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arXiv:1905.06671v1 [math.AT] 16 May 2019

2-Segal objects and algebras in spans

Walker H. Stern
Abstract.

We define a category parameterizing Calabi-Yau algebra objects in an infinity category of spans. Using this category, we prove that there are equivalences of infinity categories relating, firstly: 2-Segal simplicial objects in C to algebra objects in Span(C); and secondly: 2-Segal cyclic objects in C to Calabi-Yau algebra objects in Span(C).

Introduction

2-Segal objects and associativity

A familiar concept in higher category theory is that of Segal objects in an \infty-category 𝒞\mathcal{C}, that is, simplicial objects X:Δop𝒞X:\Delta^{\operatorname{op}}\to\mathcal{C} such that the natural map

XnX1×X0X1×X0×X0X1×n.X_{n}\to\overbrace{X_{1}\times_{X_{0}}X_{1}\times_{X_{0}}\cdots\times_{X_{0}}X_{1}}^{\times n}.

is an equivalence. Introduced by Rezk in [16], Segal objects show up in a variety of guises, from monoidal \infty-categories (cf. [11]) to the nerves of 1-categories. Of particular interest is the algebraic content of the Segal condition. Given a Segal set XX, the span

(1) X1×X0X1X2X1X_{1}\times_{X_{0}}X_{1}\leftarrow X_{2}\to X_{1}

can be read as a multiplication law, owing to the invertibility of the left hand morphism. Moreover, the Segal condition on higher simplices also expresses the associativity of this multiplication.

The Segal condition on a simplicial set was generalized to the ‘higher-dimensional’ 2-Segal condition by Dyckerhoff and Kapranov [5] and Gálvez-Carrillo, Kock, and Tonks [9] (2-Segal spaces are called decomposition spaces in the latter). In a sense, the 2-Segal condition no longer requires that the span (1) define a multiplication, but retains the higher associativity conditions encoded in the higher simplices. More precisely, the 2-Segal condition on a simplicial object X:Δop𝒞X:\Delta^{\operatorname{op}}\to\mathcal{C} requires that the diagrams

Xn{\lx@inpgf@ignorespaces X_{n}}Xi,,j{\lx@inpgf@ignorespaces X_{i,\ldots,j}}X1,i,j,{\lx@inpgf@ignorespaces X_{1,\ldots i,j,\ldots}}Xi,j{\lx@inpgf@ignorespaces X_{i,j}}

all be pullback diagrams in 𝒞\mathcal{C}. The 2-Segal condition is indeed a generalization of the Segal condition, insofar as every Segal simplicial object is 2-Segal.

A 2-Segal object XX is said to be unital if, additionally, the diagrams

Xn1{\lx@inpgf@ignorespaces X_{n-1}}Xn{\lx@inpgf@ignorespaces X_{n}}Xi{\lx@inpgf@ignorespaces X_{i}}Xi,i+1{\lx@inpgf@ignorespaces X_{i,i+1}}

are pullback in 𝒞\mathcal{C}. Throughout this paper, we will use the term ‘2-Segal object’ to refer to a unital 2-Segal object in the terminology of [5].

The sense in which such structures encode associativity relies on thinking of spans

X1×X1××X1{\lx@inpgf@ignorespaces X_{1}\times X_{1}\times\cdots\times X_{1}}Xn{\lx@inpgf@ignorespaces X_{n}}X1{\lx@inpgf@ignorespaces X_{1}}

as ‘nn-fold multiplications’, regardless of whether the left-hand morphisms are equivalences. We then compose by concatenating spans and taking a pullback, thinking of the result as a ‘space of compositions’. In this language, the 2-Segal condition says that the space of compositions of nn-fold multiplications with mm-fold multiplications is precisely the space of n+m1n+m-1-fold multiplications.

There are a number of ways to make this intuitive picture rigorous (see, for example, the relation to Hall algebras presented in [5], and the connection with operads from [17]). The present paper concerns itself with one such perspective, namely, considering the relation between 2-Segal objects in an \infty-category 𝒞\mathcal{C} and algebra objects in an \infty-category Span(𝒞)\operatorname{Span}(\mathcal{C}) whose morphisms are spans in 𝒞\mathcal{C}. Several results in this direction have already appeared in the literature. In the original Dyckerhoff-Kapranov paper [5], monads and algebra objects in (,2)(\infty,2)-categories of spans were constructed from 2-Segal objects. More recently, Penney [15] defined lax algebras in spans coming from simplicial objects, and showed that the associativity of these lax algebras was equivalent to the 2-Segal condition. In this paper, we restrict to \infty-categories of spans, and prove:

Theorem A.

Let 𝒞\mathcal{C} be an \infty-category with small limits. There is an equivalence of \infty-categories

{Algebra objectsin Span(𝒞)}{2-Segal simplicalobjects in 𝒞}.\left\{\begin{subarray}{c}\text{Algebra objects}\\ \text{in }\operatorname{Span}(\mathcal{C})\end{subarray}\right\}\simeq\left\{\begin{subarray}{c}\text{2-Segal simplical}\\ \text{objects in }\mathcal{C}\end{subarray}\right\}.

This theorem appears in full detail in the text as Theorem 2.25. The functoriality of Theorem 2.25 is somewhat unusual. The \infty-category Span(𝒞)\operatorname{Span}(\mathcal{C}) is defined via an adjunction as is [5]. Morphisms of algebra objects in Span(𝒞)\operatorname{Span}(\mathcal{C}) are then defined to be natural transformations of the corresponding adjoint diagram in 𝒞\mathcal{C}, rather than natural transformations in Span(𝒞)\operatorname{Span}(\mathcal{C}).

Polygons, surfaces, and topological field theories

There is an additional geometric intuition underlying the 2-Segal condition. Fix a standard n+1n+1-gon PnP_{n}, and a simplicial object X:Δop𝒞X:\Delta^{\operatorname{op}}\to\mathcal{C}. The set of vertices VnV_{n} of PnP_{n} defines a simplicial set ΔVn\Delta^{V_{n}}. For any triangulation 𝒯\mathcal{T} of PnP_{n} with vertices in PnP_{n}, one can define a simplicial subset Δ𝒯ΔVn\Delta^{\mathcal{T}}\subset\Delta^{V_{n}} whose 2-simplices correspond to the triangles in 𝒯\mathcal{T}. Taking limits of the simplicial object XX over the corresponding categories of simplices, the inclusion Δ𝒯ΔVn\Delta^{\mathcal{T}}\subset\Delta^{V_{n}} yields a morphism

XnlimΔ/Δ𝒯Xk.X_{n}\to\lim_{\Delta_{/\Delta^{\mathcal{T}}}}X_{k}.

By [5, Proposition 2.3.2], the 2-Segal condition is equivalent to the condition that this morphism be an equivalence for every n2n\geq 2 and every such triangulation 𝒯\mathcal{T} of PnP_{n}. Intuitively, this means that the 2-Segal condition allows one to glue together the XnX_{n} to get invariants of 2-dimensional simplicial complexes.

The connection of 2-Segal spaces to 2-dimensional geometry can be extended further with recourse to 2-Segal cyclic objects, that is cyclic objects in 𝒞\mathcal{C} whose underlying simplicial objects are 2-Segal. In [4, Section V.2], Dyckerhoff and Kapranov construct invariants X(S,M)X(S,M) of stable marked surface (S,M)(S,M) with boundary, associated to a 2-Segal cyclic object X:Λop𝒞X:\Lambda^{\operatorname{op}}\to\mathcal{C}. For the subset NMN\subset M of marked points on the boundary of SS, this invariant comes equipped with a projection X(S,M)X1|M|X(S,M)\to X_{1}^{|M|}. More suggestively, if we label some of these marked points as ‘incoming’ and the rest as ‘outgoing’, we can read the invariant X(S,M)X(S,M) as a span

X1|Nin|X(S,M)X1|Nout|.X_{1}^{|N_{\operatorname{in}}|}\leftarrow X(S,M)\rightarrow X_{1}^{|N_{\operatorname{out}}|}.

Moreover, the X(S,M)X(S,M) come equipped with coherent actions of the mapping class group. It is therefore natural to ask whether the invariants X(S,M)X(S,M) form an open, oriented, \infty-categorical topological field theory in Span(𝒞)\operatorname{Span}(\mathcal{C}).

Such open, oriented theories have attracted some attention in the literature already. In [2], Costello considers open oriented theories equipped with a set of D-branes and valued in the (dg-)category of chain complexes. He shows that such field theories are equivalent to Calabi-Yau AA_{\infty} categories — a generalization of the Calabi-Yau algebras in chain complexes. A similar classification which has more bearing on the situation detailed above, is that of Lurie:

Theorem ([14, Theorem 4.2.11]).

Let 𝒞\mathcal{C} be a symmetric monoidal \infty-category. The following types of data are equivalent:

  1. (1)

    Open oriented topological field theories in 𝒞\mathcal{C}.

  2. (2)

    Calabi-Yau algebra objects in 𝒞\mathcal{C}.

Based on this theorem, the latter half of this paper seeks to relate cyclic 2-Segal objects to Calabi-Yau algebras. Such a relation is realized by:

Theorem B.

Let 𝒞\mathcal{C} be an \infty-category with small limits. There is an equivalence of \infty-categories

{Calabi-YauAlgebra objectsin Span(𝒞)}{2-Segal cyclicobjects in 𝒞}.\left\{\begin{subarray}{c}\text{Calabi-Yau}\\ \text{Algebra objects}\\ \text{in }\operatorname{Span}(\mathcal{C})\end{subarray}\right\}\simeq\left\{\begin{subarray}{c}\text{2-Segal cyclic}\\ \text{objects in }\mathcal{C}\end{subarray}\right\}.

This appears in the text in full detail as Theorem 3.29. As a consequence of Theorem 3.29, we see that 2-Segal cyclic objects in 𝒞\mathcal{C} are equivalent to open oriented topological field theories in 𝒞\mathcal{C}.

Examples and consequences

Once the correspondence of Theorem 3.29 is established, a wealth of avenues to construct topological field theories open up. A number of examples of interest have already been explored in the literature.

  • Per [6], the Waldhausen S-construction also gives rise to many cyclic 2-segal spaces. An interesting special case is discussed in [6, 3, 4], where various versions of topological Fukaya categories are constructed as invariants X(S,M)X(S,M) associated to 2-Segal objects arising from the Waldhausen S-construction.

  • 1-Segal cyclic objects also provide a zoo of interesting examples. As a particular example, consider a morphism f:ABf:A\to B in the \infty-category of spaces 𝒮\mathcal{S}. The Čech nerve of this morphism is the 1-Segal simplicial space

    {\lx@inpgf@ignorespaces\cdots}A×BA×BA{\lx@inpgf@ignorespaces A\times_{B}A\times_{B}A}A×BA{\lx@inpgf@ignorespaces A\times_{B}A}A{\lx@inpgf@ignorespaces A}

    which realizes to BB. An appropriately chosen circle action on BB equips the Čech nerve with a canonical cyclic structure, and similarly, a cyclic structure on the Čech nerve equips its realization with a coherent S1S^{1}-action. Loosely speaking, the surface invariant X(S,M)X(S,M) associated to this cyclic Čech nerve of ff is the space of ‘S1S^{1}-equivariant BB-local systems on the circle bundle of a twisted tangent bundle of (S,M)(S,M) equipped with reduction of structure group to AA over the marked points’. When BB is BSL2()BSL_{2}(\mathbb{R}) and AA is BUBU, where UU is the subgroup of upper unitriangular matrices, this construction can be related to the higher Teichmüller spaces constructed by Fock and Goncharov in [8].

  • Another interesting incarnation of the cyclic Čech nerve construction is its application to a morphism f:Xf:\ast\to X into a connected space XX. In this context, the Čech nerve has the loop space ΩX\Omega X based at f()f(\ast) as its space of 11-simplices, and we expect the resulting surface invariants to relate to string topology.

Theorem 3.29 and Theorem 2.25 also bear an interesting relation to another construction in the literature. Following Cisinski and Moerdijk (cf. [1]), Walde defines a notion of a cyclic \infty-operad in [17], and shows that there are equivalences of \infty-categories

{invertible cyclic-operads}{2-Segal cyclicobjects in 𝒮}\left\{\begin{subarray}{c}\text{invertible cyclic}\\ \infty\text{-operads}\end{subarray}\right\}\simeq\left\{\begin{subarray}{c}\text{2-Segal cyclic}\\ \text{objects in }\mathcal{S}\end{subarray}\right\}

and

{invertible-operads}{2-Segal simplicialobjects in 𝒮}.\left\{\begin{subarray}{c}\text{invertible}\\ \infty\text{-operads}\end{subarray}\right\}\simeq\left\{\begin{subarray}{c}\text{2-Segal simplicial}\\ \text{objects in }\mathcal{S}\end{subarray}\right\}.

Which now has the immediate implication of relating invertible (cyclic) \infty-operads to (Calabi-Yau) algebras in Span(𝒮)\operatorname{Span}(\mathcal{S}).

There are also a number of possible generalizations of Theorems 2.25 and 3.29. For instance, the cyclic category Λ\Lambda is one example of a crossed simplicial group, a notion defined by Fiedorowicz and Loday [7] and Krasauskas [10]. In [4], invariants analogous to the X(S,M)X(S,M) were constructed for functors X:Δ𝔊op𝒞X:\Delta\mathfrak{G}^{\operatorname{op}}\to\mathcal{C} satisfying the 2-Segal condition, where Δ𝔊\Delta\mathfrak{G} is a crossed simplicial group. We expect that the relation between open topological field theories in spans and 2-Segal cyclic objects generalizes to this additional structure, which will be the basis for some future work on the subject.

Acknowledgements

I thank my doctoral advisor, Tobias Dyckerhoff for his advice and guidance. I am also grateful to the Max Planck Institute for Mathematics in Bonn and the Universität Hamburg for supporting my studies.

1. The menagerie: notations, conventions, and constructions

In this section, we will lay out the fundamental definitions and constructions that will be used in the proof of the main result. Along the way, we will also prove basic relations between these definitions, to alleviate the density of later arguments.

1.1. Linear and cyclic orders

Definition 1.1.

The simplex category Δ\Delta has objects the standard linearly ordered sets [n]={0,1,,n}[n]=\{0,1,\ldots,n\} for n0n\geq 0 and morphisms the order-preserving maps. The enlarged simplex category \bbDelta has objects finite non-empty linearly ordered sets, and morphisms order-preserving maps.

The augmented simplex category Δ+\Delta_{+} (resp. the augmented simplex category +\bbDelta_{+}) is obtained from Δ\Delta (resp. \bbDelta) by appending an initial object \emptyset, which will also sometimes be denoted by [1][-1].

The interval category \nabla is the subcategory of Δ\Delta on the objects [n][n] for n1n\geq 1, the morphisms of which preserve maximal and minimal elements. The enlarged interval category \bbDelta is the subcategory of \bbDelta on those sets of cardinality 2\geq 2, whose morphisms preserve maximal and minimal elements.

The augmented interval category +\nabla_{+} (resp. the augmented extended interval category +\text{\raisebox{0.0pt}{\scalebox{1}[-1]{$\bbDelta$}}}_{+}) is the subcategory of Δ\Delta (resp. \bbDelta) whose objects have cardinality 1\geq 1 and whose morphisms preserve the maximal and minimal elements. ∎

Definition 1.2.

The category of the standard finite sets n¯:={1,2,,n}\underline{n}:=\{1,2,\ldots,n\} for n0n\geq 0 will be denoted Fin\operatorname{Fin}. The category of the standard finite pointed sets n:=n¯{}\langle n\rangle:=\underline{n}\amalg\{\ast\} will be denoted Fin\operatorname{Fin}_{\ast}. The category of all finite sets (resp. the category of all finite points sets) will be denoted by 𝔽in\mathbb{F}\!\!\operatorname{in} (resp. by 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast}). When convenient, we will denote by \bbGamma (resp. by Γ\Gamma) the opposites of the categories 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast} (resp. Fin\operatorname{Fin}_{\ast}). Given a pointed set S𝔽inS\in\mathbb{F}\!\!\operatorname{in}_{\ast}, we denote by SS^{\circ} the set S{}S\setminus\{\ast\}, where \ast denotes the basepoint of SS.

We additionally denote by 𝒜ss\mathcal{A}\!\operatorname{ss} the associative operad, i.e. the category whose objects are objects of 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast}, and whose morphisms ϕ:ST\phi:S\to T are morphisms in 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast} equipped with a chosen linear order on the fiber ϕ1(i)\phi^{-1}(i) for each iTi\in T^{\circ}. Composition is defined by composition in 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast}, together with the lexicographic orders. Note that there is a forgetful functor 𝒜ss𝔽in\mathcal{A}\!\operatorname{ss}\to\mathbb{F}\!\!\operatorname{in}_{\ast}, which equips N(𝒜ss)N(\mathcal{A}\!\operatorname{ss}) with the structure of an \infty-operad in the sense of [12]. ∎

Construction 1.3 (Linear interstices).

Given a linearly ordered set SS\in\bbDelta we define an inner interstice of SS to be an ordered pair (k,k+1)S×S(k,k+1)\in S\times S, where k+1k+1 denotes the successor to kk. The set of inner interstices of SS is, itself, a linearly ordered set, with the order

(k,k+1)(j,j+1)kj(k,k+1)\leq(j,j+1)\Leftrightarrow k\leq j

We will denote the linearly ordered set of inner interstices of SS by 𝕀(S)\mathbb{I}(S). Note that 𝕀([0])=\mathbb{I}([0])=\emptyset.

Given a linearly ordered set S+S\in\bbDelta_{+}, let S^\hat{S} be the set {a}S{b}\{a\}\amalg S\amalg\{b\}, where bb is taken to be maximal and aa minimal. We define an outer interstice of SS to be an inner interstice of S^\hat{S}. We will denote the linearly ordered set of outer interstices of SS by 𝕆(S)\mathbb{O}(S). Note that 𝕆()={(a,b)}\mathbb{O}(\emptyset)=\{(a,b)\}.

We define functors

𝕆:+op+;S𝕆(S)\mathbb{O}:\bbDelta_{+}^{{\operatorname{op}}}\to\text{\raisebox{0.0pt}{\scalebox{1}[-1]{$\bbDelta$}}}_{+};\quad S\mapsto\mathbb{O}(S)

and

𝕀:+op;S𝕀(S)\mathbb{I}:\text{\raisebox{0.0pt}{\scalebox{1}[-1]{$\bbDelta$}}}_{+}^{\operatorname{op}}\to\bbDelta;\quad S\mapsto\mathbb{I}(S)

as follows (we will define 𝕆\mathbb{O} explicitly, the definition of 𝕀\mathbb{I} is similar). Given a morphism f:STf:S\to T in +\bbDelta_{+}, we define a morphism 𝕆(f):𝕆(S)𝕆(T)\mathbb{O}(f):\mathbb{O}(S)\to\mathbb{O}(T) by setting

𝕆(f)(j,j+1)={(k,k+1)f(k)jj+1f(k+1)(a,a+1)jf(k)kS(b1,b)jf(k)kS.\mathbb{O}(f)(j,j+1)=\begin{cases}(k,k+1)&f(k)\leq j\leq j+1\leq f(k+1)\\ (a,a+1)&j\leq f(k)\;\forall k\in S\\ (b-1,b)&j\geq f(k)\;\forall k\in S.\end{cases}

Pictorially, we can represent the morphism 𝕆(f)\mathbb{O}(f) as a forest as in Fig. 1, thinking leaves j𝕆(T)j\in\mathbb{O}(T) as being attached to the root k𝕆(S)k\in\mathbb{O}(S) if 𝕆(f)(j)=k\mathbb{O}(f)(j)=k.

a0a_{0}a1a_{1}a2a_{2}a3a_{3}b0b_{0}b1b_{1}b2b_{2}b3b_{3}b4b_{4}
a0a_{0}a1a_{1}a2a_{2}a3a_{3}b0b_{0}b1b_{1}b2b_{2}b3b_{3}b4b_{4}
Figure 1. Left: a morphism ff of linearly ordered sets. Right: the morphism 𝕆(f)\mathbb{O}(f), visualized as a forest (blue).

Note that the functors 𝕀\mathbb{I} and 𝕆\mathbb{O} define an equivalence of categories. Since Δ+\Delta_{+} (resp. +\nabla_{+}) is the skeletal version of +\bbDelta_{+} (resp. +\text{\raisebox{0.0pt}{\scalebox{1}[-1]{$\bbDelta$}}}_{+}), all isomorphisms in these categories are identities, we see that we get an induced isomorphism of categories

O:Δ+op+:IO:\Delta_{+}^{\operatorname{op}}\overset{\cong}{\longleftrightarrow}\nabla_{+}:I

Moreover, we can define a functor +Fin\text{\raisebox{0.0pt}{\scalebox{1}[-1]{$\bbDelta$}}}_{+}\to\operatorname{Fin}_{\ast} by

S(S{})/max(S)min(s)S\mapsto(S\amalg\{\ast\})_{/\operatorname{max}(S)\sim\operatorname{min}(s)\sim\ast}

We then find that the induced functor

Δ+opΔ+op𝑂+Fin\Delta_{+}^{{\operatorname{op}}}\hookrightarrow\Delta_{+}^{\operatorname{op}}\overset{O}{\to}\nabla_{+}\to\operatorname{Fin}_{\ast}

is precisely the functor cut:ΔopFin\operatorname{cut}:\Delta^{\operatorname{op}}\to\operatorname{Fin}_{\ast} defined in [12, 4.1.2.9]. ∎

Definition 1.4.

Given two linearly ordered sets S,T+S,T\in\bbDelta_{+} define the ordinal sum STS\oplus T to be the set STS\amalg T equipped with the linear order defined by the orders on SS and TT and the proscription that for all sSs\in S and tTt\in T, sts\leq t. The ordinal sum defines a monoidal structure on +\bbDelta_{+}.

Given two linearly ordered sets S,T+S,T\in\text{\raisebox{0.0pt}{\scalebox{1}[-1]{$\bbDelta$}}}_{+}, with bb the maximum of SS and aa the minimum of TT, define the imbrication STS\star T to be the linearly ordered set (ST)/ab(S\oplus T)_{/a\sim b} (note that since aa is the successor to bb in STS\oplus T, there is a canonical linear order on STS\star T compatible with the quotient map). ∎

Lemma 1.5.

The functor 𝕆\mathbb{O} is a monoidal functor sending the ordinal sum to the imbrication.

Definition 1.6.

A cyclic order on a finite set SS is a transitive \mathbb{Z}-action on SS. Equivalently, this is simply transitive action of /|S|\mathbb{Z}/|S| on SS. ∎

Definition 1.7.

Given a cyclic set SS, and a collection {[ni]}iS\{[n_{i}]\}_{i\in S} of objects in Δ+\Delta_{+}, we define a cyclic set S([ni])\bigcup^{S}([n_{i}]) as follows. The underlying set is iS[ni]\coprod_{i\in S}[n_{i}], and the cyclic order is given by the /n\mathbb{Z}/n-action (where n:=iS(ni+1)n:=\sum_{i\in S}(n_{i}+1)) that sends

j[ni]{j+1j<ni0[ni+1]j=nij\in[n_{i}]\mapsto\begin{cases}j+1&j<n_{i}\\ 0\in[n_{i+1}]&j=n_{i}\end{cases}

where i+1i+1 denotes the successor of ii in the cyclic order on SS. We call this order on iS[ni]\coprod_{i\in S}[n_{i}] the lexicographic (cyclic) order. ∎

Definition 1.8.

A morphism of cyclically ordered sets STS\to T consists of a map of sets ϕ:ST\phi:S\to T, and a linear order on each fiber such that the lexicographic cyclic order on SS agrees with the predefined cyclic order on SS.

The cyclic category has as its objects the standard cyclicly ordered sets n\langle n\rangle for n0n\geq 0, and as its morphisms the maps of finite sets respecting the cyclic order. The enlarged cyclic category \bbLambda has as its objects all finite, non-empty, cyclically ordered sets, and as its morphisms the maps which respect the cyclic order. ∎

Construction 1.9 (Cyclic Duality).

In analogy to the construction of the linear interstice functors, we define a duality

𝔻:op\mathbb{D}:\bbLambda^{{\operatorname{op}}}\to\bbLambda

on the cyclic category. Let SS\in\bbLambda be a cyclicly ordered set. We define a cyclic interstice of SS to be an ordered pair (a,a+1)S×S(a,a+1)\in S\times S, where a+1a+1 denotes the successor of aa under the cyclic order. We denote the set of cyclic interstices of SS by 𝔻(S)\mathbb{D}(S). The set 𝔻(S)\mathbb{D}(S) inherits a canonical cyclic order from SS, which can be visualized as in Fig. 2.

×\times×\times×\times×\times×\times×\times
Figure 2. A cyclic set with its cyclic order visualized via an embedding into the oriented circle (black), together with its set of cyclic interstices (blue crosses).

The functor 𝔻\mathbb{D} is specified on morphisms by an analogue of Construction 1.3, namely, for f:STf:S\to T in \bbLambda, we set

𝔻(f)(j,j+1):=kwhere \mathbb{D}(f)(j,j+1):=k\quad\text{where }

This functor is an equivalence of categories.Since Λ\Lambda is the skeletal version of \bbLambda, 𝔻\mathbb{D} descends to an equivalence D:ΛopΛD:\Lambda^{\operatorname{op}}\to\Lambda

Construction 1.10 (Cyclic closures).

We define a functor 𝕂:\mathbb{K}:\bbDelta\to\bbLambda in the following way. Given a linearly ordered set SS of cardinality n+1n+1, there is a unique order-preserving bijection ϕ:S[n]\phi:S\to[n]. We define a bijection

Sr(n);jexp(2πiϕ(j)n+1)S\to r(n);\quad j\mapsto\exp\left(\frac{2\pi i\phi(j)}{n+1}\right)

to the nthn^{\operatorname{th}} roots of unity in S1S^{1}. The orientation on S1S^{1} then yields a canonical cyclic order on SS. Passing to skeletal versions yields the well-known functor κ:ΔΛ\kappa:\Delta\to\Lambda.

