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An untwisted E2 table misses mapping-torus monodromy

Statement

For the mapping torus of a homeomorphism h:FF, the coefficient system bHq(Fb;R) over S1 has monodromy h. Hence the formal untwisted table Hp(S1;Hq(F;R)) can differ from the correct groups Hp(S1;Hq(F;R)h). For F=S1, R=Z, and a reflection h, the q=1 row changes from (Z,Z) in degrees (p=0,p=1) to (Z/2,0).

Facts & Assumptions

Given: A homeomorphism h:FF, its mapping-torus bundle FThS1, and in the explicit case a reflection of S1.

[F1]

Fiber transport and monodromy action identifies transport around the base loop with the gluing map up to fiber homotopy.

[F2]

Fiber transport gives the Serre local systems turns its induced homology maps into the coefficient local systems.

[F3]

Cellular chains compute local homology computes base homology from the lifted one-cell incidence and the specified monodromy.

Proof

technique · direct
1.1

Lift one positive circuit of the base interval in the mapping-torus model (F×[0,1])/(x,1)(h(x),0). Its endpoint identification on the fiber is h, so [F1] and [F2] give monodromy h on Hq(F;R). Therefore the correct base groups retain this local system rather than replacing it by a constant copy of its stalk.

F1F2
2.1

Let F=S1 and let h be a reflection. On H1(S1;Z)=Z, h=1. Give the base circle one vertex and one edge. Its lifted edge boundary evaluates through [F3] to T1:ZZ. For the correct monodromy T=1, this is multiplication by 2, so the q=1 row is H0(S1;Z1)=Z/2 and H1(S1;Z1)=0. If monodromy is discarded, T=1 makes the differential zero, giving H0=Z and H1=Z instead.

F3step 1.1
3.1

In the q=0 row the reflection acts trivially on H0(S1;Z), so the untwisted and correct rows agree there; the discrepancy is specifically caused by monodromy, not by the fiber groups. This comparison computes only the proposed coefficient rows and does not invoke or assert convergence of a Serre spectral sequence. No AC is used.

F2F3step 2.1

Depends on

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