the proof from that review, thank you.
hopefully this doesn't come across as too obnoxious, but both quotient groups and quotient topologies have universal properties which justify the construction
you can prove that if X is a topological space, and ~ is an equivalence relation on the underlying set of X, then for any continuous map f : X -> Y for another space Y, satisfying x \sim x' -> f(x) \sim f(x'), there is a unique factoring of f through the quotient map f : X -> X/\sim
Somewhat similar to Noether's first isomorphism theorem
How would you check x~x’ => f(x)~f(x’), Do you have to do it explicitly or is there a roundabout way. Continuing an example with homotopies if you have a homotopy between f,g:X->Y being
H:X x I -> Y with H(x,0)=f and H(x,1)=g. Is there is a relation that satisfies x~y => H(x,t) ~ H(y,t)?
The only thing I can think of is picking the relation to be x~y iff H(x,t)=H(y,t)
But then I dont know what X/~ would be or look like
Oh wait I made a mistake in asking
I cant think of a relation that makes that work
Oh you might have written it wrong
because x~y=>f(x)~f(y)?
that is a property that that map can satisfy but does not have to
what clerk is saying is that maps that do end up satisfying that
have the unique factorization described
Then why is the equivalence relation based on the underlying set because f(x) is in Y, not X?
Or is it that the equivalence relation cant be anything like a~b if a and b satisfy a property specific to X
It should probably be x ~ x' → f(x) = f(x') right?
We don't have an equivalence relation on Y
Yea thats why I was confused
because if there was an equivalence relation on X it would have to be independent of elements of X and say something about the set in general
oh yes
im silly
sorry very tired
there is a more general statement where like
X and Y come equipped with equivalenve relations X/~ and Y/~'
Oh
and a map f: X -> Y "descends" to a map X/~ -> Y/~'
if the condition clerk wrote is satisfied
These universal property things are category theory related, right?
They are often formalized with category theory but often you don't really need any real category theory to discuss them
categories help us see how all universal properties can be seen as the same type of thing i guess
Hmm this looks awfully similar to the exercise I was doing yesterday and the solution that moldi and Max had in mind. What does this mean though? How do you know that h factors through the quotient?
wait let me check Munkres
Okay there's a theorem that says that if p:X->Y is a quotient map and g: X -> Z is contant on each fiber of p, then g induces a map f:Y -> Z such that fp = g. I guess that this solution uses this theorem
first isomorphism theorem for topological spaces
Is that actually a thing?
yeah i just made it
already have one 
First isomorphism theorem is just the universal property of the quotient 
🤔
I mean, it pretty much is the first isomorphism theorem, lmao
😻
:catlove:
yeah sorry all that was a mistake
i shouldn't have written ~ between elements of Y but rather equality =
unacceptable, two more strikes and you're banned
What's your hand wavy summary of the baire ct?
To me it seems like it establishes thar small sets (nowhere dense) cannot be countably combined to something large (ie with nonempty interior)
And in vector spaces I guess this makes sense because open sets have to, like… stretch in all dimensions?
Not sure how good this mental model is.
(I guess my goal is to get a feel for what the role of baire is in certain proofs, but that gets into analysis territory)
There is this website called proof wiki and it shows you how to make the map explicitly, but the proof starts off as defining f:X/~->Y as a relation, I guess its harder to write it explicitly because you need to go from taking normal looking elements in X to elements in Y into taking equivalence classes formed by elements in X to elements in Y
In our case where h(s,1)=x we would just need to make the equivalence class from [x]=S1 x {1} in S1 x I / S1 x {1} map where f[x]=h(s,1)=x and then all the other elements in S1 x I / S1 x {1} have equivalence classes that look like their original elements in S1 x I so we can have f[(s,t)]=h(s,t).
Thats what I am thinking atleast
i usually do it in the converse way. if a set is comeagre then it should be almost everything. so it states that the intersection of sets that are almost everything is nonempty. this gives nonconstructive existence proofs: if you want to prove there exists x such that P(x), decompose the predicate P into an infinite conjunction $\bigwedge_{n\in \mathbb{N}} P_n(x)$ and then prove each $P_n$ holds on an open dense set
diligentClerk
in classical algebraic geometry the analogue would be conditions where each $P_n$ holds away from the vanishing set of a polynomial (which is open and dense in the Zariski topology). Points that live in a large collection of open dense sets are "generic", and many important results in classical AG (I think to both Krull and Noether) asserted the existence of points sufficiently generic for whatever argument. Scheme theory just adjoins a formal generic point to the space which lives in every open dense set by definition, I guess the fact that this works shows that the arguments are really taking place in the opens of the sheaf and so the points are inessential.
diligentClerk
Don't take any of this too seriously though, I'm not really knowledgeable about these kinds of arguments
Ah, that's a great perspective! I think I will start to look for things that „work almost everywhere“ and see what other, stronger properties I can get by taking conjunctions. I think this will be really helpful when I dive deeper into the proofs.
in computability theory this perspective is very common. Computability theory is the study of the powerset of the natural numbers together with the Turing reducibility preorder, and the resulting poset you get when you quotient out by the preorder, and questions about the poset can often be phrased in terms of existence proofs for sets. for example, if you want to prove it's not linear, you show that there exist incomparable elements. if you want to prove it's dense you assume A, B are given and show there exists some C in between A and B. If you want to prove it doesn't have meets, you have to construct two elements that don't have a meet - actually the way this is done is you construct a pair of elements A, A' together with an ascending sequence {D_n} such that each D_n is less than both A, A', but any B which is below both A and A' lies below some D_n, so the {D_n} are cofinal among elements less than both A and A' - and this proves that A, A' can't have a greatest lower bound.
the reason this strategy works is that there are only countably many computer programs/Turing machines/inputs for those programs/outputs for those programs/etc. so the property "A is not computable" is the conjunction of "A is not computable by turing machine 1" "A is not computable by Turing machine 2"...
if you want construct A where A is not Turing reducible to B, you have to satisfy "Turing machine 1 does not carry out a reduction of A to B" and "Turing machine 2 does not carry out a reduction of A to B" and...
i guess i should be clear about what topology i'm talking about lol
the powerset of the natural numbers is 2^N so you can equip it with the product topology on {0,1}^N
which is homeomorphic to the Cantor set, it's compact, hausdorff and totally disconnected. very nice space
(done)
That whole range of arguments kinda sounds like a countable version of compactness, or a local-global principle as long as you stay countable
(here I mean FO compactness)
Does that coincide with compact-open? Because compact sets are precisely the finite ones in N, and that reminds me of the product topology generators
Yeah, that's interesting. I wonder if what you're commenting on can be explained by the fact that both 2^\omega and the type space arising in the Compactness theorem for FOL are the Stone space of ultrafilters on a boolean algebra. So it's the same special type of compactness that arises from Stone's representation theorem, you see a lot of that in logic because of the ubiquity of Boolean algebras in logic
I don't know if it's the compact open topology. Your argument makes sense tho. Shouldn't be too hard to work out
Wondering if someone knows what o(1) stands for in this this version for the Manin conjecture? The full paper is here: https://arxiv.org/pdf/math/0511041.pdf
some function that goes to zero as B goes to infinity, probably
just judging by the picture
thanks! that does make sense
the boundary is always closed, since it's the closure intersected with the complement's closure, correct?
Yes
Thanks for answering the probably most stupid question I have asked here 
I'm having a hard time understanding why the transition functions for a vector bundle should be linear
Essentially this boils down to whether or not $\phi_U^{-1}\circ \phi_V(x,v)$ is linear in $v$
PTYamin
Which I dont really see why it should be
on the same page
Coldilocks
ah ok
yup
thanks!
All that might become conceptually clearer if you realize that a trivialization associated to U is actually an isomorphism in the category of U-vector bundles.
Then chart changes give an automorphism of the relevant product bundle in the category of U\cap V-bundles.
Does anyone know if the following statement is true or false? Let $A$ be a simplicial abelian group. Consider $\pi_n(UA,0)$, where $U$ is the forgetful functor from Simplicial Abelian group to Simplicial Set. Let $x\in UA$ be a sum of degenerate element of $A$. Is it true that x is homotopic to $0$?
ClearlyHalfAlive743
noob question here: Let F be a map from M to N, two topological spaces. N has the trivial topology {∅, N}. Is it true that F is always continuous?
I wonder because this seems to be written in this lecture (example b on the right), although I can't make sense of it.
Yes (exercise)
what does it mean for a map to be continuous?
i see it now. since the preimage of the codomain must be the whole domain.. (right?) it was the preimage concept that confused me
Judging by the picture, if for every open V in the codomain, the prelecturers head is open in the domain.
Yes
kind of a simple question but does anyone know if this is true for * all * complex polyhedra?
i think its a polyhedron in which a line that connects two vertices is contained in its interior
like convex as opposed to concave
like cubes and tetrahedrons i thikn
oh wait
does it imply that?
just asking if thats true (im not really sure)
if all convex polyhedra are topologically equivalent
sorry if that sounds like a dumb quesiton btw
im supposed to write a passage but i dont know much ab the topic so am checking
wait really?
for all convex polyhedron or are there some exceptions
alright thanks, much appreciated!
Yep

