Atiyah–Hirzebruch Spectral Sequence
   HOME

TheInfoList



OR:

In mathematics, the Atiyah–Hirzebruch spectral sequence is a spectral sequence for calculating generalized cohomology, introduced by in the special case of topological K-theory. For a
CW complex A CW complex (also called cellular complex or cell complex) is a kind of a topological space that is particularly important in algebraic topology. It was introduced by J. H. C. Whitehead (open access) to meet the needs of homotopy theory. This cla ...
X and a generalized cohomology theory E^\bullet, it relates the generalized cohomology groups : E^i(X) with 'ordinary' cohomology groups H^j with coefficients in the generalized cohomology of a point. More precisely, the E_2 term of the spectral sequence is H^p(X;E^q(pt)), and the spectral sequence converges conditionally to E^(X). Atiyah and Hirzebruch pointed out a generalization of their spectral sequence that also generalizes the Serre spectral sequence, and reduces to it in the case where E=H_. It can be derived from an exact couple that gives the E_1 page of the Serre spectral sequence, except with the ordinary cohomology groups replaced with E. In detail, assume X to be the total space of a Serre fibration with fibre F and base space B. The
filtration Filtration is a physical separation process that separates solid matter and fluid from a mixture using a ''filter medium'' that has a complex structure through which only the fluid can pass. Solid particles that cannot pass through the filte ...
of B by its n-skeletons B_n gives rise to a filtration of X. There is a corresponding spectral sequence with E_2 term :H^p(B; E^q(F)) and converging to the associated graded ring of the filtered ring :E_\infty^ = E^(X). This is the Atiyah–Hirzebruch spectral sequence in the case where the fibre F is a point.


Examples


Topological K-theory

For example, the complex topological K-theory of a point is :KU(*) = \mathbb ,x^/math> where x is in degree 2 By definition, the terms on the E_2-page of a finite CW-complex X look like :E_2^(X) = H^p(X;KU^q(pt)) Since the K-theory of a point is : K^q(pt) = \begin \mathbb & \text \\ 0 & \text \end we can always guarantee that :E_2^(X) = 0 This implies that the spectral sequence collapses on E_2 for many spaces. This can be checked on every \mathbb^n, algebraic curves, or spaces with non-zero cohomology in even degrees. Therefore, it collapses for all (complex) even dimensional smooth complete intersections in \mathbb^n.


Cotangent bundle on a circle

For example, consider the cotangent bundle of S^1. This is a fiber bundle with fiber \mathbb so the E_2-page reads as : \begin \vdots &\vdots & \vdots \\ 2 & H^0(S^1;\mathbb) & H^1(S^1;\mathbb) \\ 1 & 0 & 0 \\ 0 & H^0(S^1;\mathbb) & H^1(S^1;\mathbb) \\ -1 & 0 & 0 \\ -2 & H^0(S^1;\mathbb) & H^1(S^1;\mathbb) \\ \vdots &\vdots & \vdots \\ \hline & 0 & 1 \end


Differentials

The odd-dimensional differentials of the AHSS for complex topological K-theory can be readily computed. For d_3 it is the Steenrod square Sq^3 where we take it as the composition : \beta \circ Sq^2 \circ r where r is reduction mod 2 and \beta is the Bockstein homomorphism (connecting morphism) from the short exact sequence :0 \to \mathbb \to \mathbb \to \mathbb/2 \to 0


Complete intersection 3-fold

Consider a smooth complete intersection 3-fold X (such as a complete intersection Calabi-Yau 3-fold). If we look at the E_2-page of the spectral sequence : \begin \vdots & \vdots & \vdots & \vdots & \vdots & \vdots & \vdots & \vdots \\ 2 & H^0(X; \mathbb) & 0 & H^2(X;\mathbb) & H^3(X;\mathbb) & H^4(X;\mathbb) & 0 & H^6(X;\mathbb) \\ 1 & 0 & 0 & 0 & 0 & 0 & 0 & 0 \\ 0 & H^0(X; \mathbb) & 0 & H^2(X;\mathbb) & H^3(X;\mathbb) & H^4(X;\mathbb) & 0 & H^6(X;\mathbb)\\ -1 & 0 & 0 & 0 & 0 & 0 & 0 & 0 \\ -2 & H^0(X; \mathbb) & 0 & H^2(X;\mathbb) & H^3(X;\mathbb) & H^4(X;\mathbb) & 0 & H^6(X;\mathbb)\\ \vdots & \vdots & \vdots & \vdots & \vdots & \vdots & \vdots & \vdots \\ \hline & 0 & 1 & 2 & 3 & 4 & 5 & 6 \end we can see immediately that the only potentially non-trivial differentials are : \begin d_3:E_3^ \to E_3^ \\ d_3:E_3^ \to E_3^ \end It turns out that these differentials vanish in both cases, hence E_2 = E_\infty. In the first case, since Sq^k:H^i(X;\mathbb/2) \to H^(X;\mathbb/2) is trivial for k > i we have the first set of differentials are zero. The second set are trivial because Sq^2 sends H^3(X;\mathbb/2) \to H^5(X) = 0 the identification Sq^3 = \beta \circ Sq^2 \circ r shows the differential is trivial.


