Borsuk–Ulam theorem

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mathematics, the Borsuk–Ulam theorem states that every continuous function from an n-sphere into Euclidean n-space maps some pair of antipodal points to the same point.
Antipodal points are opposite points on the sphere
File:Borsuk ulam.svg
Matching antipodal points of a squashed balloon animal

Informally, the Borsuk–Ulam theorem states that, for a "balloon animal" (or any arbitrarily distorted shape) made out of a spherical balloon, and then squashed into a plane (letting the air out somehow), at least one pair of points that were opposite each other on the original sphere will be squashed onto the same point of the plane.

Statement

Formally, the theorem states that every continuous function from an n-sphere into n-dimensional Euclidean space must map some pair of antipodal points to the same point. Two points on a sphere are called antipodal if they lie in exactly opposite directions from the center—like the North and South Poles.

The Borsuk–Ulam theorem has several equivalent statements in terms of odd functions. Recall that Sn is the n-sphere and Bn is the n-ball:

  • If g:Snn is a continuous odd function, then there exists an xSn such that: g(x)=0.
  • If g:Bnn is a continuous function which is odd on Sn1 (the boundary of Bn), then there exists an xBn such that: g(x)=0.

Examples

More compactly: if f:Snn is continuous then there exists an xSn such that: f(x)=f(x).

The case n=1 can be illustrated by saying that there always exist a pair of opposite points on the Earth's equator with the same temperature. The same is true for any circle. This assumes the temperature varies continuously in space, which is, however, not always the case.[1]

The case n=2 is often illustrated by saying that at any moment, there is always a pair of antipodal points on the Earth's surface with equal temperatures and equal barometric pressures, assuming that both parameters vary continuously in space.

History

According to Template:Harvtxt, the first historical mention of the statement of the Borsuk–Ulam theorem appears in Template:Harvtxt. The first proof was given by Template:Harvs, where the formulation of the problem was attributed to Stanisław Ulam. Since then, many alternative proofs have been found by various authors, as collected by Template:Harvtxt.

Equivalent statements

The following statements are equivalent to the Borsuk–Ulam theorem.[2]

With odd functions

A function g is called odd (aka antipodal or antipode-preserving) if for every x, g(x)=g(x).

The Borsuk–Ulam theorem is equivalent to each of the following statements:

(1) Each continuous odd function Snn has a zero.

(2) There is no continuous odd function SnSn1.

Here is a proof that the Borsuk-Ulam theorem is equivalent to (1):

() If the theorem is correct, then it is specifically correct for odd functions, and for an odd function, g(x)=g(x) iff g(x)=0. Hence every odd continuous function has a zero.

() For every continuous function f:Snn, the following function is continuous and odd: g(x)=f(x)f(x). If every odd continuous function has a zero, then g has a zero, and therefore, f(x)=f(x).

To prove that (1) and (2) are equivalent, we use the following continuous odd maps:

  • the obvious inclusion i:Sn1n{0},
  • and the radial projection map p:n{0}Sn1 given by xx|x|.

The proof now writes itself.

((1)(2)) We prove the contrapositive. If there exists a continuous odd function f:SnSn1, then if is a continuous odd function Snn{0}.

((1)(2)) Again we prove the contrapositive. If there exists a continuous odd function f:Snn{0}, then pf is a continuous odd function SnSn1.

Proofs

1-dimensional case

The 1-dimensional case can easily be proved using the intermediate value theorem (IVT).

Let g be the odd real-valued continuous function on a circle defined by g(x)=f(x)f(x). Pick an arbitrary x. If g(x)=0 then we are done. Otherwise, without loss of generality, g(x)>0. But g(x)<0. Hence, by the IVT, there is a point y at which g(y)=0.

General case

Algebraic topological proof

Assume that h:SnSn1 is an odd continuous function with n>2 (the case n=1 is treated above, the case n=2 can be handled using basic covering theory). By passing to orbits under the antipodal action, we then get an induced continuous function h:nn1 between real projective spaces, which induces an isomorphism on fundamental groups. By the Hurewicz theorem, the induced ring homomorphism on cohomology with 𝔽2 coefficients [where 𝔽2 denotes the field with two elements],

𝔽2[a]/an+1=H*(n;𝔽2)H*(n1;𝔽2)=𝔽2[b]/bn,

sends b to a. But then we get that bn=0 is sent to an0, a contradiction.[3]

One can also show the stronger statement that any odd map Sn1Sn1 has odd degree and then deduce the theorem from this result.

Combinatorial proof

The Borsuk–Ulam theorem can be proved from Tucker's lemma.[2][4][5]

Let g:Snn be a continuous odd function. Because g is continuous on a compact domain, it is uniformly continuous. Therefore, for every ϵ>0, there is a δ>0 such that, for every two points of Sn which are within δ of each other, their images under g are within ϵ of each other.

Define a triangulation of Sn with edges of length at most δ. Label each vertex v of the triangulation with a label l(v)±1,±2,,±n in the following way:

  • The absolute value of the label is the index of the coordinate with the highest absolute value of g: |l(v)|=argmaxk(|g(v)k|).
  • The sign of the label is the sign of g at the above coordinate, so that: l(v)=sgn(g(v)|l(v)|)|l(v)|.

Because g is odd, the labeling is also odd: l(v)=l(v). Hence, by Tucker's lemma, there are two adjacent vertices u,v with opposite labels. Assume w.l.o.g. that the labels are l(u)=1,l(v)=1. By the definition of l, this means that in both g(u) and g(v), coordinate #1 is the largest coordinate: in g(u) this coordinate is positive while in g(v) it is negative. By the construction of the triangulation, the distance between g(u) and g(v) is at most ϵ, so in particular |g(u)1g(v)1|=|g(u)1|+|g(v)1|ϵ (since g(u)1 and g(v)1 have opposite signs) and so |g(u)1|ϵ. But since the largest coordinate of g(u) is coordinate #1, this means that |g(u)k|ϵ for each 1kn. So |g(u)|cnϵ, where cn is some constant depending on n and the norm || which you have chosen.

The above is true for every ϵ>0; since Sn is compact there must hence be a point u in which |g(u)|=0.

Corollaries

  • No subset of n is homeomorphic to Sn
  • The ham sandwich theorem: For any compact sets A1, ..., An in n we can always find a hyperplane dividing each of them into two subsets of equal measure.

Equivalent results

Above we showed how to prove the Borsuk–Ulam theorem from Tucker's lemma. The converse is also true: it is possible to prove Tucker's lemma from the Borsuk–Ulam theorem. Therefore, these two theorems are equivalent. Template:Analogous fixed-point theorems

Generalizations

  • In the original theorem, the domain of the function f is the unit n-sphere (the boundary of the unit n-ball). In general, it is true also when the domain of f is the boundary of any open bounded symmetric subset of n containing the origin (Here, symmetric means that if x is in the subset then -x is also in the subset).[6]
  • More generally, if M is a compact n-dimensional Riemannian manifold, and f:Mn is continuous, there exists a pair of points x and y in M such that f(x)=f(y) and x and y are joined by a geodesic of length δ, for any prescribed δ>0.[7][8]
  • Consider the function A which maps a point to its antipodal point: A(x)=x. Note that A(A(x))=x. The original theorem claims that there is a point x in which f(A(x))=f(x). In general, this is true also for every function A for which A(A(x))=x.[9] However, in general this is not true for other functions A.[10]

See also

Notes

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References

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External links

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  3. Joseph J. Rotman, An Introduction to Algebraic Topology (1988) Springer-Verlag Template:ISBN (See Chapter 12 for a full exposition.)
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