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Simplicial Structures in Topology

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VI.1 Fundamental Group 209<br />

We now construct the pushout<br />

∂W = ∨ n j=1S1 ∨ f j<br />

j<br />

��<br />

W = ∨ n j=1 D2 j ∨ f j<br />

In other words, we construct a space X by glu<strong>in</strong>g n two-dimensional disks D2 j to Y<br />

by means of the functions f j , j = 1,...,n, one for each relation r j.<br />

We may consider the space Y as the geometric realization of a one-dimensional<br />

simplicial complex with 2m + 1 vertices<br />

��<br />

Y<br />

��<br />

��<br />

X<br />

a0;a 1 1 ,a1 2 ;a2 1 ,a2 2 ;...;am 1 ,am 2<br />

(the vertices a i 1 ,ai 2 correspond to two dist<strong>in</strong>ct po<strong>in</strong>ts of S1 i , a0 =(e1,...,em)), and<br />

3m 1-simplexes<br />

{a0,a 1 1},{a 1 1,a 1 2},{a 1 2,a0};...;{a0,a m 1 },{am 1 ,am 2 },{am 2 ,a0}<br />

(each group of three 1-simplexes corresponds to a circle). After this, we view<br />

the disk D2 j , that corresponds to the relation r j given by a word of length p, as<br />

a regular 3p-polyhedron, j = 1,...,n. In this manner, the disk D2 j is glued to Y<br />

— as we did <strong>in</strong> Theorem (VI.1.15) — by means of the closed path of geometric<br />

1-simplexes<br />

�r j =(|{a0,a i1<br />

1 }|.|{ai1<br />

1 ,ai1<br />

2 }|.|{ai1<br />

2 ,a0}|) ε1 ...(|{a0,a ip<br />

1 }|.|{aip<br />

1 ,aip<br />

2 }|.|{aip<br />

2 ,a0}|) εp .<br />

On the other hand, the fundamental group of Y is the free group generated by �gi,<br />

i = 1,...,n where each �gi equals the homotopy class of the closed geometric path<br />

|{a0,a i 1 }|.|{ai 1 ,ai 2 }|.|{ai 2 ,a0}|.<br />

We conclude the proof by apply<strong>in</strong>g Theorem (VI.1.15). �<br />

Theorem (VI.1.16) may be used backward for comput<strong>in</strong>g the fundamental group<br />

of certa<strong>in</strong> two-dimensional polyhedra: actually, if a polyhedron |K| is constructed<br />

as <strong>in</strong> the theorem, we have at once the generators and the relations that def<strong>in</strong>e<br />

the fundamental group of |K|. For <strong>in</strong>stance, let |K| = T 2 be the torus; if<br />

we use the triangulation given <strong>in</strong> Sect. III.5.1 and <strong>in</strong>dicate the sides 01,12,20<br />

and 03,34,40, respectively, with a and b, we see that π(T 2 ,0) is the group def<strong>in</strong>ed<br />

by the generators a,b and the relation aba −1 b −1 ; therefore, π(T 2 ,0) ∼ =<br />

Z × Z.

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