ScalingStacks

4.2. Lax cocenter

4.2.1. Lax bi-22-representations

A lax bi-22-representation on 𝒱{\mathcal{V}} is a lax monoidal differential functor E:π’°βŠ—π’°β†’End⁑(𝒱)E:{\mathcal{U}}\otimes{\mathcal{U}}\to\operatorname{End}\nolimits({\mathcal{V}}). It corresponds to the data of

  • β€’

    differential endofunctors Ei,j=E⁑(eiβŠ—ej)E_{i,j}=E(e^{i}\otimes e^{j}) of 𝒱{\mathcal{V}}

  • β€’

    morphisms of differential algebras HiβŠ—Hjβ†’End⁑(Ei,j)H_{i}\otimes H_{j}\to\operatorname{End}\nolimits(E_{i,j})

  • β€’

    morphisms of differential functors ΞΌ(i,j),(iβ€²,jβ€²):Ei,j​Eiβ€²,jβ€²β†’Ei+iβ€²,j+jβ€²\mu_{(i,j),(i^{\prime},j^{\prime})}:E_{i,j}E_{i^{\prime},j^{\prime}}\to E_{i+i^{\prime},j+j^{\prime}}

such that

  1. (1)

    ΞΌ(i,j),(iβ€²,jβ€²)\mu_{(i,j),(i^{\prime},j^{\prime})} is equivariant for the action of (HiβŠ—Hj)βŠ—(Hiβ€²βŠ—Hjβ€²)(H_{i}\otimes H_{j})\otimes(H_{i^{\prime}}\otimes H_{j^{\prime}}), where the action on Ei+iβ€²,j+jβ€²E_{i+i^{\prime},j+j^{\prime}} is the restriction of the action of Hi+iβ€²βŠ—Hj+jβ€²H_{i+i^{\prime}}\otimes H_{j+j^{\prime}} via the morphism (aβŠ—b)βŠ—(aβ€²βŠ—bβ€²)↦a​fi​(aβ€²)βŠ—b​fj​(bβ€²)(a\otimes b)\otimes(a^{\prime}\otimes b^{\prime})\mapsto af_{i}(a^{\prime})\otimes bf_{j}(b^{\prime})

  2. (2)

    ΞΌ(i+iβ€²,j+jβ€²),(iβ€²β€²,jβ€²β€²)∘(ΞΌ(i,j),(iβ€²,jβ€²)​Eiβ€²β€²,jβ€²β€²)=ΞΌ(i,j),(iβ€²+iβ€²β€²,jβ€²+jβ€²β€²)∘(Ei,j​μ(iβ€²,jβ€²),(iβ€²β€²,jβ€²β€²))\mu_{(i+i^{\prime},j+j^{\prime}),(i^{\prime\prime},j^{\prime\prime})}\circ(\mu_{(i,j),(i^{\prime},j^{\prime})}E_{i^{\prime\prime},j^{\prime\prime}})=\mu_{(i,j),(i^{\prime}+i^{\prime\prime},j^{\prime}+j^{\prime\prime})}\circ(E_{i,j}\mu_{(i^{\prime},j^{\prime}),(i^{\prime\prime},j^{\prime\prime})}).

Consider two actions of 𝒰{\mathcal{U}} given by (F1,Ο„1)(F_{1},\tau_{1}) and (E2,Ο„2)(E_{2},\tau_{2}) on 𝒱{\mathcal{V}} and a closed morphism of functors Ξ»:F1​E2β†’E2​F1\lambda:F_{1}E_{2}\to E_{2}F_{1} such that the following diagrams commute:

(4.2.1) F12​E2\textstyle{F_{1}^{2}E_{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}F1​λ\scriptstyle{F_{1}\lambda}Ο„1​E2\scriptstyle{\tau_{1}E_{2}}F1​E2​F1\textstyle{F_{1}E_{2}F_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}λ​F1\scriptstyle{\lambda F_{1}}E2​F12\textstyle{E_{2}F_{1}^{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​τ1\scriptstyle{E_{2}\tau_{1}}F12​E2\textstyle{F_{1}^{2}E_{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}F1​λ\scriptstyle{F_{1}\lambda}F1​E2​F1\textstyle{F_{1}E_{2}F_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}λ​F1\scriptstyle{\lambda F_{1}}E2​F12\textstyle{E_{2}F_{1}^{2}}     F1​E22\textstyle{F_{1}E_{2}^{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}λ​E2\scriptstyle{\lambda E_{2}}F1​τ2\scriptstyle{F_{1}\tau_{2}}E2​F1​E2\textstyle{E_{2}F_{1}E_{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​λ\scriptstyle{E_{2}\lambda}E22​F1\textstyle{E_{2}^{2}F_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„2​F1\scriptstyle{\tau_{2}F_{1}}F1​E22\textstyle{F_{1}E_{2}^{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}λ​E2\scriptstyle{\lambda E_{2}}E2​F1​E2\textstyle{E_{2}F_{1}E_{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​λ\scriptstyle{E_{2}\lambda}E22​F1\textstyle{E_{2}^{2}F_{1}}
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Remark 4.2.1. The data of Ξ»\lambda and the required relations are described graphically as:

[Uncaptioned image]

Define morphisms

Ξ»i,1=(Ξ»F1iβˆ’1)βˆ˜β‹―βˆ˜(F1iβˆ’2Ξ»F1)∘(F1iβˆ’1Ξ»):F1iE2β†’E2F1i\lambda_{i,1}=(\lambda F_{1}^{i-1})\circ\cdots\circ(F_{1}^{i-2}\lambda F_{1})\circ(F_{1}^{i-1}\lambda):F_{1}^{i}E_{2}\to E_{2}F_{1}^{i}

and

Ξ»i,j=(E2jβˆ’1Ξ»i,1)βˆ˜β‹―βˆ˜(E2Ξ»i,1E2jβˆ’2)∘(Ξ»i,1E2jβˆ’1):F1iE2jβ†’E2jF1i.\lambda_{i,j}=(E_{2}^{j-1}\lambda_{i,1})\circ\cdots\circ(E_{2}\lambda_{i,1}E_{2}^{j-2})\circ(\lambda_{i,1}E_{2}^{j-1}):F_{1}^{i}E_{2}^{j}\to E_{2}^{j}F_{1}^{i}.

We define a lax bi-22-representation on 𝒱{\mathcal{V}} by Ei,j=E2i​F1jE_{i,j}=E_{2}^{i}F_{1}^{j}. The actions of HiH_{i} on E2iE_{2}^{i} and HjH_{j} on F1jF_{1}^{j} provide an action of HiβŠ—HjH_{i}\otimes H_{j} on Ei,jE_{i,j} and ΞΌ(i,j),(iβ€²,jβ€²)=E2i​λj,i′​F1jβ€²\mu_{(i,j),(i^{\prime},j^{\prime})}=E_{2}^{i}\lambda_{j,i^{\prime}}F_{1}^{j^{\prime}}:

ΞΌ(i,j),(iβ€²,jβ€²):E2i​F1j​E2i′​F1jβ€²β†’E2i​λj,i′​F1jβ€²E2i​E2i′​F1j​F1jβ€²=E2i+i′​F1j+jβ€².\mu_{(i,j),(i^{\prime},j^{\prime})}:E_{2}^{i}F_{1}^{j}E_{2}^{i^{\prime}}F_{1}^{j^{\prime}}\xrightarrow{E_{2}^{i}\lambda_{j,i^{\prime}}F_{1}^{j^{\prime}}}E_{2}^{i}E_{2}^{i^{\prime}}F_{1}^{j}F_{1}^{j^{\prime}}=E_{2}^{i+i^{\prime}}F_{1}^{j+j^{\prime}}.
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Remark 4.2.2. One can also consider the notion of colax 22-representation. A colax 22-representation on 𝒱{\mathcal{V}} is the same data as a lax 22-representation on 𝒱opp{\mathcal{V}}^{\operatorname{opp}\nolimits}.

4.2.2. Category

Let 𝒲{\mathcal{W}} be a differential category endowed with a lax action (Ei,j)(E_{i,j}) of 𝒰2{\mathcal{U}}^{2}.

We define a differential category Ξ”E​𝒲\Delta_{E}{\mathcal{W}}.

