8.3 Equivariant Bott periodicity and localization theorems
6 min read•july 30, 2024
Equivariant Bott periodicity extends to spaces with group actions. It establishes a natural between groups of a space X and its . This powerful result connects equivariant and through the .
link equivariant K-theory to . The recovers equivariant K-theory from fixed points by inverting elements in the . These results bridge equivariant and non-equivariant K-theory, showcasing connections to representation theory and geometry.
Equivariant Bott Periodicity
Statement and Proof
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Equivariant Bott periodicity extends the fundamental result in topological K-theory relating the K-theory of a space X to the K-theory of its suspension ΣX, to spaces with a group action
For a G and a compact G-space X, there exists a natural isomorphism between the G-equivariant K-theory groups KG(X) and KG(Σ2X), where Σ2X represents the double suspension of X with the induced G-action
The proof involves constructing an explicit homotopy equivalence between the G-equivariant K-theory spectra of X and Σ2X, utilizing and the
The equivariant Thom isomorphism establishes a connection between the G-equivariant K-theory of a G-equivariant vector bundle and the K-theory of its Thom space, playing a crucial role in establishing the periodicity isomorphism
Equivariant Bott periodicity can also be derived from the non-equivariant case by considering the Borel construction and employing the associated with the fibration EG×GX→BG
Alternative Derivation and Spectral Sequences
The Borel construction, which associates a classifying space EG×GX to a G-space X, provides an alternative approach to deriving equivariant Bott periodicity from the non-equivariant case
The spectral sequence associated with the fibration EG×GX→BG relates the equivariant K-theory of X to the non-equivariant K-theory of the Borel construction EG×GX
By applying the non-equivariant Bott periodicity theorem to the space EG×GX and analyzing the spectral sequence, one can deduce the equivariant Bott periodicity isomorphism between KG(X) and KG(Σ2X)
This approach highlights the interplay between equivariant and non-equivariant K-theory, and demonstrates the power of spectral sequence techniques in studying equivariant cohomology theories
Computing Equivariant K-theory
Applications of Bott Periodicity
Equivariant Bott periodicity serves as a powerful tool for computing equivariant K-theory groups by reducing the problem to understanding the K-theory of simpler spaces related by suspension
For a compact Lie group G acting freely on a sphere S2n−1, the equivariant K-theory of the quotient space S2n−1/G can be determined using Bott periodicity and the equivariant K-theory of a point, KG(pt), which is isomorphic to the representation ring R(G)
When G acts trivially on a space X, equivariant Bott periodicity implies that the equivariant K-theory KG(X) is isomorphic to the tensor product of the non-equivariant K-theory K(X) with the representation ring R(G)
This result allows for the computation of equivariant K-theory in terms of non-equivariant K-theory and representation theory in the case of trivial group actions
Künneth Theorem and Product Spaces
For a compact Lie group G acting on a product space X×Y, the equivariant , in conjunction with Bott periodicity, can be employed to express KG(X×Y) in terms of the equivariant K-theory groups of X and Y
The equivariant Künneth theorem provides a decomposition of the equivariant K-theory of a product space in terms of tensor products of the equivariant K-theory groups of the individual factors
By iteratively applying the equivariant Künneth theorem and Bott periodicity, one can compute the equivariant K-theory of higher-dimensional and relate it to the equivariant K-theory of the constituent spaces
This computational technique is particularly useful in studying the equivariant K-theory of and other spaces with a torus action that can be decomposed into simpler pieces
Localization Theorems for Equivariant K-theory
Atiyah-Segal Localization Theorem
The Atiyah-Segal localization theorem establishes a connection between the equivariant K-theory of a G-space X and the equivariant K-theory of its fixed point subspaces XH, where H is a subgroup of G
For a compact Lie group G acting on a compact space X, the theorem asserts that the equivariant K-theory of X can be recovered from the equivariant K-theory of the fixed point subspaces XH, as H ranges over the closed subgroups of G, by inverting certain elements in the representation ring R(G)
Specifically, the localization theorem states that the map KG(X)→∏HKH(XH), induced by the inclusion of fixed point subspaces, becomes an isomorphism after inverting the elements 1−[V] in R(G), where V ranges over the non-trivial irreducible representations of G
The proof of the localization theorem typically involves analyzing the equivariant K-theory spectral sequence associated with the filtration of X by the fixed point subspaces XH and applying the localization theorem for the representation ring R(G)
Variations and Generalizations
Variations and generalizations of the localization theorem, such as the , provide more refined information about the relationship between the equivariant K-theory of a space and its fixed point subspaces
The Atiyah-Bott-Berline-Vergne localization formula is particularly useful in the case of a compact Lie group G acting on a compact manifold X with isolated fixed points
The formula expresses the equivariant K-theory of X as a sum of local contributions from the fixed points, involving the non-equivariant K-theory of the fixed points and the representations of G on the tangent spaces at the fixed points
Other variations of the localization theorem, such as the and the equivariant index theorem, relate equivariant K-theory to other geometric and topological invariants, such as characteristic classes and indices of elliptic operators
These generalizations demonstrate the rich interplay between equivariant K-theory, representation theory, and geometry, and provide powerful tools for computing and understanding equivariant invariants in various settings
Equivariant vs Non-Equivariant K-theory
Relationship via Localization Theorems
Localization theorems provide a bridge between equivariant K-theory and non-equivariant K-theory by expressing the equivariant K-theory of a G-space X in terms of the ordinary K-theory of its fixed point subspaces
In the case of a trivial G-action on X, the localization theorem implies that the equivariant K-theory KG(X) is isomorphic to the tensor product of the non-equivariant K-theory K(X) with the localized representation ring R(G)I, where I is the ideal generated by the elements 1−[V] for non-trivial irreducible representations V of G
This result allows for the computation of equivariant K-theory in terms of non-equivariant K-theory and representation theory in the case of trivial group actions
For a compact Lie group G acting on a compact manifold X with isolated fixed points, the Atiyah-Bott-Berline-Vergne localization formula expresses the equivariant K-theory of X as a sum of local contributions from the fixed points, involving the non-equivariant K-theory of the fixed points and the representations of G on the tangent spaces at the fixed points
Connections to Representation Theory
Localization theorems can be used to compute the equivariant K-theory of G/H in terms of the representation theory of the subgroup H, by considering the fixed points of the action of a maximal torus of G
This technique is particularly effective for flag varieties and other homogeneous spaces of Lie groups, where the fixed points of the torus action are isolated and can be described explicitly
The relationship between equivariant K-theory and representation theory can be further explored using the Borel-Weil-Bott theorem, which relates the equivariant K-theory of flag varieties to the irreducible representations of the corresponding Lie group
The Borel-Weil-Bott theorem provides a geometric realization of irreducible representations in terms of equivariant line bundles on flag varieties, and allows for the computation of the equivariant K-theory of these spaces in terms of representation-theoretic data
The interplay between equivariant K-theory, representation theory, and geometric representation theory is a rich and active area of research, with applications to a wide range of topics in mathematics and mathematical physics, including gauge theory, string theory, and the Langlands program