Via the equivalences 𝕆\mathbb{O} and 𝔻\mathbb{D} we can then define a functor :Λ\mathbb{C}:\text{\raisebox{0.0pt}{\scalebox{1}[-1]{$\bbDelta$}}}\to\Lambda such that the diagram

op{\lx@inpgf@ignorespaces\bbDelta^{\operatorname{op}}} \bbDelta op{\lx@inpgf@ignorespaces\bbLambda^{\operatorname{op}}}{\lx@inpgf@ignorespaces\bbLambda}𝕂\scriptstyle{\lx@inpgf@ignorespaces\mathbb{K}}𝕆\scriptstyle{\lx@inpgf@ignorespaces\mathbb{O}}\scriptstyle{\lx@inpgf@ignorespaces\mathbb{C}}𝔻\scriptstyle{\lx@inpgf@ignorespaces\mathbb{D}}

commutes up to natural isomorphism. The functor \mathbb{C} admits the following explicit description on objects. Let SS\in\text{\raisebox{0.0pt}{\scalebox{1}[-1]{$\bbDelta$}}} with maximal element bb and minimal element aa. Then (S)\mathbb{C}(S) can be identified with with quotient of 𝕂(S)\mathbb{K}(S) by the identification aba\sim b. Once again, we have that \mathbb{C} descends to a functor C:ΛC:\nabla\to\Lambda. ∎

Definition 1.11.

Given an object SS\in\bbLambda, a linear order on SS compatible with the cyclic order consists of a pair ([n],ϕ)([n],\phi) consisting of an object [n]Δ[n]\in\Delta, and an isomorphism ϕ:𝕂([n])S\phi:\mathbb{K}([n])\cong S.

We introduce one more equivalent variant of \bbLambda, which we will denote 𝚲\boldsymbol{\Lambda}. The objects of 𝚲\boldsymbol{\Lambda} consist of pairs (S,ϕ)(S,\phi) where SS\in\bbLambda, and ϕ:𝕂([n])S\phi:\mathbb{K}([n])\cong S is a compatible linear order on SS. The morphisms of SS are simply the morphisms of \bbLambda. It is clear that the forgetful functor 𝚲\boldsymbol{\Lambda}\to\bbLambda is an equivalence. ∎

Construction 1.12.

The functor 𝕂\mathbb{K} clearly extends to a functor 𝐊:𝚲\mathbf{K}:\bbDelta\to\boldsymbol{\Lambda} by choosing the identity as the compatible linear order. We can then define functors 𝐃:𝚲op𝚲\mathbf{D}:\boldsymbol{\Lambda}^{\operatorname{op}}\to\boldsymbol{\Lambda} and 𝐂:𝚲\mathbf{C}:\text{\raisebox{0.0pt}{\scalebox{1}[-1]{$\bbDelta$}}}\to\boldsymbol{\Lambda} such that the diagram

op{\lx@inpgf@ignorespaces\bbDelta^{\operatorname{op}}} \bbDelta 𝚲op{\lx@inpgf@ignorespaces\boldsymbol{\Lambda}^{\operatorname{op}}}𝚲{\lx@inpgf@ignorespaces\boldsymbol{\Lambda}}𝕂\scriptstyle{\lx@inpgf@ignorespaces\mathbb{K}}𝐎\scriptstyle{\lx@inpgf@ignorespaces\mathbf{O}}𝐂\scriptstyle{\lx@inpgf@ignorespaces\mathbf{C}}𝐃\scriptstyle{\lx@inpgf@ignorespaces\mathbf{D}}

commutes strictly. ∎

Lemma 1.13.

Let SS\in\bbLambda, a set {[ni]}iS\{[n_{i}]\}_{i\in S} of elements in Δ+\Delta_{+}, and a compatible linear order ϕ:𝕂([m])S\phi:\mathbb{K}([m])\cong S, there is a canonical isomorphism

𝕂(i[m][nϕ(i)])S[ni]\mathbb{K}\left(\bigoplus_{i\in[m]}[n_{\phi(i)}]\right)\cong\bigcup\nolimits^{S}[n_{i}]

which acts as the identity on underlying sets.

Proof.

We compare the /n\mathbb{Z}/n-actions. When ji[m][ni]j\in\bigoplus_{i\in[m]}[n_{i}] is not maximal, the successor function for the ordinal sum agrees with the /n\mathbb{Z}/n-action on S[ni]\bigcup^{S}[n_{i}]. If jj is maximal, we have that the action on the left sends jj to 0nϕ(0)0\in n_{\phi(0)}, which agrees with the definition of the cyclic order on the right. ∎

1.2. Calabi-Yau algebras

Throughout the following section, we take 𝒞𝔽in\mathcal{C}^{\otimes}\to\mathbb{F}\!\!\operatorname{in}_{\ast} to be a symmetric monoidal \infty-category with monoidal unit 1\bbOne and tensor product \otimes.

Construction 1.14.

There is a functor B:𝒜ssB:\bbLambda\to\mathcal{A}\!\operatorname{ss} defined as follows. On objects, send each SS\in\bbLambda to S{}S\amalg\{\ast\}, forgetting the cyclic order. On morphisms, send f:STf:S\to T to its underlying map of sets. Define a linear order on the fibers of ff by choosing embeddings of SS and TT into S1S^{1} compatible with the cyclic order, and representing ff as a commutative diagram

S1{\lx@inpgf@ignorespaces S^{1}}S1{\lx@inpgf@ignorespaces S^{1}}S{\lx@inpgf@ignorespaces S}T{\lx@inpgf@ignorespaces T}f~\scriptstyle{\lx@inpgf@ignorespaces\tilde{f}}α\scriptstyle{\lx@inpgf@ignorespaces\alpha}f\scriptstyle{\lx@inpgf@ignorespaces f}β\scriptstyle{\lx@inpgf@ignorespaces\beta}

where f~\tilde{f} is monotone of degree 1. For iTi\in T, the preimage of β(i)\beta(i) under f~\tilde{f} is an interval, and β(f1(i))f~1(β(i))\beta(f^{-1}(i))\subset\tilde{f}^{-1}(\beta(i)). The orientation of S1S^{1} induces an orientation of f~1(β(i))\tilde{f}^{-1}(\beta(i)), and hence a linear order on f1(i)f^{-1}(i). ∎

Definition 1.15.

The cyclic bar object of an algebra object X:𝒜ss𝒞X:\mathcal{A}\!\operatorname{ss}\to\mathcal{C}^{\otimes} is the composition B(X)B^{\ast}(X). A cyclic trace on XX is a natural transformation η\eta from B(X)B^{\ast}(X) to the constant cyclic object on 1𝒞\bbOne\in\mathcal{C}. We call a pair (X,η)(X,\eta) consisting of an algebra object in 𝒞\mathcal{C}^{\otimes} and a cyclic trace a trace algebra. ∎

Remark 1.16.

A natural transformation to a constant cyclic object may be modeled as a functor from the category \bbLambda_{\diamond} obtained from \bbLambda by formally adjoining a terminal object. We denote the terminal object of \bbLambda_{\diamond} by \diamond. ∎

Definition 1.17.

A morphism γ:XX1\gamma:X\otimes X\to\bbOne in 𝒞\mathcal{C} is called non-degenerate if there exists a morphism η:1XX\eta:\bbOne\to X\otimes X such that

  • The composite

    XX1ηid1XXXid1γ1XXX\overset{\simeq}{\to}X\otimes\bbOne\overset{\eta\otimes{\operatorname{id}}_{\bbOne}}{\longrightarrow}X\otimes X\otimes X\overset{{\operatorname{id}}_{\bbOne}\otimes\gamma}{\longrightarrow}\bbOne\otimes X\overset{\simeq}{\to}X

    is homotopic to the identity.

  • The composite

    X1Xid1ηXXXγid1X1XX\overset{\simeq}{\to}\bbOne\otimes X\overset{{\operatorname{id}}_{\bbOne}\otimes\eta}{\longrightarrow}X\otimes X\otimes X\overset{\gamma\otimes{\operatorname{id}}_{\bbOne}}{\longrightarrow}X\otimes\bbOne\overset{\simeq}{\to}X

    is homotopic to the identity.

Definition 1.18.

Let (X,η)(X,\eta) be a trace algebra in 𝒞\mathcal{C}, and let η2:XX1\eta_{2}:X\otimes X\to\bbOne be the map induced by 2\langle 2\rangle\to\diamond in \bbLambda_{\diamond} under η\eta. We call (X,η)(X,\eta) a Calabi-Yau algebra in 𝒞\mathcal{C} if η2\eta_{2} is non-degenerate. ∎

Remark 1.19.

The definition above is precisely that of [14, Example 4.2.8]. When Hochschild homology is defined, the map η:B(X)1\eta:B^{\ast}(X)\to\bbOne is equivalently an S1S^{1}-equivariant trace

S1X1.\int_{S^{1}}X\to\bbOne.

Definition 1.20.

Let 𝒜ssCY\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}} be the category with

  • Objects ob(𝒜ss){}\operatorname{ob}(\mathcal{A}\!\operatorname{ss})\amalg\{\diamond\}.

  • Morphisms between S,T𝒜ssS,T\in\mathcal{A}\!\operatorname{ss}

    Hom𝒜ssCY(S,T):=Hom𝒜ss(S,T).\operatorname{Hom}_{\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}}(S,T):=\operatorname{Hom}_{\mathcal{A}\!\operatorname{ss}}(S,T).
  • For S𝒜ssS\in\mathcal{A}\!\operatorname{ss},

    Hom𝒜ssCY(,S):=\operatorname{Hom}_{\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}}(\diamond,S):=\emptyset

    and a morphism SS\to\diamond is a choice of a subset TST\subset S^{\circ} and a cyclic order on TT.

  • For S,T𝒜ssS,T\in\mathcal{A}\!\operatorname{ss}, and morphisms ϕ:ST\phi:S\to T and ψ:T\psi:T\to\diamond, the composite ψϕ\psi\circ\phi is given by the induced cyclic order

Note that 𝒜ssCY\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}} comes equipped with a functor 𝒜ssCY𝔽in\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}\to\mathbb{F}\!\!\operatorname{in}_{\ast} sending 1\diamond\mapsto\langle 1\rangle. ∎

Construction 1.21.

Let \bbLambda\to\bbLambda_{\diamond} and 𝒜ss𝒜ssCY\mathcal{A}\!\operatorname{ss}\to\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}} be the inclusions. Define a functor F:𝒜ssCYF:\bbLambda_{\diamond}\to\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}} by setting F=BF=B on \bbLambda\subset\bbLambda_{\diamond}, and sending \diamond\mapsto\diamond. By definition, the diagram

(2) {\lx@inpgf@ignorespaces\bbLambda}{\lx@inpgf@ignorespaces\bbLambda_{\diamond}}𝒜ss{\lx@inpgf@ignorespaces\mathcal{A}\!\operatorname{ss}}𝒜ssCY{\lx@inpgf@ignorespaces\mathcal{A}\!\operatorname{ss}_{C}Y}B\scriptstyle{\lx@inpgf@ignorespaces B}F\scriptstyle{\lx@inpgf@ignorespaces F}

commutes. ∎

Definition 1.22.

We take 𝔓\mathfrak{P} to be the categorical pattern of [12, Proposition 2.1.4.6]. In the following proof, we will freely make reference to this proposition, and Appendix B from the same. ∎

Lemma 1.23.

The diagram

N(){\lx@inpgf@ignorespaces N(\bbLambda)}N(){\lx@inpgf@ignorespaces N(\bbLambda_{\diamond})}N(𝒜ss){\lx@inpgf@ignorespaces N(\mathcal{A}\!\operatorname{ss})}N(𝒜ssCY){\lx@inpgf@ignorespaces N(\mathcal{A}\!\operatorname{ss}_{C}Y)}B\scriptstyle{\lx@inpgf@ignorespaces B}F\scriptstyle{\lx@inpgf@ignorespaces F}

induces an 𝔓\mathfrak{P}-anodyne morphism of \infty-categories

θ:N(𝒜ss)N()N()N(𝒜ssCY)\theta:N(\mathcal{A}\!\operatorname{ss})\coprod_{N(\bbLambda)}N(\bbLambda_{\diamond})\to N(\mathcal{A}\!\operatorname{ss}_{{\operatorname{CY}}})

over 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast}, where the non-degenerate marked simplices are precisely the inert morphisms of 𝒜ss\mathcal{A}\!\operatorname{ss}.

Proof.

An nn-simplex of N(𝒜ss)N()N()N(\mathcal{A}\!\operatorname{ss})\coprod_{N(\bbLambda)}N(\bbLambda_{\diamond}) is an equivalence class in N(𝒜ss)N()N(\mathcal{A}\!\operatorname{ss})\amalg N(\bbLambda_{\diamond}) under the relation that

(S0S1Sn)N(𝒜ss)n(T0T1Tn)N()n\underbrace{(S_{0}\to S_{1}\to\cdots\to S_{n})}_{\in N(\mathcal{A}\!\operatorname{ss})_{n}}\sim\underbrace{(T_{0}\to T_{1}\to\cdots\to T_{n})}_{\in N(\bbLambda)_{n}}

if and only if

B(T0T1Tn)=(S0S1Sn).B(T_{0}\to T_{1}\to\cdots\to T_{n})=(S_{0}\to S_{1}\to\cdots\to S_{n}).

In particular, θ\theta is injective, and a bijection on 0-simplices.

We proceed by induction. For ease of notation, we set Q=N(𝒜ss)N()N()Q=N(\mathcal{A}\!\operatorname{ss})\coprod_{N(\bbLambda)}N(\bbLambda_{\diamond}).

  1. (1)

    Suppose f:Sf:S\to\diamond is a 1-simplex not contained in the image of θ\theta. Then SS is determined by TST\subsetneq S^{\circ} and a cyclic order on SS. Adding a basepoint to TT to get Tf𝒜ssCYT_{f}\in\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}} we get a factorization of ff as

    Tf{\lx@inpgf@ignorespaces T_{f}}S{\lx@inpgf@ignorespaces S}{\lx@inpgf@ignorespaces\diamond}α\scriptstyle{\lx@inpgf@ignorespaces\alpha}f\scriptstyle{\lx@inpgf@ignorespaces f}β\scriptstyle{\lx@inpgf@ignorespaces\beta}

    in 𝒜ssCY\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}. Taking such a 2-simplex σf\sigma_{f} for every such ff, we can form the pushout

    {f}(Λ12){\lx@inpgf@ignorespaces\coprod_{\{f\}}(\Lambda^{2}_{1})^{\flat}}Q0{\lx@inpgf@ignorespaces Q_{0}}{f}(Δ2){\lx@inpgf@ignorespaces\coprod_{\{f\}}(\Delta^{2})^{\flat}}Q1{\lx@inpgf@ignorespaces Q_{1}}

    The morphism on the left is of type (C1C_{1}) from [12, B.1.1], so we get a factorization

    Q0{\lx@inpgf@ignorespaces Q_{0}}Q1{\lx@inpgf@ignorespaces Q_{1}}N(𝒜ssCY){\lx@inpgf@ignorespaces N(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}})}τ1\scriptstyle{\lx@inpgf@ignorespaces\tau_{1}}θ\scriptstyle{\lx@inpgf@ignorespaces\theta}θ1\scriptstyle{\lx@inpgf@ignorespaces\theta_{1}}

    where τ1\tau_{1} is 𝔓\mathfrak{P}-anodyne, and θ1\theta_{1} is bijective on 11-simplices.

  2. (2)

    Now suppose that σ:Δ2𝒜ssCY\sigma:\Delta^{2}\to\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}} is a 2-simplex not in the image of θ1\theta_{1}. Then σ\sigma must be given by a sequence

    S1{\lx@inpgf@ignorespaces S_{1}}S2{\lx@inpgf@ignorespaces S_{2}}{\lx@inpgf@ignorespaces\diamond}g\scriptstyle{\lx@inpgf@ignorespaces g}f\scriptstyle{\lx@inpgf@ignorespaces f}

    (if σ\sigma does not contain \diamond, it is the image of a simplex in 𝒜ss\mathcal{A}\!\operatorname{ss}, if it contains two copies of \diamond, it is degenerate). Consequently, we get two 2-simplices, σfg\sigma_{f\circ g} and σg\sigma_{g} in the image of θ1\theta_{1}. Moreover, gg restricts to a morphism

    g:TfgTf,g:T_{f\circ g}\to T_{f},

    and we get a 2-simplex S1S2TfS_{1}\to S_{2}\to T_{f}. We then note that the Λ13\Lambda^{3}_{1} horn

    Tf{\lx@inpgf@ignorespaces T_{f}}Tfg{\lx@inpgf@ignorespaces T_{f\circ g}}S1{\lx@inpgf@ignorespaces S_{1}}{\lx@inpgf@ignorespaces\diamond}

    can be filled to a 2-simplex S1TfS_{1}\to T_{f}\to\diamond via a horn of type (C1C_{1}). Finally, we get a Λ23\Lambda^{3}_{2}-horn

    S2{\lx@inpgf@ignorespaces S_{2}}Tf{\lx@inpgf@ignorespaces T_{f}}S1{\lx@inpgf@ignorespaces S_{1}}{\lx@inpgf@ignorespaces\diamond}f\scriptstyle{\lx@inpgf@ignorespaces f}g\scriptstyle{\lx@inpgf@ignorespaces g}fg\scriptstyle{\lx@inpgf@ignorespaces f\circ g}

    of type (C1C_{1}). This gives us a factorization of θ\theta as Q0τ2Q2θ2N(𝒜ssCY)Q_{0}\overset{\tau_{2}}{\to}Q_{2}\overset{\theta_{2}}{\to}N(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}) where τ1\tau_{1} is 𝔓\mathfrak{P}-anodyne and θ2\theta_{2} is bijective on simplices of dimension 2\leq 2.

  3. (3)

    Now suppose inductively that we have obtained a factorization through θn1:QnN(𝒜ssCY)\theta_{n-1}:Q_{n}\to N(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}) such that

    • θn1\theta_{n-1} is bijective on kk-simplices for kn1k\leq n-1.

    • The image of θn1\theta_{n-1} contains all nn-simplices of the form

      S0S1Sn1S_{0}\to S_{1}\to\cdots\to S_{n-1}\to\diamond

      where Sn1S_{n-1}\to\diamond is a 1-simplex in the image of Λ\Lambda_{\diamond}.

    Suppose given an nn-simplex σ\sigma not in the image of θn1\theta_{n-1}. Then, by similar reasoning to that above, σ\sigma must be of the form

    S0ϕ1S1ϕ2Sn1ϕnS_{0}\overset{\phi_{1}}{\to}S_{1}\overset{\phi_{2}}{\to}\cdots\to S_{n-1}\overset{\phi_{n}}{\to}\diamond

    with Sn+1S_{n+1}\to\diamond not in the image of Λ\Lambda_{\diamond}. Define ψk:=ϕnϕn1ϕnk\psi_{k}:=\phi_{n}\circ\phi_{n-1}\circ\cdots\circ\phi_{n-k}, we then get nn-simplices in the image of θn1\theta_{n-1}

    S0ϕ1S1ϕ2Sk^Sn1TϕnS_{0}\overset{\phi_{1}}{\to}S_{1}\overset{\phi_{2}}{\to}\cdots\to\widehat{S_{k}}\to S_{n-1}\to T_{\phi_{n}}{\to}\diamond

    and an nn-simplex in the image of θn1\theta_{n-1}

    S0S1Sn1Tf.S_{0}\to S_{1}\to\cdots\to S_{n-1}\to T_{f}.

    These nn nn-simplices form a Λnn+1\Lambda^{n+1}_{n}-horn in N(𝒜ssCY)N(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}) which, once again, can be filled by a pushout of type (C1C_{1}).

We therefore get a factorization

Q0Q1N(𝒜ssCY)Q_{0}\to Q_{1}\to\cdots\to N(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}})

which exhausts N(𝒜ssCY)N(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}). Each morphism in this sequence is 𝔓\mathfrak{P}-anodyne, and so the transfinite composition Q0N(𝒜ssCY)Q_{0}\to N(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}) is 𝔓\mathfrak{P}-anodyne. ∎

Corollary 1.24.

The \infty-category of trace algebras in 𝒞\mathcal{C} is equivalent to the full subcategory of Map𝔽in(N(𝒜ssCY),𝒞)\operatorname{Map}^{\sharp}_{\mathbb{F}\!\!\operatorname{in}_{\ast}}(N(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}),\mathcal{C}^{\otimes}) sending \diamond to 1\bbOne.

Definition 1.25.

We define the \infty-category of Calabi-Yau algebras in 𝒞\mathcal{C} to be the full subcategory of Map𝔽in(N(𝒜ssCY),𝒞)\operatorname{Map}^{\sharp}_{\mathbb{F}\!\!\operatorname{in}_{\ast}}(N(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}),\mathcal{C}^{\otimes}) on those objects which

  1. (1)

    send \diamond to 1\bbOne, and

  2. (2)

    send the morphism 2\langle 2\rangle\to\diamond in \bbLambda_{\diamond} to a non-degenerate morphism X×X1X\times X\to\bbOne.

1.3. Cartesian monoidal structures

Throughout this paper, we will model (symmetric) monoidal structions by Cartesian fibrations, rather than the coCartesian fibrations used in [12]. These fibrations will be defined via adjunctions with the following. Throughout this section, 𝒞\mathcal{C} will denote an \infty-category which admits finite products.

Definition 1.26.

The category Δ\Delta^{\amalg} has as its objects pairs ([n],{i,j})([n],\{i,j\}), where [n]Δ[n]\in\Delta and iji\leq j are elements in [n][n]. The morphisms ([n],{i,j})([m],{k,})([n],\{i,j\})\to([m],\{k,\ell\}) consist of a morphism ϕ:[n][m]\phi:[n]\to[m] such that ϕ(i)kϕ(j)\phi(i)\leq k\leq\ell\leq\phi(j). We will, in general, think of {i,j}\{i,j\} as an interval inside [n][n], and denote by {ij}\{i\leq j\} the linearly ordered set

{ij}:={i,i+1,,j}[n].\{i\leq j\}:=\{i,i+1,\ldots,j\}\subset[n].

The category 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast}^{\amalg} has as its objects pairs (S,T)(S,T) where S𝔽inS\in\mathbb{F}\!\!\operatorname{in}_{\ast} and TST\subset S^{\circ}. A morphism (S,T)(P,Q)(S,T)\to(P,Q) consists of a morphism ϕ:SP\phi:S\to P in 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast} such that ϕ(T)Q\phi(T)\subset Q. We will sometimes denote by \bbGamma^{\amalg} the category (𝔽in)op(\mathbb{F}\!\!\operatorname{in}_{\ast}^{\amalg})^{\operatorname{op}}. ∎

Remark 1.27.

We can provide an alternate characterization of Δ\Delta^{\amalg} and 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast}^{\amalg}. The functor ΔΔ\Delta^{\amalg}\to\Delta is the coCartesian fibration defined as a Grothendieck construction of the functors

ΔCat;[n]I[n]op.\Delta\to\operatorname{Cat};\quad[n]\mapsto I_{[n]}^{\operatorname{op}}.

The functor 𝔽in𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast}^{\amalg}\to\mathbb{F}\!\!\operatorname{in} is the Cartesian fibration defined as a Grothendieck construction of the (contravariant) power set functor

𝔽inopCat;S𝒫(S).\mathbb{F}\!\!\operatorname{in}_{\ast}^{{\operatorname{op}}}\to\operatorname{Cat};\quad S\mapsto\mathcal{P}(S^{\circ}).

Note that, as in [5, Remark 10.3.2], these constructions relate to the constructions Δ×Δ\Delta^{\times}\to\Delta and Γ×Fin\Gamma^{\times}\to\operatorname{Fin}_{\ast} from [11, Proposition 1.2.8] and [12, Proposition 2.4.1.5] respectively. In particular, the functor Γ×Fin\Gamma^{\times}\to\operatorname{Fin}_{\ast} is the Cartesian fibration arising as the Grothendieck construction of

𝔽inCat;S𝒫(S)op.\mathbb{F}\!\!\operatorname{in}^{\ast}\to\operatorname{Cat};\quad S\mapsto\mathcal{P}(S^{\circ})^{\operatorname{op}}.

For an \infty-category 𝒟\mathcal{D} with enough colimits, the functor 𝔽in𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast}^{\amalg}\to\mathbb{F}\!\!\operatorname{in}_{\ast} can therefore be used to construct a coCartesian fibration 𝒟𝔽in\mathcal{D}^{\amalg}\to\mathbb{F}\!\!\operatorname{in}_{\ast} modeling the coCartesian symmetric monoidal structure on 𝒟\mathcal{D}. ∎

Construction 1.28.

The functor cut:Δ𝔽inop\operatorname{cut}:\Delta\to\mathbb{F}\!\!\operatorname{in}_{\ast}^{\operatorname{op}} yields a functor Δ(𝔽in)op\Delta^{\amalg}\to(\mathbb{F}\!\!\operatorname{in}_{\ast}^{\amalg})^{\operatorname{op}}. To see this, we first note that for {i,j}[n]\{i,j\}\subset[n] in Δ\Delta^{\amalg}, we have 𝕆({ij})𝕆([n])\mathbb{O}(\{i\leq j\})\subset\mathbb{O}([n]). On objects we therefore define {i,j}[n](𝕆([n]),𝕆({ij}))\{i,j\}\subset[n]\mapsto(\mathbb{O}([n]),\mathbb{O}(\{i\leq j\}))

Given a morphism f:([n],{i,j})f:([n],\{i,j\}) to ([m],{k,})([m],\{k,\ell\}) in Δ\Delta^{\amalg}, we get a morphism 𝕆(f):𝕆([m])𝕆([n])\mathbb{O}(f):\mathbb{O}([m])\to\mathbb{O}([n]). Moreover, the condition that f(i)kf(j)f(i)\leq k\leq\ell\leq f(j) ensures that 𝕆(f)(𝕆({k}))𝕆({ij})\mathbb{O}(f)\left(\mathbb{O}(\{k\leq\ell\})\right)\subset\mathbb{O}(\{i\leq j\}). ∎

Construction 1.29 (Cartesian monoidal structures).

Given an \infty-category 𝒞\mathcal{C} with finite products, we can associate two Cartesian fibrations to 𝒞\mathcal{C} as follows.

We define a functor of \infty-categories 𝒞¯Δ\overline{\mathcal{C}^{\boxtimes}}\to\Delta via the universal property

HomΔ(K,𝒞¯)HomSetΔ(K×ΔΔ,𝒞).\operatorname{Hom}_{\Delta}(K,\overline{\mathcal{C}^{\boxtimes}})\cong\operatorname{Hom}_{\operatorname{Set}_{\Delta}}(K\times_{\Delta}\Delta^{\amalg},\mathcal{C}).

