LECTURES ON ZARISKI VAN-KAMPEN THEOREM 1. Introduction ...
LECTURES ON ZARISKI VAN-KAMPEN THEOREM 1. Introduction ...
LECTURES ON ZARISKI VAN-KAMPEN THEOREM 1. Introduction ...
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<strong>LECTURES</strong> <strong>ON</strong> <strong>ZARISKI</strong> <strong>VAN</strong>-<strong>KAMPEN</strong> <strong>THEOREM</strong> 11<br />
σ i<br />
σ i+1<br />
σ i<br />
≀<br />
homotopic<br />
σ i+1<br />
σ i<br />
σ i+1<br />
Figure 4.5. σ i σ i+1 σ i = σ i+1 σ i σ i+1<br />
The fact that B n is generated by σ 1 , ... , σ n−1 is easy to see. The relations<br />
actually hold can be checked easily by drawing braids. The difficult part is that<br />
any other relations among the generators can be derived from these relations. See<br />
[1] for the proof.<br />
We can define an action from right of the braid group B n on the free group F n<br />
by the following<br />
⎧<br />
⎪⎨ a j if j ≠ i, i +1<br />
a σi<br />
j := a i a i+1 a −1<br />
i if j = i<br />
(4.1)<br />
⎪⎩<br />
a i if j = i +<strong>1.</strong><br />
Check that this definition is compatible with the defining relation of the braid<br />
group. In the next section, we will explain the geometric meaning of this action.<br />
5. Monodromy on fundamental groups<br />
We denote the conjunction of paths α : I → X and β : I → X on the topological<br />
space X in such a way that αβ is defined if and only if α(1) = β(0).<br />
5.<strong>1.</strong> Fundamental groups and locally trivial fiber spaces. Let p : E → B be<br />
a locally trivial fiber space. Suppose that p : E → B has a section<br />
s : B → E;<br />
that is, s is a continuous map satisfying p ◦ s =id B . We choose a base point ˜b of<br />
E and b of B in such a way that ˜b = s(b) holds. We then put<br />
F b := p −1 (b).