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I came across some notation that I’m having trouble understanding in Hansen-Scholze’s preprint ‘Relative Perversity.’ In the last paragraph of Proposition 3.4 there is the notation $A\widehat{\otimes^{\mathbf L}}Rg_*\mathbf Z_\ell$. Here, $A$ is in $D_{\mathrm{cons}}(X,\mathbf Q_\ell)$ on a qcqs scheme $X$, separated and of finite presentation over $S$ (say $f:X\to S$) and $g:T\to S$ is a pro-étale map. (The notation should probably read $A\widehat{\otimes^{\mathbf L}}f^\ast Rg_\ast\mathbf Z_\ell$.) The authors say $\widehat{\otimes^{\mathbf L}}$ means the $\ell$-adically completed tensor product, using an integral structure on $A$; i.e. we suppose $A=A_0\otimes_{\mathbf Z_\ell}\mathbf Q_\ell$ where $A_0\in D_{\mathrm{cons}}(X,\mathbf Z_\ell)$. But what does that mean when $A$ has field coefficients? Dropping the $R$ and $\mathbf L$s, I would normally write $A\widehat{\otimes}f^\ast g_\ast\mathbf Z_\ell=\lim_n(A\otimes f^\ast g_\ast\mathbf Z_\ell\otimes\mathbf Z/\ell^n)$ (everything is derived) but this is null. If what is meant is rather $(A_0\widehat\otimes f^\ast g_\ast\mathbf Z_\ell)\otimes\mathbf Q_\ell$, this is nonzero but then I have trouble understanding their ensuing argument (namely, why this would be independent of the choice of integral model $A_0$).

Separately, in that same paragraph the authors claim an integral structure on $A$ exists ‘at least up to direct factors.’ Their Corollary 2.4 claims an equivalence $D_{\mathrm{cons}}(X,\mathbf Z_\ell)\otimes_{\mathbf Z_\ell}\mathbf Q_\ell\to D_{\mathrm{cons}}(X,\mathbf Q_\ell)$. (The functor sends $A_0\mapsto A_0\otimes_{\mathbf Z_\ell}\mathbf Q_\ell$.) I believe the $\infty$-category on the left-hand side is obtained by inverting $\ell$ and taking the idempotent completion. The idempotent completion is still a little mysterious to me. I suppose it’s a matter of finding some $\mathcal F\in D_{\mathrm{cons}}(X,\mathbf Z_\ell)$ which has no nontrivial direct summand but does after extending scalars. I suppose this can be seen on the level of triangulated categories but I don’t yet have an example.

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    $\begingroup$ In fact, since $D_{cons}(X,\mathbf{Z}_\ell)$ has a bounded $t$-structure, we have a vanishing $K$-group in degree $-1$: $K_{-1}(D_{cons}(X,\mathbf{Z}_\ell))=0$. That means precisely that all the Verdier quotients of $D_{cons}(X,\mathbf{Z}_\ell)$ already are idempotent complete. $\endgroup$ Commented Dec 4, 2022 at 10:26
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    $\begingroup$ For references: Theorem 2.35 in Benjamin Antieau, David Gepner, Jeremiah Heller arxiv.org/abs/1610.07207 for the vanishing of $K_{-1}$. For the interpretation of $K_{-1}=0$ in terms of Verdier quotients, this is in the paper of Marco Schlichting Negative K-theory of derived categories (end of Section 1). $\endgroup$ Commented Dec 4, 2022 at 10:34
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    $\begingroup$ Hence, at the end of the day, $D_{cons}(X,\mathbf{Q}_\ell)$ has the same objects as $D_{cons}(X,\mathbf{Z}_\ell)$ and the mapping spaces of $D_{cons}(X,\mathbf{Q}_\ell)$ are those of $D_{cons}(X,\mathbf{Z}_\ell)$ tensored by $\mathbf{Q}$. $\endgroup$ Commented Dec 4, 2022 at 10:39
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    $\begingroup$ In fact, one can also see this in a more elementary way. See Section B.2 in this paper: cambridge.org/core/journals/compositio-mathematica/article/… $\endgroup$ Commented Dec 4, 2022 at 11:00
  • $\begingroup$ Thank you @D.-C.Cisinski, that completely clarifies the confusion of my second paragraph. $\endgroup$
    – Tomo
    Commented Dec 5, 2022 at 0:41

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Scholze explained to me that he meant by this is the following: consider $-\widehat\otimes f^*g_*\mathbf Z_\ell$ as a functor $D_{\mathrm{cons}}(X,\mathbf Z_\ell)\to D_{\mathrm{comp}}(X,\mathbf Z_\ell)$; then inverting $\ell$ yields a functor $D_{\mathrm{cons}}(X,\mathbf Z_\ell)\to D(X,\mathbf Q_\ell)$ and it factors via the Verdier quotient $D_{\mathrm{cons}}(X,\mathbf Q_\ell)=D_{\mathrm{cons}}(X,\mathbf Z_\ell)[\ell^{-1}]$ (this by their Corollary 2.4) if $(-\widehat\otimes f^*g_*\mathbf Z_\ell)[\ell^{-1}]$ sends torsion sheaves to zero, which it clearly does. Therefore in particular this functor is independent (up to isomorphism) of the integral model chosen.

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  • $\begingroup$ Is that the same as some form of solid tensor product with $f^*g_*\mathbf Q_\ell$? $\endgroup$
    – Z. M
    Commented Feb 21, 2023 at 6:59
  • $\begingroup$ That’s an interesting question, as I don’t know that the solid tensor product has been defined outside of the condensed context; i.e. on the pro-étale site of a scheme larger than a point. But I see the resemblance, as in this case we have some $A\in D_{\mathrm{cons}}(X,\mathbf Q_\ell)$ and forming a tensor product with $f^*g_*\mathbf Z_\ell$, so it’s like $\mathbf Q_\ell\otimes\mathbf Z_\ell$ which is what the solid tensor product was devised to handle. $\endgroup$
    – Tomo
    Commented Feb 23, 2023 at 0:45
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    $\begingroup$ Constructible sheaves should be much easier, but it should be possible to talk about pro-étale $\mathbb Z$-sheaves being solid, by virtue of the exodromy equivalence which identifies pro-étale $\mathbb Z$-sheaves with (condensed) functors from the Galois (condensed) category to the category of condensed abelian groups. I am not sure how to compare this with solid sheaves in Fargues–Scholze. $\endgroup$
    – Z. M
    Commented Feb 24, 2023 at 22:02

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