In this final section, we prove that our definitions of co/cartesian morphisms and co/cartesian fibrations coincide with the corresponding “point-set” definitions in quasicategories; as these latter have been studied extensively, it will follow that all quasicategorical results regarding co/cartesian morphisms and co/cartesian fibrations can be applied either when working model-independently or when working in some other model category of ∞ \infty -categories. In order to directly align with the definitions given in [Lur09 , §2.4] we will focus on the cartesian variants, but of course our results will immediately apply to the cocartesian variants as well (simply by taking opposites).
0MWH
Definition 3.2 . Let 𝙴 → 𝚙 𝙱 {\tt E}\xrightarrow{{\tt p}}{\tt B} be an inner fibration in s 𝒮 et s{\mathcal{S}\textup{et}} . Following [Lur09 , Definition 2.4.1.1] , we will say that an edge Δ 1 → 𝚏 𝙴 \Delta^{1}\xrightarrow{{\tt f}}{\tt E} is JL-𝚙 {\tt p} -cartesian (or simply JL-cartesian ) if the induced map
𝙴 / 𝚏 → 𝙴 / 𝚏 ( 1 ) × 𝙱 / 𝚙 ( 𝚏 ( 1 ) ) 𝙱 / 𝚙 ( 𝚏 ) {\tt E}_{/{\tt f}}\rightarrow{\tt E}_{/{\tt f}(1)}\underset{{\tt B}_{/{\tt p}({\tt f}(1))}}{\times}{\tt B}_{/{\tt p}({\tt f})}
lies in ( 𝐖 ∩ 𝐅 ) Joyal ⊂ s 𝒮 et ({\bf W}\cap{\bf F})_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}} . In this case, we will refer to the edge 𝚏 ∈ 𝙴 1 {\tt f}\in{\tt E}_{1} as a JL-𝚙 {\tt p} -cartesian lift (or simply a JL-cartesian lift ) of the edge 𝚙 ( 𝚏 ) ∈ 𝙱 1 {\tt p}({\tt f})\in{\tt B}_{1} relative to the vertex 𝚏 ( 1 ) ∈ 𝙴 0 {\tt f}(1)\in{\tt E}_{0} . Following [Lur09 , Definition 2.4.2.1] , we then say that the morphism 𝚏 {\tt f} is a JL-cartesian fibration if every vertex of
hom ¯ ( Δ 1 , 𝙱 ) × ev 1 , 𝙱 , 𝚏 𝙴 \underline{\hom}(\Delta^{1},{\tt B})\underset{\textup{ev}_{1},{\tt B},{\tt f}}{\times}{\tt E}
admits an 𝚏 {\tt f} -cartesian lift.
0MWJ
Proof. We must show that the map
𝙴 / 𝚏 → 𝙴 / 𝚏 ( 1 ) × 𝙱 / 𝚙 ( 𝚏 ( 1 ) ) 𝙱 / 𝚙 ( 𝚏 ) {\tt E}_{/{\tt f}}\rightarrow{\tt E}_{/{\tt f}(1)}\underset{{\tt B}_{/{\tt p}({\tt f}(1))}}{\times}{\tt B}_{/{\tt p}({\tt f})}
in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} lies in ( 𝐖 ∩ 𝐅 ) Joyal ({\bf W}\cap{\bf F})_{\textup{Joyal}} .
First of all, using the characterization 𝐅 Joyal = rlp ( ( 𝐖 ∩ 𝐂 ) Joyal ) {\bf F}_{\textup{Joyal}}=\textup{rlp}(({\bf W}\cap{\bf C})_{\textup{Joyal}}) , it is easy to see
•
that the object 𝙴 / 𝚏 ( 1 ) ∈ s 𝒮 et Joyal {\tt E}_{/{\tt f}(1)}\in s{\mathcal{S}\textup{et}}_{\textup{Joyal}} is fibrant and
•
that the map 𝙱 / 𝚙 ( 𝚏 ) → 𝙱 / 𝚙 ( 𝚏 ( 1 ) ) {\tt B}_{/{\tt p}({\tt f})}\rightarrow{\tt B}_{/{\tt p}({\tt f}(1))} is a fibration in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} .
