Chain complex

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In mathematics, a chain complex is a construct originally used in the field of algebraic topology. It is an algebraic means of representing the relationships between the cycles and boundaries in various dimensions of some "space". Here the "space" could be a topological space or an algebraic construction such as a simplicial complex. More generally, homological algebra includes the study of chain complexes in the abstract, without any reference to an underlying space. In this case, chain complexes are studied axiomatically as algebraic structures.

Applications of chain complexes usually define and apply their homology groups (cohomology groups for cochain complexes); in more abstract settings various equivalence relations are applied to complexes (for example starting with the chain homotopy idea). Chain complexes are easily defined in abelian categories, also.

1 Formal definition
2 Fundamental terminology
3 Examples
- 3.1 Singular homology
- 3.2 de Rham cohomology
4 Chain maps
5 Chain homotopy
6 See also
7 References

A chain complex $(A_\bullet, d_\bullet)$ is a sequence of abelian groups or modules ... A_-2, A_-1, A₀, A₁, A₂, ... connected by homomorphisms (called boundary operators) d_n : A_n→A_n−1, such that the composition of any two consecutive maps is zero: d_n o d_n+1 = 0 for all n. They are usually written out as:

$\cdots \to A_{n+1} \begin{matrix} d_{n+1} \\ \to \\ \, \end{matrix} A_n \begin{matrix} d_n \\ \to \\ \, \end{matrix} A_{n-1} \begin{matrix} d_{n-1} \\ \to \\ \, \end{matrix} A_{n-2} \to \cdots \to A_2 \begin{matrix} d_2 \\ \to \\ \, \end{matrix} A_1 \begin{matrix} d_1 \\ \to \\ \, \end{matrix} A_0 \begin{matrix} d_0 \\ \to \\ \, \end{matrix} A_{-1} \begin{matrix} d_{-1} \\ \to \\ \, \end{matrix} A_{-2} \begin{matrix} d_{-2} \\ \to \\ \, \end{matrix} \cdots$

A variant on the concept of chain complex is that of cochain complex. A cochain complex $(A^\bullet, d^\bullet)$ is a sequence of abelian groups or modules A_-2, A_-1, A₀, A₁, A₂, ... connected by homomorphisms d_n : A_n→A_n+1, such that the composition of any two consecutive maps is zero: d_n+1 o d_n = 0 for all n:

$\cdots \to A_{-2} \begin{matrix} d_{-2} \\ \to \\ \, \end{matrix} A_{-1} \begin{matrix} d_{-1} \\ \to \\ \, \end{matrix} A_0 \begin{matrix} d_0 \\ \to \\ \, \end{matrix} A_1 \begin{matrix} d_1 \\ \to \\ \, \end{matrix} A_2 \to \cdots \to A_{n-1} \begin{matrix} d_{n-1} \\ \to \\ \, \end{matrix} A_n \begin{matrix} d_n \\ \to \\ \, \end{matrix} A_{n+1} \to \cdots.$

The idea is basically the same. In either case, the index i in A_i is referred to as the degree.

A bounded chain complex is one in which almost all the A_i are 0; i.e., a finite complex extended to the left and right by 0's. An example is the complex defining the homology theory of a (finite) simplicial complex. A chain complex is bounded above if all degrees above some fixed degree N are 0, and is bounded below if all degrees below some fixed degree are 0. Clearly, a complex is bounded above and below iff the complex is bounded.

Leaving out the indices, the basic relation on d can be thought of as

d² = 0.

The elements of the individual groups of a chain complex are called chains (or cochains in the case of a cochain complex.) The image of d is the group of boundaries, or in a cochain complex, coboundaries. The kernel of d (i.e., the subgroup sent to 0 by d) is the group of cycles, or in the case of a cochain complex, cocycles. From the basic relation, the (co)boundaries lie inside the (co)cycles. This phenomenon is studied in a systematic way using (co)homology groups.

Suppose we are given a topological space X.

Define C_n(X) for natural n to be the free abelian group formally generated by singular n-simplices in X, and define the boundary map

$\partial_n: C_n(X) \to C_{n-1}(X): \, (\sigma: [v_0,\ldots,v_n] \to X) \mapsto (\partial_n \sigma = \sum_{i=0}^n (-1)^i \sigma|[v_0,\ldots, \hat v_i, \ldots, v_n]),$

where the hat denotes the omission of a vertex. That is, the boundary of a singular simplex is alternating sum of restrictions to its faces. It can be shown ∂² = 0, so $(C_\bullet, \partial_\bullet)$ is a chain complex; the singular homology $H_\bullet(X)$ is the homology of this complex; that is,

$H_n(X) = \ker \partial_n / \mbox{im } \partial_{n+1}.$

The differential k-forms on any smooth manifold M form an abelian group (in fact an R-vector space) called Ω^k(M) under addition. The exterior derivative d_k maps Ω^k(M) to Ω^k+1(M), and d ² = 0 follows essentially from symmetry of second derivatives, so the vector spaces of k-forms along with the exterior derivative are a cochain complex:

$\Omega^0(M)\ \stackrel{d_0}{\to}\ \Omega^1(M) \to \Omega^2(M) \to \Omega^3(M) \to \cdots.$

The homology of this complex is the de Rham cohomology

$H^0_{\mathrm{DR}}(M, F) = \ker d_0 =$ {locally constant functions on M with values in F} $\cong F$ ^{#{connected pieces of M}}

$H^k_{\mathrm{DR}}(M) = \ker d_k / \mathrm{im} \, d_{k-1}.$

A chain map f between two chain complexes $(A_\bullet, d_{A,\bullet})$ and $(B_\bullet, d_{B,\bullet})$ is a collection of maps $f_n : A_n \rightarrow B_n$ for each n that intertwines with the differentials on the two chain complexes: $f_n \circ d_{A,n}= d_{B,n} \circ f_{n+1}$ . Such a map sends cycles to cycles and boundaries to boundaries, and thus descends to a map on homology: $(f_n)_*:H_\bullet(A_\bullet, d_{A,\bullet}) \rightarrow H_\bullet(B_\bullet, d_{B,\bullet})$ .

A continuous map of topological spaces induces chain maps in both the singular and de Rham chain complexes described above (and in general for the chain complex defining any homology theory of topological spaces) and thus a continuous map induces a map on homology. Because the map induced on a composition of maps is the composition of the induced maps, these homology theories are functors from the category of topological spaces with continuous maps to the category of abelian groups with group homomorphisms.

Chain homotopies give an important equivalence relation between chain maps. Chain homotopic chain maps induce the same maps on homology groups. A particular case is that homotopic maps between two spaces X and Y induce the same maps from homology of X to homology of Y. Chain homotopies have a geometric interpretation; it is described, for example, in the book of Bott and Tu. See Homotopy category of chain complexes for further information.

Raoul Bott and Loring Tu, Differential Forms in Algebraic Topology. Springer-Verlag, 1982.

Retrieved from "http://en.wikipedia.org/wiki/Chain_complex"

Category: Homological algebra

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