Similarly, we define a functor 𝒞ׯ\overline{\mathcal{C}^{\times}}\to\bbGamma via the universal property

Hom(K,𝒞¯)HomSetΔ(K×,𝒞).\operatorname{Hom}_{\bbGamma}(K,\overline{\mathcal{C}^{\boxtimes}})\cong\operatorname{Hom}_{\operatorname{Set}_{\Delta}}(K\times_{\bbGamma}\bbGamma^{\amalg},\mathcal{C}).

Both of these are Cartesian fibrations by dint of [13, 3.2.2.13].

We now let 𝒞𝒞¯\mathcal{C}^{\boxtimes}\subset\overline{\mathcal{C}^{\boxtimes}} be the full subcategory on those objects G:I[n]op𝒞G:I_{[n]}^{\operatorname{op}}\to\mathcal{C} for which GG displays G({ij})G(\{i\leq j\}) as a product over G({kk+1})G(\{k\leq k+1\}) for ik<ji\leq k<j.

Similarly, we let 𝒞×𝒞ׯ\mathcal{C}^{\times}\subset\overline{\mathcal{C}^{\times}} be the full subcategory on those objects G:𝒫(S)op𝒞G:\mathcal{P}(S^{\circ})^{{\operatorname{op}}}\to\mathcal{C} for which GG displays G(S)G(S) as a product over G(i)G(i) for iSi\in S. ∎

Proposition 1.30.

The functor 𝒞Δ\mathcal{C}^{\boxtimes}\to\Delta is a Cartesian fibration exhibiting the Cartesian monoidal structure on 𝒞\mathcal{C}.

Proof.

This is [5, Prop. 10.3.8]. ∎

Proposition 1.31.

The functor 𝒞×\mathcal{C}^{\times}\to\bbGamma is a Cartesian fibration exhibiting the Cartesian symmetric monoidal structure on 𝒞\mathcal{C}.

Proof.

The proof of this statement is, mutatis mutandis, the same as the proof of [12, Proposition 2.4.1.5]. ∎

1.4. \infty-Categories of Spans

We will briefly recall here the requisite constructions and definitions for \infty-categories of spans. For a fuller exposition, see [5, Chapter 10]. Throughout this section, we will assume that 𝒞\mathcal{C} is now an \infty-category with small limits.

Definition 1.32.

Let SS be a linearly ordered set. We define ISI_{S} to be the poset of non-empty sub-intervals {ij}S\{i\leq j\}\subset S.

Let Δn\Delta^{n} be the standard nn-simplex. We define the spine 𝒥nΔn\mathcal{J}^{n}\subset\Delta^{n} to be

𝒥n:=Δ{0,1}Δ{1}Δ{1,2}Δ{n1}Δ{n1,n}.\mathcal{J}^{n}:=\Delta^{\{0,1\}}\coprod_{\Delta^{\{1\}}}\Delta^{\{1,2\}}\cdots\coprod_{\Delta^{\{n-1\}}}\Delta^{\{n-1,n\}}.

Construction 1.33 (Categories of Spans).

We define the functor Tw:ΔSetΔ\operatorname{Tw}:\Delta\to\operatorname{Set}_{\Delta} by

[n]N(I[n])op.[n]\mapsto N(I_{[n]})^{\operatorname{op}}.

By left Kan extension along the Yoneda embedding and restriction, we get an adjunction, which we will also denote by

(3) Tw:SetΔSetΔ:Span¯.\operatorname{Tw}:\operatorname{Set}_{\Delta}\leftrightarrow\operatorname{Set}_{\Delta}:\overline{\operatorname{Span}}.

For an \infty-category 𝒟\mathcal{D}, the simplicial set Tw(𝒟)\operatorname{Tw}(\mathcal{D}) is an \infty-category, which we will call the twisted arrow \infty-category of 𝒟\mathcal{D}. Note that Tw(𝒟)\operatorname{Tw}(\mathcal{D}) comes with a canonical projection η𝒟:Tw(𝒟)𝒟\eta_{\mathcal{D}}:\operatorname{Tw}(\mathcal{D})\to\mathcal{D}. If 𝒟\mathcal{D} is the nerve of a 1-category DD, Tw(𝒟)\operatorname{Tw}(\mathcal{D}) can be identified with the nerve of the 1-category Tw(D)\operatorname{Tw}(D) whose objects are morphisms f:abf:a\to b in 𝒟\mathcal{D} and whose morphisms fgf\to g are commutative diagrams

a{\lx@inpgf@ignorespaces a}b{\lx@inpgf@ignorespaces b}c{\lx@inpgf@ignorespaces c}d{\lx@inpgf@ignorespaces d}f\scriptstyle{\lx@inpgf@ignorespaces f}g\scriptstyle{\lx@inpgf@ignorespaces g}

in DD, i.e. factorizations f=hgf=h\circ g\circ\ell.

Given XSetΔX\in\operatorname{Set}_{\Delta}, we can extend the adjunction 3 to an adjunction

TwX:(SetΔ)/X(SetΔ)/X:Span¯X\operatorname{Tw}_{X}:(\operatorname{Set}_{\Delta})_{/X}\leftrightarrow(\operatorname{Set}_{\Delta})_{/X}:\overline{\operatorname{Span}}_{X}

by setting TwX(SX)\operatorname{Tw}_{X}(S\to X) to be the composite

Tw(S)Tw(X)ηXX\operatorname{Tw}(S)\to\operatorname{Tw}(X)\overset{\eta_{X}}{\to}X

and by setting Span¯X(SX)\overline{Span}_{X}(S\to X) to be the left-hand column of the pullback

Span¯X(S){\lx@inpgf@ignorespaces\overline{\operatorname{Span}}_{X}(S)}Span¯(S){\lx@inpgf@ignorespaces\overline{\operatorname{Span}}(S)}X{\lx@inpgf@ignorespaces X}Span¯(X){\lx@inpgf@ignorespaces\overline{\operatorname{Span}}(X)}

in SetΔ\operatorname{Set}_{\Delta}.

Let p:SXp:S\to X be a map of simplicial sets. We call an nn-simplex in Span¯X(S)\overline{\operatorname{Span}}_{X}(S) represented by a map σ:Tw(Δn)S\sigma:\operatorname{Tw}(\Delta^{n})\to S a Segal simplex if, for every ΔkΔn\Delta^{k}\subset\Delta^{n}, the composite diagram

{0,k}Tw(𝒥k)Tw(Δk)Tw(Δn)𝜎S\{0,k\}\star\operatorname{Tw}(\mathcal{J}^{k})\subset\operatorname{Tw}(\Delta^{k})\subset\operatorname{Tw}(\Delta^{n})\overset{\sigma}{\to}S

is a pp-limit diagram. We denote by SpanX(S)Span¯X(S)\operatorname{Span}_{X}(S)\subset\overline{\operatorname{Span}}_{X}(S) the simplicial subset consisting of the Segal simplices. ∎

Proposition 1.34 ([5, 10.2.31]).

Let p:𝒞N(Δ)p:\mathcal{C}^{\otimes}\to N(\Delta) be a Cartesian fibration exhibiting a monoidal structure on 𝒞[1]\mathcal{C}^{\otimes}_{[}1] such that pp admits relative pullbacks. Then SpanΔ(𝒞)N(Δ)\operatorname{Span}_{\Delta}(\mathcal{C}^{\otimes})\to N(\Delta) is a Cartesian fibration exhibiting a monoidal structure on Span(𝒞[1])\operatorname{Span}_{\ast}(\mathcal{C}^{\otimes}_{[1]}).

Corollary 1.35.

Let p:𝒞N(Γ)p:\mathcal{C}^{\otimes}\to N(\Gamma) be a Cartesian fibration exhibiting a symmetric monoidal structure on 𝒞1\mathcal{C}^{\otimes}_{\langle 1\rangle} such that pp admits relative pullbacks. Then SpanΓ(𝒞)N(Γ)\operatorname{Span}_{\Gamma}(\mathcal{C}^{\otimes})\to N(\Gamma) is a Cartesian fibration exhibiting a symmetric monoidal structure on Span(𝒞)\operatorname{Span}_{\ast}(\mathcal{C}^{\otimes}).

Corollary 1.36.

Let 𝒞\mathcal{C} be an \infty-category that admits small limits. Then the functors

SpanΔ(𝒞)\displaystyle\operatorname{Span}_{\Delta}(\mathcal{C}^{\boxtimes}) N(Δ)\displaystyle\to N(\Delta)
Span(𝒞×)\displaystyle\operatorname{Span}_{\bbGamma}(\mathcal{C}^{\times}) N()\displaystyle\to N(\bbGamma)

are Cartesian fibrations exhibiting a monoidal or a symmetric monoidal structure on Span(𝒞)\operatorname{Span}_{\ast}(\mathcal{C}) respectively.

Remark 1.37.

The monoidal structures from Corollary 1.36 can be seen as ‘pointwise cartesian’ monoidal structure, with monoidal product given by the product in 𝒞\mathcal{C}. ∎

2. Algebras in Spans

Throughout this section, we set Θ:=Tw(Δ)×ΔΔ\Theta:=\operatorname{Tw}(\Delta)\times_{\Delta}\Delta^{\amalg}. Morphisms in Θ\Theta will be represented as diagrams

{i,j}{\lx@inpgf@ignorespaces\{i,j\}}[n]{\lx@inpgf@ignorespaces{{[n]}}}[m]{\lx@inpgf@ignorespaces{{[m]}}}{i,j}{\lx@inpgf@ignorespaces\{i^{\prime},j^{\prime}\}}[n]{\lx@inpgf@ignorespaces{[n^{\prime}]}}[m]{\lx@inpgf@ignorespaces{[m^{\prime}]}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}f\scriptstyle{\lx@inpgf@ignorespaces f}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f^{\prime}}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}

in Δ\Delta. In this section and the next, 𝒞\mathcal{C} will denote an \infty-category with small limits. We will, on occasion, denote an object {i,j}[n]𝑓[m]\{i,j\}\subset[n]\overset{f}{\to}[m] in Θ\Theta by the pair (f,{i,j})(f,\{i,j\}).

2.1. Conditions on functors

Suppose we are given a functor G:Θ𝒞G:\Theta\to\mathcal{C}, which corresponds to a functor

G~:Tw(Δ)𝒞\tilde{G}:\operatorname{Tw}(\Delta)\to\mathcal{C}^{\boxtimes}

over Δ\Delta.

Proposition 2.1.

The functor GG defines a functor G¯:ΔSpanΔ(𝒞)\overline{G}:\Delta\to\operatorname{Span}_{\Delta}(\mathcal{C}^{\boxtimes}) if and only if, for every simplex [n0]ϕ1[n1]ϕ2ϕk[nk][n_{0}]\overset{\phi_{1}}{\to}[n_{1}]\overset{\phi_{2}}{\to}\cdots\overset{\phi_{k}}{\to}[n_{k}] in Δ\Delta and every interval {i,j}[n0]\{i,j\}\subset[n_{0}], the corresponding diagram

(4) G(ϕnϕ1,{i,j}){\lx@inpgf@ignorespaces G(\phi_{n}\circ\cdots\circ\phi_{1},\{i,j\})}G(ϕ1,{i,j}){\lx@inpgf@ignorespaces G(\phi_{1},\{i,j\})}{\lx@inpgf@ignorespaces\cdots}G(ϕk,{ψk1(i),ψk1(j)}){\lx@inpgf@ignorespaces G(\phi_{k},\{\psi_{k-1}(i),\psi_{k-1}(j)\})}G([n0],{i,j}){\lx@inpgf@ignorespaces G([n_{0}],\{i,j\})}G([n1],{ψ1(i),ψ1(j)}){\lx@inpgf@ignorespaces G([n_{1}],\{\psi_{1}(i),\psi_{1}(j)\})}{\lx@inpgf@ignorespaces\cdots}G([nk1],{ψk1(i),ψk1(j)}){\lx@inpgf@ignorespaces G([n_{k-1}],\{\psi_{k-1}(i),\psi_{k-1}(j)\})}G([nk],{ψk(i),ψk(j)}){\lx@inpgf@ignorespaces G([n_{k}],\{\psi_{k}(i),\psi_{k}(j)\})}

where ψi:=ϕiϕi1ϕ1\psi_{i}:=\phi_{i}\circ\phi_{i-1}\circ\cdots\circ\phi_{1}, is a limit diagram in 𝒞\mathcal{C}.

Proof.

By definition, GG defines a functor

G¯:ΔSpanΔ(𝒞)\overline{G}:\Delta\to\operatorname{Span}_{\Delta}(\mathcal{C}^{\boxtimes})

if and only if every restriction of G~\tilde{G} to Tw(Δn)Tw(Δ)\operatorname{Tw}(\Delta^{n})\subset\operatorname{Tw}(\Delta) is a Segal simplex in 𝒞\mathcal{C}^{\boxtimes}.

Let ΔkΔ\Delta^{k}\hookrightarrow\Delta be the simplex

[n0]ϕ1[n1]ϕ2ϕk[nk].[n_{0}]\overset{\phi_{1}}{\to}[n_{1}]\overset{\phi_{2}}{\to}\cdots\overset{\phi_{k}}{\to}[n_{k}].

Then by [5, Lemma 10.2.13], there is a functor

H:(Δ1×Tw(Δk))×ΔΔ𝒞H:\left(\Delta^{1}\times\operatorname{Tw}(\Delta^{k})\right)\times_{\Delta}\Delta^{\amalg}\to\mathcal{C}

representing a homotopy

H~:Δ1×Tw(Δk)𝒞.\tilde{H}:\Delta^{1}\times\operatorname{Tw}(\Delta^{k})\to\mathcal{C}^{\boxtimes}.

This homotopy has components that are Cartesian morphisms, and the component G~0:=H~|{0}×Tw(Δk)\tilde{G}_{0}:=\tilde{H}|_{\{0\}\times\operatorname{Tw}(\Delta^{k})} has image contained in 𝒞[n0]\mathcal{C}^{\boxtimes}_{[n_{0}]}. Since this is the case, the condition that G~\tilde{G} is a pp-limit diagram when restricted to the Segal cone is equivalent to the condition that G~0\tilde{G}_{0} is a limit diagram in 𝒞[n0]\mathcal{C}^{\boxtimes}_{[n_{0}]} when restricted to the Segal cone. This can be checked componentwise, using one component for each subinterval of [n0][n_{0}].

Fix one such subinterval, {i,j}\{i,j\}. Then the coresponding Segal cone diagram in 𝒞\mathcal{C} will be

G0(ϕnϕ1,{i,j}){\lx@inpgf@ignorespaces G_{0}(\phi_{n}\circ\cdots\circ\phi_{1},\{i,j\})}G0(ϕ1,{i,j}){\lx@inpgf@ignorespaces G_{0}(\phi_{1},\{i,j\})}{\lx@inpgf@ignorespaces\cdots}G0(ϕk,{i,j}){\lx@inpgf@ignorespaces G_{0}(\phi_{k},\{i,j\})}G0([n0],{i,j}){\lx@inpgf@ignorespaces G_{0}([n_{0}],\{i,j\})}G0([n1],{i,j}){\lx@inpgf@ignorespaces G_{0}([n_{1}],\{i,j\})}{\lx@inpgf@ignorespaces\cdots}G0([nk1],{i,j}){\lx@inpgf@ignorespaces G_{0}([n_{k-1}],\{i,j\})}G0([nk],{i,j}){\lx@inpgf@ignorespaces G_{0}([n_{k}],\{i,j\})}

Since the homotopy has Cartesian components, HH will restrict to a natural equivalence between this diagram and the diagram (1)(1). Therefore, a simplex is Segal if and only if all such diagrams are limit diagrams. ∎

2.1.1. Cartesian morphisms and equivalences

Suppose GG represents a coalgebra object. Given an inert morphism Δ1{ϕ}Δ\Delta^{1}\overset{\{\phi\}}{\to}\Delta (ϕ:[n][m]\phi:{[n]}\to{[m]}), GG must send ϕ\phi to a Cartesian morphism in SpanΔ(𝒞)\operatorname{Span}_{\Delta}(\mathcal{C}^{\boxtimes}). This means that the adjoint map

Tw(Δ1)𝒞\operatorname{Tw}(\Delta^{1})\to\mathcal{C}^{\boxtimes}

is comprised only of Cartesian morphisms. Therefore:

  • For the source map ϕ[n]\phi\to{[n]} in Tw(Δ)\operatorname{Tw}(\Delta), and for any {i,j}[n]\{i,j\}\in{[n]}, the induced morphism

    G(ϕ,{i,j})G([n],{i,j})G(\phi,\{i,j\})\to G({[n]},\{i,j\})

    is an equivalence.

  • For the target map ϕ[m]\phi\to{[m]} in Tw(Δ)\operatorname{Tw}(\Delta), and for any {i,j}[n]\{i,j\}\in{[n]} The induced morphism

    G(ϕ,{i,j})G([m],{ϕ(i),ϕ(j)})G(\phi,\{i,j\})\to G({[m]},\{\phi(i),\phi(j)\})

    is an equivalence.

We will write ϕi,j:[i,,j][n]\phi_{i,j}:[i,\ldots,j]\to{[n]} for the inert morphism which includes the interval [i,,j][i,\ldots,j].

Proposition 2.2.

Suppose GG represents a coalgebra object. Let f:[n][m]f:{[n]}\to{[m]} be a morphism in Δ\Delta, viewed as an object in Tw(Δ)\operatorname{Tw}(\Delta).

  1. (1)

    Let f|{i,j}:[i,,j][m]f|_{\{i,j\}}:[i,\ldots,j]\to{[m]} be the restriction of ff to [i,,j][n][i,\ldots,j]\subset{[n]}. Then the induced morphism

    G(f|{i,j},{i,j})G(f,{i,j})G(f|_{\{i,j\}},\{i,j\})\to G(f,\{i,j\})

    is an equivalence.

  2. (2)

    Let f~:[n][i,,j][m]\tilde{f}:{[n]}\to[i,\ldots,j]\subset{[m]} be a morphism such that composing with the inert morphism ϕi,j:[i,,j][m]\phi_{i,j}:[i,\ldots,j]\to{[m]} yields ff. Then the induced morphism

    G(f,{i,j})G(f~,{i,j})G(f,\{i,j\})\to G(\tilde{f},\{i,j\})

    is an equivalence.

Proof.

Applying our conclusion from above, we find that in case (1), the diagram

G(f|{i,j},{i,j}){\lx@inpgf@ignorespaces{G(f|_{\{i,j\}},\{i,j\})}}G(ϕi,j,{i,j}){\lx@inpgf@ignorespaces G(\phi_{i,j},\{i,j\})}G(f,{i,j}){\lx@inpgf@ignorespaces G(f,\{i,j\})}G(id[n],{i,j}){\lx@inpgf@ignorespaces G(id_{{[n]}},\{i,j\})}

Must be pullback. Therefore, since G(ϕi,j,{i,j})G(id[n],{i,j})G(\phi_{i,j},\{i,j\})\to G({\operatorname{id}}_{{[n]}},\{i,j\}) must be an equivalence, so must G(f|{i,j},{i,j})G(f,{i,j})G(f|_{\{i,j\}},\{i,j\})\to G(f,\{i,j\}).

Similarly, in case (2), the diagram

G(f,{i,j}){\lx@inpgf@ignorespaces G(f,\{i,j\})}G(f~,{i,j}){\lx@inpgf@ignorespaces G(\tilde{f},\{i,j\})}G(ϕi,j,{i,j}){\lx@inpgf@ignorespaces G(\phi_{i,j},\{i,j\})}G(id[i,,j],{i,j}){\lx@inpgf@ignorespaces G(id_{[i,\ldots,j]},\{i,j\})}

must be pullback. Therefore, since G(ϕi,j,{i,j})G(id[i,,j],{i,j})G(\phi_{i,j},\{i,j\})\to G({\operatorname{id}}_{[i,\ldots,j]},\{i,j\}) must be an equivalence, so must G(f,{i,j})G(f~,{i,j})G(f,\{i,j\})\to G(\tilde{f},\{i,j\}). ∎

Lemma 2.3.

Suppose GG sends the morphisms from Proposition 2.2 to equivalences. Let

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\lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.39998pt} \lx@inpgf@ignorespaces{}{}{}{}{{}}{}{}{{}}\lxSVG@stroke\lxSVG@drawpath@unclipped{M 43.93 -24.72 L 76.76 -24.72}{fill:none} {{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}}}{{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}{{{\lx@inpgf@ignorespaces}}{\lxSVG@begingroup@{_scopebegin=1} \lxSVG@transformcm{1.0}{0.0}{0.0}{1.0}{55.67801pt}{-17.8686pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 77.04 -24.72)} \lxSVG@begingroup@{_scopebegin=1} \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}{40.11694pt}{-14.15475pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 55.51 -19.59)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}} \lxSVG@closescope {}{ {}{}{}}{}{ {}{}{}} {{{{{}}{ {}{}}{}{}{{}{}}}}}{}{{{{{}}{ {}{}}{}{}{{}{}}}}}{{}}{}{}{}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{}{{{}{}}}\lxSVG@begingroup@{_scopebegin=1} \lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.39998pt} \lx@inpgf@ignorespaces{}{}{}{}{{}}{}{}{{}}\lxSVG@stroke\lxSVG@drawpath@unclipped{M 102.67 -12.44 L 102.67 11.91}{fill:none} {{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}}}{{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}{{{\lx@inpgf@ignorespaces}}{\lxSVG@begingroup@{_scopebegin=1} \lxSVG@transformcm{0.0}{1.0}{-1.0}{0.0}{74.19856pt}{8.8089pt}\lxSVG@begingroup@{transform=matrix(0.0 1.0 -1.0 0.0 102.67 12.19)} \lxSVG@begingroup@{_scopebegin=1} \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}{66.8458pt}{-2.82997pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 92.49 -3.92)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}} \lxSVG@closescope \lxSVG@closescope {\lx@inpgf@ignorespaces}{\lx@inpgf@ignorespaces}{\lx@inpgf@ignorespaces}\hss}\lxSVG@discardpath\lxSVG@closescope \hss}}\lxSVG@closescope\endpgfpicture}}}}\mkern-300.0mu\right\}

be a morphism such that gg restricts to an isomorphism [i,,j][i,,j][i,\ldots,j]\overset{\cong}{\to}[i^{\prime},\ldots,j^{\prime}] and g¯\overline{g} restricts to an isomorphism [f(i),f(i)+1,,f(j)][f(i),f(i)+1,,f(j)][f^{\prime}(i^{\prime}),f^{\prime}(i^{\prime})+1,\ldots,f^{\prime}(j^{\prime})]\overset{\cong}{\to}[f(i),f(i)+1,\ldots,f(j)]. Then GG sends μ\mu to an equivalence.

Proof.

