5.01 Van Kampen's theorem
Below the video you will find accompanying notes and some pre-class questions.
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Notes
Van Kampen's theorem
(2.33) Given A,B,C,f,g, you can define the amalgamated product A⋆CB=⟨generators of A, generators of B | relations of A, relations of B, amalgamated relations⟩.
Amalgamated relations
(4.30) What does this mean? We have f(c)∈A and we have already in the presentation of A⋆CB the generators and relations of A, so I can make sense of the element f(c) in the amalgamated product. Similarly, g(c)∈B and we can think of this as an element in the amalgamated product. The corresponding amalgamated relation is just saying that these two elements agree.
(5.13) Geometrically, in the context of Van Kampen's theorem, C consists of loops living in the intersection U∩V; the amalgamated relations are then saying ``you can think of these loops as living in U; you can think of them living in V; it makes no difference''.
Examples
We have π1(U)=π1(V)={1} as both U and V are simply-connected discs. Since U∩V is homotopy equivalent to the circle, π1(U∩V)=Z=⟨c⟩ (i.e. one generator, c, and no relations).
The amalgamated product π1(U)⋆π1(U∩V)π1(V) has the empty set of generators coming from π1(U) and the empty set of generators coming from π1(V). Therefore it has no generators and the amalgamated product is trivial.
(9.07) The fact that π1(U∩V) is nontrivial doesn't affect this computation: it would only enter into the relations in the group. Indeed, for each c∈π1(U∩V), we have i∗c=1∈π1(U) and j∗c=1∈π1(V), so the amalgamated relations all become 1=1, which we don't need to include as a relation because it holds in any group.
The upshot of all of this is the statement that π1(S2)={1}.
(10.37) Since U≃S1 and V≃S1 we have π1(U)=π1(V)=Z. Moreover, U∩V is contractible, so π1(U∩V)={1}. The amalgamated product has a generator a coming from π1(U) and a generator b coming from π1(V). There are no relations coming from π1(U), none coming from π1(V) and also no amalgamated relations (since π1(U∩V) is trivial).
(11.57) A presentation for π1(S1∨S1) is therefore ⟨a,b⟩
- π1(U) is trivial, as U is a disc;
- π1(U∩V)=Z;
- π1(V)=⟨a,b⟩, as V≃S1∨S1.
(16.03) Van Kampen's theorem then tells us π1(T2)=⟨a,b | i∗(c)=j∗(c)⟩, where
- c∈Z is a generator,
- i∗:Z→{1} is the trivial map,
- j∗:Z→⟨a,b⟩ sends a generator
for Z to some word in a,b
(18.00) This relation is equivalent to ab=ba, so the group we get is just the abelian group Z2.
Pre-class questions
- The Klein bottle K is obtained from a square by identifying
opposite sides as in the figure below. By mimicking the calculation
for T2, find a presentation for π1(K) using Van
Kampen's theorem.
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