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A free-face interval expansion has zero torsion

Statement

Starting from the one-vertex complex X={v}, attach a new vertex w and a 1-cell e running from v to w. The new vertex is a free face of the new 1-cell, so X↪Y is an elementary expansion. The relative universal-cover chains are 0→Z⟨e⟩→ 1 Z⟨w⟩→0, so that τ(X↪Y)=0 in Wh(1). The same computation over any group π produces the boundary unit ±g and the zero Whitehead class.

Facts & Assumptions

Given: The one-vertex complex X={v}, a new vertex w and a new 1-cell e attached from v to w, giving Y=X∪{w}∪e.

[F1]

An elementary expansion of dimension n is an inclusion X↪Y together with a homeomorphism Φ:(Dn,D+n−1)→(Qn,Qn−1) and a characteristic map φ:Qn→Y such that φ∣Qn−1 is a characteristic map for the new (n−1)-cell en−1, all other boundary values of φ lie in X, and Y=X∪en−1∪en; equivalently the new (n−1)-cell is a free face of the new n-cell, and the pair deformation retracts onto X (Elementary expansions and collapses of finite CW complexes, Cell attachment by a characteristic map).

[F2]

The relative cellular chains of a finite CW pair over the universal cover with chosen oriented lifts are finite free right Z[π1]-modules on the lifts of the relative cells, concentrated in the degrees in which relative cells occur, and the boundary is right group-ring linear (Based cellular chains of a universal cover as finite free right group-ring modules, Universal-cover boundaries, maps and homotopies respect the right group-ring action).

[F3]

If j:X↪Y is an elementary expansion of finite CW complexes, then τ(j)=0 in Wh(π1Y), componentwise, and the only nonzero relative cellular boundary of the pair in suitable oriented lifts is R→ ±g R in two consecutive degrees, with g∈π1Y and [±g]=0 in Wh(π1Y) (An elementary CW expansion has zero Whitehead torsion).

[F4]

τ of a homotopy equivalence of finite CW complexes is the image in the target Whitehead group of the contraction torsion of its algebraic mapping cone; K1 is written additively with [I]=0 and [A−1]=−[A], and K~1(R)=K1(R)/⟨[−1]⟩, so both [1] and [−1] vanish in K~1(R) (Whitehead torsion of a finite CW homotopy equivalence, K₁ of a ring and the Whitehead group of a discrete group).

[F5]

Every nonempty convex subset of Rn is contractible, a contractible space has trivial fundamental group at each basepoint, and the induced maps on all homotopy groups are functorial and invariant under based homotopies (Every nonempty convex subset of Rn is contractible, A contractible space has trivial fundamental group, Higher homotopy groups are functorial and based homotopy invariant).

Proof

technique · direct
1.1

Realize Y as the CW complex with vertex set {v,w} and the single 1-cell e attached by the map q:S0={−1,+1}→Y0 with q(−1)=v and q(+1)=w. With Q1=D1=[−1,1], Q0=D+0={+1} and φ the characteristic map of e, the restriction φ∣Q0 is a characteristic map for the new 0-cell w (mapping +1 homeomorphically onto w), the remaining boundary value φ(−1)=v lies in X, and Y=X∪{w}∪e. Hence X↪Y is an elementary expansion of dimension 1 by [F1], and the new vertex w is a free face of e.

F1
1.2

The pair (Y,X) deformation retracts onto X by [F1]; the retraction r:Y→X therefore satisfies r∘i=idX for the inclusion i:X={v}↪Y and i∘r≃idY. The one-point space X is a nonempty convex subset of R1, hence contractible with π1(X,v)=1 by [F5], and functoriality together with based-homotopy invariance of the induced maps gives i∗∘r∗=(i∘r)∗=id and r∗∘i∗=(r∘i)∗=id on π1, so i∗:π1(X,v)→π1(Y,v) is an isomorphism and π1(Y,v)=1; the edge e supplies a path from v to w, so basepoint change also gives π1(Y,w)=1.

F1F5
1.3

Over the universal cover the pair (Y,X) has exactly two relative cells, the lift of w in degree 0 and the lift of e in degree 1, so by [F2] the relative based chain complex T∙ is concentrated in degrees 0 and 1 with a single displayed basis vector in each degree and its differential has the 1×1 right-module matrix ±1: the characteristic map restricts to a homeomorphism on the free face, so the incidence of w in the boundary of the lift of e is ±1. This is the complex displayed in the statement, where the orientation is chosen so that the entry is 1.

F1F2
2.1

With the contraction s(e0)=e1 for the displayed differential d(e1)=e0, the odd-to-even map (d+s)odd:T1→T0 is d and has the 1×1 matrix (1). Thus τ(T∙)=[1]=0 in K~1(Z). Reversing either cell orientation changes the matrix to (−1), whose class is also 0 in the reduced group. The resulting image in Wh(1) vanishes.

F2F4step 1.3
2.2

By [F3] applied to the elementary expansion j:X↪Y of step 1.1, τ(X↪Y)=0 in Wh(π1Y)=Wh(1) by step 1.2; the relative boundary is the unit ±g of [F3] with g the group element determined by the chosen lifts, and [±g]=0 in Wh(π1Y) since here g=1.

F3step 1.1step 1.2
3.1

The identical computation applies to an elementary expansion performed on any finite CW complex: by [F3] the only nonzero relative cellular boundary of the pair is the unit ±g in two consecutive degrees and the class [±g] dies in Wh(π1Y), so the boundary unit ±g produces zero Whitehead class over any group π.

F3∎

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