Twisted K-theory

The Atiyah–Hirzebruch spectral sequence can be used to compute twisted K-theory groups as well. In short, twisted K-theory is the group completion of the isomorphism classes of vector bundles defined by gluing data (U_,g_) where : g_g_g_ = \lambda_ for some cohomology class \lambda \in H^3(X,\mathbb). Then, the spectral sequence reads as : E_2^ = H^p(X;KU^q(*)) \Rightarrow KU^_\lambda(X) but with different differentials. For example, : E_3^ = E_2^ = \begin \vdots & \vdots & \vdots & \vdots & \vdots \\ 2 & H^0(S^3;\mathbb) & 0 & 0 & H^3(S^3;\mathbb) \\ 1 & 0 & 0 & 0 & 0 \\ 0 & H^0(S^3;\mathbb) & 0 & 0 & H^3(S^3;\mathbb) \\ -1 & 0 & 0 & 0 & 0 \\ -2 & H^0(S^3;\mathbb) & 0 & 0 & H^3(S^3;\mathbb) \\ \vdots & \vdots & \vdots & \vdots & \vdots \\ \hline& 0 & 1 & 2 & 3 \end On the E_3-page the differential is : d_3 = Sq^3 + \lambda Higher odd-dimensional differentials d_ are given by Massey products for twisted K-theory tensored by \mathbb. So : \begin d_5 &= \ \\ d_7 &= \ \end Note that if the underlying space is
formal Formal, formality, informal or informality imply the complying with, or not complying with, some set of requirements (forms, in Ancient Greek). They may refer to: Dress code and events * Formal wear, attire for formal events * Semi-formal attire ...
, meaning its rational homotopy type is determined by its rational cohomology, hence has vanishing Massey products, then the odd-dimensional differentials are zero. Pierre Deligne,
Phillip Griffiths Phillip Augustus Griffiths IV (born October 18, 1938) is an American mathematician, known for his work in the field of geometry, and in particular for the complex manifold approach to algebraic geometry. He was a major developer in particula ...
, John Morgan, and Dennis Sullivan proved this for all compact Kähler manifolds, hence E_\infty = E_4 in this case. In particular, this includes all smooth projective varieties.


Twisted K-theory of 3-sphere

The twisted K-theory for S^3 can be readily computed. First of all, since Sq^3 = \beta \circ Sq^2 \circ r and H^2(S^3) = 0, we have that the differential on the E_3-page is just cupping with the class given by \lambda. This gives the computation : KU_\lambda^k = \begin \mathbb & k \text \\ \mathbb/\lambda & k \text \end


Rational bordism

Recall that the rational bordism group \Omega_*^\otimes \mathbb is isomorphic to the ring : \mathbb \mathbb^0 mathbb^2 mathbb^4 mathbb^6\ldots] generated by the bordism classes of the (complex) even dimensional projective spaces mathbb^/math> in degree 4k. This gives a computationally tractable spectral sequence for computing the rational bordism groups.


Complex cobordism

Recall that MU^*(pt) = \mathbb _1,x_2,\ldots/math> where x_i \in \pi_(MU). Then, we can use this to compute the complex cobordism of a space X via the spectral sequence. We have the E_2-page given by :E_2^ = H^p(X;MU^q(pt))


See also

*
Quillen–Lichtenbaum conjecture In mathematics, the Quillen–Lichtenbaum conjecture is a conjecture relating étale cohomology to algebraic K-theory introduced by , who was inspired by earlier conjectures of . and proved the Quillen–Lichtenbaum conjecture at the prime 2 for s ...


References

* * * {{DEFAULTSORT:Atiyah-Hirzebruch spectral sequence Spectral sequences K-theory