Branch of algebraic topology
In mathematics , topological K -theory is a branch of algebraic topology . It was founded to study vector bundles on topological spaces , by means of ideas now recognised as (general) K-theory that were introduced by Alexander Grothendieck . The early work on topological K -theory is due to Michael Atiyah and Friedrich Hirzebruch .
Definitions
Let X be a compact Hausdorff space and
k
=
R
{\displaystyle k=\mathbb {R} }
or
C
{\displaystyle \mathbb {C} }
. Then
K
k
(
X
)
{\displaystyle K_{k}(X)}
is defined to be the Grothendieck group of the commutative monoid of isomorphism classes of finite-dimensional k -vector bundles over X under Whitney sum . Tensor product of bundles gives K -theory a commutative ring structure. Without subscripts,
K
(
X
)
{\displaystyle K(X)}
usually denotes complex K -theory whereas real K -theory is sometimes written as
K
O
(
X
)
{\displaystyle KO(X)}
. The remaining discussion is focused on complex K -theory.
As a first example, note that the K -theory of a point is the integers. This is because vector bundles over a point are trivial and thus classified by their rank and the Grothendieck group of the natural numbers is the integers.
There is also a reduced version of K -theory,
K
~ ~ -->
(
X
)
{\displaystyle {\widetilde {K}}(X)}
, defined for X a compact pointed space (cf. reduced homology ). This reduced theory is intuitively K (X ) modulo trivial bundles . It is defined as the group of stable equivalence classes of bundles. Two bundles E and F are said to be stably isomorphic if there are trivial bundles
ε ε -->
1
{\displaystyle \varepsilon _{1}}
and
ε ε -->
2
{\displaystyle \varepsilon _{2}}
, so that
E
⊕ ⊕ -->
ε ε -->
1
≅ ≅ -->
F
⊕ ⊕ -->
ε ε -->
2
{\displaystyle E\oplus \varepsilon _{1}\cong F\oplus \varepsilon _{2}}
. This equivalence relation results in a group since every vector bundle can be completed to a trivial bundle by summing with its orthogonal complement. Alternatively,
K
~ ~ -->
(
X
)
{\displaystyle {\widetilde {K}}(X)}
can be defined as the kernel of the map
K
(
X
)
→ → -->
K
(
x
0
)
≅ ≅ -->
Z
{\displaystyle K(X)\to K(x_{0})\cong \mathbb {Z} }
induced by the inclusion of the base point x 0 into X .
K -theory forms a multiplicative (generalized) cohomology theory as follows. The short exact sequence of a pair of pointed spaces (X , A )
K
~ ~ -->
(
X
/
A
)
→ → -->
K
~ ~ -->
(
X
)
→ → -->
K
~ ~ -->
(
A
)
{\displaystyle {\widetilde {K}}(X/A)\to {\widetilde {K}}(X)\to {\widetilde {K}}(A)}
extends to a long exact sequence
⋯ ⋯ -->
→ → -->
K
~ ~ -->
(
S
X
)
→ → -->
K
~ ~ -->
(
S
A
)
→ → -->
K
~ ~ -->
(
X
/
A
)
→ → -->
K
~ ~ -->
(
X
)
→ → -->
K
~ ~ -->
(
A
)
.
{\displaystyle \cdots \to {\widetilde {K}}(SX)\to {\widetilde {K}}(SA)\to {\widetilde {K}}(X/A)\to {\widetilde {K}}(X)\to {\widetilde {K}}(A).}
Let Sn be the n -th reduced suspension of a space and then define
K
~ ~ -->
− − -->
n
(
X
)
:=
K
~ ~ -->
(
S
n
X
)
,
n
≥ ≥ -->
0.
{\displaystyle {\widetilde {K}}^{-n}(X):={\widetilde {K}}(S^{n}X),\qquad n\geq 0.}
Negative indices are chosen so that the coboundary maps increase dimension.
It is often useful to have an unreduced version of these groups, simply by defining:
K
− − -->
n
(
X
)
=
K
~ ~ -->
− − -->
n
(
X
+
)
.
{\displaystyle K^{-n}(X)={\widetilde {K}}^{-n}(X_{+}).}
Here
X
+
{\displaystyle X_{+}}
is
X
{\displaystyle X}
with a disjoint basepoint labeled '+' adjoined.[ 1]
Finally, the Bott periodicity theorem as formulated below extends the theories to positive integers.
Properties
K
n
{\displaystyle K^{n}}
(respectively,
K
~ ~ -->
n
{\displaystyle {\widetilde {K}}^{n}}
) is a contravariant functor from the homotopy category of (pointed) spaces to the category of commutative rings. Thus, for instance, the K -theory over contractible spaces is always
Z
.
{\displaystyle \mathbb {Z} .}
The spectrum of K -theory is
B
U
× × -->
Z
{\displaystyle BU\times \mathbb {Z} }
(with the discrete topology on
Z
{\displaystyle \mathbb {Z} }
), i.e.
K
(
X
)
≅ ≅ -->
[
X
+
,
Z
× × -->
B
U
]
,
{\displaystyle K(X)\cong \left[X_{+},\mathbb {Z} \times BU\right],}
where [ , ] denotes pointed homotopy classes and BU is the colimit of the classifying spaces of the unitary groups :
B
U
(
n
)
≅ ≅ -->
Gr
-->
(
n
,
C
∞ ∞ -->
)
.