toki, i explained something similar to you a while ago
this is your time to shine
maybe
convex stuff homeo to balls
oh like bounded and convex subset is homeo to the disk
if it's star shaped just normalize along rays
convex does imply star shaped around any interior point, yes
Except for pointy balls like B[x,0] :3
?
Locally compact hausdorff implies regular right?
yes
Is there a way to show singletons are closed in regular spaces without directly mentioning that it is hausdorff or going through the proof that singletons are closed in hausdorff spaces?
My idea is
Let X be a topological space and x in X. Suppose {x}^c is closed, then x and {x}^c admit disjoint open neighborhoods U,V respectively. Then {x}^c is open?
Yea my proof isnt right
yea i realized
its possible that {x} and {x}^c are neither open or closed
You can union those
Ah ok thats good proof
What do you mean this is weaker? I thought being regular was a stronger condition
Or are you talking about the condition of singletons being closed is weaker
Yea it isnt iff right, what js a counter example
Counter example for singletons being closed but not hausdorff
And standard topology?
Line with two origins is a common construction in topology
you can google it to see a defn
From https://ncatlab.org/nlab/search?query=line+with+two+origins
Direct page found at: line with two origins
non hausdorff spaces 
You just take the origin as the example for the two pointsv
And then they cannt be any disjoint neighbors
What is an example of a regular space that people think of as the standard example
Oh I guess R
I didn't read the whole conversation but singletons aren't necessarily closed in a regular space
Only if it's T3
Regular is being able to separate a point from a closed set not containing it
T3 is additionally being T1
That's how I was taught it
That's also equivalent to being regular and T2 which is how it's sometimes defined
Given a closed set and a point not in that set, there exist disjoint open neighborhoods of both the set and the point
I never formally learned seperation axioms, tbh my ungraduate topology is meh, there is no graduate topology so idk what that would entail
Only learned about Hausdorff and thas it
Im a noob and browse wikipedia and look things up when people post about them.
It looks like graduate topology isnt a thing for most schools and they are separated into topics classes
Yeup Im agree in ignorance. I am trying to learn AT through Allen Hatcher’s book but Im slowly losing a motivation for learning math as I progress through the topic. I for some reason thought that topology would have a lot more applications in physical world
It probably does but I havent learned a lot
Honestly
AT in particular
Doesn’t have that many
If you want some topology with applications
Fred Schiller has some good YouTube videos
Topolgy usually serves as a foundation for other math subjects.
Persistent homology is screaming
Until someone explains to me why it’s useful in neuro
Besides just stating that as a fact
I’ll keep dunking
King
is the burden of proof on the dunker or dunkee
not having any practical uses IS the motivation for learning it
What is α, what is ξ, what is p? Notation is not that consistent with regards to all that
From guessing I would've said that ξ is not a point but a vector (the brackets will probably refer to a commutator, right?)
no it does not it refers to equivilance class
Oh, I see.
kinda cringe notation ik xd
well not really but ehh kinda cringe
since ec's are denoted with []
ping me again cause I can see u typing alot
@past pasture the short answer is that since our target space is ℝ^m, we can identify tangent vectors in T_φα(p) ℝ^m with actual elements (or “points”) of ℝ^m
there, the author implicitly considers ℝ^m to be a manifold with only one atlas, namely the identity
And so for equivalence classes [β,ξ] in T_whatever ℝ^m, where β in {β}=B is said atlas, there is only one reasonable representative

