ScalingStacks

4. 22-representation theory

We recall that kk is a field of characteristic 22.

4.1. Monoidal category

4.1.1. Definition

Let 𝒰{\mathcal{U}} be the differential strict monoidal category generated by an object ee and a map Ο„:e2β†’e2\tau:e^{2}\to e^{2} subject to the relations

(4.1.1) d⁑(Ο„)=1,Ο„2=0​ and ​eβ€‹Ο„βˆ˜Ο„β€‹e∘e​τ=τ​e∘eβ€‹Ο„βˆ˜Ο„β€‹e.d(\tau)=1,\ \tau^{2}=0\text{ and }e\tau\circ\tau e\circ e\tau=\tau e\circ e\tau\circ\tau e.

There are isomorphisms of differential monoidal categories opp:π’°β†’βˆΌπ’°opp{\operatorname{opp}\nolimits}:{\mathcal{U}}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\mathcal{U}}^{\operatorname{opp}\nolimits} and rev:π’°β†’βˆΌπ’°rev\mathrm{rev}:{\mathcal{U}}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\mathcal{U}}^{\mathrm{rev}} given on generators by e↦ee\mapsto e and τ↦τ\tau\mapsto\tau.

The following result is clear.

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Proposition 4.1.1. The objects of the category 𝒰{\mathcal{U}} are the ene^{n}, nβ‰₯0n\geq 0. We have Hom⁑(en,em)=0\operatorname{Hom}\nolimits(e^{n},e^{m})=0 if nβ‰ mn\neq m and there is an isomorphism of differential algebras

Hnβ†’βˆΌEnd⁑(en),Ti↦eiβˆ’1​τ​enβˆ’iβˆ’1.H_{n}\xrightarrow{\sim}\operatorname{End}\nolimits(e^{n}),\ T_{i}\mapsto e^{i-1}\tau e^{n-i-1}.

There is a commutative diagram

HmβŠ—Hn\textstyle{H_{m}\otimes H_{n}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}TiβŠ—Tj↦Ti​Tm+j\scriptstyle{T_{i}\otimes T_{j}\mapsto T_{i}T_{m+j}}can\scriptstyle{{\mathrm{can}}}∼\scriptstyle{\sim}Hm+n\textstyle{H_{m+n}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}∼\scriptstyle{\sim}can\scriptstyle{{\mathrm{can}}}End⁑(Em)βŠ—End⁑(En)\textstyle{\operatorname{End}\nolimits(E^{m})\otimes\operatorname{End}\nolimits(E^{n})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}βŠ—\scriptstyle{\otimes}End⁑(Em+n)\textstyle{\operatorname{End}\nolimits(E^{m+n})}

The isomorphism opp:π’°β†’βˆΌπ’°opp{\operatorname{opp}\nolimits}:{\mathcal{U}}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\mathcal{U}}^{\operatorname{opp}\nolimits} gives rise to the isomorphism of differential algebras

opp:Hnβ†’βˆΌHnopp,Ti↦Ti.{\operatorname{opp}\nolimits}:H_{n}\xrightarrow{\sim}H_{n}^{\operatorname{opp}\nolimits},\ T_{i}\mapsto T_{i}.

The isomorphism rev:π’°β†’βˆΌπ’°rev\mathrm{rev}:{\mathcal{U}}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\mathcal{U}}^{\mathrm{rev}} gives rise to the isomorphism of differential algebras

ΞΉn:Hnβ†’βˆΌHn,Ti↦Tnβˆ’i.\iota_{n}:H_{n}\xrightarrow{\sim}H_{n},\ T_{i}\mapsto T_{n-i}.

The functor βˆ’βŠ—En-\otimes E^{n} induces an injective morphism of differential algebras Hr=End⁑(Er)β†’Hr+n=End⁑(Er+n),Ti↦TiH_{r}=\operatorname{End}\nolimits(E^{r})\to H_{r+n}=\operatorname{End}\nolimits(E^{r+n}),\ T_{i}\mapsto T_{i} and we will identify HrH_{r} with a subalgebra of Hr+nH_{r+n} via this morphism.

The functor EnβŠ—βˆ’E^{n}\otimes- induces a morphism of differential algebras

fn:Hr=End⁑(Er)β†’Hn+r=End⁑(En+r),Ti↦Tn+i.f_{n}:H_{r}=\operatorname{End}\nolimits(E^{r})\to H_{n+r}=\operatorname{End}\nolimits(E^{n+r}),\ T_{i}\mapsto T_{n+i}.

Note that HnH_{n} commutes with fn​(Hr)f_{n}(H_{r}) and that fn=ΞΉn+r∘ιrf_{n}=\iota_{n+r}\circ\iota_{r}.

4.1.2. 22-representations

Let 𝒱{\mathcal{V}} be a differential category.

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Definition 4.1.2. A 22-representation on 𝒱{\mathcal{V}} is the data of a strict monoidal differential functor 𝒰→End⁑(𝒱){\mathcal{U}}\to\operatorname{End}\nolimits({\mathcal{V}}).

The data of a 22-representation on 𝒱{\mathcal{V}} is the same as the data of a differential endofunctor EE of 𝒱{\mathcal{V}} and of Ο„=Ο„E∈End⁑(E2)\tau=\tau_{E}\in\operatorname{End}\nolimits(E^{2}) satisfying (4.1.1).

Note that a 22-representation on 𝒱{\mathcal{V}} extends to a 22-representation on 𝒱¯\bar{{\mathcal{V}}} and on 𝒱i{\mathcal{V}}^{i} (uniquely up to an equivalence unique up to isomorphism).

A morphism of 22-representations (𝒱,E,Ο„)β†’(𝒱′,Eβ€²,Ο„)({\mathcal{V}},E,\tau)\to({\mathcal{V}}^{\prime},E^{\prime},\tau) is the data of a differential functor Ξ¦:𝒱→𝒱′\Phi:{\mathcal{V}}\to{\mathcal{V}}^{\prime} and of an isomorphism of functors Ο†:Φ​Eβ†’βˆΌE′​Φ\varphi:\Phi E\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}E^{\prime}\Phi (with d⁑(Ο†)=0d(\varphi)=0) such that Ο„β€²β€‹Ξ¦βˆ˜Eβ€²β€‹Ο†βˆ˜Ο†β€‹E=Eβ€²β€‹Ο†βˆ˜Ο†β€‹Eβˆ˜Ξ¦β€‹Ο„:Φ​E2β†’Eβ€²2​Φ\tau^{\prime}\Phi\circ E^{\prime}\varphi\circ\varphi E=E^{\prime}\varphi\circ\varphi E\circ\Phi\tau:\Phi E^{2}\to E^{\prime 2}\Phi.

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Example 4.1.3. Let 𝒱=kβ€‹βˆ’diff{\mathcal{V}}=k\operatorname{\!-diff}\nolimits and E=Ο„=0E=\tau=0. This is the β€œtrivial” 22-representation.

Let 𝒱{\mathcal{V}} be a 22-representation. The opposite 22-representation is (π’±β€‹βˆ’diff,Eβ€²,Ο„β€²)({\mathcal{V}}\operatorname{\!-diff}\nolimits,E^{\prime},\tau^{\prime}), where E′​(ΞΆ)=΢​EE^{\prime}(\zeta)=\zeta E and τ′​(ΞΆ)=ΞΆβ€‹Ο„βˆˆEnd⁑(Eβ€²2​(ΞΆ))\tau^{\prime}(\zeta)=\zeta\tau\in\operatorname{End}\nolimits(E^{\prime 2}(\zeta)) for ΞΆβˆˆπ’±β€‹βˆ’diff\zeta\in{\mathcal{V}}\operatorname{\!-diff}\nolimits. Note that the canonical functor 𝒱→(π’±β€‹βˆ’diff)β€‹βˆ’diff,v↦(΢↦΢⁑(v)){\mathcal{V}}\to({\mathcal{V}}\operatorname{\!-diff}\nolimits)\operatorname{\!-diff}\nolimits,\ v\mapsto(\zeta\mapsto\zeta(v)) is a fully faithful morphism of 22-representations.

Assume EE has a left adjoint E∨E^{\vee}. We still denote by Ο„\tau the endomorphism of (E∨)2(E^{\vee})^{2} corresponding to Ο„\tau (cf Β§2.1.1). The pair (E∨,Ο„)(E^{\vee},\tau) defines the left dual 22-representation of (E,Ο„)(E,\tau). Similarly, if EE has a right adjoint ∨E{{}^{\vee}E}, we obtain a right dual 22-representation (E∨,Ο„)({{}^{\vee}E},\tau) of (E,Ο„)(E,\tau).

