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Cohomology

Algebraic structure used in topology

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In its general abstract formulation, cohomology is a sequence of abelian groups often defined from a cochain complex. Cohomology can be viewed as a method of assigning richer algebraic invariants to a space than homology. Some versions of cohomology arise by dualizing the construction of homology.

From its start in topology, this idea became a dominant method in the mathematics of the second half of the twentieth century. From the initial idea of homology as a method of constructing algebraic invariants of topological spaces, the range of applications of homology and cohomology theories has spread throughout geometry and algebra. The terminology tends to hide the fact that cohomology, a contravariant theory, is more natural than homology in many applications. At a basic level, this has to do with functions and pullbacks in geometric situations: given spaces X and Y, and some function F on Y, for any mapping f:X→Y, composition with F gives rise to a function F∘f on X. The most important cohomology theories have a product, the cup product, which gives them a ring structure. Because of this feature, cohomology is usually a stronger invariant than homology.

Overview

Cohomology is a family of related constructions that occur in several areas of mathematics. The common pattern is that one has objects called cochains, a coboundary operator measuring the failure of a cochain to satisfy a compatibility condition, and cohomology classes obtained by identifying cochains that differ by a trivial or exact contribution.

Example

A simple example is the de Rham cohomology of the circle. One considers here smooth functions on the circle, which can be thought of as periodic functions f:R→R, such that f(θ+2π)=f(θ) for all θ. (Here we are parametrizing the functions by radian measure around the unit circle.) The differential of a function f(θ) is defined by the expression df(θ)=f′(θ)dθ. Differentials of a periodic function have the property that their integral over a whole period is zero: by the fundamental theorem of calculus, ∫02πf′(θ)dθ=f(2π)−f(0)=0, because f is periodic over the circle. A differential df(θ) is sometimes called an exact differential.

Another type of differential can also be considered, which is not necessarily exact. An example is dθ by itself. This does not have an integral of zero over a whole period. On the contrary, ∫02πdθ=2π. So the differential dθ is inexact. Any differential form g(θ)dθ, with g(θ) appropriately periodic is a differential on the circle. It is inexact precisely when ∫02πg(θ)dθ≠0, and exact when ∫02πg(θ)dθ=0. Indeed, in the latter case we can write g(θ)=f′(θ) where f(θ)=∫0θg(t)dt, the key point being that f(θ) is periodic (and so defines a function on the circle). Moreover, any differential g(θ)dθ can be made exact by subtracting from it Cdθ where C=12π∫02πg(θ)dθ.

What we have therefore shown is that, although there are many differentials on the circle (exact or inexact), the quotient space of inexact differentials modulo exact differentials is one-dimensional, parametrized by the constant differential Cdθ.

Here the coboundaries are the exact differentials and the cochains are all differentials. The quotient of cochains modulo coboundaries is one-dimensional. That is, the first de Rham cohomology group of the circle is isomorphic to the real numbers R (as an additive group), H1(S1,R)≅R.

The circle, being one dimensional, has this one positive cohomology group. Its only other cohomology group H0(S1,R) consists of functions whose differential is zero, i.e., constants. Cohomology generalizes this basic setup to higher dimensions and other situations.

Cochains and coboundaries

Cohomology is often expressed by a cochain complex

C0→d0C1→d1C2→d2⋯

with dn+1dn=0. The n-th cohomology group is then

Hn(C∙)=ker⁡(dn)/im⁡(dn−1).

Elements of ker⁡(dn) are called cocycles, elements of im⁡(dn−1) are called coboundaries, and elements of the quotient group are called cohomology classes. In the case of the example of the de Rham cohomology of the circle, C0 is all smooth periodic functions, d0 is the differential of a function, C1 is all differentials g(θ)dθ where g is smooth and periodic, and all higher Ci and di are zero.

One informal way to understand cohomology is that cocycles are locally or formally consistent data, while coboundaries are data that arise from a more elementary choice. The cohomology group measures the part of the consistent data that cannot be removed in this way. Thus in the case of de Rham cohomology of the circle, a more elementary choice is a function, the formally consistent data is a periodic one-form which is always locally the differential of some function, and the integral of a one-form over the whole circle is the part that cannot be absorbed into the differential of a function. For this reason, cohomology often appears in questions about whether local data can be glued globally, whether a construction can be lifted or extended, or whether two objects that look locally equivalent are globally different. This interpretation is especially explicit in sheaf cohomology, where cohomology measures the failure of local sections of a sheaf to glue to global sections.

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