I mean it's slight abuse of notation if I see that correctly
because when the author writes ξ they mean [β,ξ]_whatever, it's just that φ_β = id_ℝ^m
yw :3
lux is writing in latex without even needing latex 
That definition gave me cancer
There's no sane reason for writing it like that, surely
differential geometry is notorious for dense notation, i don't think this equation is really out of place with what you'd see in any diff geo book
Tterra in shambles.
this is garbage writing
Let me get this straight: a two dimensional CW complex can be a disk. A three dimensional CW complex could "look like the mapping cylinder"? So like a cylinder glued to the disk. Is this right? And attaching a 2-cell is basically gluing something homeomorphic to the 2D ball?
this is what differential geometry is, to me
tokidoki can you explain more about what you mean? A disk is definitely a 2D CW complex but i don't understand the bit after that. when we talk about attaching a 2-cell we mean taking an existing complex X, taking a map phi: S^1 -> X and forming the pushout of phi along the inclusion S^1 -> D^2
kolar michor slovak 
yeah it's a really interesting book i'm just having trouble getting too much intuition from it
and it's a bit dense lol
i've read warner and that took me ... a long time
this one is maybe even more challenging
oh sorry for not responding. I mean that when we attach a 2 cell, intuitively, we just glue something homeomorphic to a 2 dimensional ball into the existing complex. Is this right?
yeah, along its boundary

