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Twisted K-theory : ウィキペディア英語版
Twisted K-theory
In mathematics, twisted K-theory (also called K-theory with local coefficients) is a variation on K-theory, a mathematical theory from the 1950s that spans algebraic topology, abstract algebra and operator theory.
More specifically, twisted K-theory with twist ''H'' is a particular variant of K-theory, in which the twist is given by an integral 3-dimensional cohomology class. It is special among the various twists that K-theory admits for two reasons. First, it admits a geometric formulation. This was provided in two steps; the first one was done in 1970 (Publ. Math. de l'IHÉS) by Peter Donovan and Max Karoubi (); the second one in 1988 by Jonathan Rosenberg in (Continuous-Trace Algebras from the Bundle Theoretic Point of View ).
In physics, it has been conjectured to classify D-branes, Ramond-Ramond field strengths and in some cases even spinors in type II string theory. For more information on twisted K-theory in string theory, see K-theory (physics).
In the broader context of K-theory, in each subject it has numerous isomorphic formulations and, in many cases, isomorphisms relating definitions in various subjects have been proven. It also has numerous deformations, for example, in abstract algebra K-theory may be twisted by any integral cohomology class.
==The definition==
To motivate Rosenberg's geometric formulation of twisted K-theory, start from the Atiyah-Jänich theorem, stating that
:Fred(\mathcal H),
the Fredholm operators on Hilbert space \mathcal H, is a classifying space for ordinary, untwisted K-theory. This means that the K-theory of the space ''M'' consists of the homotopy classes of maps
:(Fred(\mathcal H) )
from ''M'' to Fred(\mathcal H).
A slightly more complicated way of saying the same thing is as follows. Consider the trivial bundle of Fred(\mathcal H) over M, that is, the Cartesian product of M and Fred(\mathcal H). Then the K-theory of M consists of the homotopy classes of sections of this bundle.
We can make this yet more complicated by introducing a trivial
:PU(\mathcal H)
bundle P over M, where PU(\mathcal H) is the group of projective unitary operators on the Hilbert space \mathcal H. Then the group of maps
:(Fred(\mathcal H) )_
from P to Fred(\mathcal H) which are equivariant under an action of PU(\mathcal H) is equivalent to the original groups of maps
:(Fred(\mathcal H) ).
This more complicated construction of ordinary K-theory is naturally generalized to the twisted case. To see this, note that PU(\mathcal H) bundles on M are classified by elements H of the third integral cohomology group of M. This is a consequence of the fact that PU(\mathcal H) topologically is a representative Eilenberg-MacLane space
:K(\mathbf Z,2).
The generalization is then straightforward. Rosenberg has defined
:''K''''H''(''M''),
the twisted K-theory of M with twist given by the 3-class H, to be the space of homotopy classes of sections of the trivial Fred(\mathcal H) bundle over M that are covariant with respect to a PU(\mathcal H) bundle P_H fibered over M with 3-class H, that is
:K_H(M)=(Fred(\mathcal H) )_.
Equivalently, it is the space of homotopy classes of sections of the Fred(\mathcal H) bundles associated to a PU(\mathcal H) bundle with class H.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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