-The first formula stems from \(j\) an open inclusion, whose algebraic model is \(j^* M \simeq R \otimes M\).\footnote{Localizations which obey this formula are called ``smashing'', and they are quite interesting: the arithmetic localizations and \(L_d\) form a complete list of smashing localizations in \(\CatOf{Spectra}\)~\cite[7.5.6]{RavenelOrangeBook}, and smashing localizations (which are localizations at ring spectra) agree with their nilpotent completions~\cite{BousfieldLocalization}. (This can also be taken as an explanation of our interest in continuous Morava \(E\)--theory: by working internally to \(\CatOf{Spectra}_\Gamma\), we are forcing \(\widehat L_\Gamma\) to become smashing.) The smashing localization \(L_d\) is also particularly interesting: the Adams resolution of \(L_d \S\) is weakly equivalent to a finite resolution~\cite[8.2.4]{RavenelOrangeBook}, from which it follows that every \(E(d)\)--Adams resolution is weakly finite, and hence that there is a universal horizontal vanishing line in \(E(d)\)--Adams spectral sequences. In turn, if the ambient prime \(p\) is very large compared to the height of \(\Gamma\), the sparsity of the degrees \(|v_j|\) couples to this universal vanishing line to show that the \(E(d)\)--Adams spectral sequence always collapses, so that the theory of \(E(d)\)--local spectra is perfectly captured by the context \(\context{E(d)}\)~\cite[4.4.2, 6.2.10]{RavenelOrangeBook}. Higher categorical versions of this statement are now also known~\cite{BSS,Pstragowski}.} The second formula can be compared to the inclusion \(j\) of the formal infinitesimal neighborhood of a closed subscheme, whose algebraic model is \(j^* M = \lim_j (R/I^j \otimes M)\).\footnote{In keeping with our discussion of continuous Morava \(E\)--theory, it is also possible to consider the object \(\{\left( M_0(v^I) \sm L_d X \right)\}_I\) itself as a pro-spectrum. This is interesting to explore: Davis and Lawson have shown that setting \(X = \S\) gives an \(E_\infty\)--ring pro-spectrum~\cite{DavisLawson}, even though none of the individual objects are \(E_\infty\)--ring spectra themselves~\cite{MNN}.}
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