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Geometric cancellation is a unit entry in the handle matrix

Statement

Assume ACω. In the situation of the matrix definition, suppose the attaching sphere Ai of the (k+1)-handle gi meets the belt sphere Bj of the k-handle ej transversely in exactly one point. Then the oriented entry is Mij=±1, equal to the local intersection sign of that point; in particular a geometrically cancelling pair has a unit entry in Z. Without orientations the mod-2 entry is 1∈Z2, also a unit.

Facts & Assumptions

Given: An index-ordered presentation with 1≤k≤n−2 and transverse attaching and belt spheres, a (k+1)-handle gi whose attaching sphere Ai meets the belt sphere Bj of the k-handle ej transversely in exactly one point.

[F1]

Attaching-belt intersection matrix of adjacent-index handles: the entry Mij is the oriented intersection number I(Ai,Bj) when the spheres carry the orientations induced by the framings and the boundary orientation, and the mod-2 number I2(Ai,Bj) otherwise.

[F2]

The oriented intersection number and The local oriented intersection sign: for transverse complementary-dimensional submanifolds the oriented intersection number is the finite sum ∑p∈A∩Bε(p) of local signs, each of which lies in {+1,−1}; the empty intersection contributes 0.

[F3]

The mod 2 intersection number and The oriented intersection number reduces to the mod 2 number: the mod-2 intersection number is #(A∩B) mod 2, and in the common oriented setting it is the reduction modulo two of the oriented number.

[F4]

The Axiom of Countable Choice (ACω): ACω is assumed, as in the matrix definition; the single-entry computation below is choice-free.

Proof

technique · direct
1.1F1F2F4given

By [F1] the entry is the oriented intersection number of Ai and Bj in the middle boundary. By hypothesis the transverse intersection is exactly one point P, so by [F2] the finite sum has the single term ε(P), and ε(P)∈{+1,−1} by definition of the local sign. Hence Mij=ε(P)=±1, a unit of Z. No other entry is involved.

2.1F3step 1.1

For the mod-2 version, [F3] gives I2(Ai,Bj)=#(Ai∩Bj) mod 2=1 mod 2=1∈Z2, a unit of Z2; and in the oriented setting this agrees with the reduction of the oriented entry by [F3].

3.1step 1.1step 2.1given∎

Therefore a geometrically cancelling pair — one transverse intersection point of the attaching sphere with the belt sphere — has a unit entry in the attaching-belt intersection matrix, over Z with value the local sign of that point and over Z2 with value 1.

Depends on

Used by

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Sources