Hence, it follows from the Reedy trick that this fiber product is in fact a homotopy pullback in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} . Thus, this map in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} presents the map
ℰ / f → ℰ / f ( 1 ) × ℬ / p ( f ( 1 ) ) ℬ / p ( f ) , \mathcal{E}_{/f}\rightarrow\mathcal{E}_{/f(1)}\underset{\mathcal{B}_{/p(f(1))}}{\times}\mathcal{B}_{/p(f)},
in 𝒞 at ∞ {{\mathcal{C}\textup{at}}_{\infty}} , which can be canonically identified with the map
ℰ / f ( 0 ) → ℰ f ( 1 ) × ℬ / p ( f ( 1 ) ) ℬ / p ( f ( 0 ) ) \mathcal{E}_{/f(0)}\rightarrow\mathcal{E}_{f(1)}\underset{\mathcal{B}_{/p(f(1))}}{\times}\mathcal{B}_{/p(f(0))}
in 𝒞 at ∞ {{\mathcal{C}\textup{at}}_{\infty}} and therefore lies in 𝐖 Joyal {\bf W}_{\textup{Joyal}} by assumption.
To see that it also lies in 𝐅 Joyal {\bf F}_{\textup{Joyal}} , we argue as follows. We claim that there is a Quillen adjunction
α : Fun ( [ 1 ] , s 𝒮 et Joyal ) Reedy ⇄ ( s 𝒮 et Joyal ) Δ 1 / : β , \alpha:\textup{Fun}([1],s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}}\rightleftarrows(s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\Delta^{1}/}:\beta,
where
•
we equip [ 1 ] [1] with the Reedy category structure determined by the degree function 0 ↦ 0 0\mapsto 0 and 1 ↦ 1 1\mapsto 1 ,
•
we define
β ( Δ 1 → 𝚢 𝚈 ) = ( 𝚈 / 𝚢 → 𝚈 / 𝚢 ( 1 ) ) , \beta(\Delta^{1}\xrightarrow{{\tt y}}{\tt Y})=({\tt Y}_{/{\tt y}}\to{\tt Y}_{/{\tt y}(1)}),
and
•
we define
α ( 𝚉 → 𝚆 ) = ( Δ 1 → ( 𝚉 ⋆ Δ 1 ∐ 𝚉 ⋆ Δ { 1 } 𝚆 ⋆ Δ { 1 } ) ) . \alpha({\tt Z}\rightarrow{\tt W})=\left(\Delta^{1}\rightarrow\left({\tt Z}\star\Delta^{1}\coprod_{{\tt Z}\star\Delta^{\{1\}}}{\tt W}\star\Delta^{\{1\}}\right)\right).
It is not hard to see that indeed α ⊣ β \alpha\dashv\beta , so it suffices to show that α \alpha is a left Quillen functor. For this, given a map
𝚉 1 {\lx@inpgf@ignorespaces{\tt Z}_{1}} 𝚆 1 {\lx@inpgf@ignorespaces{\tt W}_{1}} 𝚉 2 {\lx@inpgf@ignorespaces{\tt Z}_{2}} 𝚆 2 {\lx@inpgf@ignorespaces{\tt W}_{2}} 𝚐 1 \scriptstyle{\lx@inpgf@ignorespaces{\tt g}_{1}} 𝚐 2 \scriptstyle{\lx@inpgf@ignorespaces{\tt g}_{2}}
in Fun ( [ 1 ] , s 𝒮 et Joyal ) Reedy \textup{Fun}([1],s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}} (reading the square vertically), observe that for this to be a (resp. acyclic) cofibration is precisely to require that the two relative latching maps 𝚉 1 → 𝚉 2 {\tt Z}_{1}\rightarrow{\tt Z}_{2} and 𝚆 1 ∐ 𝚉 1 𝚉 2 → 𝚆 2 {\tt W}_{1}\coprod_{{\tt Z}_{1}}{\tt Z}_{2}\rightarrow{\tt W}_{2} are (resp. acyclic) cofibrations. For simplicity, let us write the composite
Fun ( [ 1 ] , s 𝒮 et ) → 𝛼 s 𝒮 et Δ 1 / → s 𝒮 et \textup{Fun}([1],s{\mathcal{S}\textup{et}})\xrightarrow{\alpha}s{\mathcal{S}\textup{et}}_{\Delta^{1}/}\rightarrow s{\mathcal{S}\textup{et}}
of our left adjoint with the evident forgetful functor simply as Fun ( [ 1 ] , s 𝒮 et ) → α ′ s 𝒮 et \textup{Fun}([1],s{\mathcal{S}\textup{et}})\xrightarrow{\alpha^{\prime}}s{\mathcal{S}\textup{et}} . Now, assuming our map 𝚐 1 → 𝚐 2 {\tt g}_{1}\rightarrow{\tt g}_{2} is a cofibration in Fun ( [ 1 ] , s 𝒮 et Joyal ) Reedy \textup{Fun}([1],s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}} , then its image α ′ ( 𝚐 1 ) → α ′ ( 𝚐 2 ) \alpha^{\prime}({\tt g}_{1})\rightarrow\alpha^{\prime}({\tt g}_{2}) fits into the diagram
