- Vector fields on spheres
In
mathematics , the discussion of vector fields on spheres was a classical problem ofdifferential topology , beginning with thehairy ball theorem , and early work on the classification ofdivision algebra s.Specifically, the question is how many linearly independent vector fields can be constructed on a sphere in "N"-dimensional
Euclidean space . A definitive answer was made in 1962 byFrank Adams . It was already known, by direct construction usingClifford algebra s, that there were at least ρ("N") such fields (see definition below). Adams appliedhomotopy theory to prove that no more independent vector fields could be found.Technical details
In detail, the question applies to the 'round spheres' (not
exotic sphere s); and to theirtangent bundle s. The case of "N" odd is taken care of by thePoincaré–Hopf index theorem (seehairy ball theorem ), so the case "N" even is an extension of that. The maximum number of continuous ("smooth" would be no different here) pointwise linearly-independent vector fields onthe ("N" − 1)-sphere is computable by this formula: write "N" as the product of an odd number "A" and apower of two 2"B". Write:"B" = "c" + 4"d", 0 ≤ "c" < 4.
Then
:ρ("N") = 2"c" + 8"d" − 1.
The construction of the fields is related to the real
Clifford algebra s, which is a theory with a periodicity "modulo" 8 that also shows up here. By theGram–Schmidt process , it is the same to ask for (pointwise) linear independence or fields that give anorthonormal basis at each point.Radon–Hurwitz numbers
The numbers ρ("n") are the Radon–Hurwitz numbers, so-called from the earlier work of
Johann Radon (1922) andAdolf Hurwitz (1923) in this area. Arecurrence relation is easy to give.The first few values of ρ(2"n") are given by OEIS|id=A053381::1, 3, 1, 7, 1, 3, 1, 8, 1, 3, 1, 7, 1, 3, 1, 9, ...For odd "n", the function ρ("n") is zero.
These numbers occur also in other, related areas. In
matrix theory , the Radon–Hurwitz number counts the maximum size of a linear subspace of the real "n"×"n" matrices, for which each non-zero matrix is asimilarity , i.e. a product of anorthogonal matrix and ascalar matrix . The classical results were revisited in 1952 byBeno Eckmann . They are now applied in areas includingcoding theory andtheoretical physics .References
*J. F. Adams, "Vector Fields on Spheres", Annals of Math 75 (1962) 603–632.
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