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Remark 4.1.4. One can also consider a lax 22-representation on 𝒱{\mathcal{V}}: this is the data of a lax monoidal differential functor 𝒰→End⁑(𝒱){\mathcal{U}}\to\operatorname{End}\nolimits({\mathcal{V}}).

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Remark 4.1.5. The category 𝒰{\mathcal{U}} has a structure of differential graded monoidal category with Ο„\tau in degree βˆ’1-1 and one can consider (lax) 22-representations on differential graded categories.

4.1.3. Pointed case

We denote by π’°βˆ™{\mathcal{U}}^{\bullet} the strict monoidal differential pointed category generated by an object ee and a map Ο„βˆˆEnd⁑(e2)\tau\in\operatorname{End}\nolimits(e^{2}) subject to the relations (4.1.1). Its objects are the ene^{n}, nβ‰₯0n\geq 0, Hom⁑(en,em)=0\operatorname{Hom}\nolimits(e^{n},e^{m})=0 for mβ‰ nm\neq n and End⁑(en)=Hnβˆ™\operatorname{End}\nolimits(e^{n})=H_{n}^{\bullet}.

Let 𝒱{\mathcal{V}} be a differential pointed category.

A 22-representation on 𝒱{\mathcal{V}} is the data of a strict monoidal differential pointed functor π’°βˆ™β†’End⁑(𝒱){\mathcal{U}}^{\bullet}\to\operatorname{End}\nolimits({\mathcal{V}}). This is equivalent to the data of an endofunctor EE of the differential pointed category 𝒱{\mathcal{V}} and Ο„βˆˆEnd⁑(E2)\tau\in\operatorname{End}\nolimits(E^{2}) such that (E,Ο„)(E,\tau) induce a 22-representation on k⁑[𝒱]k[{\mathcal{V}}].

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.

4.3. Diagonal action

4.3.1. Category

Consider a differential category 𝒲{\mathcal{W}} endowed with two actions of 𝒰{\mathcal{U}} given by (E1,Ο„1)(E_{1},\tau_{1}) and (E2,Ο„2)(E_{2},\tau_{2}) and a closed morphism of functors Οƒ:E2​E1β†’E1​E2\sigma:E_{2}E_{1}\to E_{1}E_{2} such that the following diagrams commute:

(4.3.1) E22​E1\textstyle{E_{2}^{2}E_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​σ\scriptstyle{E_{2}\sigma}Ο„2​E1\scriptstyle{\tau_{2}E_{1}}E2​E1​E2\textstyle{E_{2}E_{1}E_{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}σ​E2\scriptstyle{\sigma E_{2}}E1​E22\textstyle{E_{1}E_{2}^{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​τ2\scriptstyle{E_{1}\tau_{2}}E22​E1\textstyle{E_{2}^{2}E_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​σ\scriptstyle{E_{2}\sigma}E2​E1​E2\textstyle{E_{2}E_{1}E_{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}σ​E2\scriptstyle{\sigma E_{2}}E1​E22\textstyle{E_{1}E_{2}^{2}}     E2​E12\textstyle{E_{2}E_{1}^{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}σ​E1\scriptstyle{\sigma E_{1}}E2​τ1\scriptstyle{E_{2}\tau_{1}}E1​E2​E1\textstyle{E_{1}E_{2}E_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​σ\scriptstyle{E_{1}\sigma}E12​E2\textstyle{E_{1}^{2}E_{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„1​E2\scriptstyle{\tau_{1}E_{2}}E2​E12\textstyle{E_{2}E_{1}^{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}σ​E1\scriptstyle{\sigma E_{1}}E1​E2​E1\textstyle{E_{1}E_{2}E_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​σ\scriptstyle{E_{1}\sigma}E12​E2\textstyle{E_{1}^{2}E_{2}}
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Remark 4.3.1. The data of Οƒ\sigma and the relations can be described graphically as follows:

[Uncaptioned image]

We define a differential category 𝒱=Δσ​𝒲{\mathcal{V}}=\Delta_{\sigma}{\mathcal{W}}.

βˆ™\bullet\ The objects of 𝒱{\mathcal{V}} are pairs (m,Ο€)(m,\pi) where mβˆˆπ’²Β―im\in\overline{{\mathcal{W}}}^{i} and Ο€βˆˆZ​Hom𝒲¯i⁑(E2​(m),E1​(m))\pi\in Z\operatorname{Hom}\nolimits_{\overline{{\mathcal{W}}}^{i}}(E_{2}(m),E_{1}(m)) such that the following diagram commutes

(4.3.2) E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π\scriptstyle{E_{2}\pi}Ο„2\scriptstyle{\tau_{2}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ\scriptstyle{\sigma}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π\scriptstyle{E_{1}\pi}E12​(m)\textstyle{E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„1\scriptstyle{\tau_{1}}E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π\scriptstyle{E_{2}\pi}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ\scriptstyle{\sigma}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π\scriptstyle{E_{1}\pi}E12​(m)\textstyle{E_{1}^{2}(m)}

βˆ™\bullet\ Hom𝒱⁑((m,Ο€),(mβ€²,Ο€β€²))\operatorname{Hom}\nolimits_{\mathcal{V}}((m,\pi),(m^{\prime},\pi^{\prime})) 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

E2​(m)\textstyle{E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο€\scriptstyle{\pi}E2​f\scriptstyle{E_{2}f}E1​(m)\textstyle{E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​f\scriptstyle{E_{1}f}E2​(mβ€²)\textstyle{E_{2}(m^{\prime})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο€β€²\scriptstyle{\pi^{\prime}}E1​(mβ€²)\textstyle{E_{1}(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‰=ωσ:𝒱→𝒲¯i,(m,Ο€)↦m\omega=\omega_{\sigma}:{\mathcal{V}}\to\overline{{\mathcal{W}}}^{i},\ (m,\pi)\mapsto m. Note that 𝒱{\mathcal{V}} is strongly pretriangulated and idempotent-complete.

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Remark 4.3.2. The structure of objects and maps in 𝒱{\mathcal{V}} can be described graphically as follows:

[Uncaptioned image]
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Remark 4.3.3. Assume E1E_{1} admits a left adjoint F1F_{1}. The data of the map Οƒ:E2​E1β†’E1​E2\sigma:E_{2}E_{1}\to E_{1}E_{2} corresponds by adjunction to the data of a map

Ξ»:F1​E2β†’βˆ™Ξ·1F1​E2​E1​F1β†’F1​σ​F1F1​E1​E2​F1β†’Ξ΅1βˆ™E2​F1.\lambda:F_{1}E_{2}\xrightarrow{\bullet\eta_{1}}F_{1}E_{2}E_{1}F_{1}\xrightarrow{F_{1}\sigma F_{1}}F_{1}E_{1}E_{2}F_{1}\xrightarrow{\varepsilon_{1}\bullet}E_{2}F_{1}.

The commutativity of the diagrams (4.3.1) is equivalent to the commutativity of the diagrams (4.2.1). Assume the diagrams commute. We obtain a lax bi-22-representation (Ei,j)(E_{i,j}) on 𝒲{\mathcal{W}} (cf Β§4.2.1).

Let (m,Ο‚)βˆˆΞ”E​𝒲(m,\varsigma)\in\Delta_{E}{\mathcal{W}}. We have an adjunction isomorphism

Ο•:Hom⁑(E2​(m),E1​(m))β†’βˆΌHom⁑(F1​E2​(m),m).\phi:\operatorname{Hom}\nolimits(E_{2}(m),E_{1}(m))\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}\operatorname{Hom}\nolimits(F_{1}E_{2}(m),m).

Let Ο€=Ο•βˆ’1​(Ο‚)∈Z​Hom⁑(E2​(m),E1​(m))\pi=\phi^{-1}(\varsigma)\in Z\operatorname{Hom}\nolimits(E_{2}(m),E_{1}(m)). The object (m,Ο€)(m,\pi) is in Δσ​𝒲\Delta_{\sigma}{\mathcal{W}} and (m,Ο‚)↦(m,Ο€)(m,\varsigma)\mapsto(m,\pi) defines a fully faithful functor of differential categories Ξ”E​𝒲→Δσ​𝒲\Delta_{E}{\mathcal{W}}\to\Delta_{\sigma}{\mathcal{W}}.

