TheoremComplete

Chain Complexes and Homology - Applications

Homology theory provides powerful computational and theoretical tools with applications throughout algebra and topology.

Theorem1.4Euler-PoincarΓ© Formula

Let Cβˆ™C_\bullet be a chain complex of finite-dimensional vector spaces with finitely many non-zero terms. Then:

Ο‡(Cβˆ™)=βˆ‘n(βˆ’1)ndim⁑(Cn)=βˆ‘n(βˆ’1)ndim⁑(Hn(Cβˆ™))\chi(C_\bullet) = \sum_{n} (-1)^n \dim(C_n) = \sum_{n} (-1)^n \dim(H_n(C_\bullet))

where Ο‡(Cβˆ™)\chi(C_\bullet) is the Euler characteristic.

Proof

For each nn, the short exact sequence 0β†’Znβ†’Cnβ†’Bnβˆ’1β†’00 \to Z_n \to C_n \to B_{n-1} \to 0 gives: dim⁑(Cn)=dim⁑(Zn)+dim⁑(Bnβˆ’1)\dim(C_n) = \dim(Z_n) + \dim(B_{n-1})

Similarly, 0β†’Bnβ†’Znβ†’Hnβ†’00 \to B_n \to Z_n \to H_n \to 0 gives: dim⁑(Zn)=dim⁑(Bn)+dim⁑(Hn)\dim(Z_n) = \dim(B_n) + \dim(H_n)

Combining these and summing alternately: βˆ‘(βˆ’1)ndim⁑(Cn)=βˆ‘(βˆ’1)n(dim⁑(Bn)+dim⁑(Hn)+dim⁑(Bnβˆ’1))\sum (-1)^n \dim(C_n) = \sum (-1)^n (\dim(B_n) + \dim(H_n) + \dim(B_{n-1}))

The boundary terms telescope to zero, leaving βˆ‘(βˆ’1)ndim⁑(Hn)\sum (-1)^n \dim(H_n).

β– 
ExampleEuler Characteristic of Surfaces

For a closed orientable surface Ξ£g\Sigma_g of genus gg, the simplicial chain complex satisfies:

  • dim⁑(H0)=1\dim(H_0) = 1 (one connected component)
  • dim⁑(H1)=2g\dim(H_1) = 2g (fundamental group)
  • dim⁑(H2)=1\dim(H_2) = 1 (orientation)

The Euler characteristic is Ο‡(Ξ£g)=1βˆ’2g+1=2βˆ’2g\chi(\Sigma_g) = 1 - 2g + 1 = 2 - 2g.

Theorem1.5Universal Coefficient Theorem (Homology)

Let Cβˆ™C_\bullet be a chain complex of free abelian groups and GG any abelian group. Then there is a natural short exact sequence:

0β†’Hn(Cβˆ™)βŠ—Gβ†’Hn(Cβˆ™βŠ—G)β†’Tor1(Hnβˆ’1(Cβˆ™),G)β†’00 \to H_n(C_\bullet) \otimes G \to H_n(C_\bullet \otimes G) \to \text{Tor}_1(H_{n-1}(C_\bullet), G) \to 0

This sequence splits (non-naturally).

Remark

The Universal Coefficient Theorem relates homology with different coefficient groups. It shows that homology with coefficients in GG can be computed from homology with integer coefficients, up to a correction term involving the Tor functor.

ExampleHomology with Field Coefficients

When G=FG = \mathbb{F} is a field, Tor1(Hnβˆ’1(Cβˆ™),F)=0\text{Tor}_1(H_{n-1}(C_\bullet), \mathbb{F}) = 0 since fields are flat. Thus: Hn(Cβˆ™;F)β‰…Hn(Cβˆ™;Z)βŠ—FH_n(C_\bullet; \mathbb{F}) \cong H_n(C_\bullet; \mathbb{Z}) \otimes \mathbb{F}

This means homology with field coefficients simply tensorizes the integer homology with the field.

Theorem1.6KΓΌnneth Formula

Let Cβˆ™C_\bullet and Dβˆ™D_\bullet be chain complexes of free abelian groups. Then:

Hn(Cβˆ™βŠ—Dβˆ™)≅⨁p+q=n(Hp(Cβˆ™)βŠ—Hq(Dβˆ™))βŠ•β¨p+q=nβˆ’1Tor1(Hp(Cβˆ™),Hq(Dβˆ™))H_n(C_\bullet \otimes D_\bullet) \cong \bigoplus_{p+q=n} (H_p(C_\bullet) \otimes H_q(D_\bullet)) \oplus \bigoplus_{p+q=n-1} \text{Tor}_1(H_p(C_\bullet), H_q(D_\bullet))

Remark

The KΓΌnneth formula computes the homology of a tensor product of chain complexes from the homologies of the factors. It's essential for computing homology of product spaces.