if X is the old complex and X' is the new complex
then set theoretically X' is the disjoint union of X with the interior of the disk
because the gluing is along the edge of the disk, the circle
hatcher's appendix on CW complexes is pretty good, Strom's modern classical homotopy theory has a pretty good intro to CW complexes
Okay so let's say that I want to glue a cylinder to a space. Then I have to glue the boundary of that cylinder to the space. But this seems weird since if I take the whole boundary and glue on to the space, then I will have no cylider glued there at all
So if I want to glue a cylinder, I only want to glue along the circle below the cylinder
Like the lower part of the cylinder
But hatcher says that I need to take the whole boundary
yeah I need to think over this again lmao
are you talking about a solid cylinder
or a hollow cylinder
you're gluing on an n dimensional thing along its n-1-dimensional boundary
can you be more specific about what you mean by a cylinder
Just a solid cylinder that is filled in. So the boundary of that will be a hollow cylinder
gotcha. yeah if you only glue along the boundary, it won't have the effect of identifying points inside the cylinder with points inside the complex. that's hard to visualize because there's no good way to realize this in 3D space, you'd have to work in 4D so that the interior of the cylinder is disjoint from the complex
so when you say this
But this seems weird since if I take the whole boundary and glue on to the space, then I will have no cylider glued there at all
i think i disagree with that, the interior of the cylinder will still be there
yeah okay I see
You know what, let me draw a picture brb
So now when I try to map the sphere to the blue region, the whole boundary would need to be glued to the blue space and then the whole sphere just collapses
no wait, shouldn't psi go from S² to X¹?
But that's even weirder
you can totally define a projection from the boundary S^2 onto that flat surface
it'll collapse down the sphere but not the interior
there will just be a 3d blob with the property that if you start at the bottom and move to the top you'll end up where you started.
kind of like if you took a solid donut and glued it to the plane along a cross sectional disk
except whenever you reach the edge of the donut you collapse back to the plane
these are not really good ones to get intuition for lol
you want to start with like
the case where the boundary of the cell is already kind of laid out for you
for example take three points
x, y, z
now if you have a copy of D^1 (the unit interval) its boundary is S^0, a pair of points; there are natural homeomorphisms S^0 \cong {x,y}, S^0 \cong {y,z} and S^0 \cong {x,z}
if you were to glue three copies of D^1 along each of those attachment maps, you'd have a graph with three nodes and three edges which was homeomorphic to a triangle
You could also have the attachment map S^0 -> {x} which sends both points to x, then gluing D^1 along that attachment map would give you a closed loop, an edge which starts and ends at the same point
Now if you take the triangle T we just built
then if you have a copy of D^2, you can glue it to the triangle by choosing a homeomorphism between S^1 and the triangle T. then the gluing of D^2 to the complex along that map would be a solid triangle, because you'd be using the solid disk to fill in the interior
If you took two copies of D^2 and glued them both to the triangle along the same homeomorphisms, then you'd have two solid disks which are disjoint on their interiors but which agree on their boundaries, S^1 = T= S^1
this would be homeomorphic to a sphere, S^2
now you could glue a solid ball D^3 into this sphere along the attachment map S^2 -> S^2 and so on
ahhh yes okay
now I see
Thank you so much for clarifying and for taking your time! I really appreciate it! 
np good luck, enjoy topologizing
okay this might be the stupidest question asked in this channel
but what's the name of that series of books by spivak that this is from
(might not be spivak, but I'm like 90% sure)
differential geometry, there it is
I got it