We first note that, under the given hypotheses, GG will send morphisms of the form

ν:={       {0,k}   [k]   [m]     {0,k}   [k]   [m]              s         id[k]            s         h     }\nu:=\left\{\vbox{\vbox{\hbox to157.02pt{\vbox to54.3pt{\pgfpicture\makeatletter\hbox{\hskip 78.50804pt\lower-27.96979pt\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} \lxSVG@transformcm{1.0}{0.0}{0.0}{1.0}{-78.50804pt}{-20.16866pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 -108.63 -27.91)} \pgfsys@hbox{58}\lxSVG@closescope }}}{{{\lx@inpgf@ignorespaces{}}}{{}}{{}}{{}}{{}}{{}}{{}}}} \lxSVG@closescope }}} {}{}{ {}{}{}}{}{ {}{}{}} {{{{{}}{ {}{}}{}{}{{}{}}}}}{}{{{{{}}{ {}{}}{}{}{{}{}}}}}{{}}{}{}{}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{}{{{}{}}}\lxSVG@begingroup@{_scopebegin=1} \lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.39998pt} \lx@inpgf@ignorespaces\lx@inpgf@ignorespaces\hbox{\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}{-26.8206pt}{15.16867pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 -37.11 20.99)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}}\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}{-22.9317pt}{20.02144pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 -31.73 27.7)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}} \lxSVG@closescope {}{ {}{}{}}{}{ {}{}{}} {{{{{}}{ {}{}}{}{}{{}{}}}}}{}{{{{{}}{ {}{}}{}{}{{}{}}}}}{{}}{}{}{}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{}{{{}{}}}\lxSVG@begingroup@{_scopebegin=1} \lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.39998pt} \lx@inpgf@ignorespaces{}{}{}{}{{}}{}{}{{}}\lxSVG@stroke\lxSVG@drawpath@unclipped{M 26.23 24.45 L 60.27 24.45}{fill:none} {{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}}}{{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}{{{\lx@inpgf@ignorespaces}}{\lxSVG@begingroup@{_scopebegin=1} \lxSVG@transformcm{1.0}{0.0}{0.0}{1.0}{43.75851pt}{17.66867pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 60.55 24.45)} \lxSVG@begingroup@{_scopebegin=1} \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}{29.56996pt}{20.02144pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 40.92 27.7)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}} \lxSVG@closescope {}{ {}{}{}}{}{ {}{}{}} {{{{{}}{ {}{}}{}{}{{}{}}}}}{}{{{{{}}{ {}{}}{}{}{{}{}}}}}{{}}{}{}{}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{}{{{}{}}}\lxSVG@begingroup@{_scopebegin=1} \lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.39998pt} \lx@inpgf@ignorespaces{}{}{}{}{{}}{}{}{{}}\lxSVG@stroke\lxSVG@drawpath@unclipped{M 5.41 12.19 L 5.41 -11.64}{fill:none} {{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}}}{{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}{{{\lx@inpgf@ignorespaces}}{\lxSVG@begingroup@{_scopebegin=1} \lxSVG@transformcm{0.0}{-1.0}{1.0}{0.0}{3.91202pt}{-8.60895pt}\lxSVG@begingroup@{transform=matrix(0.0 -1.0 1.0 0.0 5.41 -11.91)} \lxSVG@begingroup@{_scopebegin=1} \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}{-13.52074pt}{-1.1361pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 -18.71 -1.57)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}} \lxSVG@closescope {}{}{ {}{}{}}{}{ {}{}{}} {{{{{}}{ {}{}}{}{}{{}{}}}}}{}{{{{{}}{ {}{}}{}{}{{}{}}}}}{{}}{}{}{}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{}{{{}{}}}\lxSVG@begingroup@{_scopebegin=1} \lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.39998pt} \lx@inpgf@ignorespaces\lx@inpgf@ignorespaces\hbox{\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}{-26.8206pt}{-20.16866pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 -37.11 -27.91)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}}\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}{-22.9317pt}{-15.31589pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 -31.73 -21.19)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}} \lxSVG@closescope {}{ {}{}{}}{}{ {}{}{}} {{{{{}}{ {}{}}{}{}{{}{}}}}}{}{{{{{}}{ {}{}}{}{}{{}{}}}}}{{}}{}{}{}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{}{{{}{}}}\lxSVG@begingroup@{_scopebegin=1} \lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.39998pt} \lx@inpgf@ignorespaces{}{}{}{}{{}}{}{}{{}}\lxSVG@stroke\lxSVG@drawpath@unclipped{M 26.23 -24.45 L 58.33 -24.45}{fill:none} {{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}}}{{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}{{{\lx@inpgf@ignorespaces}}{\lxSVG@begingroup@{_scopebegin=1} \lxSVG@transformcm{1.0}{0.0}{0.0}{1.0}{42.35574pt}{-17.66866pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 58.61 -24.45)} \lxSVG@begingroup@{_scopebegin=1} \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}{27.51614pt}{-25.81702pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 38.07 -35.72)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}} \lxSVG@closescope {}{ {}{}{}}{}{ {}{}{}} {{{{{}}{ {}{}}{}{}{{}{}}}}}{}{{{{{}}{ {}{}}{}{}{{}{}}}}}{{}}{}{}{}{}{}{{{}{}}}{}{{\lx@inpgf@ignorespaces}}{}{}{}{{{}{}}}\lxSVG@begingroup@{_scopebegin=1} \lxSVG@setlinewidth{\the\pgflinewidth}\lxSVG@begingroup@{stroke-width=0.39998pt} \lx@inpgf@ignorespaces{}{}{}{}{{}}{}{}{{}}\lxSVG@stroke\lxSVG@drawpath@unclipped{M 83.9 -12.16 L 83.9 11.64}{fill:none} {{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}}}{{}{{}}{}{}{{}}{{{\lx@inpgf@ignorespaces}}{{{\lx@inpgf@ignorespaces}}{\lxSVG@begingroup@{_scopebegin=1} \lxSVG@transformcm{0.0}{1.0}{-1.0}{0.0}{60.63188pt}{8.60896pt}\lxSVG@begingroup@{transform=matrix(0.0 1.0 -1.0 0.0 83.9 11.91)} \lxSVG@begingroup@{_scopebegin=1} \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}{62.98465pt}{-2.42163pt}\lxSVG@begingroup@{transform=matrix(1.0 0.0 0.0 1.0 87.15 -3.35)} \pgfsys@hbox{58}\lxSVG@closescope }}} \lxSVG@closescope }}} \lxSVG@closescope \lxSVG@closescope {\lx@inpgf@ignorespaces}{\lx@inpgf@ignorespaces}{\lx@inpgf@ignorespaces}\hss}\lxSVG@discardpath\lxSVG@closescope \hss}}\lxSVG@closescope\endpgfpicture}} }}\mkern-350.0mu\right\}

to equivalences, where hh sends [s(i),s(i)+1,,s(j)][s^{\prime}(i^{\prime}),s^{\prime}(i^{\prime})+1,\ldots,s^{\prime}(j^{\prime})] isomorphically to [m]{[m]}. This follows from composing

{0,k}{\lx@inpgf@ignorespaces\{0,k\}}[k]{\lx@inpgf@ignorespaces{{[k]}}}[m]{\lx@inpgf@ignorespaces{[m]}}{0,k}{\lx@inpgf@ignorespaces\{0,k\}}[k]{\lx@inpgf@ignorespaces{{[k]}}}[m]{\lx@inpgf@ignorespaces{[m^{\prime}]}}{0,k}{\lx@inpgf@ignorespaces\{0,k\}}[k]{\lx@inpgf@ignorespaces{{[k]}}}[m]{\lx@inpgf@ignorespaces{[m]}}\subseteqs\scriptstyle{\lx@inpgf@ignorespaces s}id[k]\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}_{{{[k]}}}}\subseteqs\scriptstyle{\lx@inpgf@ignorespaces s^{\prime}}id[k]\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}_{{{[k]}}}}h\scriptstyle{\lx@inpgf@ignorespaces h}\subseteqs\scriptstyle{\lx@inpgf@ignorespaces s}ψ\scriptstyle{\lx@inpgf@ignorespaces\psi}

Where ψ\psi is the inclusion of the interval [f(0),,f(k)][f(0),\ldots,f(k)]. The lower morphism is then one of the morphisms of type (2) from Proposition 2.2 and the two morphisms compose to the identity. So, by 2-out-of-3, ν\nu must be sent to an equivalence.

Now write []:=[f(i),f(i)+1,,f(j)][\ell]:=[f(i),f(i)+1,\ldots,f(j)], and consider the composition

{0,k}{\lx@inpgf@ignorespaces\{0,k\}}[k]{\lx@inpgf@ignorespaces{{[k]}}}[]{\lx@inpgf@ignorespaces{[\ell]}}{i,j}{\lx@inpgf@ignorespaces\{i,j\}}[n]{\lx@inpgf@ignorespaces{[n]}}[m]{\lx@inpgf@ignorespaces{[m]}}[k]{i,j}{\lx@inpgf@ignorespaces{{[k]}}\cong\{i^{\prime},j^{\prime}\}}[n]{\lx@inpgf@ignorespaces{[n^{\prime}]}}[m]{\lx@inpgf@ignorespaces{[m^{\prime}]}}\subseteqs\scriptstyle{\lx@inpgf@ignorespaces s}ϕi,j\scriptstyle{\lx@inpgf@ignorespaces\phi_{i,j}}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f}g\scriptstyle{\lx@inpgf@ignorespaces g}h\scriptstyle{\lx@inpgf@ignorespaces h}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f^{\prime}}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}

Where hh sends [][\ell] isomorphically to itself. The upper morphism is the composite of a morphism of type (1) from Proposition 2.2 and a morphism of the same kind as ν\nu. Moreover, the composite

{0,k}{\lx@inpgf@ignorespaces\{0,k\}}[k]{\lx@inpgf@ignorespaces{{[k]}}}[]{\lx@inpgf@ignorespaces{[\ell]}}[k]{i,j}{\lx@inpgf@ignorespaces{[k]}\cong\{i^{\prime},j^{\prime}\}}[n]{\lx@inpgf@ignorespaces{[n^{\prime}]}}[m]{\lx@inpgf@ignorespaces{[m^{\prime}]}}\subseteqs\scriptstyle{\lx@inpgf@ignorespaces s}ϕi,j\scriptstyle{\lx@inpgf@ignorespaces\phi_{i^{\prime},j^{\prime}}}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f^{\prime}}h\scriptstyle{\lx@inpgf@ignorespaces h^{\prime}}

is also the composite of a morphism of type (1) from Proposition 2.2 and a morphism of the same kind as ν\nu. Therefore, by the 2-out-of-3 property, μ\mu must be sent to an equivalence. ∎

Definition 2.4.

We define EE to be the set of all morphisms of the form from Lemma 2.3. Note that EE is closed under composition. ∎

Corollary 2.5.

A functor G:Θ𝒞G:\Theta\to\mathcal{C} defines a coalgebra object if and only if

  1. (1)

    GG sends degenerate intervals to the terminal object.

  2. (2)

    GG sends ({i,j}[n]𝑓[m])(\{i,j\}\subset{[n]}\overset{f}{\to}{[m]}) together with its projections to sub-intervals to a product diagram.

  3. (3)

    GG sends the morphisms in EE to equivalences.

  4. (4)

    GG sends all diagrams of the form Eq. 4 to limit diagrams.

2.1.2. Forgetting degenerate intervals

Definition 2.6.

We denote by AlgSp(𝒞)\operatorname{Alg}_{\operatorname{Sp}}(\mathcal{C}) the full sub-\infty-category of Fun(Θ,𝒞)\operatorname{Fun}(\Theta,\mathcal{C}) on those functors satisfying conditions (1)-(4) from the corollary. We denote by Fun(Θ,𝒞)\operatorname{Fun}^{\ast}(\Theta,\mathcal{C}) the full sub-\infty-category of functors sending every degenerate interval to a terminal object in 𝒞\mathcal{C} (i.e., those functors satisfying condition (1) from the corollary).

Let Ω\Omega be the full subcategory of Θ\Theta on those objects {i,j}[n]𝑓[m]\{i,j\}\subset{[n]}\overset{f}{\to}{[m]} such that the interval {i,j}\{i,j\} is not degenerate (i.e. iji\neq j). Pulling back along the inclusion ΩΘ\Omega\to\Theta induces a functor S:Fun(Θ,𝒞)Fun(Ω,𝒞)S:\operatorname{Fun}^{\ast}(\Theta,\mathcal{C})\to\operatorname{Fun}(\Omega,\mathcal{C}). ∎

Definition 2.7.

Given a 1-category DD, call an object dDd\in D attracting if, for all aDa\in D,

HomD(a,d),andHomD(d,a)=.\operatorname{Hom}_{D}(a,d)\neq\emptyset,\quad\text{and}\quad\operatorname{Hom}_{D}(d,a)=\emptyset.

Lemma 2.8.

Let dDd\in D be an attracting object, denote by Fun(D,𝒞)\operatorname{Fun}^{\ast}(D,\mathcal{C}) the full sub-\infty-category on those functors sending dd to the terminal object, and denote by DD^{\circ} the full subcategory on all objects other than dd. Then the functor

Fun(D,𝒞)Fun(D,𝒞)\operatorname{Fun}^{\ast}(D,\mathcal{C})\to\operatorname{Fun}(D^{\circ},\mathcal{C})

is an equivalence.

Proof.

Without loss of generality, we assume that 𝒞\mathcal{C} has a unique terminal object. when ff sends dd to the terminal object. Denote by 𝒞𝒞\mathcal{C}^{\prime}\subset\mathcal{C} the largest subcategory not containing morphisms from the terminal object to any other object, and denote by 𝒞\mathcal{C}^{\circ} the full subcategory on non-terminal objects. Then we have an equivalence 𝒞(𝒞)\mathcal{C}^{\prime}\simeq(\mathcal{C}^{\circ})^{\!\rotatebox{30.0}{${\triangle}$}} since the hom-spaces to the terminal object are all contractible. Any simplex in Fun(D,𝒞)\operatorname{Fun}^{\ast}(D,\mathcal{C}) factors through Fun(D,𝒞)\operatorname{Fun}^{\ast}(D,\mathcal{C}^{\prime}), so it will suffice to show that

Fun(D,(𝒞))(D,𝒞)\operatorname{Fun}^{\ast}(D,(\mathcal{C}^{\circ})^{\!\rotatebox{30.0}{${\triangle}$}})\to(D^{\circ},\mathcal{C})

is a trivial Kan fibration.

Unwinding the definitions, this amounts to solving the extension problem

(Δn×D)Δn×DΔn×D{\lx@inpgf@ignorespaces\left(\partial\Delta^{n}\times D\right)\coprod_{\partial\Delta^{n}\times D^{\circ}}\Delta^{n}\times D^{\circ}}(𝒞){\lx@inpgf@ignorespaces(\mathcal{C}^{\circ})^{\!\rotatebox{30.0}{${\triangle}$}}}Δn×D{\lx@inpgf@ignorespaces\Delta^{n}\times D}f\scriptstyle{\lx@inpgf@ignorespaces f}

where ff sends Δn×D\partial\Delta^{n}\times D to the cone point. However, this implies that ff factors through (Δn×D)(\Delta^{n}\times D^{\circ})^{\!\rotatebox{30.0}{${\triangle}$}}. Pulling back along Δn×D(Δn×D)\Delta^{n}\times D\to(\Delta^{n}\times D^{\circ})^{\!\rotatebox{30.0}{${\triangle}$}} then gives the desired extension.

Corollary 2.9.

The functor S:Fun(Θ,𝒞)Fun(Ω,𝒞)S:\operatorname{Fun}^{\ast}(\Theta,\mathcal{C})\to\operatorname{Fun}(\Omega,\mathcal{C}) is an equivalence of \infty-categories.

Proof.

We again assume that 𝒞\mathcal{C} has a unique terminal object. Let Θdeg\Theta^{deg} be the full subcategory on only the degenerate intervals. We can write Fun(Θ,𝒞)\operatorname{Fun}^{\ast}(\Theta,\mathcal{C}) as a pullback in SetΔ\operatorname{Set}_{\Delta}

Fun(Θ,𝒞){\lx@inpgf@ignorespaces\operatorname{Fun}^{\ast}(\Theta,\mathcal{C})}Fun(Θ,𝒞){\lx@inpgf@ignorespaces\operatorname{Fun}(\Theta,\mathcal{C})}Fun(Θdeg,){\lx@inpgf@ignorespaces\operatorname{Fun}(\Theta^{deg},\ast)}Fun(Θdeg,𝒞){\lx@inpgf@ignorespaces\operatorname{Fun}(\Theta^{deg},\mathcal{C})}

There is a natural transformation of diagrams to the pullback diagram

Fun(ΘΘdeg,𝒞){\lx@inpgf@ignorespaces\operatorname{Fun}^{\ast}(\Theta\coprod_{\Theta^{deg}}\ast,\mathcal{C})}Fun(Θ,𝒞){\lx@inpgf@ignorespaces\operatorname{Fun}(\Theta,\mathcal{C})}Fun(,𝒞){\lx@inpgf@ignorespaces\operatorname{Fun}^{\ast}(\ast,\mathcal{C})}Fun(Θdeg,𝒞){\lx@inpgf@ignorespaces\operatorname{Fun}(\Theta^{deg},\mathcal{C})}

Since this natural transformation is an isomorphism on the bottom three objects, the universal property of the pullback gives us an isomorphism Fun(Θ,𝒞)Fun(ΘΘdeg,𝒞)\operatorname{Fun}^{\ast}(\Theta,\mathcal{C})\cong\operatorname{Fun}^{\ast}(\Theta\coprod_{\Theta^{deg}}\ast,\mathcal{C}). ΘΘdeg\ast\in\Theta\coprod_{\Theta^{deg}}\ast is an attracting object, and so Lemma 2.8 yields the desired result. ∎

2.2. The localization

Construction 2.10.

Let ϕ:([n],{i,j})([m],{k,})\phi:([n],\{i,j\})\to([m],\{k,\ell\}) be a morphism in Δ\Delta^{\amalg}. and write {ij}\{i\leq j\} for the linearly ordered set {i,i+1,,j}\{i,i+1,\ldots,j\}. Applying 𝕆\mathbb{O} to ϕ\phi, we obtain a diagram

𝕆([m]){\lx@inpgf@ignorespaces\mathbb{O}([m])}𝕆([n]){\lx@inpgf@ignorespaces\mathbb{O}([n])}𝕆({k}){\lx@inpgf@ignorespaces\mathbb{O}(\{k\leq\ell\})}𝕆({ij}){\lx@inpgf@ignorespaces\mathbb{O}(\{i\leq j\})}𝕀({k}){\lx@inpgf@ignorespaces\mathbb{I}(\{k\leq\ell\})}𝕀({ij}){\lx@inpgf@ignorespaces\mathbb{I}(\{i\leq j\})}𝕆(ϕ)\scriptstyle{\lx@inpgf@ignorespaces\mathbb{O}(\phi)}\subseteq\subseteq\subseteq\subseteq

Since, ϕ(i)kϕ(j)\phi(i)\leq k\leq\ell\leq\phi(j), we see that, for every a{k}a\in\{k\leq\ell\}, there exists a b{ij}b\in\{i\leq j\} such that ϕ(b)aa+1ϕ(b+1)\phi(b)\leq a\leq a+1\leq\phi(b+1). That is, 𝕆(ϕ)\mathbb{O}(\phi) descends uniquely to a map

res(ϕ):𝕀({k})𝕀({ij}).\operatorname{res}(\phi):\mathbb{I}(\{k\leq\ell\})\to\mathbb{I}(\{i\leq j\}).

Note that we here apply the convention that 𝕀([0])=\mathbb{I}([0])=\emptyset. We therefore obtain a functor

res:ΔΔ+op\operatorname{res}:\Delta^{\amalg}\to\Delta_{+}^{\operatorname{op}}

which sends all non-degenerate intervals into ΔΔ+\Delta\subset\Delta_{+}. ∎

Definition 2.11.

Define a category Δ\Delta^{\star} to have objects finite (non-empty) ordered tuples of elements in Δ\Delta. The morphisms of Δ\Delta^{\star} from ([n0],,[nk])([m0],,[m])([n_{0}],\ldots,[n_{k}])\to([m_{0}],\ldots,[m_{\ell}]) consist of

  1. (1)

    A morphism ϕ:[][k]\phi:[\ell]\to[k] in Δ\Delta.

  2. (2)

    For each i{0,1,k}i\in\{0,1,\ldots k\}, with ϕ1(i)=(j1,,jr)\phi^{-1}(i)=(j_{1},\ldots,j_{r}), a morphism

    fi:[mj1][mj2][mjr][ni]f_{i}:[m_{j_{1}}]\star[m_{j_{2}}]\star\cdots\star[m_{j_{r}}]\to[n_{i}]

    in Δ\Delta.

Satisfying the conditions that

  1. (1)

    If there is a pp\in\langle\ell\rangle^{\circ} with r>maxjϕ1(i)(j)r>\max_{j\in\phi^{-1}(i)}(j), then fif_{i} hits ni[ni]n_{i}\in[n_{i}].

  2. (2)

    If there is a pp\in\langle\ell\rangle^{\circ} with r<minjϕ1(i)(j)r<\min_{j\in\phi^{-1}(i)}(j), then fif_{i} hits 0[ni]0\in[n_{i}].

Remark 2.12.

We could equivalently define the morphisms to be

  1. (1)

    A morphism ϕ:[][k]\phi:[\ell]\to[k] in Δ\Delta.

  2. (2)

    A morphism

    f:[m1][m2][m][n1][n2][nk]f:[m_{1}]\star[m_{2}]\star\cdots\star[m_{\ell}]\to[n_{1}]\star[n_{2}]\star\cdots\star[n_{k}]

    in Δ\Delta.

Satisfying the condition that, for any i[k]i\in[k] with ϕ1(i)=(j1,,jr)\phi^{-1}(i)=(j_{1},\ldots,j_{r}), the restriction

fi:[mj1][mj2][mjr][n1][n2][nk]f_{i}:[m_{j_{1}}]\star[m_{j_{2}}]\star\cdots\star[m_{j_{r}}]\to[n_{1}]\star[n_{2}]\star\cdots\star[n_{k}]

has image contained in [ni][n_{i}]. ∎

01201234012345012345
Figure 3. A pictorial representation of a morphism μ\mu in Ω\Omega, viewed as a triple of composable morphisms [n]𝑔[n]f[m]g¯[m][n]\overset{g}{\to}[n^{\prime}]\overset{f^{\prime}}{\to}[m^{\prime}]\overset{\overline{g}}{\to}[m] in Δ\Delta. The dual forest is drawn in black, the chosen subintervals of [n][n] and [n][n^{\prime}] marked in red, and the induced morphism (μ)\mathcal{L}(\mu) is drawn in blue. Note that that source of (μ)\mathcal{L}(\mu) is the imbrication of the sets {f(i),f(i)+1,f(i+1)}\{f^{\prime}(i),f^{\prime}(i)+1,\ldots f^{\prime}(i+1)\}.
Construction 2.13.

We now define a functor :ΩΔ\mathcal{L}:\Omega\to\Delta^{\star}. On objects it is given by

{i,j}[n]𝑓[m]({f(i)f(i+1)},,{f(j1)f(j)})\{i,j\}\subset[n]\overset{f}{\to}[m]\mapsto\left(\{f(i)\leq f(i+1)\},\ldots,\{f(j-1)\leq f(j)\}\right)

where {f(k)f(k+1)}:={f(k),f(k)+1),,f(k+1)}\{f(k)\leq f(k+1)\}:=\{f(k),f(k)+1),\ldots,f(k+1)\} are considered to be ordered via the order on [m][m]. Note that the indexing set of ({i,j},f)\mathcal{L}(\{i,j\},f) is precisely 𝕀({ij})\mathbb{I}(\{i\leq j\})

On morphisms, \mathcal{L} is more complicated. A morphism in Ω\Omega is given by a commutative diagram of the form

μ={    [k]:={i,j}      [n]    f          g         [m]   [k]:={i,j}      [n]    f         [m]    g¯          }\mu=\left\{\vbox{\vbox{\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 30.70322pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\halign{\entry@#!@&&\entry@@#!@\cr&&\cr&&\crcr}}}\ignorespaces{\hbox{\kern-26.49489pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.5pt\hbox{$\textstyle{[k]:=\{i,j\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\kern 37.41153pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{\subset}$}}}}}\ignorespaces{}{\hbox{\kern 56.10599pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.5pt\hbox{$\textstyle{[n]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 82.41908pt\raise 6.1111pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.75pt\hbox{$\scriptstyle{f}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 100.46947pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 54.7325pt\raise-16.00446pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-0.8264pt\hbox{$\scriptstyle{g}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 64.88495pt\raise-23.99109pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 100.46947pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.5pt\hbox{$\textstyle{[m]}$}}}}}}}{\hbox{\kern-30.70322pt\raise-32.00891pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.5pt\hbox{$\textstyle{[k^{\prime}]:=\{i^{\prime},j^{\prime}\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\kern 38.81432pt\raise-32.00891pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{\subset}$}}}}}\ignorespaces{}{\hbox{\kern 54.70322pt\raise-32.00891pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.5pt\hbox{$\textstyle{[n^{\prime}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 81.06665pt\raise-38.58725pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-2.21725pt\hbox{$\scriptstyle{f^{\prime}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 99.06668pt\raise-32.00891pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 99.06668pt\raise-32.00891pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.5pt\hbox{$\textstyle{[m^{\prime}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 110.63731pt\raise-16.00446pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-2.83888pt\hbox{$\scriptstyle{\overline{g}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 110.63731pt\raise-8.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces}}}}}}\right\}

where g(i)ijg(j)g(i)\leq i^{\prime}\leq j^{\prime}\leq g(j). We define (μ)\mathcal{L}(\mu) to be a pair (ϕf,ψf)(\phi_{f},\psi_{f}). We then write ϕf:=res(g):𝕀({ij})𝕀({ij})\phi_{f}:=\operatorname{res}(g):\mathbb{I}(\{i^{\prime}\leq j^{\prime}\})\to\mathbb{I}(\{i\leq j\}).

Since the diagram commutes, for each pair {p,p+1}{i,j}[n]\{p,p+1\}\subset\{i,j\}\subset[n], we have that g¯(f(g(p)))=p\overline{g}(f(g(p)))=p and g¯(f(g(p+1)))=p+1\overline{g}(f(g(p+1)))=p+1, so that g¯\overline{g} descends to a map of ordered sets

g¯p:{f(g(p)f(g(p)+1)}{f(g(p+1)1)f(g(p+1))}{f(p)f(p+1)}\overline{g}_{p}:\{f^{\prime}(g(p)\leq f^{\prime}(g(p)+1)\}\star\cdots\star\{f^{\prime}(g(p+1)-1)\leq f^{\prime}(g(p+1))\}\to\{f(p)\leq f(p+1)\}

It is easy to verify that conditions (1) and (2) from the definition of Δ\Delta^{\star} are satisfied by the g¯p\overline{g}_{p}. On morphisms, therefore, we define

(μ):=(ϕ(g),{g¯p}ip<j).\mathcal{L}(\mu):=\left(\phi(g),\left\{\overline{g}_{p}\right\}_{i\leq p<j}\right).

This is functorial via the functoriality of res\operatorname{res} and the restriction of g¯\overline{g}. ∎

2.2.1. Decomposing morphisms

Construction 2.14.

Given a morphism

f:[m][n]f:[m]\to[n]

in Δ\Delta, we can uniquely decompose it as follows: Let [1]=:[1i][m][1]=:[1_{i}]\subset[m] be the interval {i1i}\{i-1\leq i\}, and let [ni][n][n_{i}]\subset[n] be the interval {f(i1)f(i)}\{f(i-1)\leq f(i)\}. Moreover, let [nleft][n_{left}] and [nright][n_{right}] be the intervals {0f(0)}\{0\leq f(0)\} and {f(m)n}\{f(m)\leq n\} in [n][n] respectively. Then ff is completely determined by the decomposition of [n][n], since, given such a decomposition, we can reconstruct ff by defining fi:[1i][ni]f_{i}:[1_{i}]\to[n_{i}] to be the unique map preserving maximal and minimal elements, so that ff is the composition

f=f1fm:[11][1m][n1][nm][nleft][n1][nm][nright].f=f_{1}\star\cdots\star f_{m}:[1_{1}]\star\cdots\star[1_{m}]\to[n_{1}]\star\cdots[n_{m}]\hookrightarrow[n_{left}]\star[n_{1}]\star\cdots[n_{m}]\star[n_{right}].

We can clarify the indexing of the decomposition of [n][n] by noting that the pairs (i1,i)(i-1,i) considered above are precisely the inner interstices of [m][m]. Hence, we have decomposed ff as a morphism

(i1,i)𝕀([m]){i1,i}(i1,i)𝕀([m])[ni].\bigstar_{(i-1,i)\in\mathbb{I}([m])}\{i-1,i\}\to\bigstar_{(i-1,i)\in\mathbb{I}([m])}[n_{i}].

Definition 2.15.

Given a morphism γ:[n][m]\gamma:[n]\to[m] in Δ\Delta, we can uniquely factor γ\gamma as

[n]γ1[mγ]γ2[m][n]\overset{\gamma_{1}}{\to}[m_{\gamma}]\overset{\gamma_{2}}{\hookrightarrow}[m]

where [m]=[k][mγ][].[m]=[k]\oplus[m_{\gamma}]\oplus[\ell]. Applying OO, we get

OPENO([m])O([mγ])O)[n].O([m])\to O([m_{\gamma}])\to O)[n].

Where O([m])O([mγ])O([m])\to O([m_{\gamma}]) acts as projection onto a sub-interval. We call O([mγ])O([m_{\gamma}]) the minimal interval of γ\gamma. ∎

Lemma 2.16.

