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Math4202Topology II (Lecture 30)

Math4202 Topology II (Lecture 30)

Algebraic Topology

We skipped a few chapters about Jordan curve theorem, which will be your final project soon. LOL, I will embedded the link once I’m done.

Seifert-Van Kampen Theorem

The Seifert-Van Kampen Theorem

Let X=UVX=U\cup V be a union of two open subspaces. Suppose that UVU\cap V, U,VU,V are path connected. Fix x0UVx_0\in U\cap V.

Let HH be a group (arbitrary). And now we assume ϕ1,ϕ2\phi_1,\phi_2 be a group homomorphism, and ϕ1:π1(U,x0)H\phi_1:\pi_1(U,x_0)\to H, and ϕ2:π1(V,x0)H\phi_2:\pi_1(V,x_0)\to H.

Seifert-Van Kampen Theorem

Let i1,i2,j1,j2,i12i_1,i_2,j_1,j_2,i_{12} be group homomorphism induced by the inclusion maps.

Assume this diagram commutes.

ϕ1i1=ϕ2i2\phi_1\circ i_1=\phi_2\circ i_2

There is a group homomorphism Φ:π1(X,x0)H\Phi:\pi_1(X,x_0)\to H making the diagram commute. Φj1=ϕ1\Phi\circ j_1=\phi_1 and Φj2=ϕ2\Phi\circ j_2=\phi_2.

We may change the base point using conjugations.

Side notes about free product of two groups

Consider arbitrary group G1,G2G_1,G_2, then G1×G2G_1\times G_2 is a group.

Note that the inclusion map i1:G1G1×G2i_1:G_1\to G_1\times G_2 is a group homomorphism and the inclusion map i2:G2G1×G2i_2:G_2\to G_1\times G_2 is a group homomorphism. The image of them commutes since (e,g2)(g1,e)=(g1,g2)=(g1,e)(e,g2)(e,g_2)(g_1,e)=(g_1,g_2)=(g_1,e)(e,g_2).

The universal property

Then we want to have a group GG such that for all group homomorphism ϕ:G1H\phi:G_1\to H and G2HG_2\to H, such that there always exists a map Φ:GH\Phi: G\to H such that:

  • Φi1=ϕ1\Phi\circ i_1=\phi_1
  • Φi2=ϕ2\Phi\circ i_2=\phi_2

How to construct the free group?

We consider

G1G2=S={g1h1g2h2:g1,g2G1,h1,h2G2}/G_1*G_2=S=\{g_1h_1g_2h_2:g_1,g_2\in G_1,h_1,h_2\in G_2\}/\sim

And we set gieG2gi+1gigi+1g_ie_{G_2}g_{i+1}\sim g_ig_{i+1} for giG1g_i\in G_1 and gi+1G2g_{i+1}\in G_2.

And hjeG1hj+1hjhj+1h_je_{G_1}h_{j+1}\sim h_jh_{j+1} for hjG2h_j\in G_2 and hj+1G1h_{j+1}\in G_1.

And we define the group operation

(g1h1gkhk)(h1g1hlgl)=g1h1gkhkg1h2hlgl(g_1 h_1\cdots g_k h_k)*(h_1' g_1'\cdots h_l' g_l')=g_1 h_1\cdots g_k h_k g_1' h_2'\cdots h_l' g_l'

And the inverse is defined

(g1h1gkhk)1=hk1gk1h11g11(g_1 h_1\cdots g_k h_k)^{-1}=h_k^{-1} g_k^{-1}\cdots h_1^{-1} g_1^{-1}

And G=SG=S is a well-defined group.

The homeomorphism GHG\to H is defined as

Φ((g1h1gkhk))=ϕ1(g1)ϕ2(h1)ϕ1(gk)ϕ2(hk)\Phi((g_1 h_1\cdots g_k h_k))=\phi_1(g_1)\circ \phi_2(h_1)\circ \cdots \circ \phi_1(g_k)\circ \phi_2(h_k)

Note \circ is the group operation in HH.

Group with such universal property is unique, so we don’t need to worry for that too much.

Back to the Seifert-Van Kampen Theorem:

Let H=π1(U,x0)π1(V,x0)H=\pi_1(U,x_0)* \pi_1(V,x_0).

Let NN be the least normal subgroup in the free product HH, containing i1(g)i2(g)1i_1(g)i_2(g)^{-1}, gπ1(UV,x0)\forall g\in \pi_1(U\cap V,x_0).

Note i1(g)π1(U,x0)i_1(g)\in \pi_1(U,x_0) and i2(g)π1(V,x0)i_2(g)\in \pi_1(V,x_0). You may think of them as G1,G2G_1,G_2 in the free group descriptions.

Seifert-Van Kampen Theorem (classical version)

There is an isomorphism between π1(U,x0)π1(V,x0)/N\pi_1(U,x_0)* \pi_1(V,x_0)/N and π1(UV,x0)\pi_1(U\cup V,x_0).

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