1.08 Brouwer's fixed point theorem
Below the video you will find accompanying notes and some pre-class questions.
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Notes
Brouwer's fixed point theorem

(3.45) If there were a fixed point, we would not know which ray to draw (as F(x)=x), so this map is only well-defined because we have assumed there are no fixed points.
(3.58) We claim that:
- G is continuous; this is intuitively clear, but requires proof (below).
- G(x)=x if x∈∂D2; this is clear, because if x∈∂D2, no matter where F(x) is, the ray from F(x) to x intersects the boundary at x, so G(x)=x.

(9.20) It remains to prove claim 1 (that G is continuous). We can write G as a composition H∘j where:
- j:D2→D2×D2∖{(x,x) : x∈D2} is the map j(x)=(x,F(x)).
- (11.30) H:D2×D2∖{(x,x) : x∈D2} is the map defined as follows. Given two distinct points x≠y in D2, let H(x,y) denote the point where the ray from y through x intersects ∂D2.
(13.25) We can write H explicitly in coordinates. The ray from y through x is given in parametric form by y+t(x−y). The condition that the ray meets the boundary of the disc is |y+t(x−y)|2=1,
Pre-class questions
- Brouwer's fixed point theorem tells us that continuous maps between 2-discs have fixed points. Is the same true for maps between 2-dimensional annuli? (An annulus is S1×[0,1]).
- Brouwer's fixed point theorem also holds for maps F:Dn→Dn where Dn is the n-dimensional disc; can the proof
above be adapted to cover this case, or are new ideas required?
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