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K-theory

Branch of mathematics

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K-theory involves the construction of families of K-functors that map from topological spaces or schemes, or to be even more general: any object of a homotopy category to associated rings; these rings reflect some aspects of the structure of the original spaces or schemes. As with functors to groups in algebraic topology, the reason for this functorial mapping is that it is easier to compute some topological properties from the mapped rings than from the original spaces or schemes. Examples of results gleaned from the K-theory approach include the Grothendieck–Riemann–Roch theorem, Bott periodicity, the Atiyah–Singer index theorem, and the Adams operations.

In high energy physics, K-theory and in particular twisted K-theory have appeared in Type II string theory where it has been conjectured that they classify D-branes, Ramond–Ramond field strengths and also certain spinors on generalized complex manifolds. In condensed matter physics K-theory has been used to classify topological insulators, superconductors and stable Fermi surfaces. For more details, see K-theory (physics).

Grothendieck completion

The Grothendieck completion of an abelian monoid into an abelian group is a necessary ingredient for defining K-theory since all definitions start by constructing an abelian monoid from a suitable category and turning it into an abelian group through this universal construction. Given an abelian monoid (A,+′) let ∼ be the relation on A2=A×A defined by

(a1,a2)∼(b1,b2)

if there exists a c∈A such that a1+′b2+′c=a2+′b1+′c. Then, the set G(A)=A2/∼ has the structure of a group (G(A),+) where:

[(a1,a2)]+[(b1,b2)]=[(a1+′b1,a2+′b2)].

Equivalence classes in this group should be thought of as formal differences of elements in the abelian monoid. This group (G(A),+) is also associated with a monoid homomorphism i:A→G(A) given by a↦[(a,0)], which has a certain universal property.

To get a better understanding of this group, consider some equivalence classes of the abelian monoid (A,+). Here we will denote the identity element of A by 0 so that [(0,0)] will be the identity element of (G(A),+). First, (0,0)∼(n,n) for any n∈A since we can set c=0 and apply the equation from the equivalence relation to get n=n. This implies

[(a,b)]+[(b,a)]=[(a+b,a+b)]=[(0,0)]

hence we have an additive inverse [(b,a)] for each [(a,b)]∈G(A). This should give us the hint that we should be thinking of the equivalence classes [(a,b)] as formal differences a−b. Another useful observation is the invariance of equivalence classes under scaling:

(a,b)∼(a+k,b+k) for any k∈A.

The Grothendieck completion can be viewed as a functor G:AbMon→AbGrp, and it has the property that it is left adjoint to the corresponding forgetful functor U:AbGrp→AbMon. That means that, given a morphism ϕ:A→U(B) of an abelian monoid A to the underlying abelian monoid of an abelian group B, there exists a unique abelian group morphism G(A)→B.

Example for natural numbers

An illustrative example to look at is the Grothendieck completion of N. We can see that G((N,+))=(Z,+). For any pair (a,b) we can find a minimal representative (a′,b′) by using the invariance under scaling. For example, we can see from the scaling invariance that

(4,6)∼(3,5)∼(2,4)∼(1,3)∼(0,2)

In general, if k:=min{a,b} then

(a,b)∼(a−k,b−k) which is of the form (c,0) or (0,d).

This shows that we should think of the (a,0) as positive integers and the (0,b) as negative integers.

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