Given an interval {i,j}[n]\{i,j\}\subset[n] and a morphism η:({i,j}[n])({r,r+k}[m])\eta:(\{i,j\}\subset[n])\to(\{r,r+k\}\subset[m]) in Δ\Delta^{\amalg}, let [p,,q][p,\ldots,q] be the minimal interval of γ:=res(η)\gamma:=\operatorname{res}(\eta). Then η|[p+1,,q1]=O(γ)|[p+1,,q1]\eta|_{[p+1,\ldots,q-1]}=O(\gamma)|_{[p+1,\ldots,q-1]}.

Proof.

If [p+1,,q1][p+1,\ldots,q-1] is empty, the statement is vacuously true. Otherwise, note that for s[p+1,,q1]s\in[p+1,\ldots,q-1], the requirement that res(η)=γ\operatorname{res}(\eta)=\gamma means that γ(η(s))s<γ(η(s)+1)\gamma(\eta(s))\leq s<\gamma(\eta(s)+1). Such an η(s)\eta(s) always exists, and this inequality uniquely determines η(s)\eta(s). (Note that, for pp or qq in [p,,q][p,\ldots,q], we only have one-half of the inequality so that uniqueness need not hold.) ∎

2.2.2. Constructing morphisms

In what follows, we will be interested in the weak fibers of the functor :ΩΔ\mathcal{L}:\Omega\to\Delta^{\star}. We first note that, given an object M=([m1],,[mk])ΔM=([m_{1}],\ldots,[m_{k}])\in\Delta^{\star}, the fiber ΩM\Omega_{M} is non-empty. We can explicitly build an object

{0,k}[k]fM[m1][m2][mk]=:[m]\{0,k\}\subset[k]\overset{f_{M}}{\to}[m_{1}]\star[m_{2}]\star\cdots\star[m_{k}]=:[m]

in the fiber over MM, given by

fM(i)={0[mi+1]i<kmk[mk]i=k.f_{M}(i)=\begin{cases}0\in[m_{i+1}]&i<k\\ m_{k}\in[m_{k}]&i=k.\end{cases}
Definition 2.17.

For M=([m1],,[mk])ΔM=([m_{1}],\ldots,[m_{k}])\in\Delta^{\star}, we define a subcategory ΩMEΩM\Omega_{M}^{E}\subset\Omega_{M} as follows. The objects of ΩME\Omega_{M}^{E} are the same as those of ΩM\Omega_{M}, but the morphisms are only those in EE. ∎

Lemma 2.18.

The object {0,k}[k]fM[m]\{0,k\}\subset[k]\overset{f_{M}}{\to}[m] is an initial object in ΩME\Omega_{M}^{E}.

Proof.

Given another object

{i,j}[n]𝑓[m]\{i,j\}\subset[n]\overset{f}{\to}[m^{\prime}]

in ΩME\Omega_{M}^{E}, and a morphism

{0,k}\textstyle{\{0,k\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[k]\textstyle{[k]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}fM\scriptstyle{f_{M}}ϕ\scriptstyle{\phi}[m]\textstyle{[m]}{i,j}\textstyle{\{i,j\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[n]\textstyle{[n]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}f\scriptstyle{f}[m]\textstyle{[m^{\prime}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}h\scriptstyle{h}

ϕ\phi must be the inclusion of [i,,j][i,\ldots,j], since any such morphism in EE will induce an isomorphism [k][i,,j][k]\to[i,\ldots,j]. Moreover, hh is clearly uniquely determined by the condition that it maps [f(i),f(i+1),,f(j)][f(i),f(i+1),\ldots,f(j)] isomorphically to [m][m]. ∎

Suppose given an object

Z:={{i,j}[n]𝑓[]}Z:=\left\{\{i,j\}\subset[n]\overset{f}{\to}[\ell]\right\}

in Ω\Omega whose image under \mathcal{L} is ([i+1],,[j])([\ell_{i+1}],\ldots,[\ell_{j}]), and a morphism

g:([i+1],,[j])([m0],,[mk1])g:([\ell_{i+1}],\ldots,[\ell_{j}])\to([m_{0}],\ldots,[m_{k-1}])

in Δ\Delta^{\star}. Write γ:[k1][i+1,,j]Δ\gamma:[k-1]\to[i+1,\ldots,j]\in\Delta and g¯:[m0][mk1][i+1][j]\overline{g}:[m_{0}]\star\cdots\star[m_{k-1}]\to[\ell_{i+1}]\star\cdots\star[\ell_{j}] for the morphisms defining gg. Denote by [nc]:=[p,,q]{i,j}[n][n_{c}]:=[p,\ldots,q]\subset\{i,j\}\subset[n] the minimal interval of γ\gamma and by ψ:[i,,j][nc]\psi:[i,\ldots,j]\to[n_{c}] the projection as above, and let {0,k}[k]fM[m]:=[m0][mk1]\{0,k\}\subset[k]\overset{f_{M}}{\to}[m]:=[m_{0}]\star\cdots\star[m_{k-1}] be the minimal object in Ω\Omega representing the target.

Note that, by definition, the morphism g¯\overline{g} has image contained in [p+1][q]=:[c][\ell_{p+1}]\star\cdots\star[\ell_{q}]=:[\ell_{c}]. We introduce some notation for specific decompositions:

[n]=[n][nc][nr][n]=[n_{\ell}]\star[n_{c}]\star[n_{r}]
[]=[][c][r][\ell]=[{\ell_{\ell}}]\star[{\ell_{c}}]\star[{\ell_{r}}]
Lemma 2.19.

There is a morphism in Ω\Omega

{p,q}\textstyle{\{p,q\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[p,,q]\textstyle{[p,\ldots,q]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}f|{p,q}\scriptstyle{f|_{\{p,q\}}}ν\scriptstyle{\nu}[c]\textstyle{[\ell_{c}]}{0,k}\textstyle{\{0,k\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[1][k][1]\textstyle{[1]\star[k]\star[1]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}fM\scriptstyle{f_{M}^{\prime}}[1][m][2]\textstyle{[\ell^{1}]\star[m]\star[\ell^{2}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}g¯\scriptstyle{\overline{g}^{\prime}}

which extends to a morphism μZ,M\mu_{Z,M} in Ω\Omega covering gg

μZ,M:={    Z   =   {i,j}      [n][nc][nr]                 [][c][r]   ZM   :=   {0,k}      [n][1][k][1][nr]          [][1][m][2][r]           }\mu_{Z,M}:=\left\{\vbox{\vbox{\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 11.20903pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\halign{\entry@#!@&&\entry@@#!@\cr&&&\cr&&&\crcr}}}\ignorespaces{\hbox{\kern-6.77083pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{Z\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\kern 17.69734pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-1.83437pt\hbox{$\textstyle{=}$}}}}}\ignorespaces{}{\hbox{\kern 36.40166pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{\{i,j\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\kern 82.55028pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{\subset}$}}}}}\ignorespaces{}{\hbox{\kern 107.89665pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{[n_{\ell}]\star[n_{c}]\star[n_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 245.45328pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 143.85251pt\raise-24.32pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 245.45328pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{[{\ell_{\ell}}]\star[{\ell_{c}}]\star[{\ell_{r}}]}$}}}}}}}{\hbox{\kern-11.20903pt\raise-32.26447pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{Z_{M}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\kern 17.93123pt\raise-32.26447pt\hbox{\hbox{\kern 0.0pt\raise-2.15277pt\hbox{$\textstyle{:=}$}}}}}\ignorespaces{}{\hbox{\kern 35.20903pt\raise-32.26447pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{\{0,k\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\kern 74.28543pt\raise-32.26447pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{\subset}$}}}}}\ignorespaces{}{\hbox{\kern 90.17433pt\raise-32.26447pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{[n_{\ell}]\star[1]\star[k]\star[1]\star[n_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 221.53069pt\raise-32.26447pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 221.53069pt\raise-32.26447pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{[{\ell_{\ell}}]\star[\ell^{1}]\star[m]\star[\ell^{2}]\star[{\ell_{r}}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 278.65564pt\raise-8.05554pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces}}}}}}\right\}

Moreover, given any other morphism ZXZ\to X covering gg, there is a unique morphism ZMXZ_{M}\to X in EE such that the diagram

Z\textstyle{Z\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ZM\textstyle{Z_{M}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}X\textstyle{X}

commutes.

Proof.

In the first diagram, we define the map ν\nu on [p+1,,q1][p+1,\ldots,q-1] to be the unique map from Lemma 2.16 dual to γ\gamma under res\operatorname{res}, and send the endpoints to the endpoints of [1][k][1][1]\star[k]\star[1]. Then we write

[c]=[1][cm][2],[\ell_{c}]=[\ell^{1}]\star[\ell_{c}^{m}]\star[\ell^{2}],

where [cm][\ell_{c}^{m}] is the minimal interval containing the image of g¯:[m][]\overline{g}:[m]\to[\ell]. Note that g¯:[m][cm]\overline{g}:[m]\to[\ell_{c}^{m}] hits both endpoints. We then define

g¯:=id[1]g¯id[2]:[1][m][2][c]\overline{g}^{\prime}:={\operatorname{id}}_{[\ell^{1}]}\star\overline{g}\star{\operatorname{id}}_{[\ell^{2}]}:[\ell^{1}]\star[m]\star[\ell^{2}]\to[\ell_{c}]

(which then, by definition, hits both endpoints), and

fM:[1][k][1][1][m][2]f_{M}^{\prime}:[1]\star[k]\star[1]\to[\ell^{1}]\star[m]\star[\ell^{2}]

to be fMf_{M} on [k][k], and to send endpoints to endpoints. Then we can decompose the diagram as

{p,q}\textstyle{\{p,q\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[1p+1][1q]\textstyle{[1_{p+1}]\star\cdots\star[1_{q}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}f|{p,q}\scriptstyle{f|_{\{p,q\}}}ν\scriptstyle{\nu}[p+1][q]\textstyle{[\ell_{p+1}]\star\cdots\star[\ell_{q}]}{0,k}\textstyle{\{0,k\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[1][kp+1][kq][1]\textstyle{[1]\star[k_{p+1}]\star\cdots\star[k_{q}]\star[1]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}fM\scriptstyle{f_{M}^{\prime}}[1][mp+1][mq][2]\textstyle{[\ell^{1}]\star[m_{p+1}]\star\cdots\star[m_{q}]\star[\ell^{2}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}g¯\scriptstyle{\overline{g}^{\prime}}

by decomposing the morphisms ν\nu, f|{p,q}f|_{\{p,q\}}, and fMνf_{M}^{\prime}\circ\nu. The condition that the diagram commute is then equivalent to the conditions that, (1) for each r{p+2,,q1}r\in\{p+2,\ldots,q-1\}, the endpoints of [mr][m_{r}] are sent to the endpoints of [r][\ell_{r}] by g¯\overline{g}, and (2) that g¯\overline{g} sends the endpoints of [1][mp+1][\ell^{1}]\star[m_{p+1}] and [mq][2][m_{q}]\star[\ell^{2}] to the endpoints of [p+1][\ell_{p+1}] and [q][\ell_{q}], respectively. Since

[mr]=a𝕀([kr])[fM(a1),fM(a1)+1,,fM(a)][m_{r}]=\bigstar_{a\in\mathbb{I}([k_{r}])}[f_{M}^{\prime}(a-1),f_{M}^{\prime}(a-1)+1,\ldots,f_{M}^{\prime}(a)]

we see that case (1) is true by the definition of Δ\Delta^{\star}. Case (2) is true by construction.

This diagram is defined so that the maps ν\nu, fMf_{M}^{\prime}, g¯\overline{g}^{\prime}, and f|{p,q}f|_{\{p,q\}} preserve endpoints. Therefore, we can take the appropriate star products with the morphisms id[n]{\operatorname{id}}_{[n_{\ell}]}, id[nr]{\operatorname{id}}_{[n_{r}]}, id[]{\operatorname{id}}_{[\ell_{\ell}]}, id[r]{\operatorname{id}}_{[\ell_{r}]}, f|[n]:[n][]f|_{[n_{\ell}]}:[n_{\ell}]\to[\ell_{\ell}], and f|[nr]:[nr][r]f|_{[n_{r}]}:[n_{r}]\to[\ell_{r}] to get a commutative diagram

Z\textstyle{Z\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}=\textstyle{=}{i,j}\textstyle{\{i,j\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[n][nc][nr]\textstyle{[n_{\ell}]\star[n_{c}]\star[n_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[][c][r]\textstyle{[{\ell_{\ell}}]\star[{\ell_{c}}]\star[{\ell_{r}}]}ZM\textstyle{Z_{M}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}:=\textstyle{:=}{0,k}\textstyle{\{0,k\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[n][1][k][1][nr]\textstyle{[n_{\ell}]\star[1]\star[k]\star[1]\star[n_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[][1][m][2][r]\textstyle{[{\ell_{\ell}}]\star[\ell^{1}]\star[m]\star[\ell^{2}]\star[{\ell_{r}}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

By construction, the morphism res(ν):[k1]i+1,,j\operatorname{res}(\nu):[k-1]\to\langle i+1,\ldots,j\rangle is γ\gamma, and the morphism g¯\overline{g}^{\prime} restricts to g¯\overline{g} on [m][m], so this diagram determines a morphism in Ω\Omega covering gg. Call this morphism μZ,M:ZZM\mu_{Z,M}:Z\to Z_{M}.

Now suppose we are given a morphism

Z\textstyle{Z\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}=\textstyle{=}{i,j}\textstyle{\{i,j\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[n]\textstyle{[n]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}f\scriptstyle{f}ρ\scriptstyle{\rho}[]\textstyle{[\ell]}X\textstyle{X\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}:=\textstyle{:=}{0,k}\textstyle{\{0,k\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[a]\textstyle{[a]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}h\scriptstyle{h}[b]\textstyle{[b]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}w\scriptstyle{w}

covering gg. We can decompose this into

Z\textstyle{Z\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}=\textstyle{=}{i,j}\textstyle{\{i,j\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[n][nc][nr]\textstyle{[n_{\ell}]\star[n_{c}]\star[n_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}f\scriptstyle{f}ρ\scriptstyle{\rho}[][c][r]\textstyle{[{\ell_{\ell}}]\star[{\ell_{c}}]\star[{\ell_{r}}]}ZM\textstyle{Z_{M}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}:=\textstyle{:=}{0,k}\textstyle{\{0,k\}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\subset}[a][ac][ar]\textstyle{[a_{\ell}]\star[a_{c}]\star[a_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}h\scriptstyle{h}[b][bc][br]\textstyle{[{b_{\ell}}]\star[b_{c}]\star[{b_{r}}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}w\scriptstyle{w}

Where {0,k}[ac]\{0,k\}\subset[a_{c}]. By Lemma 2.16, we know that ρ\rho is uniquely determined on all of [nc][n_{c}] except the endpoints. This allows us to further decompose the diagram

[nc]\textstyle{[n_{c}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}f\scriptstyle{f}ρ\scriptstyle{\rho}[c]\textstyle{[{\ell_{c}}]}[ac]\textstyle{[a_{c}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}h\scriptstyle{h}[bc]\textstyle{[b_{c}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}w\scriptstyle{w}

as a diagram where the bottom map is a star product with fMf_{M}.

[nc]\textstyle{[n_{c}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}f\scriptstyle{f}ρ\scriptstyle{\rho}[c]\textstyle{[{\ell_{c}}]}[ac1][k][ac2]\textstyle{[a_{c}^{1}]\star[k]\star[a_{c}^{2}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}h\scriptstyle{h}[bc1][m][bc2]\textstyle{[b_{c}^{1}]\star[m]\star[b_{c}^{2}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}w\scriptstyle{w}

If there is morphism ZMXZ_{M}\to X in EE commuting with the morphisms ZXZ\to X and μZ,M\mu_{Z,M}, it must, in particular, restrict to a commutative diagram

[nc]\textstyle{[n_{c}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[c]\textstyle{[{\ell_{c}}]}[1][k][1]\textstyle{[1]\star[k]\star[1]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[1][m][2]\textstyle{[\ell^{1}]\star[m]\star[\ell^{2}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[ac1][k][ac2]\textstyle{[a_{c}^{1}]\star[k]\star[a_{c}^{2}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}h\scriptstyle{h}[bc1][m][bc2]\textstyle{[b_{c}^{1}]\star[m]\star[b_{c}^{2}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

Moreover, since the morphism is in EE, the bottom square must restrict to the commutative diagram

[k]\textstyle{[k]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}fM\scriptstyle{f_{M}}id\scriptstyle{{\operatorname{id}}}[m]\textstyle{[m]}[k]\textstyle{[k]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}fM\scriptstyle{f_{M}}[m]\textstyle{[m]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}id\scriptstyle{{\operatorname{id}}}

As a result, the component morphism [1][k][1][ac1][k][ac2][1]\star[k]\star[1]\to[a_{c}^{1}]\star[k]\star[a_{c}^{2}] is uniquely determined by the commutativity of the left-hand triangle. Additionally, since w:[b][]w:[b]\to[\ell] must restrict to g¯\overline{g} on [m][m], we can decompose ww as a star product

w=w1g¯w2:[bc1][m][bc2][1][cm][2]w=w^{1}\star\overline{g}\star w^{2}:[b_{c}^{1}]\star[m]\star[b_{c}^{2}]\to[\ell^{1}]\star[\ell_{c}^{m}]\star[\ell^{2}]

Therefore, the component morphism

[bc1][m][bc2][1][m][2][b_{c}^{1}]\star[m]\star[b_{c}^{2}]\to[\ell^{1}]\star[m]\star[\ell^{2}]

is uniquely determined, and must be w1id[m]w2w^{1}\star{\operatorname{id}}_{[m]}\star w^{2}.

We now extend back to the full diagram

[n][nc][nr]\textstyle{[n_{\ell}]\star[n_{c}]\star[n_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[][c][r]\textstyle{[\ell_{\ell}]\star[{\ell_{c}}]\star[\ell_{r}]}[n][1][k][1][nr]\textstyle{[n_{\ell}]\star[1]\star[k]\star[1]\star[n_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[][1][m][2][r]\textstyle{[\ell_{\ell}]\star[\ell^{1}]\star[m]\star[\ell^{2}]\star[\ell_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[a][ac1][k][ac2][ar]\textstyle{[a_{\ell}]\star[a_{c}^{1}]\star[k]\star[a_{c}^{2}]\star[a_{r}]}[b][bc1][m][bc2][br]\textstyle{[b_{\ell}]\star[b_{c}^{1}]\star[m]\star[b_{c}^{2}]\star[b_{r}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

and note that, since the vertical components of the back square restrict to identities on [n][n_{\ell}], [nr][n_{r}], [][\ell_{\ell}], and [r][\ell_{r}], the bottom square is uniquely determined by the morphisms [n][a][n_{\ell}]\to[a_{\ell}], [nr][ar][n_{r}]\to[a_{r}], b][]b_{\ell}]\to[\ell_{\ell}], and [br][r][b_{r}]\to[\ell_{r}]. So there is a unique morphism ZMXZ_{M}\to X in Ω\Omega with the desired properties. ∎

Proposition 2.20.

The functor :ΩΔ\mathcal{L}:\Omega\to\Delta^{\star} is an \infty-categorical localization at the morphisms in EE.

Proof.

Consider the inclusion ιM:ΩMEΩMΩ/M\iota_{M}:\Omega_{M}^{E}\subset\Omega_{M}\hookrightarrow\Omega_{/M}, and

Z:={{i,j}[n]fZ[]+gZ:([i],,[j])([m1],,[mk]) in ΔZ:=\begin{cases}\{i,j\}\subset[n]\overset{f_{Z}}{\to}[\ell]&+\\ g_{Z}:([\ell_{i}],\ldots,[\ell_{j}])\to([m_{1}],\ldots,[m_{k}])&\text{ in }\Delta^{\star}\end{cases}

in Ω/M\Omega_{/M}. Denote the overcategory (ΩME)Z/:=ΩME×Ω/M(Ω/M)Z/\left(\Omega^{E}_{M}\right)_{Z/}:=\Omega^{E}_{M}\times_{\Omega_{/M}}\left(\Omega_{/M}\right)_{Z/}. Lemma 2.19 tells us that (ΩME)Z/\left(\Omega^{E}_{M}\right)_{Z/} is non-empty, and that the object ZMZ_{M} constructed in the lemma is an initial object. Moreover, by Lemma 2.18, ΩME\Omega_{M}^{E} has an initial object. Therefore, by [17, Lemma 3.1.1], \mathcal{L} is a localization at the morphisms of EE. ∎

2.2.3. Algebra conditions

Denote by Funalg(Δ,𝒞)\operatorname{Fun}^{alg}(\Delta^{\star},\mathcal{C}) the full sub-\infty-category of functors ff which

  1. (A)

    send the diagrams

    (j[n1][mj],,j[n][mj])\textstyle{(\bigstar_{j\in[n_{1}]}[m_{j}],\ldots,\bigstar_{j\in[n_{\ell}]}[m_{j}])\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}([n1],,[n])\textstyle{([n_{1}],\ldots,[n_{\ell}])\ignorespaces\ignorespaces\ignorespaces\ignorespaces}([m1],,[mk])\textstyle{([m_{1}],\ldots,[m_{k}])\ignorespaces\ignorespaces\ignorespaces\ignorespaces}([1],,[1]×k)\textstyle{(\underbrace{[1],\ldots,[1]}_{\times k})}

    opposite the diagrams

    [mi]\textstyle{\bigstar[m_{i}]}[n1][n]\textstyle{[n_{1}]\star\cdots\star[n_{\ell}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[m1][mk]\textstyle{[m_{1}]\star\cdots\star[m_{k}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[1][1]\textstyle{[1]\star\cdots\star[1]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}id\scriptstyle{\operatorname{id}}{0,m1},{0,mk}\scriptstyle{\{0,m_{1}\},\ldots\{0,m_{k}\}}

    to pullback diagrams.

  2. (B)

    send the diagrams

    ([m1],,[mk])\textstyle{([m_{1}],\ldots,[m_{k}])\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[m1]\textstyle{[m_{1}]}[m2]\textstyle{[m_{2}]}\textstyle{\cdots}[mk1]\textstyle{[m_{k-1}]}[mk]\textstyle{[m_{k}]}

    to product diagrams.

Proposition 2.21.

There is an equivalence of \infty-categories

AlgSp(𝒞)Funalg(Δ,𝒞).\operatorname{Alg}_{\operatorname{Sp}}(\mathcal{C})\simeq\operatorname{Fun}^{alg}(\Delta^{\star},\mathcal{C}).
Proof.

It is clear that condition (B) corresponds to condition (2) from Corollary 2.5. For condition (A), first consider a 3-simplex [n0]ϕ1[n1]ϕ2[n2]ϕ3[n3][n_{0}]\overset{\phi_{1}}{\to}[n_{1}]\overset{\phi_{2}}{\to}[n_{2}]\overset{\phi_{3}}{\to}[n_{3}] in Δ\Delta. The corresponding limit diagram Eq. 4 can be written as

G(ϕ2ϕ1,{i,j})\textstyle{G(\phi_{2}\circ\phi_{1},\{i,j\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G(ϕ1,{i,j})\textstyle{G(\phi_{1},\{i,j\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G(ϕ2,{ϕ1(i),ϕ1(j)})\textstyle{G(\phi_{2},\{\phi_{1}(i),\phi_{1}(j)\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G(ϕ3,{ψ2(i),ψ2(j)})\textstyle{G(\phi_{3},\{\psi_{2}(i),\psi_{2}(j)\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G([n1],{ψ1(i),ψ1(j)})\textstyle{G([n_{1}],\{\psi_{1}(i),\psi_{1}(j)\})}G([n2],{ψ2(i),ψ2(j)})\textstyle{G([n_{2}],\{\psi_{2}(i),\psi_{2}(j)\})}

However, by (the dual of) [13, Proposition 4.4.2.2], this diagram is a limit if and only if the induced diagram

G(ϕ2ϕ1,{i,j})\textstyle{G(\phi_{2}\circ\phi_{1},\{i,j\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G([n1],{ψ1(i),ψ1(j)})\textstyle{G([n_{1}],\{\psi_{1}(i),\psi_{1}(j)\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G([n2],{ψ2(i),ψ2(j)})\textstyle{G([n_{2}],\{\psi_{2}(i),\psi_{2}(j)\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G(ϕ3,{ϕ1(i),ϕ1(j)})\textstyle{G(\phi_{3},\{\phi_{1}(i),\phi_{1}(j)\})}

is pullback. However, combining these two diagrams, we get

G(ϕ2ϕ1,{i,j})\textstyle{G(\phi_{2}\circ\phi_{1},\{i,j\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G([n1],{ψ1(i),ψ1(j)})\textstyle{G([n_{1}],\{\psi_{1}(i),\psi_{1}(j)\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G([n2],{ψ2(i),ψ2(j)})\textstyle{G([n_{2}],\{\psi_{2}(i),\psi_{2}(j)\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G(ϕ1,{i,j})\textstyle{G(\phi_{1},\{i,j\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G(ϕ3,{ϕ1(i),ϕ1(j)})\textstyle{G(\phi_{3},\{\phi_{1}(i),\phi_{1}(j)\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G(ϕk,{ψ2(i),ψ2(j)})\textstyle{G(\phi_{k},\{\psi_{2}(i),\psi_{2}(j)\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G([n1],{ψ1(i),ψ1(j)})\textstyle{G([n_{1}],\{\psi_{1}(i),\psi_{1}(j)\})}G([n2],{ψ2(i),ψ2(j)})\textstyle{G([n_{2}],\{\psi_{2}(i),\psi_{2}(j)\})}

By the pasting property for pullback diagrams, we thus see that it is sufficient to require that each of the diagrams corresponding to the sub-2-simplices of our simplex is pullback. Iterating this argument, we find that property (4) of corollary 2.5 is satisfied if and only if it is satisfied on 2-simplices. Since condition (A) is the image of this 2-simplex condition under \mathcal{L}, this proves the proposition. ∎

Lemma 2.22.

A functor fFun(Δ,𝒞)f\in\operatorname{Fun}(\Delta^{\star},\mathcal{C}) satisfies condition (A) if and only if it satisfies condition (A) for collections where all but one of the [mi][m_{i}] are equal to [1][1].

Proof.