Assume now Ξ»\lambda is invertible. The canonical map fi:(E0,1​E1,0)iβ†’Ei,if_{i}:(E_{0,1}E_{1,0})^{i}\to E_{i,i} is invertible. Let Ο‚i=bi∘fiβˆ’1\varsigma_{i}=b_{i}\circ f_{i}^{-1}. Consider r∈{1,…,iβˆ’1}r\in\{1,\ldots,i-1\}. We have

Ο‚i∘(TrβŠ—1)\displaystyle\varsigma_{i}\circ(T_{r}\otimes 1) =brβˆ’1∘(E01​E10)rβˆ’1​(Ο‚2∘(T1βŠ—1)∘f2)∘(E01​E10)r+1​biβˆ’rβˆ’1∘fiβˆ’1\displaystyle=b_{r-1}\circ(E_{01}E_{10})^{r-1}(\varsigma_{2}\circ(T_{1}\otimes 1)\circ f_{2})\circ(E_{01}E_{10})^{r+1}b_{i-r-1}\circ f_{i}^{-1}
=brβˆ’1∘(E01​E10)rβˆ’1​(Ο‚2∘(1βŠ—T1)∘f2)∘(E01​E10)r+1​biβˆ’rβˆ’1∘fiβˆ’1\displaystyle=b_{r-1}\circ(E_{01}E_{10})^{r-1}(\varsigma_{2}\circ(1\otimes T_{1})\circ f_{2})\circ(E_{01}E_{10})^{r+1}b_{i-r-1}\circ f_{i}^{-1}
=Ο‚i∘(1βŠ—Tr)\displaystyle=\varsigma_{i}\circ(1\otimes T_{r})

As a consequence, the functor above is an isomorphism of differential categories Ξ”Eβ€‹π’²β†’βˆΌΞ”Οƒβ€‹π’²\Delta_{E}{\mathcal{W}}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}\Delta_{\sigma}{\mathcal{W}}.

4.3.2. 11-arrows

We define now a differential functor E:𝒱→𝒱E:{\mathcal{V}}\to{\mathcal{V}}.

βˆ™\bullet\ Let (m,Ο€)βˆˆπ’±(m,\pi)\in{\mathcal{V}}. Let mβ€²=Β Β Β Β E2​(m)βŠ•E1​(m)   π         m^{\prime}={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 35.11345pt\hbox{{\hbox{\kern-35.11345pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{E_{2}(m)\oplus E_{1}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-6.76079pt\raise 19.04272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.50694pt\hbox{$\scriptstyle{\pi}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 19.91682pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}}. We define

Ο€β€²=(Οƒβˆ˜E2β€‹Ο€βˆ˜Ο„2Οƒ0Ο„1∘E1β€‹Ο€βˆ˜Οƒ):E2​(mβ€²)β†’E1​(mβ€²)\pi^{\prime}=\left(\begin{matrix}\sigma\circ E_{2}\pi\circ\tau_{2}&\sigma\\ 0&\tau_{1}\circ E_{1}\pi\circ\sigma\end{matrix}\right):E_{2}(m^{\prime})\to E_{1}(m^{\prime})
Ο€β€²:\textstyle{\pi^{\prime}:}E22​(m)βŠ•E2​E1​(m)\textstyle{E_{2}^{2}(m)\oplus E_{2}E_{1}(m)}E1​E2​(m)βŠ•E12​(m)\textstyle{E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}E2​π\scriptstyle{E_{2}\pi}E1​π\scriptstyle{E_{1}\pi}Οƒβˆ˜E2β€‹Ο€βˆ˜Ο„2\scriptstyle{\sigma\circ E_{2}\pi\circ\tau_{2}}Ο„1∘E1β€‹Ο€βˆ˜Οƒ\scriptstyle{\tau_{1}\circ E_{1}\pi\circ\sigma}Οƒ\scriptstyle{\sigma}
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Remark 4.3.4. The graphical description of Ο€β€²\pi^{\prime} is the following:

[Uncaptioned image]
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Lemma 4.3.5. (mβ€²,Ο€β€²)(m^{\prime},\pi^{\prime}) is an object of 𝒱{\mathcal{V}}.

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Proof. Note that d⁑(Ο€β€²)=0d(\pi^{\prime})=0.

Let a=Ο„1∘E1β€‹Ο€β€²βˆ˜Οƒβ‘(mβ€²)∘E2​π′a=\tau_{1}\circ E_{1}\pi^{\prime}\circ\sigma(m^{\prime})\circ E_{2}\pi^{\prime} and b=E1β€‹Ο€β€²βˆ˜Οƒβ‘(mβ€²)∘E2β€‹Ο€β€²βˆ˜Ο„2b=E_{1}\pi^{\prime}\circ\sigma(m^{\prime})\circ E_{2}\pi^{\prime}\circ\tau_{2}. We have

a11\displaystyle a_{11} =Ο„1​E2∘E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜E1​τ2βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜E22β€‹Ο€βˆ˜E2​τ2\displaystyle=\tau_{1}E_{2}\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ E_{1}\tau_{2}\circ\sigma E_{2}\circ E_{2}\sigma\circ E_{2}^{2}\pi\circ E_{2}\tau_{2}
=Ο„1​E2∘E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜Ο„2​E1∘E22β€‹Ο€βˆ˜E2​τ2\displaystyle=\tau_{1}E_{2}\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ\sigma E_{2}\circ E_{2}\sigma\circ\tau_{2}E_{1}\circ E_{2}^{2}\pi\circ E_{2}\tau_{2}
=Ο„1​E2∘E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜E22β€‹Ο€βˆ˜Ο„2​E2∘E2​τ2\displaystyle=\tau_{1}E_{2}\circ E_{1}\sigma\circ\sigma E_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ E_{2}^{2}\pi\circ\tau_{2}E_{2}\circ E_{2}\tau_{2}
=E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​τ1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜E22β€‹Ο€βˆ˜Ο„2​E2∘E2​τ2\displaystyle=E_{1}\sigma\circ\sigma E_{1}\circ E_{2}\tau_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ E_{2}^{2}\pi\circ\tau_{2}E_{2}\circ E_{2}\tau_{2}
=E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜E22β€‹Ο€βˆ˜E2​τ2βˆ˜Ο„2​E2∘E2​τ2\displaystyle=E_{1}\sigma\circ\sigma E_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ E_{2}^{2}\pi\circ E_{2}\tau_{2}\circ\tau_{2}E_{2}\circ E_{2}\tau_{2}
=E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜E22β€‹Ο€βˆ˜Ο„2​E2∘E2​τ2βˆ˜Ο„2​E2\displaystyle=E_{1}\sigma\circ E_{1}E_{2}\pi\circ\sigma E_{2}\circ E_{2}\sigma\circ E_{2}^{2}\pi\circ\tau_{2}E_{2}\circ E_{2}\tau_{2}\circ\tau_{2}E_{2}
=E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜Ο„2​E1∘E22β€‹Ο€βˆ˜E2​τ2βˆ˜Ο„2​E2\displaystyle=E_{1}\sigma\circ E_{1}E_{2}\pi\circ\sigma E_{2}\circ E_{2}\sigma\circ\tau_{2}E_{1}\circ E_{2}^{2}\pi\circ E_{2}\tau_{2}\circ\tau_{2}E_{2}
=E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜E1​τ2βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜E22β€‹Ο€βˆ˜E2​τ2βˆ˜Ο„2​E2=b11,\displaystyle=E_{1}\sigma\circ E_{1}E_{2}\pi\circ E_{1}\tau_{2}\circ\sigma E_{2}\circ E_{2}\sigma\circ E_{2}^{2}\pi\circ E_{2}\tau_{2}\circ\tau_{2}E_{2}=b_{11},
a12\displaystyle a_{12} =Ο„1​E2∘E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜E1​τ2βˆ˜Οƒβ€‹E2∘E2​σ+Ο„1​E2∘E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​τ1∘E2​E1β€‹Ο€βˆ˜E2​σ\displaystyle=\tau_{1}E_{2}\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ E_{1}\tau_{2}\circ\sigma E_{2}\circ E_{2}\sigma+\tau_{1}E_{2}\circ E_{1}\sigma\circ\sigma E_{1}\circ E_{2}\tau_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma
=Ο„1​E2∘E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜Ο„2​E1+Ο„12​E2∘E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​E1β€‹Ο€βˆ˜E2​σ\displaystyle=\tau_{1}E_{2}\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ\sigma E_{2}\circ E_{2}\sigma\circ\tau_{2}E_{1}+\tau_{1}^{2}E_{2}\circ E_{1}\sigma\circ\sigma E_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma
=Ο„1​E2∘E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜Ο„2​E1\displaystyle=\tau_{1}E_{2}\circ E_{1}\sigma\circ\sigma E_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ\tau_{2}E_{1}
=E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜Ο„22​E1+E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​τ1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜Ο„2​E1\displaystyle=E_{1}\sigma\circ E_{1}E_{2}\pi\circ\sigma E_{2}\circ E_{2}\sigma\circ\tau_{2}^{2}E_{1}+E_{1}\sigma\circ\sigma E_{1}\circ E_{2}\tau_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ\tau_{2}E_{1}
=E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜E1​τ2βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜Ο„2​E1+E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​τ1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜Ο„2​E1=b12,\displaystyle=E_{1}\sigma\circ E_{1}E_{2}\pi\circ E_{1}\tau_{2}\circ\sigma E_{2}\circ E_{2}\sigma\circ\tau_{2}E_{1}+E_{1}\sigma\circ\sigma E_{1}\circ E_{2}\tau_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ\tau_{2}E_{1}=b_{12},
a21=0=b21​ andΒ a_{21}=0=b_{21}\text{ and }
a22\displaystyle a_{22} =Ο„1​E1∘E1​τ1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​τ1∘E2​E1β€‹Ο€βˆ˜E2​σ\displaystyle=\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ\sigma E_{1}\circ E_{2}\tau_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma
=Ο„1​E1∘E1​τ1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​τ1∘E2​E1β€‹Ο€βˆ˜E2​σ\displaystyle=\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ\sigma E_{1}\circ E_{2}\tau_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma
=Ο„1​E1∘E1​τ1βˆ˜Ο„1​E1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜Οƒβ€‹E2∘E2​σ\displaystyle=\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ\tau_{1}E_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ\sigma E_{2}\circ E_{2}\sigma
=E1​τ1βˆ˜Ο„1​E1∘E1​τ1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜Οƒβ€‹E2∘E2​σ\displaystyle=E_{1}\tau_{1}\circ\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ\sigma E_{2}\circ E_{2}\sigma
=E1​τ1βˆ˜Ο„1​E1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜E1​τ2βˆ˜Οƒβ€‹E2∘E2​σ\displaystyle=E_{1}\tau_{1}\circ\tau_{1}E_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ E_{1}\tau_{2}\circ\sigma E_{2}\circ E_{2}\sigma
=E1​τ1∘E12β€‹Ο€βˆ˜Ο„1​E2∘E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜Ο„2​E1\displaystyle=E_{1}\tau_{1}\circ E_{1}^{2}\pi\circ\tau_{1}E_{2}\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ\sigma E_{2}\circ E_{2}\sigma\circ\tau_{2}E_{1}
=E1​τ1∘E12β€‹Ο€βˆ˜Ο„1​E2∘E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜Ο„2​E1\displaystyle=E_{1}\tau_{1}\circ E_{1}^{2}\pi\circ\tau_{1}E_{2}\circ E_{1}\sigma\circ\sigma E_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ\tau_{2}E_{1}
=E1​τ1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​τ1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜Ο„2​E1=b22.\displaystyle=E_{1}\tau_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ\sigma E_{1}\circ E_{2}\tau_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ\tau_{2}E_{1}=b_{22}.

