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Milnor's join model is a contractible free G-space

Statement

For a well-pointed topological group G of CW type, the diagonal action on Milnor's EG is free, EG is contractible, and

p:EGBG

is a numerable principal G-bundle. The numeration satisfies the library's support-subordinate convention, not merely cozero containment.

The embeddings

e(itigi)=itigi in slot 2i,o(itigi)=itigi in slot 2i+1

are G-equivariantly homotopic to the identity. If a,b:TEG are continuous equivariant maps, then (1t)e(a())+to(b()) is a continuous equivariant homotopy.

For G=S1 or G=Z/2, the selected compact-group topology identifies BG with the standard weak CW colimit of the finite projective quotients CPN or RPN, respectively.

Facts & Assumptions

[F1]

The finite quotient joins provide the set of formal sums. For compact Hausdorff G, EG has their ordinary weak direct-limit topology; otherwise it has the ordinary, un-kified coordinate-label strong topology. In both branches BG has the ordinary orbit-quotient topology and weights and positive-locus labels are continuous. Continuity into the strong branch is equivalent to continuity of those coordinates; continuity out of the weak branch is checked on its compact finite stages (Milnor's infinite-join model of EG).

[F2]

A locally finite family of nonnegative continuous functions has continuous sum (A locally finite family of continuous nonnegative functions has a continuous pointwise sum); finite maxima, sums, and division by a positive function are continuous by elementary real arithmetic.

[F3]

In the library's numerability convention, the closed support of each partition function must lie inside an assigned trivializing open set, and the chart uses an ordinary product (Locally trivial fiber bundle).

[F4]

For G=S1 and G=Z/2, the compact finite quotient joins are respectively spheres S2N+1 and SN, with quotient spaces CPN and RPN, compatibly with stage inclusions (Finite join models for the circle and the two-point group).

Proof

Given: G, EG, BG, and p as in the statement.

1.1

If xh=x and ti(x)>0, equality of join representatives gives gih=gi, hence h=1. Some coordinate is positive because the coordinates sum to one, so the action is free.

F1
1.2

We construct the promised contraction rather than infer contractibility from vanishing homotopy groups. Let In=[12n,12n1] and αn(s)=2n+1s2n+1+2. For sIn, define Rs(x) by retaining the coordinates 0,,n and, for every j1, replacing the term tn+jgn+j by

F1

αn(s)tn+jgn+j  in slot n+2j1,(1αn(s))tn+jgn+j  in slot n+2j.

At s=0 this is the even-coordinate embedding R0(tigi)=tigi with the ith term placed in slot 2i; at s=1 put R1=id. At the common endpoint of In and In+1, the first tail coordinate has reached slot n+1 and every later coordinate occupies the same slot in the two formulas. Thus the formulas agree. First consider the noncompact, strong-topology branch. Fix an output slot k. Only the finitely many intervals I0,,Ik1 can change its coordinate: for s12k that output coordinate and, where positive, its label are exactly the input kth coordinate and label. On each earlier interval its weight is a continuous product of αn(s) or 1αn(s) with one input weight, or is an unchanged input weight. Wherever that output weight is positive, its label is the corresponding continuous input label. At interval endpoints the two weight formulas and their positive labels agree, so finite pasting gives continuity of the kth weight and positive-label map on the ordinary product EG×I, including at s=1. The strong-coordinate criterion of [F1] proves R:EG×IEG continuous. It is G-equivariant because it moves weights and slots without changing labels. No compact image is assumed to lie in a finite stage; Step 4.1 checks ordinary continuity separately for the compact weak branch. [F1]

1.3

In the noncompact strong branch the diagonal action is continuous for ordinary EG×G: its ith weight is ti(x), and on the open locus ti(x)>0 its ith label is gi(x)h, continuous by ordinary group multiplication. The strong-coordinate criterion in [F1] proves continuity of the action. Put Ui={bBG:ti(b)>0} and Ei=p1(Ui). The sets Ui cover BG because some weight is positive, and each Ei is a saturated open subset of EG. The map Ni:EiEi, Ni(x)=xgi(x)1, is continuous by the ordinary action and inversion; Ni(xh)=Ni(x) and its ith label is 1. Restricting the ordinary quotient map p to the saturated open Ei is still a quotient map, so Ni descends to a continuous section si:UiEi. The maps

Ui×Gp1(Ui),(b,h)si(b)h,x(p(x),gi(x))

are continuous for the ordinary product and subspace topologies: the first is the composite of si×idG with the ordinary action, and the second is continuous by the ordinary product universal property and the partial-label continuity in [F1]. They are inverse because gi(si(b)h)=h and si(p(x))gi(x)=x. Thus they are precisely the ordinary principal-bundle charts required by [F3]. Step 3.1 supplies the same charts for the compact weak branch. [F1, F3]

1.4

The coordinate family need not be locally finite, so set

F1F2

wi=max(0,tij<itj).