βˆ™\bullet\ The objects of Ξ”E​𝒲\Delta_{E}{\mathcal{W}} are pairs (m,Ο‚)(m,\varsigma) where mβˆˆπ’²Β―im\in\overline{{\mathcal{W}}}^{i} and Ο‚βˆˆZ​Hom𝒲¯i⁑(E0,1​E1,0​(m),m)\varsigma\in Z\operatorname{Hom}\nolimits_{\overline{{\mathcal{W}}}^{i}}(E_{0,1}E_{1,0}(m),m) such that for all iβ‰₯1i\geq 1, there exists Ο‚i∈Z​Hom𝒲¯i⁑(Ei,i​(m),m)\varsigma_{i}\in Z\operatorname{Hom}\nolimits_{\overline{{\mathcal{W}}}^{i}}(E_{i,i}(m),m) such that the composition bib_{i}

(4.2.2) bi:(E0,1​E1,0)i​(m)β†’(E0,1​E1,0)iβˆ’1​ς(E0,1​E1,0)iβˆ’1​(m)β†’(E0,1​E1,0)iβˆ’2​ς⋯→E0,1​E1,0​(m)β†’πœmb_{i}:(E_{0,1}E_{1,0})^{i}(m)\xrightarrow{(E_{0,1}E_{1,0})^{i-1}\varsigma}(E_{0,1}E_{1,0})^{i-1}(m)\xrightarrow{(E_{0,1}E_{1,0})^{i-2}\varsigma}\cdots\to E_{0,1}E_{1,0}(m)\xrightarrow{\varsigma}m

is equal to

(E0,1​E1,0)i​(m)β†’canEi,i​(m)β†’Ο‚im(E_{0,1}E_{1,0})^{i}(m)\xrightarrow{{\mathrm{can}}}E_{i,i}(m)\xrightarrow{\varsigma_{i}}m

and Ο‚i∘(TrβŠ—1)=Ο‚i∘(1βŠ—Tr)\varsigma_{i}\circ(T_{r}\otimes 1)=\varsigma_{i}\circ(1\otimes T_{r}) for 1≀r<i1\leq r<i.

βˆ™\bullet\ HomΞ”E​𝒲⁑((m,Ο‚),(mβ€²,ς′​(m))CLOSE\operatorname{Hom}\nolimits_{\Delta_{E}{\mathcal{W}}}((m,\varsigma),(m^{\prime},\varsigma^{\prime}(m)) is the differential submodule of Hom𝒲¯i⁑(m,mβ€²)\operatorname{Hom}\nolimits_{\overline{{\mathcal{W}}}^{i}}(m,m^{\prime}) of elements ff such that the following diagram commutes

E0,1​E1,0​(m)\textstyle{E_{0,1}E_{1,0}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο‚\scriptstyle{\varsigma}E0,1​E1,0​f\scriptstyle{E_{0,1}E_{1,0}f}m\textstyle{m\ignorespaces\ignorespaces\ignorespaces\ignorespaces}f\scriptstyle{f}E0,1​E1,0​(mβ€²)\textstyle{E_{0,1}E_{1,0}(m^{\prime})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο‚\scriptstyle{\varsigma}mβ€²\textstyle{m^{\prime}}

The composition of maps is defined by restricting that of 𝒲¯i\overline{{\mathcal{W}}}^{i}. So, we have a faithful forgetful functor Ο‰:Ξ”E​𝒲→𝒲¯i,(m,Ο‚)↦m\omega:\Delta_{E}{\mathcal{W}}\to\overline{{\mathcal{W}}}^{i},\ (m,\varsigma)\mapsto m. Note that Ξ”E​𝒲\Delta_{E}{\mathcal{W}} is strongly pretriangulated and idempotent-complete.

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Remark 4.2.3. Note that applying the self-equivalence (a,b)↦(b,a)(a,b)\mapsto(b,a) of 𝒰2{\mathcal{U}}^{2} provides another lax action Eβ€²E^{\prime} of 𝒰2{\mathcal{U}}^{2} on 𝒲{\mathcal{W}}. The corresponding differential category Ξ”E′​𝒲\Delta_{E^{\prime}}{\mathcal{W}} is not equivalent to Ξ”E​𝒲\Delta_{E}{\mathcal{W}} in general.

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

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2