The lemma follows. ∎

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Remark 4.3.6. The equalities established in the proof of the lemma above have the following graphical description:

[Uncaptioned image]

We put E⁑(m,Ο€)=(mβ€²,Ο€β€²)E(m,\pi)=(m^{\prime},\pi^{\prime}).

βˆ™\bullet\ Given f∈Hom𝒱⁑((m,Ο€),(m~,Ο€~))f\in\operatorname{Hom}\nolimits_{{\mathcal{V}}}((m,\pi),(\tilde{m},\tilde{\pi})), we put E⁑(f)=(E2​f00E1​f)E(f)=\left(\begin{matrix}E_{2}f&0\\ 0&E_{1}f\end{matrix}\right):

E2​(m)βŠ•E1​(m)\textstyle{E_{2}(m)\oplus E_{1}(m)}E2​(m~)βŠ•E1​(m~)\textstyle{E_{2}(\tilde{m})\oplus E_{1}(\tilde{m})}Ο€\scriptstyle{\pi}Ο€~\scriptstyle{\tilde{\pi}}E2​f\scriptstyle{E_{2}f}E1​f\scriptstyle{E_{1}f}
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Lemma 4.3.7. We have E⁑(f)∈Hom𝒱⁑(E⁑(m,Ο€),E⁑(m~,Ο€~))E(f)\in\operatorname{Hom}\nolimits_{{\mathcal{V}}}(E(m,\pi),E(\tilde{m},\tilde{\pi})). The construction makes EE into a differential endofunctor of 𝒱{\mathcal{V}}.

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Proof. The lemma follows from the commutativity of the following diagram:

E22​(m)βŠ•E2​E1​(m)\textstyle{E_{2}^{2}(m)\oplus E_{2}E_{1}(m)}E1​E2​(m)βŠ•E12​(m)\textstyle{E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}E22​(m~)βŠ•E2​E1​(m~)\textstyle{E_{2}^{2}(\tilde{m})\oplus E_{2}E_{1}(\tilde{m})}E1​E2​(m~)βŠ•E12​(m~)\textstyle{E_{1}E_{2}(\tilde{m})\oplus E_{1}^{2}(\tilde{m})}Οƒβˆ˜E2β€‹Ο€βˆ˜Ο„2\scriptstyle{\sigma\circ E_{2}\pi\circ\tau_{2}}Ο„1∘E1β€‹Ο€βˆ˜Οƒ\scriptstyle{\tau_{1}\circ E_{1}\pi\circ\sigma}Οƒ\scriptstyle{\sigma}E22​f\scriptstyle{E_{2}^{2}f}E2​E1​f\scriptstyle{E_{2}E_{1}f}E1​E2​f\scriptstyle{E_{1}E_{2}f}E12​f\scriptstyle{E_{1}^{2}f}Οƒβˆ˜E2​π~βˆ˜Ο„2\scriptstyle{\sigma\circ E_{2}\tilde{\pi}\circ\tau_{2}}Ο„1∘E1​π~βˆ˜Οƒ\scriptstyle{\tau_{1}\circ E_{1}\tilde{\pi}\circ\sigma}Οƒ\scriptstyle{\sigma}

∎

4.3.3. 22-arrows

We assume in Β§4.3.3 that Οƒ\sigma is invertible.

We define an endomorphism Ο„\tau of ω​E2\omega E^{2}. Let (m,Ο€)βˆˆπ’±(m,\pi)\in{\mathcal{V}}. We have E2​(m,Ο€)=(mβ€²β€²,Ο€β€²β€²)E^{2}(m,\pi)=(m^{\prime\prime},\pi^{\prime\prime}) where mβ€²β€²=[E22(m)βŠ•E2E1(m)βŠ•E1E2(m)βŠ•E12(m),βˆ‚]m^{\prime\prime}=[E_{2}^{2}(m)\oplus E_{2}E_{1}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m),\partial] and

βˆ‚=(0E2​π0Οƒβˆ˜E2β€‹Ο€βˆ˜Ο„2Οƒ00Ο„1∘E1β€‹Ο€βˆ˜ΟƒE1​π0).\partial=\left(\begin{matrix}0\\ E_{2}\pi&0\\ \sigma\circ E_{2}\pi\circ\tau_{2}&\sigma&0\\ 0&\tau_{1}\circ E_{1}\pi\circ\sigma&E_{1}\pi&0\end{matrix}\right).

We define an endomorphism Ο„\tau of mβ€²β€²m^{\prime\prime} by

(4.3.3) Ο„=(Ο„200000Οƒβˆ’100000000Ο„1).\tau=\left(\begin{matrix}\tau_{2}&0&0&0\\ 0&0&\sigma^{-1}&0\\ 0&0&0&0\\ 0&0&0&\tau_{1}\end{matrix}\right).
0P5X

Theorem 4.3.8. The endomorphism Ο„\tau of mβ€²β€²m^{\prime\prime} defines an endomorphism of E2E^{2}. The data (Δσ​𝒲,E,Ο„)(\Delta_{\sigma}{\mathcal{W}},E,\tau) is an idempotent-complete strongly pretriangulated 22-representation.

