Barratt–Priddy theorem

In homotopy theory, a branch of mathematics, the Barratt–Priddy theorem (also referred to as Barratt–Priddy–Quillen theorem) expresses a connection between the homology of the symmetric groups and mapping spaces of spheres. It is also often stated as a relation between the sphere spectrum and the classifying spaces of the symmetric groups via Quillen's plus construction.

Statement of the theorem

The mapping space Map0(Sn,Sn) is the topological space of all continuous maps f: SnSn from the n-dimensional sphere Sn to itself, under the topology of uniform convergence (a special case of the compact-open topology). These maps are required to fix a basepoint xSn, satisfying f(x)=x, and to have degree 0; this guarantees that the mapping space is connected. The Barratt–Priddy theorem expresses a relation between the homology of these mapping spaces and the homology of the symmetric groups Σn.

It follows from the Freudenthal suspension theorem and the Hurewicz theorem that the kth homology Hk(Map0(Sn,Sn)) of this mapping space is independent of the dimension n, as long as n>k. Similarly, Nakaoka (1960) proved that the kth group homology Hk(Σn) of the symmetric group Σn on n elements is independent of n, as long as n≥2k.

The Barratt–Priddy theorem states that these "stable homology groups" are the same: for n≥2k there is a natural isomorphism

H_k(\Sigma_n)\cong H_k(\text{Map}_0(S^n,S^n))

This isomorphism holds with integral coefficients (in fact with any coefficients, as is made clear in the reformulation below).

Example: first homology

This isomorphism can be seen explicitly for the first homology H1. The first homology of a group is the largest commutative quotient of that group. For the permutation groups Σn, the only commutative quotient is given by the sign of a permutation, taking values in {−1, 1}. This shows that H1(Σn)≅Z/2Z, the cyclic group of order 2, for all n≥2. (For n=1, Σ1 is the trivial group, so H1(Σn)=0.)

It follows from the theory of covering spaces that the mapping space Map0(S1,S1) of the circle S1 is contractible, so H1(Map0(S1,S1))=0. For the 2-sphere S2, the first homotopy group and first homology group of the mapping space are both infinite cyclic: π1(Map0(S2,S2))≅H1(Map0(S2,S2))≅Z. A generator for this group can be built from the Hopf fibration S3S2. Finally, once n≥3, both are cyclic of order 2: π1(Map0(Sn,Sn))≅H1(Map0(Sn,Sn))Z/2Z.

Reformulation of the theorem

The infinite symmetric group Σ is the union of the finite symmetric groups Σn, and Nakaoka's theorem implies that the group homology of Σ is the stable homology of Σn: for n≥2k, Hk(Σ)≅Hk(Σn). The classifying space of this group is denoted , and its homology of this space is the group homology of Σ: Hk()≅Hk(Σ).

We similarly denote by Map0(S,S) the union of the mapping spaces Map0(Sn,Sn) (under the inclusions induced by suspension). The homology of Map0(S,S) is the stable homology of the previous mapping spaces: for n>k, Hk(Map0(S,S))≅Hk(Map0(Sn,Sn)).

There is a natural map φ: →Map0(S,S) (one way to construct φ is via the model of as the space of finite subsets of R endowed with a certain topology). An equivalent formulation of the Barratt–Priddy theorem is that φ is a homology equivalence (or acyclic map), meaning that φ induces an isomorphism on all homology groups with any local coefficient system.

Relation with Quillen's plus construction

The Barratt–Priddy theorem implies that the space + resulting from applying Quillen's plus construction to can be identified with Map0(S,S). (Since π1(Map0(S,S))≅H1(Σ)≅Z/2Z, the map φ: →Map0(S,S) satisfies the universal property of the plus construction once it is known that φ is a homology equivalence.)

The mapping spaces Map0(Sn,Sn) are more commonly denoted by Ωn0Sn, where ΩnSn is the n-fold loop space of the n-sphere Sn, and similarly Map0(S,S) is denoted by Ω0S. Therefore the Barratt–Priddy theorem can also be stated as

B\Sigma_\infty^+\simeq \Omega_0^\infty S^\infty or
\textbf{Z}\times B\Sigma_\infty^+\simeq \Omega^\infty S^\infty

In particular, the homotopy groups of + are the stable homotopy groups of spheres:

\pi_i(B\Sigma_\infty^+)\cong \pi_i(\Omega^\infty S^\infty)\cong \lim_{n\rightarrow \infty} \pi_{n+i}(S^n)=\pi_i^s

"K-theory of F1"

The Barratt–Priddy theorem is sometimes colloquially rephrased as saying that "the K-groups of F1 are the stable homotopy groups of spheres". This is not a meaningful mathematical statement, but a metaphor expressing an analogy with algebraic K-theory.

The "field with one element" F1 is not a mathematical object; it refers to a collection of analogies between algebra and combinatorics. One central analogy is the idea that GLn(F1) should be the symmetric group Σn. The higher K-groups Ki(R) of a ring R can be defined as

K_i(R)=\pi_i(BGL_\infty(R)^+)

According to this analogy, the K-groups Ki(F1) of F1 should be defined as πi(BGL(F1)+)=πi(+), which by the Barratt–Priddy theorem is:

K_i(\mathbf{F}_1)=\pi_i(BGL_\infty(\mathbf{F}_1)^+)=\pi_i(B\Sigma_\infty^+)=\pi_i^s.

References

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