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Schwede Global Equivariant K-theory

Updated 17 November 2025
  • Schwede Global Equivariant K-theory is a framework that generalizes algebraic K-theory to incorporate finite group actions, incomplete universes, and transfer systems.
  • It employs equivariant Γ_G-spaces and Segal maps alongside bar constructions to assemble I-special data into connective equivariant spectra.
  • The approach unifies classical nonequivariant K-theory and Shimakawa models by leveraging normed permutative G-categories and group-completion techniques.

Schwede Global Equivariant K-theory is a homotopical framework generalizing algebraic K-theory to capture equivariant structure relative to a finite group GG, incomplete universes, and associated transfer systems. Central to this approach are Segal-type models for equivariant infinite loop spaces, generalizations of Γ\Gamma-spaces, and normed permutative GG-categories. This formulation unifies and extends the classical nonequivariant Segal KK-theory construction and the Shimakawa model for genuine equivariant infinite loop spaces, with applications to equivariant KK-theory of normed categories and the associated spectra (Bantelmann, 28 Oct 2025).

1. The Category ΓG\Gamma_G of Finite Based GG-Sets

The foundational indexing category in Schwede Global Equivariant K-theory is the category ΓG\Gamma_G of finite based GG-sets, as introduced by Shimakawa. Its structure is as follows:

Aspect Description Mathematical Representation
Objects Finite based GG-sets T+=T{}T_+ = T \sqcup \{*\}, TT: finite GG-set
Morphisms Based GG-maps fixing the basepoint {ϕ:T+S+ϕ()=,ϕ(gt)=gϕ(t)}\{\phi : T_+ \to S_+ \mid \phi(*) = *,\, \phi(g\cdot t) = g\cdot\phi(t)\}
Enrichment Full $G\Top_*$-enriched subcategory Objects: T+T_+; Morphisms: Based GG-maps

The category's morphisms and composition laws are inherited from the category of based GG-spaces, encoding simultaneous GG-actions and basepoint structure. This categorical enrichment is essential for modeling equivariant infinite loop spaces indexed on incomplete universes.

2. Equivariant ΓG\Gamma_G-Spaces and the Segal Condition

An equivariant ΓG\Gamma_G-space is a $G\Top_*$-enriched functor $X: \Gamma_G \to G\Top_*$, which assigns to each T+T_+ a based GG-space X(T+)X(T_+), and to each based GG-map ϕ\phi an equivariant map X(ϕ)X(\phi). For every injection ϕ:T+S+\phi: T_+\hookrightarrow S_+, the map X(ϕ)X(\phi) is required to be a (G×Σϕ)(G \times \Sigma_\phi)-cofibration, ensuring cofibrancy of the bar constructions required in later stages.

Segal maps are pivotal to encoding the "multiplicativity" of the structure. Given disjoint finite GG-sets SS and TT, the fold map induces

φS,T:X((ST)+)X(S+)X(T+),\varphi_{S,T}: X\bigl((S \sqcup T)_+\bigr) \longrightarrow X(S_+)\wedge X(T_+),

mirroring classical Segal's theory. The classical Segal maps correspond to families of coordinate projections,

δn:X(n+)X(1+)n,δn(x)=(X(δ1)x,,X(δn)x),\delta_n: X(n_+) \longrightarrow X(1_+)^n, \quad \delta_n(x) = (X(\delta_1)x,\, \dots,\, X(\delta_n)x),

capturing the expected equivalence to iterated products for special objects.

A ΓG\Gamma_G-GG-space XX is termed II-special if for every TIT\in I (where II is a GG-indexing system), the Segal map

δT:X(T+)X(1+)T\delta_T: X(T_+) \xrightarrow{\simeq} X(1_+)^T

is a GG-equivalence. This property characterizes the types of GG-sets that must be "inverted" homotopically, as dictated by the transfer system II (Bantelmann, 28 Oct 2025).

3. The Segal Machine and Incomplete GG-Spectra

Given a GG-universe UU compatible with a transfer system II, the Segal machine describes a homotopically robust method for producing genuine or incomplete equivariant spectra from the data of II-special equivariant ΓI\Gamma_I-spaces. The construction is as follows:

  • The bar-construction prolongation bIb_I sends a ΓI\Gamma_I-space XX to a functor assigning

AB(A,ΓI,X),A \mapsto B\bigl(A^\bullet,\, \Gamma_I,\, X\bigr),

with A=Map(,A)A^\bullet = \operatorname{Map}_*(-, A).

  • The restriction RUIR_U^I evaluates at the representation spheres SVS^V in UU and assembles structure maps

B((SV),ΓI,X)SWB((SVW),ΓI,X).B\bigl((S^V)^\bullet,\, \Gamma_I,\, X\bigr)\wedge S^W \longrightarrow B\bigl((S^{V\oplus W})^\bullet,\, \Gamma_I,\, X\bigr).