0P5Y

Proof. The non-zero coefficients of Ο€β€²β€²\pi^{\prime\prime} are

Ο€11β€²β€²\displaystyle\pi^{\prime\prime}_{11} =σ​E2∘E2β€‹Οƒβˆ˜E22β€‹Ο€βˆ˜E2​τ2βˆ˜Ο„2​E2\displaystyle=\sigma E_{2}\circ E_{2}\sigma\circ E_{2}^{2}\pi\circ E_{2}\tau_{2}\circ\tau_{2}E_{2}
Ο€22β€²β€²\displaystyle\pi^{\prime\prime}_{22} =σ​E1∘E2​τ1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜Ο„2​E1\displaystyle=\sigma E_{1}\circ E_{2}\tau_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ\tau_{2}E_{1}
Ο€33β€²β€²\displaystyle\pi^{\prime\prime}_{33} =Ο„1​E2∘E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜E1​τ2βˆ˜Οƒβ€‹E2\displaystyle=\tau_{1}E_{2}\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ E_{1}\tau_{2}\circ\sigma E_{2}
Ο€44β€²β€²\displaystyle\pi^{\prime\prime}_{44} =Ο„1​E1∘E1​τ1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜Οƒβ€‹E1\displaystyle=\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ\sigma E_{1}
Ο€12β€²β€²=σ​E2∘E2β€‹Οƒβˆ˜Ο„2​E1,Ο€13β€²β€²=σ​E2,Ο€24β€²β€²=σ​E1,Ο€34β€²β€²=Ο„1​E2∘E1β€‹Οƒβˆ˜Οƒβ€‹E1.\pi^{\prime\prime}_{12}=\sigma E_{2}\circ E_{2}\sigma\circ\tau_{2}E_{1},\ \pi^{\prime\prime}_{13}=\sigma E_{2},\ \pi^{\prime\prime}_{24}=\sigma E_{1},\ \pi^{\prime\prime}_{34}=\tau_{1}E_{2}\circ E_{1}\sigma\circ\sigma E_{1}.

Let a=E1β€‹Ο„βˆ˜Ο€β€²β€²a=E_{1}\tau\circ\pi^{\prime\prime} and b=Ο€β€²β€²βˆ˜E2​τb=\pi^{\prime\prime}\circ E_{2}\tau. We have

a11\displaystyle a_{11} =σ​E2∘E2β€‹Οƒβˆ˜E1​τ2∘E22β€‹Ο€βˆ˜E2​τ2βˆ˜Ο„2​E2=σ​E2∘E2β€‹Οƒβˆ˜E22β€‹Ο€βˆ˜Ο„2​E2∘E2​τ2βˆ˜Ο„2​E2\displaystyle=\sigma E_{2}\circ E_{2}\sigma\circ E_{1}\tau_{2}\circ E_{2}^{2}\pi\circ E_{2}\tau_{2}\circ\tau_{2}E_{2}=\sigma E_{2}\circ E_{2}\sigma\circ E_{2}^{2}\pi\circ\tau_{2}E_{2}\circ E_{2}\tau_{2}\circ\tau_{2}E_{2}
=σ​E2∘E2β€‹Οƒβˆ˜E22β€‹Ο€βˆ˜E2​τ2βˆ˜Ο„2​E2∘E2​τ2=b11\displaystyle=\sigma E_{2}\circ E_{2}\sigma\circ E_{2}^{2}\pi\circ E_{2}\tau_{2}\circ\tau_{2}E_{2}\circ E_{2}\tau_{2}=b_{11}
a12=E1​τ2βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜Ο„2​E1=0=b12a_{12}=E_{1}\tau_{2}\circ\sigma E_{2}\circ E_{2}\sigma\circ\tau_{2}E_{1}=0=b_{12}
a13=E1​τ2βˆ˜Οƒβ€‹E2=b13a_{13}=E_{1}\tau_{2}\circ\sigma E_{2}=b_{13}
a23\displaystyle a_{23} =E1β€‹Οƒβˆ’1βˆ˜Ο„1​E2∘E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜E1​τ2βˆ˜Οƒβ€‹E2\displaystyle=E_{1}\sigma^{-1}\circ\tau_{1}E_{2}\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ E_{1}\tau_{2}\circ\sigma E_{2}
=E1β€‹Οƒβˆ’1βˆ˜Ο„1​E2∘E1β€‹Οƒβˆ˜E1​E2β€‹Ο€βˆ˜Οƒβ€‹E2∘E2β€‹Οƒβˆ˜Ο„2​E1∘E2β€‹Οƒβˆ’1\displaystyle=E_{1}\sigma^{-1}\circ\tau_{1}E_{2}\circ E_{1}\sigma\circ E_{1}E_{2}\pi\circ\sigma E_{2}\circ E_{2}\sigma\circ\tau_{2}E_{1}\circ E_{2}\sigma^{-1}
=E1Οƒβˆ’1βˆ˜Ο„1E2∘E1Οƒβˆ˜ΟƒE2∘E2E1Ο€βˆ˜βˆ˜E2Οƒβˆ˜Ο„2E1∘E2Οƒβˆ’1\displaystyle=E_{1}\sigma^{-1}\circ\tau_{1}E_{2}\circ E_{1}\sigma\circ\sigma E_{2}\circ E_{2}E_{1}\pi\circ\circ E_{2}\sigma\circ\tau_{2}E_{1}\circ E_{2}\sigma^{-1}
=σ​E1∘E2​τ1∘E2​E1β€‹Ο€βˆ˜E2β€‹Οƒβˆ˜Ο„2​E1∘E2β€‹Οƒβˆ’1=b23\displaystyle=\sigma E_{1}\circ E_{2}\tau_{1}\circ E_{2}E_{1}\pi\circ E_{2}\sigma\circ\tau_{2}E_{1}\circ E_{2}\sigma^{-1}=b_{23}
a24=E1β€‹Οƒβˆ’1βˆ˜Ο„1​E2∘E1β€‹Οƒβˆ˜Οƒβ€‹E1=σ​E1∘E2​τ1=b24a_{24}=E_{1}\sigma^{-1}\circ\tau_{1}E_{2}\circ E_{1}\sigma\circ\sigma E_{1}=\sigma E_{1}\circ E_{2}\tau_{1}=b_{24}
a44\displaystyle a_{44} =E1​τ1βˆ˜Ο„1​E1∘E1​τ1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜Οƒβ€‹E1=Ο„1​E1∘E1​τ1βˆ˜Ο„1​E1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜Οƒβ€‹E1\displaystyle=E_{1}\tau_{1}\circ\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ\sigma E_{1}=\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ\tau_{1}E_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ\sigma E_{1}
=Ο„1​E1∘E1​τ1∘E12β€‹Ο€βˆ˜E1β€‹Οƒβˆ˜Οƒβ€‹E1∘E2​τ1=b44\displaystyle=\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ E_{1}^{2}\pi\circ E_{1}\sigma\circ\sigma E_{1}\circ E_{2}\tau_{1}=b_{44}

All the other coefficients of aa and bb vanish. We deduce that a=ba=b, hence Ο„\tau is an endomorphism of E2​(m,Ο€)E^{2}(m,\pi). It follows easily that Ο„\tau defines an endomorphism of E2E^{2}.

We have Ο„2=0\tau^{2}=0 and

d⁑(Ο„)\displaystyle d(\tau) =(d⁑(Ο„2)00000000000000d⁑(Ο„1))+Ο„βˆ˜βˆ‚+βˆ‚βˆ˜Ο„\displaystyle=\left(\begin{matrix}d(\tau_{2})&0&0&0\\ 0&0&0&0\\ 0&0&0&0\\ 0&0&0&d(\tau_{1})\end{matrix}\right)+\tau\circ\partial+\partial\circ\tau
=(id2​E2β€‹Ο€βˆ˜Ο„2idΟƒβˆ˜E2β€‹Ο€βˆ˜Ο„22idΟ„12∘E1​π2​τ1∘E1β€‹Ο€βˆ˜Οƒid)\displaystyle=\left(\begin{matrix}\operatorname{id}\nolimits&&&\\ 2E_{2}\pi\circ\tau_{2}&\operatorname{id}\nolimits&&\\ \sigma\circ E_{2}\pi\circ\tau_{2}^{2}&&\operatorname{id}\nolimits\\ &\tau_{1}^{2}\circ E_{1}\pi&2\tau_{1}\circ E_{1}\pi\circ\sigma&\operatorname{id}\nolimits\end{matrix}\right)
=id.\displaystyle=\operatorname{id}\nolimits.

