5.01 Van Kampen's theorem

Below the video you will find accompanying notes and some pre-class questions.

Notes

Van Kampen's theorem

(0.00) Let X be a topological space and let U,VX be open subsets such that UV is nonempty and path-connected. Let xUV be a basepoint. Then π1(X,x)=π1(U,x)π1(UV,x)π1(V,x).

(1.12) Here, ACB denotes the amalgamated product. Suppose you have groups A,B,C and homomorphisms f:CA and g:CA. In our case, A=π1(U,x), B=π1(V,x) and C=π1(UV,x), the map f is the pushforward map i where i:UVU is the inclusion, and g is the pushforward j where j:UVV is the inclusion.

(2.33) Given A,B,C,f,g, you can define the amalgamated product ACB=generators of A, generators of B | relations of A, relations of B, amalgamated relations.

The amalgamated relations come from elements cC: each cC gives a relation f(c)=g(c).

Amalgamated relations

(4.30) What does this mean? We have f(c)A and we have already in the presentation of ACB 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 UV; 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

(5.50) The 2-sphere X can be written as UV where U is a neighbourhood of the Northern hemisphere and V is a neighbourhood of the Southern hemisphere. The overlap UV is an annular neighbourhood of the equator. Van Kampen's theorem tells us that π1(X)=π1(U)π1(UV)π1(V).

We have π1(U)=π1(V)={1} as both U and V are simply-connected discs. Since UV is homotopy equivalent to the circle, π1(UV)=Z=c (i.e. one generator, c, and no relations).

The amalgamated product π1(U)π1(UV)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(UV) is nontrivial doesn't affect this computation: it would only enter into the relations in the group. Indeed, for each cπ1(UV), we have ic=1π1(U) and jc=1π1(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}.

(9.56) Let X=S1S1 be the wedge of two circles (i.e. the disjoint union of two circles modulo an equivalence relation which identifies one point on the first circle with one point on the second. We take U to be a neighbourhood of the first circle and V to be a neighbourhood of the second. The intersection UV is a cross-shaped neighbourhood of the point where the two circles intersect (the wedge point).

(10.37) Since US1 and VS1 we have π1(U)=π1(V)=Z. Moreover, UV is contractible, so π1(UV)={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(UV) is trivial).

(11.57) A presentation for π1(S1S1) is therefore a,b

. This has no relations: we call a group with no relations a free group on its generators. The elements of a free group a,b are words on its generators, written using as, bs, a1s, b1s, for example a2b1a14bab2.
The only simplifications one may perform with these elements are things like aa1=a1a=1 or bb1=b1b=1. In particular, the free group on two generators is not abelian (the relation ab=ba does not hold).

(13.32) Let X=T2, thought of as a square with its opposite sides identified. Let U be an open disc in the middle of the square. Let V be (a small open thickening of) the complement of U. The intersection UV is a circle. We have To see VS1S1, note that the square minus a disc is homotopy equivalent to the boundary of the square, which becomes a wedge of two circles in the quotient space.

(16.03) Van Kampen's theorem then tells us π1(T2)=a,b | i(c)=j(c), where

(16.37) This amalgamated relation j(c)=1 can be read from the picture: the boundary of the circle is homotopic to the loop b1a1ba in V. Therefore the amalgamated relation for the generator cZ is 1=b1a1ba.

(18.00) This relation is equivalent to ab=ba, so the group we get is just the abelian group Z2.

Pre-class questions

  1. 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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CC-BY-SA 4.0 Jonny Evans.