Bott periodicity theorem

Bott periodicity theorem

In mathematics, the Bott periodicity theorem is a result from homotopy theory discovered by Raoul Bott during the latter part of the 1950s, which proved to be of foundational significance for much further research, in particular in K-theory of stable complex vector bundles, as well as the stable homotopy groups of spheres. Bott periodicity can be formulated in numerous ways, with the periodicity in question always appearing as a period 2 phenomenon, with respect to dimension, for the theory associated to the unitary group. See for example topological K-theory.

There are corresponding period-8 phenomena for the matching theories, (real) KO-theory and (quaternionic) KSp-theory, associated to the real orthogonal group and the quaternionic symplectic group, respectively. They impact the stable homotopy groups of spheres even more tightly than complex K-theory.

Context and significance

The context of Bott periodicity is that the homotopy groups of spheres, which would be expected to play the basic part in algebraic topology by analogy with homology theory, have proved elusive (and the theory is complicated). The subject of stable homotopy theory was conceived as a simplification, by introducing the suspension (smash product with a circle) operation, and seeing what (roughly speaking) remained of homotopy theory once one was allowed to suspend both sides of an equation, as many times as one wished. The stable theory was still hard to compute with, in practice.

What Bott periodicity offered was an insight into some highly non-trivial spaces, with central status in topology because of the connection of their cohomology with characteristic classes, for which all the ("unstable") homotopy groups could be calculated. These spaces are the (infinite, or "stable") unitary, orthogonal and symplectic groups "U", "O" and "Sp". In this context, "stable" refers to taking the union "U" (also known as the direct limit) of the sequence of inclusions

:U(1)subset U(2)subsetcdotssubset U = igcup_{k=1}^infty U(k)

and similarly for "O" and "Sp". Bott's (now somewhat awkward) use of the word "stable" in the title of his seminal paper refers to these stable classical groups and not to stable homotopy groups.

The important connection of Bott periodicity with the stable homotopy groups of spheres pi_n^S comes via the so called stable "J"-homomorphism from the (unstable) homotopy groups of the (stable) classical groups to these stable homotopy groups pi_n^S. Originally described by George W. Whitehead, it became the subject of the famous Adams conjecture (1963) which was finally resolved in the affirmative by Daniel Quillen (1971).

Bott's original results may be succinctly summarized in:

Corollary: The (unstable) homotopy groups of the (infinite) classical groups are periodic:

:pi_k(U)=pi_{k+2}(U) ,!

:pi_k(O)=pi_{k+4}(Sp) ,!

:pi_k(Sp)=pi_{k+4}(O) , k=0,1,dots . ,!

Note: The second and third of these isomorphisms intertwine to give the desired 8-fold periodicity results:

:pi_k(O)=pi_{k+8}(O) ,!

:pi_k(Sp)=pi_{k+8}(Sp) , k=0,1,dots . ,!

Loop spaces and classifying spaces

For the theory associated to the infinite unitary group, "U", the space "BU" is the classifying space for stable complex vector bundles (a Grassmannian in infinite dimensions). One formulation of Bott periodicity describes the twofold loop space, Ω2"BU" of "BU". Here, Ω is the loop space functor, right adjoint to suspension and left adjoint to the classifying space construction. Bott periodicity states that this double loop space is essentially "BU" again; more precisely,

:Omega^2BUsimeq Z imes BU,

is essentially (that is, homotopy equivalent to) the union of a countable number of copies of "BU". An equivalent formulation is

:Omega^2Usimeq U .,

Either of these has the immediate effect of showing why (complex) topological "K"-theory is a 2-fold periodic theory.

In the corresponding theory for the infinite orthogonal group, "O", the space "BO" is the classifying space for stable real vector bundles. In this case, Bott periodicity states that, for the 8-fold loop space,

:Omega^8BOsimeq Z imes BO ;,

or equivalently,

:Omega^8Osimeq O ,,

which yields the consequence that "KO"-theory is an 8-fold periodic theory. Also, for the infinite symplectic group, "Sp", the space "BSp" is the classifying space for stable quaternionic vector bundles, and Bott periodicity states that

:Omega^8BSpsimeq Z imes BSp ;,

or equivalently

:Omega^8Spsimeq Sp .,

Thus both topological real "K"-theory (also known as "KO"-theory) and topological quaternionic "K"-theory (also known as "KSp"-theory) are 8-fold periodic theories.

Geometric model of loop spaces

One elegant formulation of Bott periodicity makes use of the observation that there are natural embeddings (as closed subgroups) between the classical groups.The loop spaces in Bott periodicity are then homotopy equivalent to the symmetric spaces of successive quotients, with additional discrete factors of mathbf{Z}.

Over the complex numbers:: U imes U subset U subset U imes U.Over the real numbers and quaternions::O imes O subset Osubset Usubset Sp subsetSp imes Sp subset Spsubset Usubset O subset O imes O.

These sequences corresponds to sequences in Clifford algebras; over the complex numbers::mathbf{C} oplus mathbf{C} subset mathbf{C}subset mathbf{C} oplus mathbf{C}.Over the real numbers and quaternions::mathbf{R} oplus mathbf{R} subset mathbf{R}subset mathbf{C}subset mathbf{H} subset mathbf{H} imes mathbf{H} subset mathbf{H} subset mathbf{C} subset mathbf{R} subset mathbf{R} oplus mathbf{R}where the division algebras indicate "matrices over that algebra".

As they are 2-periodic/8-periodic, they can be arranged in a circle, where they are called the Bott periodicity clock and Clifford algebra clock.

The Bott periodicity results then refine to a sequence of homotopy equivalences:

For complex "K"-theory::egin{align}Omega U &simeq mathbf{Z} imes BU = mathbf{Z} imes U/(U imes U)\Omega(Z imes BU)& simeq U = (U imes U)/Uend{align}

For real and quaternionic "KO"- and "KSp"-theories::egin{align} Omega(mathbf{Z} imes BO) &simeq O = (O imes O)/O& Omega(mathbf{Z} imes BSp) &simeq Sp = (Sp imes Sp)/Sp\Omega O &simeq O/U & Omega Sp &simeq Sp/U\Omega(O/U) &simeq U/Sp & Omega(Sp/U) &simeq U/O\Omega(U/Sp)&simeq mathbf{Z} imes BSp = mathbf{Z} imes Sp/(Sp imes Sp) & Omega(U/O) &simeq mathbf{Z} imes BO = mathbf{Z} imes O/(O imes O)\end{align}The resulting spaces are homotopy equivalent to the classical reductive symmetric spaces, and are the successive quotients of the terms of the Bott periodicity clock.These equivalences immediately yield the Bott periodicity theorems.

Proofs

Bott's original proof used Morse theory; subsequently, many different proofs have been given.

Applications

* Bott periodicity expresses a considerable amount regarding the topology of the orthogonal group, in particular the homotopy groups

References

*Bott, R. "The Stable Homotopy of the Classical Groups", Ann. Math. 70, 1959, 313–337.
*Giffen, C.H. "Bott periodicity and the Q-construction", Contemp. Math. 199(1996), 107–124.
*Milnor, J. "Morse Theory". Princeton University Press, 1969. ISBN 0-691-08008-9.
* [http://math.ucr.edu/home/baez/week105.html John Baez "This Week's Finds in Mathematical Physics" week 105]


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