𝚉 2 ⋆ Δ { 1 } {\lx@inpgf@ignorespaces{\tt Z}_{2}\star\Delta^{\{1\}}} 𝚆 2 ⋆ Δ { 1 } {\lx@inpgf@ignorespaces{\tt W}_{2}\star\Delta^{\{1\}}} ( 𝚆 1 ∐ 𝚉 1 𝚉 2 ) ⋆ Δ { 1 } {\lx@inpgf@ignorespaces\left({\tt W}_{1}\underset{{\tt Z}_{1}}{\coprod}{\tt Z}_{2}\right)\star\Delta^{\{1\}}} 𝚉 1 ⋆ Δ { 1 } {\lx@inpgf@ignorespaces{\tt Z}_{1}\star\Delta^{\{1\}}} 𝚆 1 ⋆ Δ { 1 } {\lx@inpgf@ignorespaces{\tt W}_{1}\star\Delta^{\{1\}}} 𝚉 2 ⋆ Δ 1 {\lx@inpgf@ignorespaces{\tt Z}_{2}\star\Delta^{1}} α ′ ( 𝚐 2 ) {\lx@inpgf@ignorespaces\alpha^{\prime}({\tt g}_{2})} 𝚉 1 ⋆ Δ 1 {\lx@inpgf@ignorespaces{\tt Z}_{1}\star\Delta^{1}} α ′ ( 𝚐 1 ) {\lx@inpgf@ignorespaces\alpha^{\prime}({\tt g}_{1})} ≈ ? \scriptstyle{\lx@inpgf@ignorespaces\stackrel{{\scriptstyle?}}{{\approx}}} ≈ ? \scriptstyle{\lx@inpgf@ignorespaces\stackrel{{\scriptstyle?}}{{\approx}}} ≈ ? \scriptstyle{\lx@inpgf@ignorespaces\stackrel{{\scriptstyle?}}{{\approx}}} ≈ ? \scriptstyle{\lx@inpgf@ignorespaces\stackrel{{\scriptstyle?}}{{\approx}}} ≈ ? \scriptstyle{\lx@inpgf@ignorespaces\stackrel{{\scriptstyle?}}{{\approx}}}
Figure 3. The diagram in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} used in the proof of Theorem 3.3 .
in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} of Figure 3 , in which
•
the front and back faces are pushouts by definition;
•
the quadrilateral contained in the top face is a pushout since in the composite
s 𝒮 et → − ⋆ Δ { 1 } s 𝒮 et Δ { 1 } / → s 𝒮 et s{\mathcal{S}\textup{et}}\xrightarrow{-\star\Delta^{\{1\}}}s{\mathcal{S}\textup{et}}_{\Delta^{\{1\}}/}\rightarrow s{\mathcal{S}\textup{et}}
where the second functor is forgetful,
–
the first functor commutes with colimits by [Lur09 , Remark 1.2.8.2] and
–
the second functor commutes with pushouts since the walking span N − 1 ( Λ 0 2 ) ∈ 𝒞 at \textup{N}^{-1}(\Lambda^{2}_{0})\in{\mathcal{C}\textup{at}} has an initial object
(although really we have only rewritten this pushout to improve readability), and the dotted arrow is then the induced map;
•
the left face is a pushout by inspection;
•
all maps labeled as cofibrations are such
–
–
by the assumption that 𝚐 1 → 𝚐 2 {\tt g}_{1}\rightarrow{\tt g}_{2} is a cofibration in Fun ( [ 1 ] , s 𝒮 et Joyal ) Reedy \textup{Fun}([1],s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}} ,
–
because 𝐂 Joyal ⊂ s 𝒮 et {\bf C}_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}} is closed under pushouts, or
–
because 𝐂 Joyal ⊂ s 𝒮 et {\bf C}_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}} is closed under composition;
and
•
the maps labeled with the symbol ≈ ? \stackrel{{\scriptstyle?}}{{\approx}} are weak equivalences in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} if 𝚐 1 → 𝚐 2 {\tt g}_{1}\rightarrow{\tt g}_{2} is additionally a weak equivalence in Fun ( [ 1 ] , s 𝒮 et Joyal ) Reedy \textup{Fun}([1],s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}}
–
by the assumption that 𝚐 1 → 𝚐 2 {\tt g}_{1}\rightarrow{\tt g}_{2} is an acyclic cofibration in Fun ( [ 1 ] , s 𝒮 et Joyal ) Reedy \textup{Fun}([1],s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}} ,
–
because ( 𝐖 ∩ 𝐂 ) Joyal ⊂ s 𝒮 et ({\bf W}\cap{\bf C})_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}} is closed under pushouts, or
–
because ( 𝐖 ∩ 𝐂 ) Joyal ⊂ s 𝒮 et ({\bf W}\cap{\bf C})_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}} is closed under composition.
