ScalingStacks

Carrying out the same analysis as above, we see that the quotient

π’žβ€²=Ψ⁑(F~R∞)/Ψ⁑(FR){\mathcal{C}}^{\prime}=\Psi(\tilde{F}_{R}^{\infty})/\Psi(F_{R})

can be described as modules over Endπ’žβ€²β‘(Gβ€²)\End_{{\mathcal{C}}^{\prime}}(G^{\prime}), where Gβ€²G^{\prime} is the cofiber of the map

i!iβˆ—R∨∞⟢R∨∞i_{!}i^{*}R^{\lor\infty}\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}R^{\lor\infty}

(here R∨∞R^{\lor\infty} is regarded as an object of F~R∞\tilde{F}_{R}^{\infty}) and hence as a spectrum Endπ’žβ€²β‘(Gβ€²)\End_{{\mathcal{C}}^{\prime}}(G^{\prime}) is equivalent to the cofiber in spectra of the map

(9.49) MapΨ⁑(F~R∞)(R∨∞,i!iβˆ—R∨∞)⟢EndΨ⁑(F~R∞)(R∨∞).\mathrm{Map}_{\Psi(\tilde{F}_{R}^{\infty})}(R^{\lor\infty},i_{!}i^{*}R^{\lor\infty})\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}\End_{\Psi(\tilde{F}_{R}^{\infty})}(R^{\lor\infty}).

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