ScalingStacks

0NQR

Proposition 9.51. Let RR be a connective A∞A_{\infty} ring spectrum. We have a natural equivalence of spectra

K​(Ψtri​(μ^​R))\textstyle{K(\Psi_{\tri}(\hat{\mu}R))\ignorespaces\ignorespaces\ignorespaces\ignorespaces}≃\scriptstyle{\simeq}K⁡((Ind⁡(Ψperf​(R)))κ/Ψperf​R)\textstyle{K((\Ind(\Psi_{\perf}(R)))^{\kappa}/\Psi_{\perf}{R})}

for any infinite cardinal κ>ω\kappa>\omega.

0NQS

Proof. For any infinite cardinal κ>ω\kappa>\omega, there is a natural inclusion map

Ψperf​(FR∞)⟶(Ind⁡(Ψperf​(R)))κ\Psi_{\perf}(F_{R}^{\infty})\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}(\Ind(\Psi_{\perf}(R)))^{\kappa}

induced by the fact that any countable wedge of copies of RR is in (Ind⁡(Ψ​(R)perf))κ(\Ind(\Psi(R)_{\perf}))^{\kappa}, and the latter is closed under retracts and stable under finite colimits. Since the inclusion Ψperf​(FR)→Ψperf​(FR∞)\Psi_{\perf}(F_{R})\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}\Psi_{\perf}(F_{R}^{\infty}) is compatible with the (Yoneda) inclusion Ψperf​(R)→(Ind⁡(Ψperf​(R)))κ\Psi_{\perf}(R)\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}(\Ind(\Psi_{\perf}(R)))^{\kappa}, we have a commutative diagram

Ψperf​(FR)\textstyle{\Psi_{\perf}(F_{R})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}≃\scriptstyle{\simeq}Ψperf​(FR∞)\textstyle{\Psi_{\perf}(F_{R}^{\infty})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ψperf​(R)\textstyle{\Psi_{\perf}(R)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(Ind⁡(Ψperf​(R)))κ.\textstyle{(\Ind(\Psi_{\perf}(R)))^{\kappa}.}

Combining this with Ψperf​(F~R)→Ψperf​(F~R∞)\Psi_{\perf}(\tilde{F}_{R})\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}\Psi_{\perf}(\tilde{F}^{\infty}_{R}) we obtain the commutative diagram

(9.52) Ψperf​(F~R)\textstyle{\Psi_{\perf}(\tilde{F}_{R})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}≃\scriptstyle{\simeq}Ψperf​(F~R∞)\textstyle{\Psi_{\perf}(\tilde{F}_{R}^{\infty})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ψperf​(FR)\textstyle{\Psi_{\perf}(F_{R})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}≃\scriptstyle{\simeq}Ψperf​(FR∞)\textstyle{\Psi_{\perf}(F_{R}^{\infty})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ψperf​(R)\textstyle{\Psi_{\perf}(R)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(Ind⁡(Ψperf​(R)))κ.\textstyle{(\Ind(\Psi_{\perf}(R)))^{\kappa}.}

and hence an induced composite map of quotients

α:Ψperf​(F~R∞)/Ψperf​(FR)⟶Ψperf​(FR∞)/Ψperf​(FR)\displaystyle\alpha\colon\Psi_{\perf}(\tilde{F}_{R}^{\infty})/\Psi_{\perf}(F_{R})\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}\Psi_{\perf}(F_{R}^{\infty})/\Psi_{\perf}(F_{R})
⟶(Ind⁡(Ψperf​(R)))κ/Ψperf​(R).\displaystyle\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}(\Ind(\Psi_{\perf}(R)))^{\kappa}/\Psi_{\perf}(R).

By the work above, α\alpha can be described as a map

Ψtri​(μ^​R)⟶(Ind⁡(Ψperf​(R)))κ/Ψperf​(R).\Psi_{\tri}(\hat{\mu}R)\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}(\Ind(\Psi_{\perf}(R)))^{\kappa}/\Psi_{\perf}(R).

Finally, since FR∞F_{R}^{\infty} has countable coproducts, the usual Eilenberg swindle implies that K⁡(FR∞)K(F_{R}^{\infty}) is contractible. We also know that K⁡(Ψperf​(F~R∞)CLOSEK(\Psi_{\perf}(\tilde{F}_{R}^{\infty}) is contractible [33, 6.1,6.3]. Therefore, applying Map⁡(𝒰wlocκ¯​(𝒮∞ω),𝒰wlocκ¯​(−))\mathrm{Map}(\underline{{\mathcal{U}}_{\mathrm{wloc}}^{\kappa}}({\mathcal{S}}_{\infty}^{\omega}),\,\underline{{\mathcal{U}}_{\mathrm{wloc}}^{\kappa}}(-)) to the commutative diagram, the fact that all of the horizontal sequences are strict-exact allows us to apply theorem 9.10 to conclude that α\alpha induces an equivalence on KK-theory spectra. ∎

Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.

Andrew J. Blumberg, David Gepner, Goncalo Tabuada

Original source: arXiv:1001.2282v4