We have E3​(m,Ο€)=([mβ€²β€²β€²,Ξ΄β€²],Ο€β€²β€²β€²)E^{3}(m,\pi)=([m^{\prime\prime\prime},\delta^{\prime}],\pi^{\prime\prime\prime}), where

mβ€²β€²β€²=E23​(m)βŠ•E22​E1​(m)βŠ•E2​E1​E2​(m)βŠ•E2​E12​(m)βŠ•E1​E22​(m)βŠ•E1​E2​E1​(m)βŠ•E12​E2​(m)βŠ•E13​(m).m^{\prime\prime\prime}=E_{2}^{3}(m)\oplus E_{2}^{2}E_{1}(m)\oplus E_{2}E_{1}E_{2}(m)\oplus E_{2}E_{1}^{2}(m)\oplus E_{1}E_{2}^{2}(m)\oplus E_{1}E_{2}E_{1}(m)\oplus E_{1}^{2}E_{2}(m)\oplus E_{1}^{3}(m).

We have

τ​E=(Ο„2​E200000000Ο„2​E10000000000Οƒβˆ’1​E200000000Οƒβˆ’1​E1000000000000000000000000Ο„1​E200000000Ο„1​E1)\tau E=\left(\begin{matrix}\tau_{2}E_{2}&0&0&0&0&0&0&0\\ 0&\tau_{2}E_{1}&0&0&0&0&0&0\\ 0&0&0&0&\sigma^{-1}E_{2}&0&0&0\\ 0&0&0&0&0&\sigma^{-1}E_{1}&0&0\\ 0&0&0&0&0&0&0&0\\ 0&0&0&0&0&0&0&0\\ 0&0&0&0&0&0&\tau_{1}E_{2}&0\\ 0&0&0&0&0&0&0&\tau_{1}E_{1}\end{matrix}\right)

and

E​τ=(E2​τ2000000000E2β€‹Οƒβˆ’10000000000000000E2​τ100000000E1​τ2000000000E1β€‹Οƒβˆ’10000000000000000E1​τ1)E\tau=\left(\begin{matrix}E_{2}\tau_{2}&0&0&0&0&0&0&0\\ 0&0&E_{2}\sigma^{-1}&0&0&0&0&0\\ 0&0&0&0&0&0&0&0\\ 0&0&0&E_{2}\tau_{1}&0&0&0&0\\ 0&0&0&0&E_{1}\tau_{2}&0&0&0\\ 0&0&0&0&0&0&E_{1}\sigma^{-1}&0\\ 0&0&0&0&0&0&0&0\\ 0&0&0&0&0&0&0&E_{1}\tau_{1}\end{matrix}\right)

Let a=(E​τ)∘(τ​E)∘(E​τ)a=(E\tau)\circ(\tau E)\circ(E\tau) and b=(τ​E)∘(E​τ)∘(τ​E)b=(\tau E)\circ(E\tau)\circ(\tau E). We have

a11=E2​τ2βˆ˜Ο„2​E2∘E2​τ2=Ο„2​E2∘E2​τ2βˆ˜Ο„2​E2=b11a_{11}=E_{2}\tau_{2}\circ\tau_{2}E_{2}\circ E_{2}\tau_{2}=\tau_{2}E_{2}\circ E_{2}\tau_{2}\circ\tau_{2}E_{2}=b_{11}
a44=E1​τ1βˆ˜Ο„1​E1∘E1​τ1=Ο„1​E1∘E1​τ1βˆ˜Ο„1​E1=b44a_{44}=E_{1}\tau_{1}\circ\tau_{1}E_{1}\circ E_{1}\tau_{1}=\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ\tau_{1}E_{1}=b_{44}
a25=E2β€‹Οƒβˆ’1βˆ˜Οƒβˆ’1​E2∘E1​τ2=Ο„2​E1∘E2β€‹Οƒβˆ’1βˆ˜Οƒβˆ’1​E2=b25a_{25}=E_{2}\sigma^{-1}\circ\sigma^{-1}E_{2}\circ E_{1}\tau_{2}=\tau_{2}E_{1}\circ E_{2}\sigma^{-1}\circ\sigma^{-1}E_{2}=b_{25}
a47=E2​τ1βˆ˜Οƒβˆ’1​E1∘E1β€‹Οƒβˆ’1=Οƒβˆ’1​E1∘E1β€‹Οƒβˆ’1βˆ˜Ο„1​E2=b47a_{47}=E_{2}\tau_{1}\circ\sigma^{-1}E_{1}\circ E_{1}\sigma^{-1}=\sigma^{-1}E_{1}\circ E_{1}\sigma^{-1}\circ\tau_{1}E_{2}=b_{47}

and all the other coefficients of aa and bb vanish. It follows that a=ba=b. This completes the proof of the theorem. ∎

4.3.4. Functoriality

We consider two differential categories 𝒲{\mathcal{W}} and 𝒲′{\mathcal{W}}^{\prime} endowed with actions (Ei,Ο„i)(E_{i},\tau_{i}) and (Eiβ€²,Ο„iβ€²)(E^{\prime}_{i},\tau^{\prime}_{i}) of 𝒰{\mathcal{U}} for i∈{1,2}i\in\{1,2\} and closed morphisms of functors Οƒ:E2​E1β†’E1​E2\sigma:E_{2}E_{1}\to E_{1}E_{2} and Οƒβ€²:E2′​E1β€²β†’E1′​E2β€²\sigma^{\prime}:E^{\prime}_{2}E^{\prime}_{1}\to E^{\prime}_{1}E^{\prime}_{2} making (4.3.1) and the similar diagram for Οƒβ€²\sigma^{\prime} commute.

Let Ξ¦:𝒲→𝒲′\Phi:{\mathcal{W}}\to{\mathcal{W}}^{\prime} be a differential functor and Ο†i:Φ​Eiβ†’βˆΌEi′​Φ\varphi_{i}:\Phi E_{i}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}E^{\prime}_{i}\Phi be closed isomorphisms of functors making (Ξ¦,Ο†i)(\Phi,\varphi_{i}) into morphisms of 22-representations for i∈{1,2}i\in\{1,2\}. Assume

(4.3.4) (E1′​φ2)∘(Ο†1​E2)∘(Φ​σ)=(σ′​Φ)∘(E2′​φ1)∘(Ο†2​E1):Φ​E2​E1β†’E1′​E2′​Φ.(E^{\prime}_{1}\varphi_{2})\circ(\varphi_{1}E_{2})\circ(\Phi\sigma)=(\sigma^{\prime}\Phi)\circ(E^{\prime}_{2}\varphi_{1})\circ(\varphi_{2}E_{1}):\Phi E_{2}E_{1}\to E^{\prime}_{1}E^{\prime}_{2}\Phi.
0P5Z

Proposition 4.3.9. There is a differential functor Δ​Φ:Δσ​𝒲→Δσ′​𝒲′\Delta\Phi:\Delta_{\sigma}{\mathcal{W}}\to\Delta_{\sigma^{\prime}}{\mathcal{W}}^{\prime} given by (m,Ο€)↦(Φ⁑(m),Ο†1​(m)∘Φ⁑(Ο€)βˆ˜Ο†2​(m)βˆ’1)(m,\pi)\mapsto(\Phi(m),\varphi_{1}(m)\circ\Phi(\pi)\circ\varphi_{2}(m)^{-1}).

There is a closed isomorphism of functors

Ο†=(Ο†2Ο†1):Δ​Φ​Eβ†’βˆΌE′​Δ​Φ.\varphi=\left(\begin{matrix}\varphi_{2}\\ &\varphi_{1}\end{matrix}\right):\Delta\Phi E\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}E^{\prime}\Delta\Phi.

If Οƒ\sigma and Οƒβ€²\sigma^{\prime} are invertible, then (Δ​Φ,Ο†)(\Delta\Phi,\varphi) defines a morphism of 22-representations Δσ​𝒲→Δσ′​𝒲′\Delta_{\sigma}{\mathcal{W}}\to\Delta_{\sigma^{\prime}}{\mathcal{W}}^{\prime}.

0P60

Proof. Let (m,Ο€)(m,\pi) be an object of Δσ​𝒲\Delta_{\sigma}{\mathcal{W}}. Let Ο€β€²=Ο†1​(m)∘Φ⁑(Ο€)βˆ˜Ο†2βˆ’1​(m)\pi^{\prime}=\varphi_{1}(m)\circ\Phi(\pi)\circ\varphi_{2}^{-1}(m), an element of Z​Hom𝒲′¯i⁑(E2′​Φ​(m),E1′​Φ​(m))Z\operatorname{Hom}\nolimits_{\overline{{\mathcal{W}}^{\prime}}^{i}}(E^{\prime}_{2}\Phi(m),E^{\prime}_{1}\Phi(m)).