Now, because the left and back faces are both pushouts, then the composite rectangle which they form is also a pushout. But this is the same as the composite rectangle formed by the front and right faces. As the front face is a pushout, it follows that the right face is also a pushout as well. Thus, the functor
Fun ( [ 1 ] , s 𝒮 et Joyal ) Reedy → α ′ s 𝒮 et Joyal \textup{Fun}([1],s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}}\xrightarrow{\alpha^{\prime}}s{\mathcal{S}\textup{et}}_{\textup{Joyal}}
preserves both cofibrations and acyclic cofibrations, since these are each closed under pushout in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} . But the cofibrations and acyclic cofibrations in ( s 𝒮 et Joyal ) Δ 1 / (s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\Delta^{1}/} are created by the forgetful functor s 𝒮 et Δ 1 / → s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\Delta^{1}/}\rightarrow s{\mathcal{S}\textup{et}}_{\textup{Joyal}} , and so the functor
Fun ( [ 1 ] , s 𝒮 et Joyal ) Reedy → 𝛼 ( s 𝒮 et Joyal ) Δ 1 / \textup{Fun}([1],s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}}\xrightarrow{\alpha}(s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\Delta^{1}/}
is indeed a left Quillen functor, as claimed.
We now return to our given composite
Δ 1 → 𝚏 𝙴 ↠ 𝚙 𝙱 \Delta^{1}\xrightarrow{{\tt f}}{\tt E}\stackrel{{\scriptstyle{\tt p}}}{{\twoheadrightarrow}}{\tt B}
in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} . This can be considered as defining a fibration in ( s 𝒮 et Joyal ) Δ 1 / (s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\Delta^{1}/} , and hence applying our right Quillen functor
( s 𝒮 et Joyal ) Δ 1 / → 𝛽 Fun ( [ 1 ] , s 𝒮 et Joyal ) Reedy (s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\Delta^{1}/}\xrightarrow{\beta}\textup{Fun}([1],s{\mathcal{S}\textup{et}}_{\textup{Joyal}})_{\textup{Reedy}}
yields another fibration. In particular, the resulting relative matching map
𝙴 / 𝚏 → 𝙴 / 𝚏 ( 1 ) × 𝙱 / 𝚙 ( 𝚏 ( 1 ) ) 𝙱 / 𝚙 ( 𝚏 ) {\tt E}_{/{\tt f}}\rightarrow{\tt E}_{/{\tt f}(1)}\underset{{\tt B}_{/{\tt p}({\tt f}(1))}}{\times}{\tt B}_{/{\tt p}({\tt f})}
at the object 1 ∈ [ 1 ] 1\in[1] must lie in 𝐅 Joyal ⊂ s 𝒮 et {\bf F}_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}} , as desired.
∎
0MWL
Proof. Suppose we are given any edge 𝚏 ∈ 𝙱 1 {\tt f}\in{\tt B}_{1} . Let us write δ 0 ( 𝚏 ) = 𝚋 2 ∈ 𝙱 0 \delta_{0}({\tt f})={\tt b}_{2}\in{\tt B}_{0} and δ 1 ( 𝚏 ) = 𝚋 1 ∈ 𝙱 0 \delta_{1}({\tt f})={\tt b}_{1}\in{\tt B}_{0} . Suppose further that we are given any vertex 𝚎 2 ∈ 𝙴 0 {\tt e}_{2}\in{\tt E}_{0} with 𝚙 ( 𝚎 2 ) = 𝚋 2 {\tt p}({\tt e}_{2})={\tt b}_{2} . Then we must find a JL-𝚙 {\tt p} -cartesian lift of the edge 𝚏 ∈ 𝙱 1 {\tt f}\in{\tt B}_{1} relative to the vertex 𝚎 2 ∈ 𝙴 0 {\tt e}_{2}\in{\tt E}_{0} .
