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The first potentially nonzero homotopy group of a wedge of higher spheres has its cell basis

Statement

Let n2, let J be any set, and let W=jJSjn have its CW wedge topology and common basepoint b. Write ιj:SjnW for the inclusions and pj:WSjn for collapse of the other summands. Then πi(W,b)=0 for 0<i<n, and Φ:jJZπn(W,b),(aj)jaj[ιj] is an isomorphism. Its inverse sends a based sphere representative u to the finitely supported vector (deg(pju))jJ. The empty wedge is a point. All statements are choice-free.

Facts & Assumptions

[F1]

Cellular attachments with finite boundary support form a CW complex constructs the CW wedge from a point and supplied disks with constant boundaries. The explicit quotient homeomorphism in Cubical and spherical models of higher homotopy agree identifies a boundary-collapsed n-cube with the oriented based sphere and identifies its based classes and operations.

[F4]

High relative cells do not change lower homotopy gives homotopy isomorphisms below the first relative cell dimension minus one, and lower connectivity.

[F5]

Based sphere maps are classified by degree gives the choice-free degree isomorphism on each sphere, sending the identity to one. Higher homotopy classes form groups and are abelian above degree one makes πn abelian for n2.

[F6]

Compact CW images have finite cell support without choice gives finite cell support for every individual compact-domain representative or homotopy. Free abelian group on a set specifies the universal mapping property of a free abelian group; its finite-support model is verified below.

Proof

Given: n,J and the standard based copies of the oriented sphere in the statement. Use the fixed based cubical quotient homeomorphism of [F1] on each copy.

1.1

Attach one n-cell for each jJ to a single vertex b, by its constant boundary map. The boundary support is the singleton vertex, so [F1] proves this is a CW complex. On each closed cell it is the quotient sphere described by [F1]; its map-out test agrees with the ordinary wedge identification of these spheres when J is nonempty. When J is empty retain the initial point. Each pj is continuous: on its own characteristic cube it is the sphere quotient, and on every other characteristic cube it is constant, so the map-out test applies. The same test makes the inclusions continuous. Since every relative cell over {b} has dimension n, [F4] proves vanishing of πi(W,b) for 0<i<n and path-connectedness.

F1F4given
1.2

Define JZ concretely as the set of functions a:JZ for which {j:a(j)0} is finite. Pointwise addition and negation stay in this set, since a sum's support lies in the union of the two finite supports; they satisfy the abelian group laws coordinatewise. Let ej be one at j and zero elsewhere. Every a is the finite sum ja(j)ej. For any abelian group G and function v:JG, the formula aja(j)v(j) is well defined: finite sums may be reordered and zeros inserted by the abelian laws. Using the union of two supports proves additivity. It sends ej to v(j), and every homomorphism with these values must have this formula by the finite decomposition of a. Thus this model satisfies exactly the universal property in [F6], including empty J. No choice of an ordering for every finite subset is made; independence shows the value is uniquely specified.

F6givenalgebra
2.1

First suppose J is finite. Give P=jJSjn its ordinary product topology. It is Hausdorff: two distinct tuples differ in some coordinate, and disjoint sphere neighborhoods in that coordinate have disjoint inverse images. For each subset KJ, the points with precisely the coordinates of K outside their basepoints form a cell of dimension nK. Its characteristic map is the product of the fixed sphere quotient maps on the cube InK, with the other coordinates at their basepoints; it is continuous by [F2] and a homeomorphism on the cube interior onto that cell. Its boundary lies in the cells indexed by proper subsets of K, since at least one block is on its cube boundary. A cube is radially homeomorphic to a disk, preserving its boundary, so these are valid characteristic disks. There are finitely many cells.

F1F2step 1.1
3.1

These cells have the CW weak topology of the actual ordinary product. Each characteristic image is compact by [F3], hence closed in P. Its map from its compact disk is a closed surjection onto its image: a closed disk subset is compact, and its image is closed in the Hausdorff target. Thus it is quotient. If a subset of P has closed inverse image in every characteristic disk, its intersection with each characteristic image is closed there and hence closed in P. The finite union of these intersections is the whole subset, so it is closed in P. This proves the weak topology; closure finiteness is automatic for the finite cell family, and the boundary and interior conditions were proved in step 2.1. The union of the cells for K1 is the axes subcomplex, identified with W by its identical sphere characteristic maps and weak topology. Every other cell has dimension at least 2n. By [F4], the inclusion WP therefore induces an isomorphism on πn, since n<2n1 exactly when n>1. This proves the product-CW assertion needed here directly, without using any published example as a prerequisite.

F1F3F4step 2.1
4.1

The coordinate map πn(P,b)jJπn(Sjn,b) is an isomorphism. To see this, a based cube in P has continuous based coordinate cubes by [F2], and a homotopy projects to coordinate homotopies. Conversely, pair any finite list of coordinate representatives to get a continuous based product cube, and pair the finite coordinate homotopies to prove independence. The two constructions undo each other pointwise. They preserve the half-cube concatenation formulas in each coordinate, so the bijection is a homomorphism. Only finitely many representatives or homotopies have been selected. By [F5], degree identifies this finite product with ZJ. Under the inclusion from step 3.1, [ιj] has identity in coordinate j and constants in the others, hence the jth integer unit vector. A finite product of copies of Z is its finite direct sum, proving both formulas in the statement for finite J.

F2F5F6step 1.2step 3.1
5.1

For arbitrary J, the displayed map Φ is well defined: every input has finite support, and the finite sum is independent of its order because πn(W,b) is abelian by [F5]. Every based sphere representative can be pulled back to a based cube by [F1]. Its image is contained in a finite subcomplex by [F3, F6], necessarily a finite subwedge WJ0 of this particular CW structure (enlarge by b if necessary). The finite result in step 4.1 expresses its class as a finite sum of the corresponding inclusions. Therefore Φ is surjective. If a finite sum of these inclusions is null in W, represent that sum by finite concatenation of their cubes and take a based nullhomotopy. Its compact cube image lies in another finite subwedge by [F3, F6]. Enlarge its finite index set to include the support of the original sum. The sum is then null in that finite subwedge, where step 4.1 says all its coefficients are zero. Thus Φ is injective.

F1F3F5F6step 1.2step 4.1
6.1

For a representative u with image in WJ0 as in step 5.1, every pju with jJ0 is constant and has degree zero by [F5]. For jJ0, its degree is exactly the corresponding coefficient in the finite computation of step 4.1. Hence the vector of degrees is finitely supported and is the inverse to Φ. Degree is invariant under based homotopy by [F5], so this formula is independent of u. The empty index set gives the trivial group of a point and the zero direct sum. A one-element index set recovers the sphere degree theorem. The restriction n2 is essential in step 3.1's strict inequality and in the abelian sum; no analogous free-abelian assertion is made for wedges of circles. Zero coefficients, constant maps and degree zero are retained in steps 4.1–5.1. All infinite-index arguments use one compact image and its finite support, not a choice over all indices. This proves the claims without AC.

F1F5F6step 3.1step 4.1step 5.1

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