We have

(E1′​π′)∘(σ′​Φ​(m))∘(E2′​π′)=(E^{\prime}_{1}\pi^{\prime})\circ(\sigma^{\prime}\Phi(m))\circ(E^{\prime}_{2}\pi^{\prime})=
=(E1′​φ1​(m))∘(E1′​Φ​π)∘(E1′​φ2βˆ’1​(m))∘(σ′​Φ​(m))∘(E2′​φ1​(m))∘(E2′​Φ​π)∘(E2′​φ2βˆ’1​(m))\displaystyle=(E^{\prime}_{1}\varphi_{1}(m))\circ(E^{\prime}_{1}\Phi\pi)\circ(E^{\prime}_{1}\varphi_{2}^{-1}(m))\circ(\sigma^{\prime}\Phi(m))\circ(E^{\prime}_{2}\varphi_{1}(m))\circ(E^{\prime}_{2}\Phi\pi)\circ(E^{\prime}_{2}\varphi_{2}^{-1}(m))
=(E1′​φ1​(m))∘(E1′​Φ​π)∘(Ο†1​(E2​(m)))∘(Φ​σ​(m))∘(Ο†2βˆ’1​(E1​(m)))∘(E2′​Φ​π)∘(E2′​φ2βˆ’1​(m))\displaystyle=(E^{\prime}_{1}\varphi_{1}(m))\circ(E^{\prime}_{1}\Phi\pi)\circ(\varphi_{1}(E_{2}(m)))\circ(\Phi\sigma(m))\circ(\varphi_{2}^{-1}(E_{1}(m)))\circ(E^{\prime}_{2}\Phi\pi)\circ(E^{\prime}_{2}\varphi_{2}^{-1}(m))
=(E1′​φ1​(m))∘(Ο†1​(E1​(m)))∘Φ⁑((E1​π)βˆ˜Οƒβ‘(m)∘(E2​π))∘(Ο†2βˆ’1​(E2​(m)))∘(E2′​φ2βˆ’1​(m))\displaystyle=(E^{\prime}_{1}\varphi_{1}(m))\circ(\varphi_{1}(E_{1}(m)))\circ\Phi\bigl((E_{1}\pi)\circ\sigma(m)\circ(E_{2}\pi)\bigr)\circ(\varphi_{2}^{-1}(E_{2}(m)))\circ(E^{\prime}_{2}\varphi_{2}^{-1}(m))

It follows that

(E1′​π′)∘(σ′​Φ​(m))∘(E2′​π′)∘(Ο„2′​Φ​(m))=(Ο„1′​Φ​(m))∘(E1′​π′)∘(σ′​Φ​(m))∘(E2′​π′),(E^{\prime}_{1}\pi^{\prime})\circ(\sigma^{\prime}\Phi(m))\circ(E^{\prime}_{2}\pi^{\prime})\circ(\tau^{\prime}_{2}\Phi(m))=(\tau^{\prime}_{1}\Phi(m))\circ(E^{\prime}_{1}\pi^{\prime})\circ(\sigma^{\prime}\Phi(m))\circ(E^{\prime}_{2}\pi^{\prime}),

hence (Φ⁑(m),Ο€β€²)(\Phi(m),\pi^{\prime}) is an object of Δσ′​𝒲′\Delta_{\sigma^{\prime}}{\mathcal{W}}^{\prime}. We put Δ​Φ​(m,Ο€)=(Φ⁑(m),Ο€β€²)\Delta\Phi(m,\pi)=(\Phi(m),\pi^{\prime}).

Let f∈HomΔσ​𝒲⁑((m,Ο€),(m~,Ο€~))f\in\operatorname{Hom}\nolimits_{\Delta_{\sigma}{\mathcal{W}}}((m,\pi),(\tilde{m},\tilde{\pi})). We have a commutative diagram

E2′​Φ​(m)\textstyle{E^{\prime}_{2}\Phi(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο†2βˆ’1​(m)\scriptstyle{\varphi_{2}^{-1}(m)}E2′​Φ​(f)\scriptstyle{E^{\prime}_{2}\Phi(f)}Φ​E2​(m)\textstyle{\Phi E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Φ​π\scriptstyle{\Phi\pi}Φ​E2​(f)\scriptstyle{\Phi E_{2}(f)}Φ​E1​(m)\textstyle{\Phi E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο†1​(m)\scriptstyle{\varphi_{1}(m)}Φ​E1​(f)\scriptstyle{\Phi E_{1}(f)}E1′​Φ​(m)\textstyle{E^{\prime}_{1}\Phi(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1′​Φ​(f)\scriptstyle{E^{\prime}_{1}\Phi(f)}E2′​Φ​(m~)\textstyle{E^{\prime}_{2}\Phi(\tilde{m})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο†2βˆ’1​(m~)\scriptstyle{\varphi_{2}^{-1}(\tilde{m})}Φ​E2​(m~)\textstyle{\Phi E_{2}(\tilde{m})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Φ​π~\scriptstyle{\Phi\tilde{\pi}}Φ​E1​(m~)\textstyle{\Phi E_{1}(\tilde{m})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο†1​(m~)\scriptstyle{\varphi_{1}(\tilde{m})}E1′​Φ​(m~)\textstyle{E^{\prime}_{1}\Phi(\tilde{m})}

and it follows that Φ⁑(f)∈HomΔσ′​𝒲′⁑(Δ​Φ​(m,Ο€),Δ​Φ​(m~,Ο€~))\Phi(f)\in\operatorname{Hom}\nolimits_{\Delta_{\sigma^{\prime}}{\mathcal{W}}^{\prime}}(\Delta\Phi(m,\pi),\Delta\Phi(\tilde{m},\tilde{\pi})). We put (Δ​Φ)​(f)=Φ​(f)(\Delta\Phi)(f)=\Phi(f). This makes Δ​Φ\Delta\Phi into a differential functor Δσ​𝒲→Δσ′​𝒲′\Delta_{\sigma}{\mathcal{W}}\to\Delta_{\sigma^{\prime}}{\mathcal{W}}^{\prime}.

We have

(Δ​Φ)​(E⁑(m,Ο€))=(    Φ⁑(E2​(m))βŠ•Ξ¦β‘(E1​(m))   Φ⁑(Ο€)Β Β Β Β Β Β Β Β Β ,Ξ²),(\Delta\Phi)(E(m,\pi))=({\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 50.11348pt\hbox{{\hbox{\kern-50.11348pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{\Phi(E_{2}(m))\oplus\Phi(E_{1}(m))}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-11.31735pt\raise 21.03578pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.75pt\hbox{$\scriptstyle{\Phi(\pi)}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 19.91682pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}},\beta),
Ξ²=(Ο†1​E2βˆ˜Ξ¦β€‹Οƒβˆ˜Ξ¦β€‹E2β€‹Ο€βˆ˜Ξ¦β€‹Ο„2βˆ˜Ο†2βˆ’1​E2Ο†1​E2βˆ˜Ξ¦β€‹Οƒβˆ˜Ο†2βˆ’1​E10Ο†1​E1βˆ˜Ξ¦β€‹Ο„1βˆ˜Ξ¦β€‹E1β€‹Ο€βˆ˜Ξ¦β€‹Οƒβˆ˜Ο†2βˆ’1​E1)\beta=\left(\begin{matrix}\varphi_{1}E_{2}\circ\Phi\sigma\circ\Phi E_{2}\pi\circ\Phi\tau_{2}\circ\varphi_{2}^{-1}E_{2}&\varphi_{1}E_{2}\circ\Phi\sigma\circ\varphi_{2}^{-1}E_{1}\\ 0&\varphi_{1}E_{1}\circ\Phi\tau_{1}\circ\Phi E_{1}\pi\circ\Phi\sigma\circ\varphi_{2}^{-1}E_{1}\end{matrix}\right)