Let us respectively write e 1 → f ~ e 2 e_{1}\xrightarrow{\tilde{f}}e_{2} and b 1 → 𝑓 b 2 b_{1}\xrightarrow{f}b_{2} for the morphisms in ℰ \mathcal{E} and ℬ \mathcal{B} presented by the maps Δ 1 → 𝚏 ~ 𝙴 \Delta^{1}\xrightarrow{\tilde{{\tt f}}}{\tt E} and Δ 1 → 𝚏 𝙱 \Delta^{1}\xrightarrow{{\tt f}}{\tt B} in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} (for any choice of edge 𝚏 ~ ∈ 𝙴 1 \tilde{{\tt f}}\in{\tt E}_{1} ). Then, according to Theorem 3.3 , for an edge 𝚏 ~ ∈ 𝙴 1 \tilde{{\tt f}}\in{\tt E}_{1} to be 𝚙 {\tt p} -cartesian, it suffices to verify that the morphism f ~ \tilde{f} in ℰ \mathcal{E} is p p -cartesian.
Now, the given data define a vertex
( 𝚏 , 𝚎 2 ) ∈ ( hom ¯ ( Δ 1 , 𝙱 ) × ev 1 , 𝙱 , 𝚙 𝙴 ) 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 s 𝒮 et s{\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 s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} . Hence, this vertex defines an object
( f , b 2 ) ∈ Fun ( [ 1 ] , ℬ ) × t , ℬ , p ℰ (f,b_{2})\in\textup{Fun}([1],\mathcal{B})\underset{t,\mathcal{B},p}{\times}\mathcal{E}
of the pullback in 𝒞 at ∞ {{\mathcal{C}\textup{at}}_{\infty}} .
Next, it is easy to check that the map
hom ¯ ( Δ 1 , 𝙴 ) → hom ¯ ( Δ 1 , 𝚙 ) hom ¯ ( Δ 1 , 𝙱 ) \underline{\hom}(\Delta^{1},{\tt E})\xrightarrow{\underline{\hom}(\Delta^{1},{\tt p})}\underline{\hom}(\Delta^{1},{\tt B})
lies in 𝐅 Joyal ⊂ s 𝒮 et {\bf F}_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}} , simply by using
•
the fact that 𝐅 Joyal = rlp ( ( 𝐖 ∩ 𝐂 ) Joyal ) {\bf F}_{\textup{Joyal}}=\textup{rlp}(({\bf W}\cap{\bf C})_{\textup{Joyal}}) ,
•
the adjunction − × Δ 1 : s 𝒮 et ⇄ s 𝒮 et : hom ¯ s 𝒮 et ( Δ 1 , − ) -\times\Delta^{1}:s{\mathcal{S}\textup{et}}\rightleftarrows s{\mathcal{S}\textup{et}}:\underline{\hom}_{s{\mathcal{S}\textup{et}}}(\Delta^{1},-) , and
•
the fact that s 𝒮 et Joyal → − × Δ 1 s 𝒮 et Joyal s{\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
hom ¯ ( Δ 1 , 𝙴 ) → ev 1 𝙴 \underline{\hom}(\Delta^{1},{\tt E})\xrightarrow{\textup{ev}_{1}}{\tt E}
also lies in 𝐅 Joyal ⊂ s 𝒮 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 𝙴 → id 𝙴 𝙴 {\tt E}\xrightarrow{\textup{id}_{{\tt E}}}{\tt E} in s 𝒮 et Joyal f s{\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 s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} . Thus, our conditions that δ 0 ( 𝚏 ~ ) = 𝚎 2 \delta_{0}(\tilde{{\tt f}})={\tt e}_{2} and that 𝚙 ( 𝚏 ~ ) = 𝚏 {\tt p}(\tilde{{\tt f}})={\tt f} translate into the single condition that 𝚏 ~ ∈ 𝙴 1 \tilde{{\tt f}}\in{\tt E}_{1} define a vertex of the limit
lim ( Δ 0 hom ¯ ( Δ 1 , 𝙴 ) 𝙴 Δ 0 hom ¯ ( Δ 1 , 𝙱 ) 𝚎 2 ev 1 hom ¯ ( Δ 1 , 𝚙 ) 𝚏 ) \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}}}{{}{}{{
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in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} .
