ScalingStacks

0MWL

Proof. Suppose we are given any edge ๐šโˆˆ๐™ฑ1{\tt f}\in{\tt B}_{1}. Let us write ฮด0โ€‹(๐š)=๐š‹2โˆˆ๐™ฑ0\delta_{0}({\tt f})={\tt b}_{2}\in{\tt B}_{0} and ฮด1โ€‹(๐š)=๐š‹1โˆˆ๐™ฑ0\delta_{1}({\tt f})={\tt b}_{1}\in{\tt B}_{0}. Suppose further that we are given any vertex ๐šŽ2โˆˆ๐™ด0{\tt e}_{2}\in{\tt E}_{0} with ๐š™โก(๐šŽ2)=๐š‹2{\tt p}({\tt e}_{2})={\tt b}_{2}. Then we must find a JL-๐š™{\tt p}-cartesian lift of the edge ๐šโˆˆ๐™ฑ1{\tt f}\in{\tt B}_{1} relative to the vertex ๐šŽ2โˆˆ๐™ด0{\tt e}_{2}\in{\tt E}_{0}.

Let us respectively write e1โ†’f~e2e_{1}\xrightarrow{\tilde{f}}e_{2} and b1โ†’๐‘“b2b_{1}\xrightarrow{f}b_{2} for the morphisms in โ„ฐ\mathcal{E} and โ„ฌ\mathcal{B} presented by the maps ฮ”1โ†’๐š~๐™ด\Delta^{1}\xrightarrow{\tilde{{\tt f}}}{\tt E} and ฮ”1โ†’๐š๐™ฑ\Delta^{1}\xrightarrow{{\tt f}}{\tt B} in sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}} (for any choice of edge ๐š~โˆˆ๐™ด1\tilde{{\tt f}}\in{\tt E}_{1}). Then, according to Theoremย 3.3, for an edge ๐š~โˆˆ๐™ด1\tilde{{\tt f}}\in{\tt E}_{1} to be ๐š™{\tt p}-cartesian, it suffices to verify that the morphism f~\tilde{f} in โ„ฐ\mathcal{E} is pp-cartesian.

Now, the given data define a vertex

(๐š,๐šŽ2)โˆˆ(homยฏโ€‹(ฮ”1,๐™ฑ)โ€‹ร—ev1,๐™ฑ,๐š™โ€‹๐™ด)0({\tt f},{\tt e}_{2})\in\left(\underline{\hom}(\Delta^{1},{\tt B})\underset{\textup{ev}_{1},{\tt B},{\tt p}}{\times}{\tt E}\right)_{0}

of the fiber product in sโ€‹๐’ฎโ€‹ets{\mathcal{S}\textup{et}}. Moreover, by [Lur09, Proposition 1.2.7.3(1)] and the Reedy trick, this fiber product is a homotopy pullback in sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}}. Hence, this vertex defines an object

(f,b2)โˆˆFunโ€‹([1],โ„ฌ)โ€‹ร—t,โ„ฌ,pโ€‹โ„ฐ(f,b_{2})\in\textup{Fun}([1],\mathcal{B})\underset{t,\mathcal{B},p}{\times}\mathcal{E}

of the pullback in ๐’žโ€‹atโˆž{{\mathcal{C}\textup{at}}_{\infty}}.

Next, it is easy to check that the map

homยฏโ€‹(ฮ”1,๐™ด)โ†’homยฏโ€‹(ฮ”1,๐š™)homยฏโ€‹(ฮ”1,๐™ฑ)\underline{\hom}(\Delta^{1},{\tt E})\xrightarrow{\underline{\hom}(\Delta^{1},{\tt p})}\underline{\hom}(\Delta^{1},{\tt B})

lies in ๐…JoyalโŠ‚sโ€‹๐’ฎโ€‹et{\bf F}_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}}, simply by using

  • โ€ข

    the fact that ๐…Joyal=rlpโ€‹((๐–โˆฉ๐‚)Joyal){\bf F}_{\textup{Joyal}}=\textup{rlp}(({\bf W}\cap{\bf C})_{\textup{Joyal}}),

  • โ€ข

    the adjunction โˆ’ร—ฮ”1:s๐’ฎetโ‡„s๐’ฎet:homยฏsโ€‹๐’ฎโ€‹et(ฮ”1,โˆ’)-\times\Delta^{1}:s{\mathcal{S}\textup{et}}\rightleftarrows s{\mathcal{S}\textup{et}}:\underline{\hom}_{s{\mathcal{S}\textup{et}}}(\Delta^{1},-), and

  • โ€ข

    the fact that sโ€‹๐’ฎโ€‹etJoyalโ†’โˆ’ร—ฮ”1sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}}\xrightarrow{-\times\Delta^{1}}s{\mathcal{S}\textup{et}}_{\textup{Joyal}} is a left Quillen functor and hence in particular preserves acyclic cofibrations.