This follows from applying the pasting law to diagrams of the form

([n1],,[n])\textstyle{([n_{1}],\ldots,[n_{\ell}])\ignorespaces\ignorespaces\ignorespaces\ignorespaces}([m1][1][1],[1],,[1])\textstyle{([m_{1}]\star[1]\star\cdots\star[1],[1],\ldots,[1])\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}([m1][m2][1],[1],,[1])\textstyle{([m_{1}]\star[m_{2}]\star\cdots\star[1],[1],\ldots,[1])\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\cdots\ignorespaces\ignorespaces\ignorespaces\ignorespaces}([1],,[1])\textstyle{([1],\ldots,[1])}([m1],[1],,[1])\textstyle{([m_{1}],[1],\ldots,[1])\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}([m1],[m2],,[1])\textstyle{([m_{1}],[m_{2}],\ldots,[1])\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\cdots\ignorespaces\ignorespaces\ignorespaces\ignorespaces}([1],,[1])\textstyle{([1],\ldots,[1])}([1],,[1],[m2],[1],,[1])\textstyle{([1],\ldots,[1],[m_{2}],[1],\ldots,[1])\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\cdots\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

If condition (A) is satisfied for squares where all but one of the [mi][m_{i}] are equal to [1][1], then the bottom right square and the right-hand rectangle are all pullback. Therefore, the top right square is pullback. Since our restricted version of condition (A) also implies that the top left square is pullback, the top rectangle is pullback. Iterating this argument then yields the lemma. ∎

2.3. Extension and restriction

Considering the full subcategory of Δ\Delta^{\star} on the objects ([n])([n]) for n0n\geq 0 we get

ι:ΔopΔ.\iota:\Delta^{op}\to\Delta^{\star}.

Taking restriction and right Kan extension gives us an adjunction of infinity categories

ι:Fun(Δ,𝒞)Fun(Δop,𝒞):ι!\iota_{\ast}:\operatorname{Fun}(\Delta^{\star},\mathcal{C})\leftrightarrow\operatorname{Fun}(\Delta^{op},\mathcal{C}):\iota_{!}

Denote by Fun×(Δ,𝒞)\operatorname{Fun}^{\times}(\Delta^{\star},\mathcal{C}) the full sub-\infty-category that sends each diagram

([m1],,[mk])\textstyle{([m_{1}],\ldots,[m_{k}])\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[m1]\textstyle{[m_{1}]}[m2]\textstyle{[m_{2}]}\textstyle{\cdots}[mk1]\textstyle{[m_{k-1}]}[mk]\textstyle{[m_{k}]}

to a limit diagram.

Proposition 2.23.

The adjunction ι:Fun(Δ,𝒞)Fun(Δop,𝒞):ι!\iota_{\ast}:\operatorname{Fun}(\Delta^{\star},\mathcal{C})\leftrightarrow\operatorname{Fun}(\Delta^{op},\mathcal{C}):\iota_{!} descends to an equivalence of \infty-categories

Fun×(Δ,𝒞)Fun(Δop,𝒞).\operatorname{Fun}^{\times}(\Delta^{\star},\mathcal{C})\simeq\operatorname{Fun}(\Delta^{op},\mathcal{C}).
Proof.

We compute the overcategory (Δop)([m1],,[mk])/(\Delta^{op})_{([m_{1}],\ldots,[m_{k}])/}. An object in the overcategory will consist of a choice of i{1,2,,k}i\in\{1,2,\ldots,k\} and a morphism [n][mi][n]\to[m_{i}]. A morphism (i,[n][mi])(j,[][mj])(i,[n]\to[m_{i}])\to(j,[\ell]\to[m_{j}]) only exists if i=ji=j, and in this case is given by a commutative diagram

[]\textstyle{[\ell]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[n]\textstyle{\ignorespaces\ignorespaces\ignorespaces\ignorespaces[n]}[mi]\textstyle{[m_{i}]}

consequently, we find that the induced diagram

(Δop)([m1],,[mk])/\textstyle{(\Delta^{op})_{([m_{1}],\ldots,[m_{k}])/}}(Δop)([m1])/\textstyle{(\Delta^{op})_{([m_{1}])/}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(Δop)([m2])/\textstyle{(\Delta^{op})_{([m_{2}])/}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}\textstyle{\cdots}(Δop)([mk1])/\textstyle{(\Delta^{op})_{([m_{k-1}])/}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(Δop)([mk])/\textstyle{(\Delta^{op})_{([m_{k}])/}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

displays (Δop)([m1],,[mk])/(\Delta^{op})_{([m_{1}],\ldots,[m_{k}])/} as a coproduct, and, hence, for any fFun(Δop,𝒞)f\in\operatorname{Fun}(\Delta^{op},\mathcal{C}), the diagram

(5) ι!f(([m1],,[mk]))\textstyle{\iota_{!}f\left(([m_{1}],\ldots,[m_{k}])\right)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ι!f([m1])\textstyle{\iota_{!}f\left([m_{1}]\right)}ι!f([m2])\textstyle{\iota_{!}f\left([m_{2}]\right)}\textstyle{\cdots}ι!f([mk1])\textstyle{\iota_{!}f\left([m_{k-1}]\right)}ι!f([mk])\textstyle{\iota_{!}f\left([m_{k}]\right)}

displays ι!f(([m1],,[mk]))\iota_{!}f\left(([m_{1}],\ldots,[m_{k}])\right) as a product. Consequently, the adjunction descends to an adjunction ι:Fun×(Δ,𝒞)Fun(Δop,𝒞):ι!\iota_{\ast}:\operatorname{Fun}^{\times}(\Delta^{\star},\mathcal{C})\leftrightarrow\operatorname{Fun}(\Delta^{op},\mathcal{C}):\iota_{!}.

Since this is a right Kan extension from a full subcategory, the counit is an equivalence. Moreover, the components of the unit are equivalences on the objects of Δop\Delta^{op}. However, for every object ([m1],,[mk])([m_{1}],\ldots,[m_{k}]), the unit induces a natural transformation of limit diagrams of the form in diagram (5). Therefore, we see that the components of the unit are equivalences for all objects, and thus, the unit is also an equivalence. ∎

Proposition 2.24.

Denote by 2SegΔ(𝒞)2\operatorname{-Seg}_{\Delta}(\mathcal{C}) the full subcategory of Fun(Δop,𝒞)\operatorname{Fun}(\Delta^{\operatorname{op}},\mathcal{C}) on unital 2-Segal objects. Then the equivalence of the previous proposition descends to an equivalence of \infty-categories

Funalg(Δ,𝒞)2SegΔ(𝒞).\operatorname{Fun}^{alg}(\Delta^{\star},\mathcal{C})\simeq 2\operatorname{-Seg}_{\Delta}(\mathcal{C}).
Proof.

Let GFunalg(Δ,𝒞)G\in\operatorname{Fun}^{alg}(\Delta^{\star},\mathcal{C}), and consider the diagram

[n]\textstyle{[n]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[n+m1]\textstyle{\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces[n+m-1]}({0,1},{1,2},,{n1,n})\textstyle{(\{0,1\},\{1,2\},\ldots,\{n-1,n\})}([1],,[m]jth,,[1])\textstyle{([1],\ldots,\overbrace{[m]}^{j^{th}},\ldots,[1])\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

in Δ\Delta^{\star}. We can expand this diagram to

[n]\textstyle{[n]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[n+m1]\textstyle{\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces[n+m-1]}({0,1},{1,2},,{n1,n})\textstyle{(\{0,1\},\{1,2\},\ldots,\{n-1,n\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}([1],,[m]jth,,[1])\textstyle{([1],\ldots,\overbrace{[m]}^{j^{th}},\ldots,[1])\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}{j1,j}\textstyle{\{j-1,j\}}[m]\textstyle{\ignorespaces\ignorespaces\ignorespaces\ignorespaces[m]}

Since the two vertical morphisms in the lower square are sent to projections onto factors of a product, the lower square is sent to a pullback diagram under GG. We therefore see that the exterior square is sent to a pullback if and only if the upper square is sent to a pullback. However, the exterior square is opposite to the diagram

[n]\textstyle{[n]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}[n+m1]\textstyle{[n+m-1]}[1]\textstyle{[1]\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}{0,m}\scriptstyle{\{0,m\}}{j1,j}\scriptstyle{\{j-1,j\}}[m]\textstyle{[m]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

in Δ\Delta, which is precisely the diagram for the 2-Segal conditions when [m][0][m]\neq[0], and is the diagram for the unitality condition when [m]=[0][m]=[0]. Therefore, we see that GFun×(Δ,𝒞)G\in\operatorname{Fun}^{\times}(\Delta^{\star},\mathcal{C}) is in Funalg(Δ,𝒞)\operatorname{Fun}^{alg}(\Delta^{\star},\mathcal{C}) if and only if the underlying simplicial object is unital 2-Segal. ∎

We can summarize our results in the following theorem.

Theorem 2.25.

There is an equivalence of \infty-categories

AlgSp(𝒞)2SegΔ(𝒞).\operatorname{Alg}_{\operatorname{Sp}}(\mathcal{C})\simeq 2\operatorname{-Seg}_{\Delta}(\mathcal{C}).

3. Calabi-Yau algebras in Spans

We now extend the results of the previous section to Calabi-Yau algebras. Throughout this section we set Θ:Tw(𝒜ssCYop)×\Theta:\operatorname{Tw}(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}^{\operatorname{op}})\times_{\bbGamma}\bbGamma^{\amalg}. We will represent morphisms in Θ\Theta diagrammatically as

Q{\lx@inpgf@ignorespaces Q}S{\lx@inpgf@ignorespaces S}T{\lx@inpgf@ignorespaces T}P{\lx@inpgf@ignorespaces P}S{\lx@inpgf@ignorespaces S^{\prime}}T{\lx@inpgf@ignorespaces T^{\prime}}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}f\scriptstyle{\lx@inpgf@ignorespaces f^{\prime}}

where f,f,g,f,\,f^{\prime},\,g, and g¯\overline{g} are morphisms in 𝒜ssCY\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}} (not 𝒜ssCYop\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}^{\operatorname{op}}).

In general, for a morphism 𝑓T\diamond\overset{f}{\leftarrow}T in 𝒜ssCY\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}, we will denote the two possible subsets of the image of \diamond in 𝔽in\mathbb{F}\!\!\operatorname{in}_{\ast} by \emptyset and {1}\{1\}.

3.1. Conditions on functors

Suppose we are given a functor

G:Θ𝒞G:\Theta\to\mathcal{C}

corresponding to a functor Tw(𝒜ssCYop)𝒞×\operatorname{Tw}(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}^{\operatorname{op}})\to\mathcal{C}^{\times} over \bbGamma.

Proposition 3.1.

The functor GG defines a functor G¯:𝒜ssCYopSpan(𝒞×)\overline{G}:\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}^{\operatorname{op}}\to\operatorname{Span}_{\bbGamma}(\mathcal{C}^{\times}) if and only if for every simplex S0ϕ1S1ϕ2S2SnS_{0}\overset{\phi_{1}}{\to}S_{1}\overset{\phi_{2}}{\to}S_{2}\to\cdots\to S_{n} in 𝒜ssCY\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}, and every subset PSnP\subset S_{n}^{\circ} the corresponding diagram

(6) G(ψn1,P){\lx@inpgf@ignorespaces G(\psi_{n-1},P)}G(ϕn,P){\lx@inpgf@ignorespaces G(\phi_{n},P)}{\lx@inpgf@ignorespaces\cdots}G(ϕ1,ψn21(P)){\lx@inpgf@ignorespaces G(\phi_{1},\psi_{n-2}^{-1}(P))}G(Sn,P){\lx@inpgf@ignorespaces G(S_{n},P)}G(Sn1,ϕn1(P)){\lx@inpgf@ignorespaces G(S_{n-1},\phi_{n}^{-1}(P))}{\lx@inpgf@ignorespaces\cdots}G(S1,ψn21(P)){\lx@inpgf@ignorespaces G(S_{1},\psi_{n-2}^{-1}(P))}G(S0,ψn11(P)){\lx@inpgf@ignorespaces G(S_{0},\psi_{n-1}^{-1}(P))}

is a limit diagram in 𝒞\mathcal{C}, where ψk:=ϕnϕn1ϕnk\psi_{k}:=\phi_{n}\circ\phi_{n-1}\cdots\circ\phi_{n-k}.

Proof.

This is, mutatis mutandis, the same as the proof of Proposition 2.1. Note that if Sk=S_{k}=\diamond, then Sj=S_{j}=\diamond for all jkj\geq k. ∎

3.1.1. Equivalences

Suppose that G:Θ𝒞G:\Theta\to\mathcal{C} represents a co-Calabi-Yau algebra. This means that, for every inert morphism ϕ:ST\phi:S\to T in 𝒜ss𝒜ssCY\mathcal{A}\!\operatorname{ss}\subset\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}, and every PTP\subset T^{\circ},

  • For the source map ϕS\phi\to S in Tw(𝒜ssCYop)\operatorname{Tw}(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}^{\operatorname{op}}), the induced morphism

    G(ϕ,P)G(S,ϕ1(P))G(\phi,P)\to G(S,\phi^{-1}(P))

    is an equivalence

  • For the target map ϕT\phi\to T in 𝒜ssCYop\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}^{\operatorname{op}}, the induced morphism

    G(ϕ,P)G(T,P)G(\phi,P)\to G(T,P)

    is an equivalence.

Lemma 3.2.

Suppose GG represents a co-Calabi-Yau algebra object. Let ϕ:ST\phi:S\to T be a morphism in 𝒜ss\mathcal{A}\!\operatorname{ss} viewed as an object in Tw(𝒜ssCYop)\operatorname{Tw}(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}^{\operatorname{op}}) and let PTP\subset T.

  1. (1)

    Let ψ2:TP\psi_{2}:T\to P be the inert morphism is 𝒜ss\mathcal{A}\!\operatorname{ss} that acts as the identity on PP and sends all other elements to the basepoint. Then the induced morphism

    G(ψ2ϕ,P)G(ϕ,P)G(\psi_{2}\circ\phi,P)\to G(\phi,P)

    is an equivalence.

  2. (2)

    Let ψ1:ϕ1(P)S\psi_{1}:\phi^{-1}(P)\to S be morphism in 𝒜ss\mathcal{A}\!\operatorname{ss} defined via the inclusion. Then the induced morphism

    G(ψ2ϕψ1,P)G(ϕ,P)G(\psi_{2}\circ\phi\circ\psi_{1},P)\to G(\phi,P)

    is an equivalence.

Proof.

By Proposition 3.1, the diagrams

G(ψ2ϕ,P){\lx@inpgf@ignorespaces G(\psi_{2}\circ\phi,P)}G(ψ2,P){\lx@inpgf@ignorespaces G(\psi_{2},P)}G(ϕ,P){\lx@inpgf@ignorespaces G(\phi,P)}G(T,P){\lx@inpgf@ignorespaces G(T,P)}

is a pullback diagram. Since ψ2\psi_{2} is inert in 𝒜ss\mathcal{A}\!\operatorname{ss}, the morphism

G(ψ2,P)\displaystyle G(\psi_{2},P) G(T,P)\displaystyle\to G(T,P)

is an equivalence. Therefore, the morphism

G(ψ2ϕ,P)G(ϕ,P)G(\psi_{2}\circ\phi,P)\to G(\phi,P)

is an equivalence.

We now note that the morphism (ψ2ϕχ,P)(ϕ,P)(\psi_{2}\circ\phi\circ\chi,P)\to(\phi,P) can be factored as

(ψ2ϕχ,P)(ψ2ϕ,P)(ϕ,P).(\psi_{2}\circ\phi\circ\chi,P)\to(\psi_{2}\circ\phi,P)\to(\phi,P).

Since the second of these morphisms is an equivalence, we need only show that the first is as well. To do this, we write down a composite

P{\lx@inpgf@ignorespaces P}P{\lx@inpgf@ignorespaces P}ϕ1(P){\lx@inpgf@ignorespaces\phi^{-1}(P)}P{\lx@inpgf@ignorespaces P}P{\lx@inpgf@ignorespaces P}S{\lx@inpgf@ignorespaces S}P{\lx@inpgf@ignorespaces P}P{\lx@inpgf@ignorespaces P}ϕ1(P){\lx@inpgf@ignorespaces\phi^{-1}(P)}\subseteqψ2ϕψ1\scriptstyle{\lx@inpgf@ignorespaces\psi_{2}\circ\phi\circ\psi_{1}}ψ1\scriptstyle{\lx@inpgf@ignorespaces\psi_{1}}\subseteqid\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}}ψ2ϕ\scriptstyle{\lx@inpgf@ignorespaces\psi_{2}\circ\phi}π\scriptstyle{\lx@inpgf@ignorespaces\pi}\subseteqid\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}}ψ2ϕψ1\scriptstyle{\lx@inpgf@ignorespaces\psi_{2}\circ\phi\circ\psi_{1}}

in Tw(𝒜ssCYop)×ΓΓ\operatorname{Tw}(\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}^{\operatorname{op}})\times_{\Gamma}\Gamma^{\amalg}, where π\pi is the inert morphism projecting SS onto the subset ϕ1(S)\phi^{-1}(S). Since the composite is the identity, it will suffice to show that the bottom square is sent to an equivalence under GG.

Denote by ν\nu the morphism defined by the bottom square. By Proposition 3.1, we can write down a pullback square

G(ψ2ϕ,P){\lx@inpgf@ignorespaces G(\psi_{2}\circ\phi,P)}G(ψ2ϕψ1,P){\lx@inpgf@ignorespaces G(\psi_{2}\circ\phi\circ\psi_{1},P)}G(π,ϕ1(P)){\lx@inpgf@ignorespaces G(\pi,\phi^{-1}(P))}G(ϕ1(P),ϕ1(P)){\lx@inpgf@ignorespaces G(\phi^{-1}(P),\phi^{-1}(P))}ν\scriptstyle{\lx@inpgf@ignorespaces\nu}

The bottom right morphism is the source map of an inert morphism, and thus is an equivalence. Therefore, ν\nu is also an equivalence. ∎

Proposition 3.3.

Suppose that GG sends the morphisms from Lemma 3.2 to equivalences. Let μ\mu be a morphism

Q{\lx@inpgf@ignorespaces Q}S{\lx@inpgf@ignorespaces S}T{\lx@inpgf@ignorespaces T}P{\lx@inpgf@ignorespaces P}U{\lx@inpgf@ignorespaces U}V{\lx@inpgf@ignorespaces V}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}h\scriptstyle{\lx@inpgf@ignorespaces h}

such that g|P:PQg|_{P}:P\to Q is an isomorphism, P=g1(Q)P=g^{-1}(Q), and g¯|f1(Q):f1(Q)h1(P)\overline{g}|_{f^{-1}(Q)}:f^{-1}(Q)\to h^{-1}(P) is an isomorphism. Then G(μ)G(\mu) is an equivalence.

Proof.

Consider the diagram

Q{\lx@inpgf@ignorespaces Q}Q{\lx@inpgf@ignorespaces Q}f1(Q){\lx@inpgf@ignorespaces f^{-1}(Q)}Q{\lx@inpgf@ignorespaces Q}S{\lx@inpgf@ignorespaces S}T{\lx@inpgf@ignorespaces T}P{\lx@inpgf@ignorespaces P}U{\lx@inpgf@ignorespaces U}V{\lx@inpgf@ignorespaces V}\subseteq\scriptstyle{\lx@inpgf@ignorespaces\subset}\subseteqproj\scriptstyle{\lx@inpgf@ignorespaces\operatorname{proj}}f\scriptstyle{\lx@inpgf@ignorespaces f}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}h\scriptstyle{\lx@inpgf@ignorespaces h}

The top square is a morphism from Lemma 3.2, and hence is sent to an equivalence. Moreover, the composite morphism can be decomposed as

Q{\lx@inpgf@ignorespaces Q}Q{\lx@inpgf@ignorespaces Q}f1(P){\lx@inpgf@ignorespaces f^{-1}(P)}P{\lx@inpgf@ignorespaces P}P{\lx@inpgf@ignorespaces P}h1(P){\lx@inpgf@ignorespaces h^{-1}(P)}P{\lx@inpgf@ignorespaces P}U{\lx@inpgf@ignorespaces U}V{\lx@inpgf@ignorespaces V}\subseteq\scriptstyle{\lx@inpgf@ignorespaces\cong}\subseteq\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\subset}\subseteqproj\scriptstyle{\lx@inpgf@ignorespaces\operatorname{proj}}h\scriptstyle{\lx@inpgf@ignorespaces h}

Since the lower square is sent to an equivalence by Lemma 3.2 and the upper square is an isomorphism, this composite is sent to an equivalence. Therefore, by the 2-out-of-3 property, G(μ)G(\mu) is an equivalence. ∎

Proposition 3.4.

Suppose that GG represents a co-Calabi-Yau algebra. Let μ\mu be a morphism

{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}T{\lx@inpgf@ignorespaces T}{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}S{\lx@inpgf@ignorespaces S}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqid\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}}h\scriptstyle{\lx@inpgf@ignorespaces h}

such that g¯|f1():f1()g1()\overline{g}|_{f^{-1}(\diamond)}:f^{-1}(\diamond)\to g^{-1}(\diamond) is an isomorphism. Then G(μ)G(\mu) is an equivalence.

Proof.

This is, mutatis mutandis, the same as the proof of Lemma 3.2 part (2). ∎

Definition 3.5.

We define the set EE of morphisms in Θ\Theta to be the set of all morphisms from Proposition 3.3 and Proposition 3.4. ∎

3.1.2. Non-degeneracy

We now consider a morphism γ\gamma in SpanΓ(𝒞×)\operatorname{Span}_{\Gamma}(\mathcal{C}^{\times}) represented by

X×X(γ1,γ2)Y.X\times X\overset{(\gamma_{1},\gamma_{2})}{\leftarrow}Y\rightarrow\ast.
Lemma 3.6.

The morphism γ\gamma is non-degenerate in the sense of Definition 1.17 if and only if γ1\gamma_{1} and γ2\gamma_{2} are equivalences.

Proof.

If γ1\gamma_{1} and γ2\gamma_{2} are equivalences, we can define a morphism

Y(γ1,γ2)X×X\ast\leftarrow Y\overset{(\gamma_{1},\gamma_{2})}{\longrightarrow}X\times X

which displays the non-degeneracy of γ\gamma.

Now suppose that γ\gamma is non-degenerate, and let η:=(η1,η2)\eta:=(\eta_{1},\eta_{2}) be a morphism

Z(η1,η2)X×X\ast\leftarrow Z\overset{(\eta_{1},\eta_{2})}{\longrightarrow}X\times X

displaying the non-degeneracy of γ\gamma. Then we have the diagram

Y{\lx@inpgf@ignorespaces Y} X{\lx@inpgf@ignorespaces X} Y×XY{\lx@inpgf@ignorespaces Y\times_{X}Y} Z{\lx@inpgf@ignorespaces Z} Y{\lx@inpgf@ignorespaces Y} Y{\lx@inpgf@ignorespaces Y} X{\lx@inpgf@ignorespaces X} X{\lx@inpgf@ignorespaces X} X{\lx@inpgf@ignorespaces X} X{\lx@inpgf@ignorespaces X} ν\scriptstyle{\lx@inpgf@ignorespaces\nu}s\scriptstyle{\lx@inpgf@ignorespaces s}k\scriptstyle{\lx@inpgf@ignorespaces k}b\scriptstyle{\lx@inpgf@ignorespaces b}a\scriptstyle{\lx@inpgf@ignorespaces a}\scriptstyle{\lx@inpgf@ignorespaces\ell}p\scriptstyle{\lx@inpgf@ignorespaces p}q\scriptstyle{\lx@inpgf@ignorespaces q}γ1\scriptstyle{\lx@inpgf@ignorespaces\gamma_{1}}γ2\scriptstyle{\lx@inpgf@ignorespaces\gamma_{2}}γ2\scriptstyle{\lx@inpgf@ignorespaces\gamma_{2}}γ1\scriptstyle{\lx@inpgf@ignorespaces\gamma_{1}}

where every square is pullback. The left hand pullback must define an equivalence in Span(𝒞)\operatorname{Span}(\mathcal{C}), and therefore, the morphism \ell is an equivalence. We thus see that γ1\gamma_{1} must have a left inverse up to homotopy. Similarly, we see that the morphism kk must be an equivalence. By the symmetry of the left-hand pullback square, qsq\circ s must be an equivalence, and thus , bνb\circ\nu is an equivalence. However, ν\nu is a pullback of γ1\gamma_{1} along an equivalence, and therefore is homotopic to γ1\gamma_{1}. Therefore, we see that γ1\gamma_{1} has a right inverse up to homotopy, and so, γ1\gamma_{1} is an equivalence. A similar argument shows that γ2\gamma_{2} is an equivalence. ∎

Construction 3.7.

Let G:Θ𝒞G:\Theta\to\mathcal{C} be a functor representing a trace co-algebra in Span(𝒞×)\operatorname{Span}_{\bbGamma}(\mathcal{C}^{\times}). In particular, we have the object

Y:=G({1}2)Y:=G(\{1\}\subset\diamond\leftarrow\langle 2\rangle)

and the object

Xn:=G({2}2𝑓n+1)X_{n}:=G(\{2\}\subset\langle 2\rangle\overset{f}{\leftarrow}\langle n+1\rangle)

where f(1)=1f(1)=1 and f(i)=2f(i)=2 for all i1i\neq 1. Finally, we have the object

Zn:=G({1}nZ_{n}:=G(\{1\}\subset\diamond\leftarrow\langle n\rangle

By 3.1, we get a pullback diagram

Zn{\lx@inpgf@ignorespaces Z_{n}}Xn{\lx@inpgf@ignorespaces X_{n}}Y{\lx@inpgf@ignorespaces Y}(2,{2}){\lx@inpgf@ignorespaces(\langle 2\rangle,\{2\})}

By 3.6, we know that the trace is non-degenerate if and only if the bottom right morphism is an equivalence. From the structure of the pullback diagram, we see that this is equivalent to requiring that the morphism ZnZnZ_{n}\to Z_{n} is an equivalence for all nn. ∎

We can summarize the conditions we have worked out in the following corollary

Corollary 3.8.

A functor G:Θ𝒞G:\Theta\to\mathcal{C} defines a Calabi-Yau co-algebra in SpanΓ(𝒞×)\operatorname{Span}_{\Gamma}(\mathcal{C}^{\times}) if and only if it satisfies the following conditions:

  1. (1)

    GG sends empty subsets to the terminal object.

  2. (2)

    GG sends PSTP\subset S\leftarrow T together with its projections to {i}ST\{i\}\subset S\leftarrow T for iPi\in P to a product diagram.

  3. (3)

    GG sends the morphisms in EE to equivalences.

  4. (4)

    GG sends all diagrams of the form Eq. 6 to limit diagrams.