Now, we claim that the above limit is in fact a homotopy limit in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} . For this, we appeal to a more elaborate version of the Reedy trick: we endow the category
N − 1 ( sd 2 ( Δ 1 ) ) = ( ∙ → ∙ ← ∙ → ∙ ← ∙ ) ∈ 𝒞 at \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 ( 0 → 1 ← 2 → 1 ← 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 : s 𝒮 et Joyal ⇄ Fun ( N − 1 ( sd 2 ( Δ 1 ) ) , s 𝒮 et Joyal ) 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 Fun ( N − 1 ( sd 2 ( Δ 1 ) ) , s 𝒮 et Joyal ) 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
hom ¯ ( Δ 1 , 𝙴 ) → ( ev 1 , hom ¯ ( Δ 1 , 𝚙 ) CLOSE 𝙴 × hom ¯ ( Δ 1 , 𝙱 ) \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 𝐅 Joyal ⊂ s 𝒮 et {\bf F}_{\textup{Joyal}}\subset s{\mathcal{S}\textup{et}} . For this, we use the characterization 𝐅 Joyal = rlp ( ( 𝐖 ∩ 𝐂 ) Joyal ) {\bf F}_{\textup{Joyal}}=\textup{rlp}(({\bf W}\cap{\bf C})_{\textup{Joyal}}) : given any solid commutative square
𝚈 {\lx@inpgf@ignorespaces{\tt Y}} hom ¯ ( Δ 1 , 𝙴 ) {\lx@inpgf@ignorespaces\underline{\hom}(\Delta^{1},{\tt E})} 𝚉 {\lx@inpgf@ignorespaces{\tt Z}} 𝙴 × hom ¯ ( Δ 1 , 𝙱 ) {\lx@inpgf@ignorespaces{\tt E}\times\underline{\hom}(\Delta^{1},{\tt B})} 𝚚 \scriptstyle{\lx@inpgf@ignorespaces{\tt q}} ≈ \scriptstyle{\lx@inpgf@ignorespaces\approx} ( ev 1 , hom ¯ ( Δ 1 , 𝚙 ) CLOSE \scriptstyle{\lx@inpgf@ignorespaces(\textup{ev}_{1},\underline{\hom}(\Delta^{1},{\tt p})}
in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} , unwinding the definitions we see that a dotted lift is equivalent to a dotted lift in the diagram
( 𝚈 × Δ 1 ) ∐ Δ { 1 } , 𝚈 , 𝚚 𝚉 {\lx@inpgf@ignorespaces({\tt Y}\times\Delta^{1})\underset{\Delta^{\{1\}},{\tt Y},{\tt q}}{\coprod}{\tt Z}} 𝙴 {\lx@inpgf@ignorespaces{\tt E}} 𝚉 × Δ 1 {\lx@inpgf@ignorespaces{\tt Z}\times\Delta^{1}} 𝙱 {\lx@inpgf@ignorespaces{\tt B}} 𝚙 \scriptstyle{\lx@inpgf@ignorespaces{\tt p}}
in s 𝒮 et s{\mathcal{S}\textup{et}} . But it is easy to see that the left map lies in ( 𝐖 ∩ 𝐂 ) Joyal ({\bf W}\cap{\bf C})_{\textup{Joyal}} , while the right map lies in 𝐅 Joyal {\bf F}_{\textup{Joyal}} by assumption. Hence the diagram in the above limit defines a fibrant object of Fun ( N − 1 ( sd 2 ( Δ 1 ) ) , s 𝒮 et Joyal ) 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 s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} and thus presents the limit
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in 𝒞 at ∞ {{\mathcal{C}\textup{at}}_{\infty}} .
Now, we have assumed that p p is a cartesian fibration, so in particular there must exist a p p -cartesian lift f ~ \tilde{f} of f f relative to the object e 2 e_{2} . This defines an object of the above limit in 𝒞 at ∞ {{\mathcal{C}\textup{at}}_{\infty}} , which must therefore be represented by a vertex of the above homotopy limit in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} : this selects the desired JL-𝚙 {\tt p} -cartesian lift 𝚏 ~ ∈ 𝙴 1 \tilde{{\tt f}}\in{\tt E}_{1} of 𝚏 ∈ 𝙱 1 {\tt f}\in{\tt B}_{1} relative to 𝚎 2 ∈ 𝙴 0 {\tt e}_{2}\in{\tt E}_{0} . So the map 𝙴 ↠ 𝚙 𝙱 {\tt E}\stackrel{{\scriptstyle{\tt p}}}{{\twoheadrightarrow}}{\tt B} in s 𝒮 et Joyal s{\mathcal{S}\textup{et}}_{\textup{Joyal}} is indeed a JL-cartesian fibration, as claimed.
∎