Moreover, the map

homยฏโ€‹(ฮ”1,๐™ด)โ†’ev1๐™ด\underline{\hom}(\Delta^{1},{\tt E})\xrightarrow{\textup{ev}_{1}}{\tt E}

also lies in ๐…JoyalโŠ‚sโ€‹๐’ฎโ€‹et{\bf F}_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}}, since by applying the dual of [Lur09, Corollary 2.4.7.12] to the map ๐™ดโ†’id๐™ด๐™ด{\tt E}\xrightarrow{\textup{id}_{{\tt E}}}{\tt E} in sโ€‹๐’ฎโ€‹etJoyalfs{\mathcal{S}\textup{et}}^{f}_{\textup{Joyal}} we see that it is a JL-cocartesian fibration, which by [Lur09, Remark 2.0.0.5] implies that it is in particular a fibration in sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}}. Thus, our conditions that ฮด0โ€‹(๐š~)=๐šŽ2\delta_{0}(\tilde{{\tt f}})={\tt e}_{2} and that ๐š™โก(๐š~)=๐š{\tt p}(\tilde{{\tt f}})={\tt f} translate into the single condition that ๐š~โˆˆ๐™ด1\tilde{{\tt f}}\in{\tt E}_{1} define a vertex of the limit

lim(ย ย ย ย ย ย ย ฮ”0ย ย ย ย ย homยฏโ€‹(ฮ”1,๐™ด)ย ย ย ๐™ดย ย ย ย ย ฮ”0ย ย ย homยฏโ€‹(ฮ”1,๐™ฑ)ย ย ย ย ย ย ย ย ย ย ย ๐šŽ2ย ย ย ย ย ย ย ย ย ย ย ย ev1ย ย ย ย ย ย ย ย ย ย ย ย homยฏโ€‹(ฮ”1,๐š™)ย ย ย ย ย ย ย ย ย ๐šย ย ย ย ย )\lim\left(\hbox to163.1pt{\vbox to87.5pt{\pgfpicture\makeatletter\hbox{\hskip 81.54857pt\lower-43.81284pt\hbox to0.0pt{\lxSVG@begingroup@{_scopebegin=1} \lxSVG@begingroup@{stroke=#000000} \lxSVG@begingroup@{fill=#000000} \lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.4pt} \lx@inpgf@ignorespaces\nullfont\hbox to0.0pt{\lxSVG@begingroup@{_scopebegin=1} {}{}{}{{}}\lx@inpgf@ignorespaces\hbox{\hbox{{\lxSVG@begingroup@{_scopebegin=1} {{}{}{{{}}{{}}{{}}{{}}{{}}}{{{\lx@inpgf@ignorespaces}}}{{}{}{{ {}{}}}{ {}{}} {{}{{\lx@inpgf@ignorespaces}}}{{}{\lx@inpgf@ignorespaces}}{}{{}{\lx@inpgf@ignorespaces}} {\lx@inpgf@ignorespaces }{{{{\lx@inpgf@ignorespaces}}\lxSVG@begingroup@{_scopebegin=1} 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\lxSVG@begingroup@{stroke-dasharray=none,stroke-dashoffset=0.0pt} \lxSVG@begingroup@{stroke-linecap=round} \lxSVG@begingroup@{stroke-linejoin=round} \lxSVG@drawpath@unclipped{M -2.88 3.32 C -2.35 1.33 -1.18 0.39 0 0 C -1.18 -0.39 -2.35 -1.33 -2.88 -3.32}{fill:none} \lxSVG@closescope \lxSVG@closescope }}{{\lx@inpgf@ignorespaces}}}}\lx@inpgf@ignorespaces\hbox{\hbox{{\lxSVG@begingroup@{_scopebegin=1} {{}{}{{ {}{}}}{ {}{}} {{}{{\lx@inpgf@ignorespaces}}}{{}{\lx@inpgf@ignorespaces}}{}{{}{\lx@inpgf@ignorespaces}} {\lx@inpgf@ignorespaces }{{{{\lx@inpgf@ignorespaces}}\lxSVG@begingroup@{_scopebegin=1} \lxSVG@transformcm{1.0}{0.0}{0.0}{1.0}{34.18051pt}{-4.43666pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 47.3 -6.14)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}} \lxSVG@closescope {}{ {}{}{}}{}{ {}{}{}} {{{{{}}{ {}{}}{}{}{{}{}}}}}{}{{{{{}}{ {}{}}{}{}{{}{}}}}}{{}}{}{}{}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{}{{{}{}}}\lxSVG@begingroup@{_scopebegin=1} 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in sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}}.