  5. (5)

    GG sends the morphisms ZnXnZ_{n}\to X_{n} from 3.7 to equivalences.

Definition 3.9.

We define AlgSpCY(𝒞)\operatorname{Alg}_{\operatorname{Sp}}^{\operatorname{CY}}(\mathcal{C}) to be the full \infty-subcategory of Fun(Θ,𝒞)\operatorname{Fun}(\Theta,\mathcal{C}) satisfying the conditions of Corollary 3.8. ∎

3.2. The localization

Definition 3.10.

Let Λ\Lambda^{\star} be the category with objects

  • finite collections {[mi]}iS\{[m_{i}]\}_{i\in S} in Δ\Delta indexed by S𝔽inS\in\mathbb{F}\!\!\operatorname{in}, and

  • n\langle n\rangle in Λ\Lambda,

and morphisms given by

  1. (1)

    a morphism {[mi]}iS{[nj]}jT\{[m_{i}]\}_{i\in S}\to\{[n_{j}]\}_{j\in T} is given by

    • a morphism ϕ:TS\phi:T\to S in 𝔽in\mathbb{F}\!\!\operatorname{in}, with a chosen linear order on each fiber, and

    • for each iSi\in S, a morphism

      jϕ1(i)[nj][mi]\bigoplus_{j\in\phi^{-1}(i)}[n_{j}]\to[m_{i}]
  2. (2)

    a morphism n{[mi]}iS\langle n\rangle\to\{[m_{i}]\}_{i\in S} is given by

    • a cyclic order on SS, and

    • a morphism

      S[mi]n\bigcup\nolimits^{S}[m_{i}]\to\langle n\rangle

      in Λ\Lambda.

  3. (3)

    Empty homsets {[mi]}n\{[m_{i}]\}\to\langle n\rangle.

Composition is defined by taking lexicographic linear and cyclic orders. It is well-defined by Lemma 1.13. ∎

Definition 3.11.

As in the case of algebra objects, we define a version of Θ\Theta on non-degenerate subsets. Let Ω\Omega be the full subcategory of Θ\Theta on those objects

QS𝑓TQ\subset S\overset{f}{\longleftarrow}T

such that QQ\neq\emptyset and f:TSf:T\to S is not id{\operatorname{id}}_{\diamond}. ∎

Lemma 3.12.

The is an equivalence of \infty-categories

Fun(Θ,𝒞)Fun(Ω,𝒞)\operatorname{Fun}^{\ast}(\Theta,\mathcal{C})\simeq\operatorname{Fun}(\Omega,\mathcal{C})

Where Fun\operatorname{Fun}^{\ast} denotes the full subcategory on those functors which send empty subsets to the terminal object of 𝒞\mathcal{C}.

Proof.

This is, mutatis mutandis, the same proof as that of Lemma 2.8. ∎

01012012345
Figure 4. A pictorial representation of a morphism μ\mu in Ω\Omega, considered as a sequence Tg¯VU𝑔ST\overset{\overline{g}}{\to}V\overset{h}{\to}U\overset{g}{\to}S of morphisms in 𝒜ss\mathcal{A}\!\operatorname{ss}. The chosen subsets QSQ\subset S and PUP\subset U are marked in red, and the induced morphism (μ)\mathcal{L}(\mu) is drawn in blue. Note that, unlike in the analogous Fig. 3, the source of (μ)\mathcal{L}(\mu) is the ordinal sum iPO(f1(i))\bigoplus_{i\in P}O(f^{-1}(i)), owing to the presence interstitial trees with roots not in PP.
Construction 3.13.

We define a functor ΩΛ\Omega\to\Lambda^{\star} as follows. Let

PS𝑓TP\subset S\overset{f}{\leftarrow}T

be an object in Ω\Omega with ff a morphism in 𝒜ss\mathcal{A}\!\operatorname{ss}. We send this object to the collection

{O(f1(i))}iP.\left\{O\left(f^{-1}(i)\right)\right\}_{i}\in P.

Let

{}𝑓S\{\diamond\}\subset\diamond\overset{f}{\leftarrow}S

be an object in Ω\Omega. Then we send this object to

D(f1())Λ.D(f^{-1}(\diamond))\in\Lambda.

To define \mathcal{L} on morphisms, we proceed by cases:

  1. (1)

    Suppose we have a diagram

    Q{\lx@inpgf@ignorespaces Q}S{\lx@inpgf@ignorespaces S}T{\lx@inpgf@ignorespaces T}P{\lx@inpgf@ignorespaces P}U{\lx@inpgf@ignorespaces U}V{\lx@inpgf@ignorespaces V}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}h\scriptstyle{\lx@inpgf@ignorespaces h}

    representing a morphism μ\mu in Ω\Omega, where all of the objects are in 𝒜ss𝒜ssCY\mathcal{A}\!\operatorname{ss}\subset\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}. (μ)\mathcal{L}(\mu) will be given by a morphism ϕμ\phi_{\mu} in Fin\operatorname{Fin}_{\ast} and a set of morphisms {ψi}iQ\{\psi_{i}\}_{i\in Q} in Δ\Delta. The morphism ϕμ\phi_{\mu} we take to be the restriction of gg to PUP\subset U^{\circ}. Fixing iQi\in Q, we see that g¯\overline{g} restricts to a morphism g¯i:f1(i)h1(g1(i))\overline{g}_{i}:f^{-1}(i)\to h^{-1}(g^{-1}(i)) of linearly ordered sets. This can be rewritten as

    g¯i:f1(i)jg1(i)h1(j)\overline{g}_{i}:f^{-1}(i)\to\bigoplus_{j\in g^{-1}(i)}h^{-1}(j)

    It therefore induces a morphism

    jg¯1(i)O(h1(i))O(f1(i))\bigstar_{j\in\overline{g}^{-1}(i)}O(h^{-1}(i))\to O(f^{-1}(i))

    We then define ψi\psi_{i} to be the composite

    jg¯1(i)PO(h1(i))jg¯1(i)O(h1(i))O(f1(i))\bigoplus_{j\in\overline{g}^{-1}(i)\cap P}O(h^{-1}(i))\to\bigstar_{j\in\overline{g}^{-1}(i)}O(h^{-1}(i))\to O(f^{-1}(i))

    See Fig. 4 for a pictorial representation.

  2. (2)

    Suppose we have a diagram

    {1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}T{\lx@inpgf@ignorespaces T}{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}V{\lx@inpgf@ignorespaces V}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqid\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}}h\scriptstyle{\lx@inpgf@ignorespaces h}

    representing a morphism μ\mu in Ω\Omega with T,U𝒜ssT,U\in\mathcal{A}\!\operatorname{ss}. Then (μ)\mathcal{L}(\mu) will be given by a morphism ψ:D(h1())D(f1())\psi:D(h^{-1}(\diamond))\to D(f^{-1}(\diamond)). The morphism g¯\overline{g} restricts to a morphism of cyclically ordered sets

    g¯:f1()h1()\overline{g}_{\diamond}:f^{-1}(\diamond)\to h^{-1}(\diamond)

    we therefore define ψ\psi to be D(g¯)D(\overline{g}_{\diamond}).

  3. (3)

    Suppose we have a diagram

    {1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}T{\lx@inpgf@ignorespaces T}P{\lx@inpgf@ignorespaces P}U{\lx@inpgf@ignorespaces U}V{\lx@inpgf@ignorespaces V}\subseteqf\scriptstyle{\lx@inpgf@ignorespaces f}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}h\scriptstyle{\lx@inpgf@ignorespaces h}

    representing a morphism μ\mu in Ω\Omega, where all objects except \diamond are in 𝒜ss\mathcal{A}\!\operatorname{ss}. The morphism (μ)\mathcal{L}(\mu) will be given by a cyclic order on PP and a morphism ψ:SO(f1(i))D(f1())\psi:\bigcup^{S}O(f^{-1}(i))\to D(f^{-1}(\diamond)). The cyclic order on PP is induced by the cyclic order on g1()Pg^{-1}(\diamond)\supset P. The morphism g¯\overline{g} restricts to a morphism

    g¯:f1()(gh)1()\overline{g}_{\diamond}:f^{-1}(\diamond)\to(g\circ h)^{-1}(\diamond)

    of cyclically ordered sets. Passing through DD gives a morphism

    D(g¯):D((gh)1())D(f1()).D(\overline{g}_{\diamond}):D((g\circ h)^{-1}(\diamond))\to D(f^{-1}(\diamond)).

    Choosing any linear order on g1()g^{-1}(\diamond) compatible with the cyclic order we can write D(g¯)D(\overline{g}_{\diamond}) as

    C(O(ig1()h1(i)))=D(K(ig1()h1(i))D(f1()CLOSECLOSEC(O(\bigoplus_{i\in g^{-1}(\diamond)}h^{-1}(i)))=D(K(\bigoplus_{i\in g^{-1}(\diamond)}h^{-1}(i))\to D(f^{-1}(\diamond)

    We then have the canonical morphism

    K(ig1()O(h1(i)))C(ig1()O(h1(i)))=C(O(ig1()h1(i)))K(\bigoplus_{i\in g^{-1}(\diamond)}O(h^{-1}(i)))\to C(\bigstar_{i\in g^{-1}(\diamond)}O(h^{-1}(i)))=C(O(\bigoplus_{i\in g^{-1}(\diamond)}h^{-1}(i)))

    And so we define ψ\psi to be the composite

    K(iPO(h1(i)))K(ig1()O(h1(i)))C(O(ig1()h1(i)))D(f1()CLOSEK(\bigoplus_{i\in P}O(h^{-1}(i)))\to K(\bigoplus_{i\in g^{-1}(\diamond)}O(h^{-1}(i)))\to C(O(\bigoplus_{i\in g^{-1}(\diamond)}h^{-1}(i)))\to D(f^{-1}(\diamond)

    See Fig. 5 for a pictorial representation.

\diamond01234567801010120
Figure 5. A morphism in Ω\Omega represented as a composite of three morphisms in 𝒜ssCY\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}, Tg¯VU𝑔T\overset{\overline{g}}{\to}V\overset{h}{\to}U\overset{g}{\to}\diamond. The chosen subset PUP\subset U is marked by red points. The corresponding interstice sets I(h1(i))I(h^{-1}(i)) are written in red numbers, and the set D(f1())D(f^{-1}(\diamond)) in blue numbers. The induced morphism (μ):PI(h1(i))D(f1())\mathcal{L}(\mu):\bigcup^{P}I(h^{-1}(i))\to D(f^{-1}(\diamond)) is drawn in blue. Note that the unmarked points in UU are the reason that we do not necessarily get a morphism C(iPI(h1(i))D(f1())CLOSEC(\bigstar_{i\in P}I(h^{-1}(i))\to D(f^{-1}(\diamond)).
Definition 3.14.

Let MΛM\in\Lambda^{\star}. We denote by ΩME\Omega_{M}^{E} the subcategory of the weak fiber ΩM\Omega_{M} whose morphisms are morphisms in EE. ∎

Proposition 3.15.

For every MM in Λ\Lambda^{\star}, there is an initial element in ΩME\Omega_{M}^{E}.

Proof.

We will complete the proof in two cases:

Suppose first that M={[mi]}iPM=\{[m_{i}]\}_{i\in P}. Then the weak fiber only involves morphisms in 𝒜ss𝒜ssCY\mathcal{A}\!\operatorname{ss}\subset\mathcal{A}\!\operatorname{ss}_{\operatorname{CY}}. We define a set

T:=iP𝕀([mi])T:=\coprod_{i\in P}\mathbb{I}([m_{i}])

and a morphism fM:TPf_{M}:T\to P by setting fM(𝕀([mi]))=if_{M}(\mathbb{I}([m_{i}]))=i. The canonical isomorphisms

ηi:O(𝕀([mi]))[mi]\eta_{i}:O(\mathbb{I}([m_{i}]))\cong[m_{i}]

equip PPfMTP\subset P\overset{f_{M}}{\longleftarrow}T with the structure of an object of ΩME\Omega_{M}^{E}. Given an element

PU𝑓VP\subset U\overset{f}{\leftarrow}V

and an isomorphism ϕi:O(f1(i))[mi]\phi_{i}:O(f^{-1}(i))\cong[m_{i}], we define a unique morphism μ\mu in ΩME\Omega_{M}^{E} given by

P{\lx@inpgf@ignorespaces P}P{\lx@inpgf@ignorespaces P}T{\lx@inpgf@ignorespaces T}P{\lx@inpgf@ignorespaces P}U{\lx@inpgf@ignorespaces U}V{\lx@inpgf@ignorespaces V}\subseteqfM\scriptstyle{\lx@inpgf@ignorespaces f_{M}}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}f\scriptstyle{\lx@inpgf@ignorespaces f}

as follows. Since this must be a morphism in EE, we see that gg must map PP identically to PP, and send UPU^{\circ}\setminus P to the basepoint. On fibers, we consider the isomorphisms

ηi1ϕi:O(f1(i))O(I[mi])\eta_{i}^{-1}\circ\phi_{i}:O(f^{-1}(i))\to O(I[m_{i}])

Since OO is fully faithful, this lifts to a unique isomorphism I(ϕi):I([mi])f1(i)I(\phi_{i}):I([m_{i}])\cong f^{-1}(i). We therefore see that g¯\overline{g} must be the coproduct of these morphisms if μ\mu is to be a morphism in the weak fiber. It is immediate that this does, indeed, define a morphism in ΩME\Omega_{M}^{E}.

Now suppose instead M=mM=\langle m\rangle. We define fM:D(m)f_{M}:D(\langle m\rangle)\to\diamond to be the morphism with fM1()=D(m)f_{M}^{-1}(\diamond)=D(\langle m\rangle). Since DD is an equivalence, we choose the isomorphism

η:D2(m)m\eta:D^{2}(\langle m\rangle)\cong\langle m\rangle

Suppose given another element

{1}𝑓T\{1\}\subset\diamond\overset{f}{\longleftarrow}T

with ϕ:D(f1())n\phi:D(f^{-1}(\diamond))\cong\langle n\rangle in the weak fiber. We define a unique morphism μΩME\mu\in\Omega_{M}^{E} given by

{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}D(mCLOSE{\lx@inpgf@ignorespaces D(\langle m\rangle}{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}T{\lx@inpgf@ignorespaces T}\subseteqfM\scriptstyle{\lx@inpgf@ignorespaces f_{M}}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}f\scriptstyle{\lx@inpgf@ignorespaces f}

as follows. The morphism gg must be the identity, so we need only define g¯\overline{g}. The condition that μ\mu be in the weak fiber implies that ηiD(g¯|D(m))=ϕi\eta_{i}\circ D(\overline{g}|_{D(\langle m\rangle)})=\phi_{i}, i.e. D(g¯|D(m))=ηi1ϕiD(\overline{g}|_{D(\langle m\rangle)})=\eta_{i}^{-1}\circ\phi_{i}. However, since DD is fully faithful, this condition defines a unique isomorphism D(m)f1()D(\langle m\rangle)\cong f^{-1}(\diamond), determining g¯\overline{g}, and thus μ\mu, uniquely. ∎

Proposition 3.16.

Suppose given an object M={[mi]}iPM=\{[m_{i}]\}_{i\in P} in Λ\Lambda^{\star}, an object

Z:={QSfZT}Z:=\left\{Q\subset S\overset{f_{Z}}{\leftarrow}T\right\}

in Ω\Omega, and a morphism

(ϕ,{γi}iQ):(Z)M(\phi,\{\gamma_{i}\}_{i\in Q}):\mathcal{L}(Z)\to M

in Λ\Lambda^{\star}. Then there is an element XM,ZX_{M,Z} in ΩME\Omega_{M}^{E} and a morphism Φ:ZXM,Z\Phi:Z\to X_{M,Z} in Ω\Omega covering (ϕ,{γi}iQ)(\phi,\{\gamma_{i}\}_{i\in Q}) such that, for any other morphism Ψ:ZX\Psi:Z\to X covering (ϕ,{γi}iQ)(\phi,\{\gamma_{i}\}_{i\in Q}), there is a unique morphism τ:XM,ZX\tau:X_{M,Z}\to X which makes the diagram

Z{\lx@inpgf@ignorespaces Z}XM,Z{\lx@inpgf@ignorespaces X_{M,Z}}X{\lx@inpgf@ignorespaces X}Ψ\scriptstyle{\lx@inpgf@ignorespaces\Psi}Φ\scriptstyle{\lx@inpgf@ignorespaces\Phi}τ\scriptstyle{\lx@inpgf@ignorespaces\tau}

commute.

Proof.

There are two cases to consider, corresponding to whether or not S=S=\diamond.

Case 1: First suppose S𝒜ssS\in\mathcal{A}\!\operatorname{ss}. In this case, we construct XM,ZX_{M,Z} as follows. Let

PPfMUP\subset P\overset{f_{M}}{\longleftarrow}U

be the object constructed in Proposition 3.16. Then, in particular, ϕ:PQS\phi:P\to Q\subset S.

For each iQi\in Q, we have a morphism

γi:jϕ1(i)[mi]O(fZ1(i))\gamma_{i}:\bigoplus_{j\in\phi^{-1}(i)}[m_{i}]\to O(f_{Z}^{-1}(i))

For each jϕ1(i)j\in\phi^{-1}(i) denote by γi([mj])\gamma_{i}([m_{j}]) the smallest subinterval of O(fZ1(i))O(f_{Z}^{-1}(i)) containing the image of [mj][m_{j}] under γi\gamma_{i}. Then γi|[mj]γi([mj])\gamma_{i}|_{[m_{j}]}\to\gamma_{i}([m_{j}]) preserves boundary, and thus corresponds to a map g¯j:I(γi([mj]))I([mj])\overline{g}_{j}:I(\gamma_{i}([m_{j}]))\to I([m_{j}]) of linearly ordered sets. Moreover, g¯j\overline{g}_{j} fits into a commutative diagram

S{\lx@inpgf@ignorespaces S}I(γi([mj])){\lx@inpgf@ignorespaces I(\gamma_{i}([m_{j}]))}P{\lx@inpgf@ignorespaces P}I([mj]){\lx@inpgf@ignorespaces I([m_{j}])}fZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}g¯j\scriptstyle{\lx@inpgf@ignorespaces\overline{g}_{j}}ϕ\scriptstyle{\lx@inpgf@ignorespaces\phi}fM\scriptstyle{\lx@inpgf@ignorespaces f_{M}}

in 𝒜ss\mathcal{A}\!\operatorname{ss}. We here use the identification of I(γi([mj]))I(\gamma_{i}([m_{j}])) with a subset of TT.

Since, by definition, U=jPI([mj])U=\coprod_{j\in P}I([m_{j}]), we can then write down a commutative diagram

(7) S{\lx@inpgf@ignorespaces S}i,jI(γi([mj])){\lx@inpgf@ignorespaces\coprod_{i,j}I(\gamma_{i}([m_{j}]))}P{\lx@inpgf@ignorespaces P}jPI([mj]){\lx@inpgf@ignorespaces\coprod_{j\in P}I([m_{j}])}fZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}i,jg¯j\scriptstyle{\lx@inpgf@ignorespaces\coprod_{i,j}\overline{g}_{j}}ϕ\scriptstyle{\lx@inpgf@ignorespaces\phi}fM\scriptstyle{\lx@inpgf@ignorespaces f_{M}}

in 𝒜ss\mathcal{A}\!\operatorname{ss}.

For each iQi\in Q, this restricts to a diagram of ordered sets

{i}{\lx@inpgf@ignorespaces\{i\}}jI(γi([mj])){\lx@inpgf@ignorespaces\coprod_{j}I(\gamma_{i}([m_{j}]))}ϕ1(i){\lx@inpgf@ignorespaces\phi^{-1}(i)}jϕ1(i)I([mj]){\lx@inpgf@ignorespaces\coprod_{j\in\phi^{-1}(i)}I([m_{j}])}fZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}jg¯j\scriptstyle{\lx@inpgf@ignorespaces\coprod_{j}\overline{g}_{j}}ϕ\scriptstyle{\lx@inpgf@ignorespaces\phi}fM\scriptstyle{\lx@inpgf@ignorespaces f_{M}}

We denote Li:=fZ1(i)jϕ1(i)I(γi([mj])CLOSEL_{i}:=f_{Z}^{-1}(i)\setminus\coprod_{j\in\phi^{-1}(i)}I(\gamma_{i}([m_{j}]), and proceed as follows.

  • For p,p+1p,p+1 in ϕ1(i)\phi^{-1}(i), if there is at least one kLik\in L_{i} such that

    I(γi([mp]))<k<I(γi([mp+1]))I(\gamma_{i}([m_{p}]))<k<I(\gamma_{i}([m_{p+1}]))

    we define a new element rpr_{p} and append it to ϕ1(i)\phi^{-1}(i) between pp and p+1p+1.

  • If there exists kLik\in L_{i} such that

    k<I(γi([mp]))k<I(\gamma_{i}([m_{p}]))

    for all pϕ1(i)p\in\phi^{-1}(i), then we append a new minimal element rminr_{min} to ϕ1(i)\phi^{-1}(i).

  • If there exists kLik\in L_{i} such that

    I(γi([mp]))<kI(\gamma_{i}([m_{p}]))<k

    for all pϕ1(i)p\in\phi^{-1}(i), then we append a new maximal element to ϕ1(i)\phi^{-1}(i).

Call the resulting set Wiϕ1(i)W_{i}\supset\phi^{-1}(i). We then set

Ri:=ULiR_{i}:=U\amalg L_{i}

and define fi:RiWif_{i}:R_{i}\to W_{i} to act as fMf_{M} on UU and on LiL_{i} to send

  • krpk\mapsto r_{p} if

    I(γi([mp]))<k<I(γi([mp+1]))I(\gamma_{i}([m_{p}]))<k<I(\gamma_{i}([m_{p+1}]))
  • krmink\mapsto r_{min} if

    k<I(γi([mp]))k<I(\gamma_{i}([m_{p}]))

    for all pϕ1(i)p\in\phi^{-1}(i)

  • krmaxk\mapsto r_{max} if

    I(γi([mp]))<kI(\gamma_{i}([m_{p}]))<k

    for all pϕ1(i)p\in\phi^{-1}(i)

We make fif_{i} into a morphism in 𝒜ss\mathcal{A}\!\operatorname{ss} by taking the linear order induced by LiL_{i} on the fibers over the rpr_{p}, rminr_{min} and rmaxr_{max}. We then define

g¯i:fZ1(i)Ri\overline{g}^{i}:f_{Z}^{-1}(i)\to R_{i}

to act as jϕ1(i)g¯j\coprod_{j\in\phi^{-1}(i)}\overline{g}_{j} on jϕ1(i)I(γi([mj]))\coprod_{j\in\phi^{-1}(i)}I(\gamma_{i}([m_{j}])) and as the identity on LiL_{i}. We further define ϕi:Wi{i}\phi_{i}:W_{i}\to\{i\} to send every element to ii. We thus have a commutative diagram

{i}{\lx@inpgf@ignorespaces\{i\}}{i}{\lx@inpgf@ignorespaces\{i\}}jI(γi([mj])){\lx@inpgf@ignorespaces\coprod_{j}I(\gamma_{i}([m_{j}]))}Pϕ1(i){\lx@inpgf@ignorespaces P\cap\phi^{-1}(i)}Wi{\lx@inpgf@ignorespaces W_{i}}Ri{\lx@inpgf@ignorespaces R_{i}}\subseteqfZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}g¯i\scriptstyle{\lx@inpgf@ignorespaces\overline{g}^{i}}\subseteqϕi\scriptstyle{\lx@inpgf@ignorespaces\phi_{i}}fi\scriptstyle{\lx@inpgf@ignorespaces f_{i}}

in 𝒜ss\mathcal{A}\!\operatorname{ss}, which covers the morphism γi:jϕ1(i)[mj]O(fZ1(i))\gamma_{i}:\bigoplus_{j\in\phi^{-1}(i)}[m_{j}]\to O(f_{Z}^{-1}(i)). Taking the coproduct over iIm(ϕ)i\in\operatorname{Im}(\phi) gives us a morphism

Im(ϕ){\lx@inpgf@ignorespaces\operatorname{Im}(\phi)}Im(ϕ){\lx@inpgf@ignorespaces\operatorname{Im}(\phi)}fZ1(Im(ϕ)){\lx@inpgf@ignorespaces f_{Z}^{-1}(\operatorname{Im}(\phi))}Pϕ1(i){\lx@inpgf@ignorespaces P\cap\phi^{-1}(i)}iWi{\lx@inpgf@ignorespaces\coprod_{i}W_{i}}iRi{\lx@inpgf@ignorespaces\coprod_{i}R_{i}}\subseteqfZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}ig¯i\scriptstyle{\lx@inpgf@ignorespaces\coprod_{i}\overline{g}^{i}}\subseteqiϕi\scriptstyle{\lx@inpgf@ignorespaces\coprod_{i}\phi_{i}}ifi\scriptstyle{\lx@inpgf@ignorespaces\coprod_{i}f_{i}}

Finally, we set

W=(iIm(ϕ)Wi)(SIm(ϕ))W=(\coprod_{i\in\operatorname{Im}(\phi)}W_{i})\amalg(S\setminus\operatorname{Im}(\phi))

and

R=(iIm(ϕ)Ri)(TfZ1(Im(ϕ)))R=(\coprod_{i\in\operatorname{Im}(\phi)}R_{i})\amalg(T\setminus f_{Z}^{-1}(\operatorname{Im}(\phi)))

We then define morphisms:

  • g:WSg:W\to S to act as iIm(ϕ)ϕi\coprod_{i\in\operatorname{Im}(\phi)}\phi_{i} on iIm(ϕ)Wi\coprod_{i\in\operatorname{Im}(\phi)}W_{i} and as the identity otherwise.

  • fM,Z:RWf_{M,Z}:R\to W to act as fif_{i} on RiR_{i} and as fZf_{Z} on TfZ1(Im(ϕ))T\setminus f_{Z}^{-1}(\operatorname{Im}(\phi)).

  • g¯:TR\overline{g}:T\to R to act as iIm(ϕ)g¯i\coprod_{i\in\operatorname{Im}(\phi)}\overline{g}^{i} on fZ1(Im(ϕ))f_{Z}^{-1}(\operatorname{Im}(\phi)) and the identity elsewhere.