At a point, its least positive coordinate has positive wi, so W=iwi is everywhere positive. If N is the last positive coordinate at b, then on a neighborhood where jNtj>1/2, every i>N satisfies ti<1/2<j<itj and hence wi=0. Thus (wi) is locally finite, W is continuous, and vi=wi/W is a locally finite partition with {vi>0}Ui. [F1, F2]

2.1

The even image uses no odd coordinate. Hence

F1step 1.2

Cu(itigi in slot 2i)=u1 in slot 1+i(1u)tigi in slot 2i

is a homotopy from the even embedding to the identity-labelled vertex in slot 1. In the noncompact strong branch, its slot-1 weight is u with label 1 where positive; its even-slot weights are (1u)ti with label gi where positive; every other weight is zero. These are continuous weights and positive-locus labels, so [F1] proves ordinary continuity of C. Reversing R and then applying C contracts that EG. Notice that C is not asserted equivariant. Splitting each even-coordinate weight as (1u)ti in slot 2i and uti in slot 2i+1, both carrying gi, likewise gives an ordinary-continuous G-equivariant homotopy from the even embedding to the odd embedding. Consequently both parity embeddings are G-equivariantly homotopic to the identity in this branch. For continuous equivariant a,b:TEG, the disjoint-support interpolation has even-slot weights (1u)ti(a(z)) and odd-slot weights uti(b(z)) on T×I. On each positive-weight locus its label is respectively gi(a(z)) or gi(b(z)), hence continuous there. The strong-coordinate criterion of [F1] proves the interpolation continuous for the ordinary product T×I; termwise it is equivariant. No compact-stage factorization is used in this branch; Step 4.1 treats the compact weak branch. [F1, step 1.2]

2.2

Cozero containment in Step 1.4 is weaker than [F3]. Choose εi=2i2, so iεi=1/2, and put ai=max(0,viεi). Some ai is positive at every point, since otherwise 1=ivi1/2. The family is locally finite, A=iai is positive and continuous, and ρi=ai/A is a partition of unity. Moreover

F2F3step 1.4

supp(ρi){viεi}Ui.

3.1

Now let G be any compact Hausdorff group, so [F1] selects the ordinary weak direct limit EG=colimNJNq. Each JNq is compact Hausdorff: the relation identifying labels at zero-weight slots is closed in (ΔN×GN+1)2, and appending zero gives a closed embedding. Hence this sequential compact-stage limit is a kω space. Its ordinary finite products with itself, G, and I have the final topology for the products of finite compact stages (Franklin--Thomas, property 4). On JMq×G, the diagonal action is the finite quotient of the continuous coordinate action and is continuous; the finite quotient map remains quotient after multiplying by compact G, since its source is compact and its target Hausdorff. The product-stage criterion therefore proves that EG×GEG is ordinary-continuous. The same ordinary action, continuous positive-locus labels, and saturated-open quotient argument of Step 1.3 give the explicit sections si and inverse ordinary charts Ui×Gp1(Ui) in this branch as well. Since each ti is stagewise continuous, Steps 1.4 and 2.2 give the same support-subordinate numeration.

F1F3step 1.3step 1.4step 2.2
4.1

Every required homotopy in the compact branch is likewise ordinary-continuous by the product-stage criterion, not by a claim that every compact image lies in a finite join. On JMq×I, the formula for R from Step 1.2 uses only the finitely many intervals before 12M and is then the identity; finite closed pasting into J2Mq proves continuity, including at s=1. The cone C and even-to-odd interpolation of Step 2.1 map JMq×I into a fixed finite join and are continuous finite quotient formulas. The disjoint-support interpolation on JMq×JNq×I is a continuous finite quotient formula into Jmax(2M,2N+1)q. Since ordinary products of these compact-stage limits have the stated final topology, all four maps are continuous on their full ordinary product domains. Composing the last one with arbitrary continuous equivariant a,b:TEG proves its asserted continuity on T×I; the formulas are G-equivariant where claimed. Reversing R and following it by C contracts EG. Finally, ordinary orbit quotients commute with this final topology: a set in BG is open exactly when its pullback to every JNq is open, equivalently when its intersection with every JNq/G is open. Thus [F4] identifies the selected BG for S1 or Z/2 literally with the standard weak CW colimit colimNCPN or colimNRPN.

F1F4step 1.2step 2.1step 3.1
5.1

Step 1.1 proves freeness in both branches. Steps 1.2, 1.3, and 2.1 prove ordinary continuity for the noncompact strong branch; Steps 3.1--4.1 prove it for the compact weak branch. The resulting ordinary charts and (ρi) satisfy the exact library numerability convention, and the contractions and parity homotopies establish every remaining assertion. The trivial and disconnected groups are included.

F1F2F3F4step 1.1step 1.2step 1.3step 1.4step 2.1step 2.2step 3.1step 4.1

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