Now, we claim that the above limit is in fact a homotopy limit in sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}}. For this, we appeal to a more elaborate version of the Reedy trick: we endow the category

Nโˆ’1(sd2(ฮ”1))=(โˆ™โ†’โˆ™โ†โˆ™โ†’โˆ™โ†โˆ™)โˆˆ๐’žat\textup{N}^{-1}(\textup{sd}^{2}(\Delta^{1}))=(\bullet\rightarrow\bullet\leftarrow\bullet\rightarrow\bullet\leftarrow\bullet)\in{\mathcal{C}\textup{at}}

with the Reedy structure determined by the degree function described by the picture (0โ†’1โ†2โ†’1โ†0)(0\rightarrow 1\leftarrow 2\rightarrow 1\leftarrow 0). Using [Hir03, Proposition 15.10.2(1)], it is easy to see that this Reedy category has cofibrant constants, and hence by [Hir03, Theorem 15.10.8(1)] we obtain a Quillen adjunction

const:s๐’ฎetJoyalโ‡„Fun(Nโˆ’1(sd2(ฮ”1)),s๐’ฎetJoyal)Reedy:lim.\textup{const}:s{\mathcal{S}\textup{et}}_{\textup{Joyal}}\rightleftarrows\textup{Fun}(\textup{N}^{-1}(\textup{sd}^{2}(\Delta^{1})),s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}}:\lim.

Then, to see that the diagram in the above limit defines a fibrant object of Funโ€‹(Nโˆ’1โ€‹(sd2โ€‹(ฮ”1)),sโ€‹๐’ฎโ€‹etJoyal)Reedy\textup{Fun}(\textup{N}^{-1}(\textup{sd}^{2}(\Delta^{1})),s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}}, since it is objectwise fibrant, it only remains to check that the latching map

homยฏโ€‹(ฮ”1,๐™ด)โ†’(ev1,homยฏโ€‹(ฮ”1,๐š™)CLOSE๐™ดร—homยฏโ€‹(ฮ”1,๐™ฑ)\underline{\hom}(\Delta^{1},{\tt E})\xrightarrow{(\textup{ev}_{1},\underline{\hom}(\Delta^{1},{\tt p})}{\tt E}\times\underline{\hom}(\Delta^{1},{\tt B})

lies in ๐…JoyalโŠ‚sโ€‹๐’ฎโ€‹et{\bf F}_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}}. For this, we use the characterization ๐…Joyal=rlpโ€‹((๐–โˆฉ๐‚)Joyal){\bf F}_{\textup{Joyal}}=\textup{rlp}(({\bf W}\cap{\bf C})_{\textup{Joyal}}): given any solid commutative square

๐šˆ{\lx@inpgf@ignorespaces{\tt Y}}homยฏโ€‹(ฮ”1,๐™ด){\lx@inpgf@ignorespaces\underline{\hom}(\Delta^{1},{\tt E})}๐š‰{\lx@inpgf@ignorespaces{\tt Z}}๐™ดร—homยฏโ€‹(ฮ”1,๐™ฑ){\lx@inpgf@ignorespaces{\tt E}\times\underline{\hom}(\Delta^{1},{\tt B})}๐šš\scriptstyle{\lx@inpgf@ignorespaces{\tt q}}โ‰ˆ\scriptstyle{\lx@inpgf@ignorespaces\approx}(ev1,homยฏโ€‹(ฮ”1,๐š™)CLOSE\scriptstyle{\lx@inpgf@ignorespaces(\textup{ev}_{1},\underline{\hom}(\Delta^{1},{\tt p})}

in sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}}, unwinding the definitions we see that a dotted lift is equivalent to a dotted lift in the diagram