{\displaystyle BU(n)\cong \operatorname {Gr} \left(n,\mathbb {C} ^{\infty }\right).}
Similarly,
K
~ ~ -->
(
X
)
≅ ≅ -->
[
X
,
Z
× × -->
B
U
]
.
{\displaystyle {\widetilde {K}}(X)\cong [X,\mathbb {Z} \times BU].}
For real K -theory use BO .
There is a natural ring homomorphism
K
0
(
X
)
→ → -->
H
2
∗ ∗ -->
(
X
,
Q
)
,
{\displaystyle K^{0}(X)\to H^{2*}(X,\mathbb {Q} ),}
the Chern character , such that
K
0
(
X
)
⊗ ⊗ -->
Q
→ → -->
H
2
∗ ∗ -->
(
X
,
Q
)
{\displaystyle K^{0}(X)\otimes \mathbb {Q} \to H^{2*}(X,\mathbb {Q} )}
is an isomorphism.
The equivalent of the Steenrod operations in K -theory are the Adams operations . They can be used to define characteristic classes in topological K -theory.
The Splitting principle of topological K -theory allows one to reduce statements about arbitrary vector bundles to statements about sums of line bundles.
The Thom isomorphism theorem in topological K -theory is
K
(
X
)
≅ ≅ -->
K
~ ~ -->
(
T
(
E
)
)
,
{\displaystyle K(X)\cong {\widetilde {K}}(T(E)),}
where T (E ) is the Thom space of the vector bundle E over X . This holds whenever E is a spin-bundle.
The Atiyah-Hirzebruch spectral sequence allows computation of K -groups from ordinary cohomology groups.
Topological K -theory can be generalized vastly to a functor on C*-algebras , see operator K-theory and KK-theory .
Bott periodicity
The phenomenon of periodicity named after Raoul Bott (see Bott periodicity theorem ) can be formulated this way:
K
(
X
× × -->
S
2
)
=
K
(
X
)
⊗ ⊗ -->
K
(
S
2
)
,
{\displaystyle K(X\times \mathbb {S} ^{2})=K(X)\otimes K(\mathbb {S} ^{2}),}
and
K
(
S
2
)
=
Z
[
H
]
/
(
H
− − -->
1
)
2
{\displaystyle K(\mathbb {S} ^{2})=\mathbb {Z} [H]/(H-1)^{2}}
where H is the class of the tautological bundle on
S
2
=
P
1
(
C
)
,
{\displaystyle \mathbb {S} ^{2}=\mathbb {P} ^{1}(\mathbb {C} ),}
i.e. the Riemann sphere .
K
~ ~ -->
n
+
2
(
X
)
=
K
~ ~ -->
n
(
X
)
.
{\displaystyle {\widetilde {K}}^{n+2}(X)={\widetilde {K}}^{n}(X).}
Ω Ω -->
2
B
U
≅ ≅ -->
B
U
× × -->
Z
.
{\displaystyle \Omega ^{2}BU\cong BU\times \mathbb {Z} .}
In real K -theory there is a similar periodicity, but modulo 8.
Applications
Topological K -theory has been applied in John Frank Adams’ proof of the “Hopf invariant one” problem via Adams operations .[ 2] Adams also proved an upper bound for the number of linearly-independent vector fields on spheres .[ 3]
Chern character
Michael Atiyah and Friedrich Hirzebruch proved a theorem relating the topological K-theory of a finite CW complex
X
{\displaystyle X}
with its rational cohomology. In particular, they showed that there exists a homomorphism
c
h
:
K
top
∗ ∗ -->
(
X
)
⊗ ⊗ -->
Q
→ → -->
H
∗ ∗ -->
(
X
;
Q
)
{\displaystyle ch:K_{\text{top}}^{*}(X)\otimes \mathbb {Q} \to H^{*}(X;\mathbb {Q} )}
such that
K
top
0
(
X
)
⊗ ⊗ -->
Q
≅ ≅ -->
⨁ ⨁ -->
k
H
2
k
(
X
;
Q
)
K
top
1
(
X
)
⊗ ⊗ -->
Q
≅ ≅ -->
⨁ ⨁ -->
k
H
2
k
+
1
(
X
;
Q
)
{\displaystyle {\begin{aligned}K_{\text{top}}^{0}(X)\otimes \mathbb {Q} &\cong \bigoplus _{k}H^{2k}(X;\mathbb {Q} )\\K_{\text{top}}^{1}(X)\otimes \mathbb {Q} &\cong \bigoplus _{k}H^{2k+1}(X;\mathbb {Q} )\end{aligned}}}
There is an algebraic analogue relating the Grothendieck group of coherent sheaves and the Chow ring of a smooth projective variety
X
{\displaystyle X}
.
See also
References
^ Hatcher. Vector Bundles and K-theory (PDF) . p. 57. Retrieved 27 July 2017 .
^ Adams, John (1960). On the non-existence of elements of Hopf invariant one . Ann. Math. 72 1.
^ Adams, John (1962). "Vector Fields on Spheres". Annals of Mathematics . 75 (3): 603–632.