By construction, this defines a commutative diagram

(8) Q{\lx@inpgf@ignorespaces Q}S{\lx@inpgf@ignorespaces S}T{\lx@inpgf@ignorespaces T}P{\lx@inpgf@ignorespaces P}W{\lx@inpgf@ignorespaces W}R{\lx@inpgf@ignorespaces R}\subseteqfZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}ig¯\scriptstyle{\lx@inpgf@ignorespaces\coprod_{i}\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}fM,Z\scriptstyle{\lx@inpgf@ignorespaces f_{M,Z}}

in 𝒜ss\mathcal{A}\!\operatorname{ss}, covering (ϕ,{γi})(\phi,\{\gamma_{i}\}), and the bottom row is in ΩM\Omega_{M}. We therefore define XM,ZX_{M,Z} to be the bottom row, and Φ\Phi to be the morphism defined by the diagram (8).

To check the remaining universal property, we let

PAfXBP\subset A\overset{f_{X}}{\leftarrow}B

and βi:O(fX1(i))[mi]\beta_{i}:O(f_{X}^{-1}(i))\cong[m_{i}] be another element in ΩME\Omega_{M}^{E}, and let ν\nu be a morphism

Q{\lx@inpgf@ignorespaces Q}S{\lx@inpgf@ignorespaces S}T{\lx@inpgf@ignorespaces T}P{\lx@inpgf@ignorespaces P}A{\lx@inpgf@ignorespaces A}B{\lx@inpgf@ignorespaces B}\subseteqfZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}ρ¯\scriptstyle{\lx@inpgf@ignorespaces\overline{\rho}}\subseteqρ\scriptstyle{\lx@inpgf@ignorespaces\rho}fX\scriptstyle{\lx@inpgf@ignorespaces f_{X}}

covering (ϕ,{γi}iQ)(\phi,\{\gamma_{i}\}_{i\in Q}).

For each iIm(ϕ)i\in\operatorname{Im}(\phi), the identity on PP and the condition nothing be sent to the basepoint uniquely determines a map of ordered sets

ζi:ρ1(i)Wi.\zeta_{i}:\rho^{-1}(i)\to W_{i}.

Moreover, the ζi\zeta_{i} together with the restriction of ρ\rho to Aρ1(Im(ϕ))A\setminus\rho^{-1}(\operatorname{Im}(\phi)) uniquely determines a map

ζ:AW\zeta:A\to W

such that the diagram

A{\lx@inpgf@ignorespaces A}S{\lx@inpgf@ignorespaces S}W{\lx@inpgf@ignorespaces W}ρ\scriptstyle{\lx@inpgf@ignorespaces\rho}ζ\scriptstyle{\lx@inpgf@ignorespaces\zeta}g\scriptstyle{\lx@inpgf@ignorespaces g}

commutes. Note that ζ|P\zeta|_{P} induces the identity PPP\to P.

Moreover, for each iIm(ϕ)i\in\operatorname{Im}(\phi) the isomorphisms I(βi)I(\beta_{i}) on I([mj])I([m_{j}]) and restriction ρ¯i:LifX1(ρ1(i))\overline{\rho}_{i}:L_{i}\to f_{X}^{-1}(\rho^{-1}(i)) uniquely determine a map

ζ¯i:RifX1(ρ1(i)).\overline{\zeta}_{i}:R_{i}\to f_{X}^{-1}(\rho^{-1}(i)).

These, together with the restriction of ρ¯\overline{\rho} to TfZ1(Im(ϕ))T\setminus f_{Z}^{-1}(\operatorname{Im}(\phi)) uniquely determine a morphism

ζ¯RB\overline{\zeta}R\to B

such that the diagram

B{\lx@inpgf@ignorespaces B}T{\lx@inpgf@ignorespaces T}R{\lx@inpgf@ignorespaces R}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}ρ¯\scriptstyle{\lx@inpgf@ignorespaces\overline{\rho}}ζ¯\scriptstyle{\lx@inpgf@ignorespaces\overline{\zeta}}

commutes, and the restriction of ζ¯\overline{\zeta} to fX1(P)f_{X}^{-1}(P) is the isomorphism iI(βi)\coprod_{i}I(\beta_{i}).

We therefore have constructed a unique morphism

(ζ,ζ¯):XZ,MX(\zeta,\overline{\zeta}):X_{Z,M}\to X

in ΩME\Omega_{M}^{E} such that the diagram

Z{\lx@inpgf@ignorespaces Z}XM,Z{\lx@inpgf@ignorespaces X_{M,Z}}X{\lx@inpgf@ignorespaces X}Ψ\scriptstyle{\lx@inpgf@ignorespaces\Psi}Φ\scriptstyle{\lx@inpgf@ignorespaces\Phi}(ζ,ζ¯)\scriptstyle{\lx@inpgf@ignorespaces(\zeta,\overline{\zeta})}

commutes.

Case 2: Now suppose that S=S=\diamond. Then ϕ\phi is completely determined by a cyclic order on PP, and γ\gamma is a morphism

γ:S[mi]D(fZ1()).\gamma:\bigcup\nolimits^{S}[m_{i}]\to D(f_{Z}^{-1}(\diamond)).

We note that, given any morphism

{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}V{\lx@inpgf@ignorespaces V}A{\lx@inpgf@ignorespaces A}B{\lx@inpgf@ignorespaces B}C{\lx@inpgf@ignorespaces C}\subseteqp\scriptstyle{\lx@inpgf@ignorespaces p}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}\scriptstyle{\lx@inpgf@ignorespaces\ell}

a choice of linear order on g1()g^{-1}(\diamond) compatible with the cyclic order uniquely determines a factorization

{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}V{\lx@inpgf@ignorespaces V}{1}{\lx@inpgf@ignorespaces\{1\}}{1}{\lx@inpgf@ignorespaces\{1\}}V{\lx@inpgf@ignorespaces V}A{\lx@inpgf@ignorespaces A}B{\lx@inpgf@ignorespaces B}C{\lx@inpgf@ignorespaces C}\subseteqp\scriptstyle{\lx@inpgf@ignorespaces p}idV\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}_{V}}\subseteqp\scriptstyle{\lx@inpgf@ignorespaces p}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}\scriptstyle{\lx@inpgf@ignorespaces\ell}

Similarly, given a morphism (ψ,η):n{[ni]}iS(\psi,\eta):\langle n\rangle\to\{[n_{i}]\}_{i\in S}, a choice of linear order on SS compatible with the cyclic order uniquely determines a factorization

n{[n]}{[ni]}.\langle n\rangle\to\{[n]\}\to\{[n_{i}]\}.

We can therefore choose a linear order on PP and define YY to be the object

{1}{1}fZT.\{1\}\subset\{1\}\overset{f_{Z}}{\leftarrow}T.

Then take (ϕY,γY)(\phi_{Y},\gamma_{Y}) to be the unique morphism yielding a factorization

(ϕ,γ):D(fZ1())K(fZ1())(ϕY,γY){[mi]}iP\mathcal{L}(\phi,\gamma):D(f^{-1}_{Z}(\diamond))\to K(f^{-1}_{Z}(\diamond))\overset{(\phi_{Y},\gamma_{Y})}{\longrightarrow}\{[m_{i}]\}_{i\in P}

We can then construct XM,YX_{M,Y} as in case 1. It is immediate that

{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}T{\lx@inpgf@ignorespaces T}{1}{\lx@inpgf@ignorespaces\{1\}}{1}{\lx@inpgf@ignorespaces\{1\}}T{\lx@inpgf@ignorespaces T}P{\lx@inpgf@ignorespaces P}WY{\lx@inpgf@ignorespaces W_{Y}}RY{\lx@inpgf@ignorespaces R_{Y}}\subseteqfZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}idT\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}_{T}}\subseteqfZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqg\scriptstyle{\lx@inpgf@ignorespaces g}fM,Y\scriptstyle{\lx@inpgf@ignorespaces f_{M,Y}}

defines a morphism Φ\Phi in Ω\Omega covering (ϕ,γ)(\phi,\gamma).

Now suppose given any other morphism Ψ=(ψ,ψ¯):ZX\Psi=(\psi,\overline{\psi}):Z\to X covering (ϕ,γ)(\phi,\gamma). A choice of linear order on ψ1()\psi^{-1}(\diamond) compatible with the chosen linear order on PP uniquely factors Ψ\Psi through YY. We therefore get a morphism τ:XM,YX\tau:X_{M,Y}\to X such that the diagram

Z{\lx@inpgf@ignorespaces Z}XM,Y{\lx@inpgf@ignorespaces X_{M,Y}}X{\lx@inpgf@ignorespaces X}Ψ\scriptstyle{\lx@inpgf@ignorespaces\Psi}Φ\scriptstyle{\lx@inpgf@ignorespaces\Phi}τ\scriptstyle{\lx@inpgf@ignorespaces\tau}

commutes.

To see that this morphism is unique, suppose that (ξ,ξ¯),(ζ,ζ¯):XM,YX(\xi,\overline{\xi}),(\zeta,\overline{\zeta}):X_{M,Y}\to X are two such morphisms. Then, choosing a linear order on ψ1()\psi^{-1}(\diamond) compatible with the chose linear order on PP uniquely factors the diagram as

Z{\lx@inpgf@ignorespaces Z}Y{\lx@inpgf@ignorespaces Y}XM,Y{\lx@inpgf@ignorespaces X_{M,Y}}X{\lx@inpgf@ignorespaces X}Ψ\scriptstyle{\lx@inpgf@ignorespaces\Psi}Φ\scriptstyle{\lx@inpgf@ignorespaces\Phi}(ξ,ξ¯),(ζ,ζ¯)\scriptstyle{\lx@inpgf@ignorespaces(\xi,\overline{\xi}),(\zeta,\overline{\zeta})}

But, by case 1, there is a unique morphism making the bottom triangle commute. Therefore, (ξ,ξ¯)=(ζ,ζ¯)(\xi,\overline{\xi})=(\zeta,\overline{\zeta}), proving the proposition. ∎

Proposition 3.17.

Suppose given an object M=mM=\langle m\rangle in Λ\Lambda^{\star}, an object

Z:={QSfZT}Z:=\left\{Q\subset S\overset{f_{Z}}{\leftarrow}T\right\}

in Ω\Omega, and a morphism

(ϕ,{γi}iQ):(Z)M(\phi,\{\gamma_{i}\}_{i\in Q}):\mathcal{L}(Z)\to M

in Λ\Lambda^{\star}. Then there is an element XM,ZX_{M,Z} in ΩME\Omega_{M}^{E} and a morphism Φ:ZXM,Z\Phi:Z\to X_{M,Z} in Ω\Omega covering (ϕ,{γi}iQ)(\phi,\{\gamma_{i}\}_{i\in Q}) such that, for any other morphism Ψ:ZX\Psi:Z\to X covering (ϕ,{γi}iQ)(\phi,\{\gamma_{i}\}_{i\in Q}), there is a unique morphism τ:XM,ZX\tau:X_{M,Z}\to X which makes the diagram

Z{\lx@inpgf@ignorespaces Z}XM,Z{\lx@inpgf@ignorespaces X_{M,Z}}X{\lx@inpgf@ignorespaces X}Ψ\scriptstyle{\lx@inpgf@ignorespaces\Psi}Φ\scriptstyle{\lx@inpgf@ignorespaces\Phi}τ\scriptstyle{\lx@inpgf@ignorespaces\tau}

commute.

Proof.

We first note that S=S=\diamond, since otherwise no such morphism (ϕ,{γi}iQ)(\phi,\{\gamma_{i}\}_{i\in Q}) can exist. Consequently, ϕ=id\phi={\operatorname{id}}_{\diamond}, and γ\gamma is a morphism of cyclically ordered sets mD(fZ1())\langle m\rangle\to D(f_{Z}^{-1}(\diamond)). We can therefore take XZ,MX_{Z,M} to be the object

{1}fMD(m)\{1\}\subset\diamond\overset{f_{M}}{\leftarrow}D(\langle m\rangle)

constructed in the proof of Proposition 3.15. We then get a commutative diagram

{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}T{\lx@inpgf@ignorespaces T}{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}D(m)(TfZ1()){\lx@inpgf@ignorespaces D(\langle m\rangle)\amalg(T\setminus f_{Z}^{-1}(\diamond))}\subseteqfZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}g¯\scriptstyle{\lx@inpgf@ignorespaces\overline{g}}\subseteqid\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}}fM\scriptstyle{\lx@inpgf@ignorespaces f_{M}}

where g¯\overline{g} acts as D(γ)D(\gamma) on fZ1()f_{Z}^{-1}(\diamond) and the identity on TfZ1()T\setminus f_{Z}^{-1}(\diamond). This morphism in Ω\Omega clearly covers (id,γ)({\operatorname{id}},\gamma).

Given XΩMEX\in\Omega_{M}^{E} and Ψ:ZX\Psi:Z\to X, represented by a diagram

{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}T{\lx@inpgf@ignorespaces T}{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}A{\lx@inpgf@ignorespaces A}\subseteqfZ\scriptstyle{\lx@inpgf@ignorespaces f_{Z}}¯\scriptstyle{\lx@inpgf@ignorespaces\overline{\ell}}\subseteqid\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}}fX\scriptstyle{\lx@inpgf@ignorespaces f_{X}}

by 3.15 that there is a unique morphism

{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}D(m){\lx@inpgf@ignorespaces D(\langle m\rangle)}{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}A{\lx@inpgf@ignorespaces A}\subseteqfM\scriptstyle{\lx@inpgf@ignorespaces f_{M}}h¯\scriptstyle{\lx@inpgf@ignorespaces\overline{h}}\subseteqid\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}}fX\scriptstyle{\lx@inpgf@ignorespaces f_{X}}

in ΩME\Omega_{M}^{E}. Via the restriction of ¯\overline{\ell} to TfZ1()T\setminus f^{-1}_{Z}(\diamond), this extends to a morphism

{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}D(m)(TfZ1()){\lx@inpgf@ignorespaces D(\langle m\rangle)\amalg(T\setminus f_{Z}^{-1}(\diamond))}{1}{\lx@inpgf@ignorespaces\{1\}}{\lx@inpgf@ignorespaces\diamond}A{\lx@inpgf@ignorespaces A}\subseteqfM\scriptstyle{\lx@inpgf@ignorespaces f_{M}}ξ¯\scriptstyle{\lx@inpgf@ignorespaces\overline{\xi}}\subseteqid\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{id}}}fX\scriptstyle{\lx@inpgf@ignorespaces f_{X}}

in ΩME\Omega_{M}^{E}.

Since all of the left-hand vertical morphisms are required to be identities, we only need to check that ξ¯g¯=¯\overline{\xi}\circ\overline{g}=\overline{\ell}, which is true by construction. The requirement that ξ¯\overline{\xi} define a morphism in ΩME\Omega_{M}^{E} uniquely determines ξ¯\overline{\xi} on D(m)D(\langle m\rangle) and the requirement that ξ¯g¯=¯\overline{\xi}\circ\overline{g}=\overline{\ell} uniquely determines ξ¯\overline{\xi} on TfZ1()T\setminus f_{Z}^{-1}(\diamond). ∎

Corollary 3.18.

The functor \mathcal{L} is an \infty-categorical localization of Ω\Omega at the morphisms of EE.

Proof.

This follows again from [17, Lemma 3.1.1]. Proposition 3.15 shows that the weak fibers ΩME\Omega_{M}^{E} have initial objects, and Proposition 3.16 and Proposition 3.17 show that the inclusions

ΩMEΩ/M\Omega_{M}^{E}\subset\Omega_{/M}

are cofinal. ∎

We now rephrase the conditions from Corollary 3.8 in terms of functors from Λ\Lambda^{\star}. Note that by forgetting degerate intervals and localizing along \mathcal{L}, we have already dealt with conditions 1 and 3.

Construction 3.19.

Given n\langle n\rangle in Λ\Lambda^{\star}, we define a morphism

σn:n{[1](i,i+1)}(i,i+1)D(n)\sigma_{n}:\langle n\rangle\to\{[1]_{(i,i+1)}\}_{(i,i+1)\in D(\langle n\rangle)}

in Λ\Lambda^{\star} as follows. Take the canonical cyclic order on D(n)D(\langle n\rangle), and define

D(n)[1](i,i+1)n\bigcup\nolimits^{D(\langle n\rangle)}[1]_{(i,i+1)}\to\langle n\rangle

sending

0[1](i,i+1)\displaystyle 0\in[1]_{(i,i+1)} i\displaystyle\mapsto i
1[1](i,i+1)\displaystyle 1\in[1]_{(i,i+1)} i+1.\displaystyle\mapsto i+1.

Note that given an object XΩnX\in\Omega_{\langle n\rangle} in the fiber over n\langle n\rangle, σn\sigma_{n} is simply the image of the source morphism in Ω\Omega.

Similarly, given an object {[mi]}iS\{[m_{i}]\}_{i\in S} in Λ\Lambda^{\star}, define two morphisms

t{mi}:{[mi]}iS\displaystyle t_{\{m_{i}\}}:\{[m_{i}]\}_{i\in S} {[1]i}iS\displaystyle\to\{[1]_{i}\}_{i\in S}
s{mi}:{[mi]}iS\displaystyle s_{\{m_{i}\}}:\{[m_{i}]\}_{i\in S} {[1](j,j+1)}(j,j+1)iSI([mi])\displaystyle\to\{[1]_{(j,j+1)}\}_{(j,j+1)\in\bigoplus_{i\in S}I([m_{i}])}

in Λ\Lambda^{\star} as follows. We define t{mi}:=(idS,{fi})t_{\{m_{i}\}}:=({\operatorname{id}}_{S},\{f_{i}\}) where fi:[1]i[mi]f_{i}:[1]_{i}\to[m_{i}] is given by the formula

fi(0)\displaystyle f_{i}(0) =0\displaystyle=0
fi(1)\displaystyle f_{i}(1) =mi\displaystyle=m_{i}

We define si:=(ϕ,{gi})s_{i}:=(\phi,\{g_{i}\}), where

ϕ:iSI([mi])S\phi:\bigoplus_{i\in S}I([m_{i}])\to S

sends I([mi])I([m_{i}]) to ii, and the morphism

gi:(j,j+1)iSI([mi])[1](j,j+1)[mi]g_{i}:\bigoplus_{(j,j+1)\in\bigoplus_{i\in S}I([m_{i}])}[1]_{(j,j+1)}\to[m_{i}]

is given by

gi(0[1](j,j+1))\displaystyle g_{i}(0\in[1]_{(j,j+1)}) =j\displaystyle=j
gi(1[1](j,j+1))\displaystyle g_{i}(1\in[1]_{(j,j+1)}) =j+1\displaystyle=j+1

Note that, given an object XΩMX\in\Omega_{M} in the fiber over M:={[mi]}iSM:=\{[m_{i}]\}_{i\in S}, the morphisms sMs_{M} and tMt_{M} are simply the images under \mathcal{L} of the source and target morphisms, respectively. ∎

Lemma 3.20.

Given a functor G:Λ𝒞G:\Lambda^{\star}\to\mathcal{C}, GG\circ\mathcal{L} satisfies condition 4 if and only if the following two conditions on GG are satisfied:

  1. (1)

    For any {[mi]}iS\{[m_{i}]\}_{i\in S}, and any {[n(j,j+1)]}(j,j+1)iSI([mi])\{[n_{(j,j+1)}]\}_{(j,j+1)\in\bigoplus_{i\in S}I([m_{i}])} the diagram

    {(j,j+1)I([m])[n(j,j+1)]}iS{\lx@inpgf@ignorespaces\{\bigstar_{(j,j+1)\in I([m])}[n_{(j,j+1)}]\}_{i\in S}}{[n(j,j+1)]}(j,j+1)iS{\lx@inpgf@ignorespaces\{[n_{(j,j+1)}]\}_{(j,j+1)\in\bigoplus_{i\in S}}}{[mi]}iS{\lx@inpgf@ignorespaces\{[m_{i}]\}_{i\in S}}{[1](j,j+1)}(j,j+1)iSI([mi]){\lx@inpgf@ignorespaces\{[1]_{(j,j+1)}\}_{(j,j+1)\in\bigoplus_{i\in S}I([m_{i}])}}tN\scriptstyle{\lx@inpgf@ignorespaces t_{N}}sM\scriptstyle{\lx@inpgf@ignorespaces s_{M}}

    is sent to a pullback under GG.

  2. (2)

    For n\langle n\rangle and any {[m(j,j+1)}(j,j+1)D(n)\{[m_{(j,j+1)}\}_{(j,j+1)\in D(\langle n\rangle)} the diagram

    C((j,j+1)D(n)[m(j,j+1)]){\lx@inpgf@ignorespaces C(\bigstar_{(j,j+1)\in D(\langle n\rangle)}[m_{(j,j+1)}])}{[m(j,j+1)}(j,j+1)D(n){\lx@inpgf@ignorespaces\{[m_{(j,j+1)}\}_{(j,j+1)\in D(\langle n\rangle)}}n{\lx@inpgf@ignorespaces\langle n\rangle}nI([mi]){\lx@inpgf@ignorespaces\langle n\rangle I([m_{i}])}tN\scriptstyle{\lx@inpgf@ignorespaces t_{N}}σM\scriptstyle{\lx@inpgf@ignorespaces\sigma_{M}}

    is sent to a pullback diagram under GG.

Proof.

Using the same technique as in the proof of Proposition 2.21, we can reduce condition 4 to a statement about pullback squares along source and target maps. The diagrams of the lemma are then the images under \mathcal{L} of the requisite pullback diagrams. ∎

Definition 3.21.

We denote by Funalg(Λ,𝒞)\operatorname{Fun}^{\operatorname{alg}}(\Lambda^{\star},\mathcal{C}) the full sub-category on those functors which

  1. (1)

    Send {[mi}iS\{[m_{i}\}_{i\in S} together with the projections to [mi][m_{i}] to product diagrams.

  2. (2)

    Send the diagrams from 3.20 to pullback diagrams.

  3. (3)

    Send the morphisms {[n]}n\{[n]\}\to\langle n\rangle to equivalences.

Corollary 3.22.

There is an equivalence of \infty-categories

AlgSpCY(𝒞)FunAlg(Λ,𝒞).\operatorname{Alg}_{\operatorname{Sp}}^{\operatorname{CY}}(\mathcal{C})\simeq\operatorname{Fun}^{\operatorname{Alg}}(\Lambda^{\star},\mathcal{C}).

3.3. Extension and restriction

Definition 3.23.

We define a category ΛΔ\Lambda_{\Delta} to be the Grothendieck construction of the functor

Δ1{K}Cat.\Delta^{1}\overset{\{K\}}{\to}\operatorname{Cat}.

explicitly, ob(ΛΔ)=ob(Λ)ob(Δ)\operatorname{ob}(\Lambda_{\Delta})=\operatorname{ob}(\Lambda)\amalg\operatorname{ob}(\Delta), with morphisms

  • f:[n][m]f:[n]\to[m] morphism in Δ\Delta

  • f:nmf:\langle n\rangle\to\langle m\rangle morphism in Λ\Lambda

  • f:[n]mf:[n]\to\langle m\rangle given by a morphism f:K([n])mf:K([n])\to\langle m\rangle in Λ\Lambda.

The category (ΛΔ)op(\Lambda_{\Delta})^{\operatorname{op}} can be identified with the full subcategory of Λ\Lambda^{\star} on the objects {[m]}\{[m]\} and n\langle n\rangle. ∎

Construction 3.24.

By taking restriction and right Kan extension along the inclusion ΛΔopΛ\Lambda_{\Delta}^{\operatorname{op}}\subset\Lambda^{\star}, we get an adjunction

ιFun(Λ,𝒞)Fun(ΛΔop,𝒞):ι!\iota_{\ast}\operatorname{Fun}(\Lambda^{\star},\mathcal{C})\leftrightarrow\operatorname{Fun}(\Lambda_{\Delta}^{\operatorname{op}},\mathcal{C}):\iota_{!}

of \infty-categories. ∎

Definition 3.25.

Denote by Fun×(Λ,𝒞)\operatorname{Fun}^{\times}(\Lambda^{\star},\mathcal{C}) the full \infty-subcategory of Fun(Λ,𝒞)\operatorname{Fun}(\Lambda^{\star},\mathcal{C}) on those functors which satisfy Item 1 from Definition 3.21. ∎

Proposition 3.26.

The adjunction of Construction 3.24 restricts to an equivalence of \infty-categories

Fun×(Λ,𝒞)Fun(ΛΔ,𝒞)\operatorname{Fun}^{\times}(\Lambda^{\star},\mathcal{C})\simeq\operatorname{Fun}(\Lambda_{\Delta},\mathcal{C})
Proof.

Since there are no morphisms {[mi]}iSn\{[m_{i}]\}_{i\in S}\to\langle n\rangle in Λ\Lambda^{\star}, this is, mutatis mutandis, the same as the proof of 2.23. ∎

Construction 3.27.

We have a full subcategory F:ΛΛΔF:\Lambda\subset\Lambda_{\Delta}. We can similarly define a functor

H:ΛΔΛH:\Lambda_{\Delta}\to\Lambda

by acting as KK on Δ\Delta and as the identity on all other objects and morphisms. This defines an adjunction

F:ΛΛΔ:HF:\Lambda\leftrightarrow\Lambda_{\Delta}:H

It is easy to see that HH is a reflective localization at the morphisms [n]n[n]\to\langle n\rangle given by isomorphisms K([n])nK([n])\cong\langle n\rangle. ∎

Proposition 3.28.

There is an equivalence of \infty-categories

Funalg(Λ,𝒞)2SegΛ(𝒞).\operatorname{Fun}^{\operatorname{alg}}(\Lambda^{\star},\mathcal{C})\simeq 2\operatorname{-Seg}_{\Lambda}(\mathcal{C}).
Proof.

Proposition 3.26 and Construction 3.27 show us that Fun(Λop,𝒞)\operatorname{Fun}(\Lambda^{{\operatorname{op}}},\mathcal{C}) is equivalent, as an \infty-category, to the full subcategory of Fun×(Λ,𝒞)\operatorname{Fun}^{\times}(\Lambda^{\star},\mathcal{C}) satisfying 1 and 3 from Definition 3.21. The relation between the 2-Segal condition and condition 2 from Definition 3.21 follows from a similar argument to the proof of Proposition 2.24. ∎

We can then summarize our results in the following theorem:

Theorem 3.29.

There is an equivalence of \infty-categories

AlgSpCY(𝒞)2SegΛ(𝒞).\operatorname{Alg}_{\operatorname{Sp}}^{\operatorname{CY}}(\mathcal{C})\simeq 2\operatorname{-Seg}_{\Lambda}(\mathcal{C}).

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