Cellular homology is a powerful tool for calculating homology groups of spaces built from simple pieces. It simplifies computations by focusing on the structure of cell attachments, making it easier to understand complex topological spaces.
This approach connects to the broader applications of algebraic topology by providing a concrete method to analyze spaces. It bridges the gap between abstract concepts and practical calculations, showcasing how algebraic tools can reveal geometric properties.
CW Complexes and Cell Attachment
Construction and Properties of CW Complexes
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CW complexes are built by attaching cells of increasing dimension to a discrete set of points (0-cells)
Cells are attached via continuous maps from the boundary of an n-dimensional ball to the (n-1)-skeleton
The resulting space has the with respect to the cell decomposition
CW complexes are Hausdorff, second-countable, and locally contractible
The dimension of a is the highest dimension of its cells
Cell Attachment and Homotopy Type
is the process of building a CW complex by attaching cells of increasing dimension
The of a CW complex is determined by the homotopy classes of the attaching maps
Attaching an to an (n-1)-connected space results in an n-connected space
Two CW complexes are if they have the same homotopy type
Cell attachment can be used to construct spaces with desired homotopy properties (, )
Cellular Chain Complexes and Boundary Operators
Construction of Cellular Chain Complexes
The C∗(X) of a CW complex X is a sequence of abelian groups Cn(X) connected by boundary operators ∂n:Cn(X)→Cn−1(X)
Cn(X) is the free abelian group generated by the n-cells of X
The ∂n encodes the incidence relations between n-cells and (n-1)-cells
The composition of two consecutive boundary operators is always zero: ∂n−1∘∂n=0
The cellular chain complex is a chain complex, satisfying the property ∂∘∂=0
Properties of Cellular Boundary Operators
The cellular boundary operator ∂n measures the degree of the attaching map of each n-cell
The degree of an attaching map is the number of times the boundary of the n-cell wraps around the (n-1)-cell, with orientation taken into account
The boundary of a sum of cells is the sum of their boundaries: ∂(a+b)=∂(a)+∂(b)
The boundary operator satisfies the Leibniz rule: ∂(a⋅b)=∂(a)⋅b+(−1)deg(a)a⋅∂(b)
The cellular boundary operators completely determine the homology of the CW complex
Cellular Homology and Cohomology
Cellular Homology Groups and Their Properties
The Hn(X) of a CW complex X is the quotient group ker(∂n)/im(∂n+1)
Elements of Hn(X) are equivalence classes of n-cycles (elements of ker(∂n)) modulo n-boundaries (elements of im(∂n+1))
Cellular homology groups are topological invariants, independent of the cell decomposition
Cellular homology satisfies the for a
The dimension of Hn(X) as a vector space is the n-th βn(X), which counts the number of "n-dimensional holes" in X
Cellular Cohomology and the Universal Coefficient Theorem
The n-th Hn(X;G) of a CW complex X with coefficients in an abelian group G is the group of homomorphisms from Hn(X) to G
Cellular cohomology groups are related to cellular homology groups by the : Hn(X;G)≅Hom(Hn(X),G)⊕Ext(Hn−1(X),G)
The Universal Coefficient Theorem allows for the computation of cohomology groups from homology groups
Cellular cohomology satisfies the Eilenberg-Steenrod axioms for a cohomology theory
The cup product gives cellular cohomology the structure of a graded ring, with the product Hp(X;R)⊗Hq(X;R)→Hp+q(X;R) induced by the diagonal map X→X×X