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Morse homology recovers the Morse inequalities

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let M be a closed manifold, let (f,X) be Morse--Smale on M, write ck=#Crit⁡k(f) (Nondegenerate critical points, nullity, index, and coindex, A Morse function on a compact manifold has finitely many critical points) and put bk=dim⁡ΛHk(M;Λ) for a field Λ (Morse homology is naturally isomorphic to singular homology, Cellular homology). Then:

  1. ck≥bk for every k;
  2. ∑i=0k(−1)k−ici≥∑i=0k(−1)k−ibi for every k;
  3. with c(t)=∑kcktk, b(t)=∑kbktk and rk=rank⁡Λ∂k the rank of the Morse differential, c(t)=b(t)+(1+t)Q(t) where Q(t)=∑krk+1tk has nonnegative integer coefficients (The mod-two Morse chain group, The signed Morse differential over the integers, Morse homology of a Morse--Smale pair);
  4. ∑k(−1)kck=χ(M)=∑k(−1)kbk (Euler characteristic of a finite CW complex, Euler–Poincare formula for finite CW complexes, Compactified unstable manifolds give the Morse--Smale CW decomposition).

Over Z the same identities hold with bk replaced by the rank of the finitely generated group Hk(M;Z).

Facts & Assumptions

Given: The Axiom of Choice, a closed manifold M, a Morse--Smale pair (f,X), and a field Λ (or Λ=Z).

[F1]

For a field Λ, take the finite free complex on the critical points whose differential is the integral signed trajectory matrix with its entries mapped from Z to Λ. The coefficient comparison identifies it, after the index sign normalization, with the cellular complex with constant coefficients Λ (Cellular boundary coefficients are the signed trajectory counts). The constant-local-system cellular theorem computes H∗(M;Λ) (Cellular chains compute local homology, Homology and cohomology with local coefficients). Thus its chain ranks are ck, its homology dimensions are bk, and its differential ranks rk are nonnegative integers. Over Z the same identification uses the integral Morse complex (The signed Morse differential over the integers, Morse homology of a Morse--Smale pair) and identifies its homology with H∗(M;Z).

[F2]

Rank-nullity for a finite-dimensional linear map gives dim⁡ker⁡∂k=ck−rk; the homology in degree k is ker⁡∂k/im⁡∂k+1, so bk=ck−rk−rk+1; this pure linear algebra uses only the finite dimensions supplied by [F1].

[F3]

The Morse--Smale CW decomposition has exactly ck cells in dimension k, and the Euler--Poincar'e formula identifies the alternating sum of the cell counts with the Euler characteristic and with the alternating sum of the homology ranks (Compactified unstable manifolds give the Morse--Smale CW decomposition, Euler characteristic of a finite CW complex, Euler–Poincare formula for finite CW complexes).

Verification

technique · direct
1.1F1F2givenalgebra

By [F1] the numbers ck, bk and rk are well-defined nonnegative integers; by rank-nullity as recorded in [F2], ck−rk=dim⁡ker⁡∂k=bk+rk+1, hence ck=bk+rk+rk+1 for every k, which immediately gives ck≥bk; this is (1).

2.1step 1.1algebra

Multiplying ci=bi+ri+ri+1 by (−1)k−i and summing over 0≤i≤k, the coefficients of r1,…,rk cancel in pairs and only the r0- and rk+1-terms survive, giving ∑i=0k(−1)k−ici=∑i=0k(−1)k−ibi+(−1)kr0+rk+1; since r0=0 and rk+1≥0, the last term is nonnegative, which gives (2).

2.2step 1.1algebra

Substituting ck=bk+rk+rk+1 into the generating series and using ∑krktk=tQ(t) and ∑krk+1tk=Q(t) gives the polynomial identity c(t)=b(t)+(1+t)Q(t) with Q(t)=∑krk+1tk≥0 coefficientwise; this is (3).

2.3F3step 1.1

By [F3] the alternating sum ∑k(−1)kck is the Euler characteristic of the CW complex with ck cells in dimension k, hence equals χ(M), and the Euler--Poincar'e formula also gives χ(M)=∑k(−1)kbk; this is (4).

3.1F1step 2.2∎

Over Z the chain groups are free of finite rank and rank-nullity for finitely generated abelian groups gives the same identities with bk the rank of Hk(M;Z); the identification rank⁡HMk=rank⁡Hk(M;Z) is the comparison theorem of [F1], so (1)--(4) hold verbatim.

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