Are those the covers of A Comprehensive Introduction to Differential Geometry?
Looks like it (C:
yeah I've never seen them in print in person but apparently those are the covers
as far as i can tell from internet pictures there's not even the title anywhere on the cover, just the picture
my uni library copy has actual titles on the cover I think
I'll have to check them out again
that would make more sense than these pictures lol, unless he titled volume 5 "All the way with Gauss-Bonnet"
pain

So honestly this is kinda hard to think about because I havent seen an explicit description of the fiber product of schemes in the non affine case
or of the diagonal map
yea these things are always funky
so at the very least it's going to be induced by universal property
so now we just have to think how this works out
It says its induced by the identity on Y
But
The only thing i really know about the fiber product here is that its the pullback of Y -> X by itself
well like
$\begin{tikzcd}
Y \times_X Y \ar[r] \ar[d] & Y \ar[d] \
Y \ar[r] & X
\end{tikzcd}$
the simplest case is when you're taking the diagonal \Delta:X->XxX where the pullback is taken along the two canonical morphisms X->Spec(Z)
Ultragirlboss
If this is all i know about the fiber product here how do i get an "identity map" in both coordinates?
I dont even know that Y x_X Y has coordinates
it does, think about what fiber product means (e.g. if you did this in the category of sets)
Well that would be the pullback of the two maps right
Explicitly its like points of the product that commute
{(x, y) | f(x) = g(y)}
is this true of schemes too??
Nvm i have done some soul searching...
Szamuely is dumb

anyway i get it now
szamuely gamered me
But this makes sense
Think about how confusing it is to read on compact mode.
Think about how confusing it is to people who aren't me and therefore are not phenomenologically aware that I am not the one typing.

At least I can trick Moth.
No u cant
Revenge for outing my Nikita prank.
You literally did this last time pretending to be nikita and i found u out
immediately

i am soul
can u change my name to moth whiteknight
no i read bernstein instead
idk i didnt feel the proofs were very geometrically motivated
a lot of times it was like
haha silly coincidence
so im reading some more stuff 2 make it less like that
just geometric rep stuff in general
i think bb localization is supposed 2 be intepreted as
looking at the nilpotent cone and springer resolution
and going from one to another
no his lecture notes on d modules
do u do these memes too
functional analysis is rep theory.
yea the only characteristic that matters
fuck all ye number theorists
pls do something fruitful with ur life
ooh what with
Sometimes you need char p results to prove a char zero result tho
yep gabe
logic ppl really be on a different plane of existence huh
Gabe says fuck number theorists while begging me to read rational points on varieties w me pls explain this
rational points over C
also i am reading why are you not reading
im literally reading moonen rn
nvm forgot u dont know ag
😔
someone told this to me too
Time to move to physics
do everything over a alg closed field and then galois descend
What about ur research tho
yep gabe
rep
semisimple
category O
yea
it is very cool ok!!!!!!!
category O is literally just fin dim



I just discovered the first examples of unicursal uniform polytopes with the same point group as the Leech lattice.