(๐šˆร—ฮ”1)โ€‹โˆฮ”{1},๐šˆ,๐ššโ€‹๐š‰{\lx@inpgf@ignorespaces({\tt Y}\times\Delta^{1})\underset{\Delta^{\{1\}},{\tt Y},{\tt q}}{\coprod}{\tt Z}}๐™ด{\lx@inpgf@ignorespaces{\tt E}}๐š‰ร—ฮ”1{\lx@inpgf@ignorespaces{\tt Z}\times\Delta^{1}}๐™ฑ{\lx@inpgf@ignorespaces{\tt B}}๐š™\scriptstyle{\lx@inpgf@ignorespaces{\tt p}}

in sโ€‹๐’ฎโ€‹ets{\mathcal{S}\textup{et}}. But it is easy to see that the left map lies in (๐–โˆฉ๐‚)Joyal({\bf W}\cap{\bf C})_{\textup{Joyal}}, while the right map lies in ๐…Joyal{\bf F}_{\textup{Joyal}} by assumption. Hence the diagram in the above limit defines a fibrant object of Funโ€‹(Nโˆ’1โ€‹(sd2โ€‹(ฮ”1)),sโ€‹๐’ฎโ€‹etJoyal)Reedy\textup{Fun}(\textup{N}^{-1}(\textup{sd}^{2}(\Delta^{1})),s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}}, and so the above limit is a homotopy limit in sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}} and thus presents the limit

lim(ย ย ย ย ย ย ย {e2}ย ย ย ย ย Funโ€‹([1],โ„ฐ)ย ย ย โ„ฐย ย ย ย ย {f}ย ย ย Funโ€‹([1],โ„ฌ)ย ย ย ย ย ย ย ย ย ย ย tย ย ย ย ย ย ย ย ย Funโ€‹([1],p)ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย )\lim\left(\hbox to183.95pt{\vbox to87.96pt{\pgfpicture\makeatletter\hbox{\hskip 91.97398pt\lower-43.97923pt\hbox to0.0pt{\lxSVG@begingroup@{_scopebegin=1} \lxSVG@begingroup@{stroke=#000000} \lxSVG@begingroup@{fill=#000000} \lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.4pt} \lx@inpgf@ignorespaces\nullfont\hbox to0.0pt{\lxSVG@begingroup@{_scopebegin=1} {}{}{}{{}}\lx@inpgf@ignorespaces\hbox{\hbox{{\lxSVG@begingroup@{_scopebegin=1} {{}{}{{{}}{{}}{{}}{{}}{{}}}{{{\lx@inpgf@ignorespaces}}}{{}{}{{ {}{}}}{ {}{}} {{}{{\lx@inpgf@ignorespaces}}}{{}{\lx@inpgf@ignorespaces}}{}{{}{\lx@inpgf@ignorespaces}} {\lx@inpgf@ignorespaces }{{{{\lx@inpgf@ignorespaces}}\lxSVG@begingroup@{_scopebegin=1} 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in ๐’žโ€‹atโˆž{{\mathcal{C}\textup{at}}_{\infty}}.

Now, we have assumed that pp is a cartesian fibration, so in particular there must exist a pp-cartesian lift f~\tilde{f} of ff relative to the object e2e_{2}. This defines an object of the above limit in ๐’žโ€‹atโˆž{{\mathcal{C}\textup{at}}_{\infty}}, which must therefore be represented by a vertex of the above homotopy limit in sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}}: this selects the desired JL-๐š™{\tt p}-cartesian lift ๐š~โˆˆ๐™ด1\tilde{{\tt f}}\in{\tt E}_{1} of ๐šโˆˆ๐™ฑ1{\tt f}\in{\tt B}_{1} relative to ๐šŽ2โˆˆ๐™ด0{\tt e}_{2}\in{\tt E}_{0}. So the map ๐™ดโ† ๐š™๐™ฑ{\tt E}\stackrel{{\scriptstyle{\tt p}}}{{\twoheadrightarrow}}{\tt B} in sโ€‹๐’ฎโ€‹etJoyals{\mathcal{S}\textup{et}}_{\textup{Joyal}} is indeed a JL-cartesian fibration, as claimed. โˆŽ

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

Aaron Mazel-Gee

Original source: arXiv:1510.02402v1