  • The composite

SIG,U:ΓI[G]I-spcbIFun(G  I,G)RUI(OrthG,U)S_I^{G,U}: \Gamma_I[G_*]^{I\textrm{-spc}} \xrightarrow{b_I} Fun(G\underline{\;}_*^I, G_*) \xrightarrow{R_U^I} (\mathrm{Orth}^{G,U})

yields a connective positive Ω\Omega-GG-spectrum indexed on UU whenever XX is II-special.

The induced map from X(1+)X(1_+) to the associated $0$th space,

X(1+)SIG,UX(0)=B(ΓI,ΓI,X)(1+)ΩVSIG,UX(SV),X(1_+) \longrightarrow S_I^{G,U}X(0) = B(\Gamma_I, \Gamma_I, X)(1_+)\xrightarrow{\sim}\Omega^V S_I^{G,U}X(S^V),

is a group-completion for all VUV \in U with VG0V^G \neq 0. This establishes an equivalence between the homotopy categories of II-special ΓI\Gamma_I-spaces and connective UU-spectra indexed on the compatible universe UU (Bantelmann, 28 Oct 2025).

4. II-Normed Permutative GG-Categories and the Segal Machine

An II-normed permutative GG-category consists of a GG_*-internal permutative GG-category A\mathcal{A}, together with external TT-norms

T:A×TA,TI,\oplus_T: \mathcal{A}^{\times T} \longrightarrow \mathcal{A}, \quad T\in I,

and coherent untwistors vTv_T realizing equivalences A×TAT\mathcal{A}^{\times T} \simeq \mathcal{A}^{\oplus T}. The construction of the ΓI\Gamma_I-GG-category A\overline{\mathcal{A}} proceeds by:

  • Building An\overline{\mathcal{A}}_n whose objects are systems (As)(A_s) indexed by subsets s{1,,n}s \subseteq \{1,\ldots,n\}, with structure isomorphisms

as,t:AsAtAst,st=,a_{s,t}: A_s\oplus A_t\cong A_{s \cup t},\quad s\cap t = \emptyset,

with morphisms given by compatible families of arrows αs:AsAs\alpha_s: A_s\to A'_s.

  • Equivariant structure under Σn\Sigma_n is defined via permutation of the index set, and GG-equivariance via the internal GG-action on A\mathcal{A}.
  • Restricting to ΓI\Gamma_I, A(T+)=(An)σ\overline{\mathcal{A}}(T_+) = (\overline{\mathcal{A}}_n)^\sigma for TnσT \cong n^\sigma.

The Segal functor

δ:A(T+)(A×T)σ\delta: \overline{\mathcal{A}}(T_+)\longrightarrow (\mathcal{A}^{\times T})^\sigma

is an internal equivalence of categories whenever TIT\in I, confirming A\overline{\mathcal{A}} is II-special. Taking the nerve and realization produces an II-special ΓI\Gamma_I-GG-space:

$B\overline{\mathcal{A}}: \Gamma_I\longrightarrow G\Top_*.$

The equivariant Segal KK-theory spectrum is then defined as

KIG,U(A):=SIG,U(BA),K_I^{G,U}(\mathcal{A}):= S_I^{G,U}(B\overline{\mathcal{A}}),

recovering Shimakawa’s genuine or incomplete equivariant KK-theory spectrum of the normed GG-category A\mathcal{A} (Bantelmann, 28 Oct 2025).

5. Equivalence of Models and Homotopical Consequences

The construction outlined above yields comparisons and equivalences between different formulations of equivariant infinite loop spaces and KK-theory:

  • As II varies between transfer systems, comparison theorems establish that for each II, the homotopy category of II-special ΓI\Gamma_I-spaces is equivalent to that of connective UU-indexed GG-spectra, where UU is the universe compatible with II.
  • The group-completion property of the $0$th space map ensures that the homotopy-theoretic content of the II-special ΓI\Gamma_I-space is reflected, after passage to spectra, in the classic group-completion context.

This suggests that the Segal machine furnishes a universal mechanism for passing from permutative GG-categories, filtered by transfer systems, to the spectrum-level geometry of equivariant KK-theory, unifying classical and Shimakawa-style approaches. The formulation is both flexible—accommodating incomplete universes and normed structures—and fundamentally homotopical in nature (Bantelmann, 28 Oct 2025).

6. Relationship to Previous Frameworks and Research Directions

Schwede Global Equivariant K-theory as developed through the segmented ΓI\Gamma_I model provides a self-contained account of Shimakawa’s equivariant infinite-loop and KK-theory machine in a modern categorical language. The introduction of II-normed permutative GG-categories and the associated bar constructions advances the program of modeling equivariant infinite loop spaces for incomplete universes. The framework highlights categorical enrichment under GG-action and advances connections to transfer systems, equivariant spectra, and homotopy theory.

Ongoing research directions include refinement of transfer system classification, understanding the interplay with norm homotopy types, and extension to broader equivariant contexts—such as global equivariant stable homotopy theory—in line with the perspectives opened in (Bantelmann, 28 Oct 2025).

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