what is the bottom equation meant to represent geometrically?
Or is it just saying that, if that derivative exists for all (a_1,...a_m) in N_0^m then it's smooth?
When they say normal subgroup generated by all the loops, they dont actually mean the subgroup generated by these elements
but the smallest normal subgroup that contains these
bruh
like, a subgroup generated by given elements is the smallest subgroup containing said elements
same for normal subgroup generated by given elements
its the smallest normal subgroup that contain those
So N is the smallest normal subgroup that contains that loop?
(Just to make sure lmao)
You should also prove that a smallest such subgroup exists while you're at it
seems like they are talking about more than 1 loop, so would be the one containing all those
but yeah
Why would you not just say normal closure
:bruh:

I don't even know where to start lmao
How do I show that something even exists?
Well there's always a smallest and largest normal subgroup
So that one has to be in between these or something idk
hint is ||intersection of normal subgroups is also normal||
hgmm okay let me think
Too direct a hint lol
Not for me lmao
oof
oh okay now I see lmao

my bad ig
You can also construct such a group explicitly
And show it must be contained in every other normal subgroup containing the set
I think you can use that fact to show that A_5 is simple or something too right?
oops sorry
The proof that An is simple is mostly just a lot of casework iirc
the fact that johnDirichletseries mentioned I mean
no wait I'm thinking of something different
Oh yeah, A_5 is the only non trivial proper normal subgroup to S_5
Construct it

Does zorn's lemma fall into the second category
Zorns counts as a construction

Ok then, construct a hamel basis for R over Q please
Constructivists in shambles
Touché
this convention is similar to that of adjoining elements to a field right
Yes
Okay so the van Kampen theorem says under nice conditions that pi_1(X) = the free product of the "components"/N where N = ker(phi), phi being the surjective map from the free product of "components" to pi_1(X). Hatcher now says N is "the normal subgroup generated by the image of the map pi_1(A \cap B) -> pi_1(A)". I guess that in both cases, the normal subgroups are equal. How?
Can you post the passage, I can’t imagine hatcher states this without proof
Yeah okay sure, wait a sec
This is the theorem along with some info about the maps at the top
wait a moment

Do you have a question about the explanation
I don't see the expiation 
The next proposition in my book is the one that I'm reading now lol, there's no other theorem or anything in between
Hatcher does proofs later
Examples and such first
Just wait for it lol
Also physical copy of Hatcher 
yeah but this isn't a example. I've already read the proof of the van Kampen theorem and seen the examples too. It's like Hatcher turns to the applications of this now
Oops sorry
You’re okay I just don’t want you to get laughed at for it in person lol
Second I’d have to find my hatcher pdf but there should be a proof of 1.20
yeah I've read the proof of 1.20 (which in my version is the van Kampen theorem) but there's no proof that the kernel is the image of the map pi_1(A \cap B) -> pi_1(A)
Maybe I somehow missed it idk
Thats like
The entire statement
Lol
Although I’m not sure where you are getting that statement @pearl holly the description of N is given elsewhere
Your description is not correct
Yeah wait that’s very wrong where are you getting that
This: kernel is the image of the map pi_1(A \cap B) -> pi_1(A)?
This?
Just type "yes" moldi lmao
wrong opinion toki
Yes that is wrong the kernel in van kampen is not the image of the intersection
The intersection can contain nontrivial homotopy classes
1.20 might be the trivial intersection version?
Its not
Oh 
Okay sorry let me retake
Oh
No
I can explain it
This follows from van kampen
Here is the intuition for van kampen
If I take the free product of pi1A and pi1B
Then I am counting some loops twice
Namely those in A cap B
So what we do is we take a quotient to force these double counted loops to be the same

Then if B is contractible
And I force every loop of pi1A that is contained in pi1AcapB to be the same as the loop in pi1B
That forced them all to be contractible
Hence the kernel is exactly as described
I've been following some lecture and I'm a little confused 0.0
If I have three groups, G_1, G_2 and H, and both G_1 and G_2 are homomorphic to H, does this necessarily mean that G_1*G_2 is homomorphic to H, where * is the free product? 
In hindsight, this is probably more of an algebra question but it's from a topology lecture, so it can't be that far off 
homomorphic ?


