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In , the Pontryagin classes, named after , are certain characteristic classes of real vector bundles. The Pontryagin classes lie in with degrees a multiple of four.


Definition
Given a real vector bundle E over M, its k-th Pontryagin class p_k(E) is defined asLawson & Michelson 90, Equation (B.12)
p_k(E) = p_k(E, \Z) = (-1)^k c_{2k}(E\otimes \Complex) \in H^{4k}(M, \Z),
where:

The rational Pontryagin class p_k(E, \Q) is defined to be the image of p_k(E) in H^{4k}(M, \Q), the 4k-cohomology group of M with coefficients.


Properties
The total Pontryagin class
p(E)=1+p_1(E)+p_2(E)+\cdots\in H^*(M,\Z),
is (modulo 2-torsion) multiplicative with respect to Whitney sum of vector bundles, i.e.,Lawson & Michelson 90, Equation (B.10)
2p(E\oplus F)=2p(E)\smile p(F)
for two vector bundles E and F over M. In terms of the individual Pontryagin classes p_k,
2p_1(E\oplus F)=2p_1(E)+2p_1(F),
2p_2(E\oplus F)=2p_2(E)+2p_1(E)\smile p_1(F)+2p_2(F)
and so on.

The vanishing of the Pontryagin classes and Stiefel–Whitney classes of a vector bundle does not guarantee that the vector bundle is trivial. For example, up to vector bundle isomorphism, there is a unique nontrivial rank 10 vector bundle E_{10} over the . (The clutching function for E_{10} arises from the homotopy group \pi_8(\mathrm{O}(10)) = \Z/2\Z.) The Pontryagin classes and Stiefel-Whitney classes all vanish: the Pontryagin classes don't exist in degree 9, and the Stiefel–Whitney class w_9 of E_{10} vanishes by the Wu formula w_9 = w_1 w_8 + Sq^1(w_8). Moreover, this vector bundle is stably nontrivial, i.e. the Whitney sum of E_{10} with any trivial bundle remains nontrivial.

Given a 2 k-dimensional vector bundle E we have

p_k(E)=e(E)\smile e(E),
where e(E) denotes the of E, and \smile denotes the of cohomology classes.


Pontryagin classes and curvature
As was shown by Shiing-Shen Chern and André Weil around 1948, the rational Pontryagin classes
p_k(E,\mathbf{Q})\in H^{4k}(M,\mathbf{Q})
can be presented as differential forms which depend polynomially on the of a vector bundle. This Chern–Weil theory revealed a major connection between algebraic topology and global differential geometry.

For a E over a n-dimensional differentiable manifold M equipped with a , the total Pontryagin class is expressed as

p=\left[1-\frac

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