and

E′​((Δ​Φ)​(m,Ο€))=(Β Β Β Β E2′​(Φ⁑(m))βŠ•E1′​(Φ⁑(m))Β Β Β Ο†1​(m)∘Φ⁑(Ο€)βˆ˜Ο†2​(m)βˆ’1Β Β Β Β Β Β Β Β Β ,Ξ²β€²),E^{\prime}((\Delta\Phi)(m,\pi))=({\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 50.11348pt\hbox{{\hbox{\kern-50.11348pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.50891pt\hbox{$\textstyle{E^{\prime}_{2}(\Phi(m))\oplus E^{\prime}_{1}(\Phi(m))}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-41.0553pt\raise 21.53079pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-2.24501pt\hbox{$\scriptstyle{\varphi_{1}(m)\circ\Phi(\pi)\circ\varphi_{2}(m)^{-1}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 19.91682pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}},\beta^{\prime}),
OPENΞ²β€²=(Οƒβ€²β€‹Ξ¦βˆ˜E2′​(Ο†1βˆ˜Ξ¦β€‹Ο€βˆ˜Ο†2βˆ’1)βˆ˜Ο„2′​Φσ′​Φ0Ο„1β€²β€‹Ξ¦βˆ˜E1′​(Ο†1βˆ˜Ξ¦β€‹Ο€βˆ˜Ο†2βˆ’1)βˆ˜Οƒβ€²β€‹Ξ¦))\beta^{\prime}=\left(\begin{matrix}\sigma^{\prime}\Phi\circ E^{\prime}_{2}(\varphi_{1}\circ\Phi\pi\circ\varphi_{2}^{-1})\circ\tau^{\prime}_{2}\Phi&\sigma^{\prime}\Phi\\ 0&\tau^{\prime}_{1}\Phi\circ E^{\prime}_{1}(\varphi_{1}\circ\Phi\pi\circ\varphi_{2}^{-1})\circ\sigma^{\prime}\Phi\end{matrix}\right))

We have

β′​(E2′​φ200E2′​φ1)=(E1′​φ200E1′​φ1)​β,\beta^{\prime}\left(\begin{matrix}E^{\prime}_{2}\varphi_{2}&0\\ 0&E^{\prime}_{2}\varphi_{1}\end{matrix}\right)=\left(\begin{matrix}E^{\prime}_{1}\varphi_{2}&0\\ 0&E^{\prime}_{1}\varphi_{1}\end{matrix}\right)\beta,

hence (Ο†2​(m)Ο†1​(m))\left(\begin{matrix}\varphi_{2}(m)\\ &\varphi_{1}(m)\end{matrix}\right) defines a closed isomorphism Δ​Φ​(E⁑(m,Ο€))β†’βˆΌE′​(Δ​Φ​(m,Ο€))\Delta\Phi(E(m,\pi))\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}E^{\prime}(\Delta\Phi(m,\pi)). The naturality of Ο†1\varphi_{1} and Ο†2\varphi_{2} implies immediately that of Ο†\varphi.

We have Ο„iβ€²β€‹Ξ¦βˆ˜Ei′​φiβˆ˜Ο†i​Ei=Ei′​φiβˆ˜Ο†i​Eiβˆ˜Ξ¦β€‹Ο„i\tau^{\prime}_{i}\Phi\circ E^{\prime}_{i}\varphi_{i}\circ\varphi_{i}E_{i}=E^{\prime}_{i}\varphi_{i}\circ\varphi_{i}E_{i}\circ\Phi\tau_{i} for i∈{1,2}i\in\{1,2\}. Together with (4.3.4), it follows that τ′​(Δ​Φ)∘Eβ€²β€‹Ο†βˆ˜Ο†β€‹E=Eβ€²β€‹Ο†βˆ˜Ο†β€‹E∘(Δ​Φ)​τ\tau^{\prime}(\Delta\Phi)\circ E^{\prime}\varphi\circ\varphi E=E^{\prime}\varphi\circ\varphi E\circ(\Delta\Phi)\tau, hence (Δ​Φ,Ο†)(\Delta\Phi,\varphi) defines a morphism of 22-representations. ∎

0P61

Remark 4.3.10. The data of Ο†1\varphi_{1} and Ο†2\varphi_{2}, the relations they are required to satisfy, and the map Ο€β€²\pi^{\prime} in the proof of the proposition are described graphically as:

[Uncaptioned image]

The following proposition is immediate.

0P62

Proposition 4.3.11. If Ξ¦\Phi is faithful, then Δ​Φ\Delta\Phi is faithful.

4.3.5. Associativity

We consider a differential category 𝒲{\mathcal{W}} together with three actions (Ei,Ο„i)(E_{i},\tau_{i}), 1≀i≀31\leq i\leq 3 of 𝒰{\mathcal{U}}.

We assume given Οƒi​j:Ei​Ejβ†’βˆΌEj​Ei\sigma_{ij}:E_{i}E_{j}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}E_{j}E_{i} for iβ‰ ji\neq j such that

(4.3.5) Οƒi​j​σj​i=id⁑ for all ​iβ‰ j​ and ​E3​σ12βˆ˜Οƒ13​E2∘E1​σ23=Οƒ23​E1∘E2​σ13βˆ˜Οƒ12​E3.\sigma_{ij}\sigma_{ji}=\operatorname{id}\nolimits\text{ for all }i\neq j\text{ and }E_{3}\sigma_{12}\circ\sigma_{13}E_{2}\circ E_{1}\sigma_{23}=\sigma_{23}E_{1}\circ E_{2}\sigma_{13}\circ\sigma_{12}E_{3}.

This ensures that by composing Οƒ\sigma’s, we obtain a transitive system of isomorphisms between Ei​Ej​EkE_{i}E_{j}E_{k}’s for {i,j,k}={1,2,3}\{i,j,k\}=\{1,2,3\}.

We also assume the analogs of the diagram (4.3.1) for the map Οƒi​j\sigma_{ij} commute.

Let (m,Ο€)βˆˆΞ”Οƒ21​(𝒲)(m,\pi)\in\Delta_{\sigma_{21}}({\mathcal{W}}). We define Ο€β€²βˆˆZ​Hom⁑(E2​E3​(m),E1​E3​(m))\pi^{\prime}\in Z\operatorname{Hom}\nolimits(E_{2}E_{3}(m),E_{1}E_{3}(m)) as the composition E2​E3​(m)β†’Οƒ23E3​E2​(m)β†’E3​(Ο€)E3​E1​(m)β†’Οƒ31E1​E3​(m)E_{2}E_{3}(m)\xrightarrow{\sigma_{23}}E_{3}E_{2}(m)\xrightarrow{E_{3}(\pi)}E_{3}E_{1}(m)\xrightarrow{\sigma_{31}}E_{1}E_{3}(m).

We have a commutative diagram

E22​E3​(m)\textstyle{E_{2}^{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​(Ο€β€²)\scriptstyle{E_{2}(\pi^{\prime})}E2​σ23\scriptstyle{E_{2}\sigma_{23}}E2​E1​E3​(m)\textstyle{E_{2}E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21​E3\scriptstyle{\sigma_{21}E_{3}}E1​E2​E3​(m)\textstyle{E_{1}E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​σ23\scriptstyle{E_{1}\sigma_{23}}E1​(Ο€β€²)\scriptstyle{E_{1}(\pi^{\prime})}E12​E3​(m)\textstyle{E_{1}^{2}E_{3}(m)}E2​E3​E2​(m)\textstyle{E_{2}E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​E3​(Ο€)\scriptstyle{E_{2}E_{3}(\pi)}Οƒ23​E2\scriptstyle{\sigma_{23}E_{2}}E2​E3​E1​(m)\textstyle{E_{2}E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​σ31\scriptstyle{E_{2}\sigma_{31}}Οƒ23​E1\scriptstyle{\sigma_{23}E_{1}}E1​E3​E2​(m)\textstyle{E_{1}E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​E3​(Ο€)\scriptstyle{E_{1}E_{3}(\pi)}E1​E3​E1​(m)\textstyle{E_{1}E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​σ31\scriptstyle{E_{1}\sigma_{31}}E3​E22​(m)\textstyle{E_{3}E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​E2​(Ο€)\scriptstyle{E_{3}E_{2}(\pi)}E3​E2​E1​(m)\textstyle{E_{3}E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​σ21\scriptstyle{E_{3}\sigma_{21}}E3​E1​E2​(m)\textstyle{E_{3}E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31​E2\scriptstyle{\sigma_{31}E_{2}}E3​E1​(Ο€)\scriptstyle{E_{3}E_{1}(\pi)}E3​E12​(m)\textstyle{E_{3}E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31​E1\scriptstyle{\sigma_{31}E_{1}}

It follows that (E3​(m),Ο€β€²)(E_{3}(m),\pi^{\prime}) defines an object of Δσ21​(𝒲)\Delta_{\sigma_{21}}({\mathcal{W}}) and we put E~3​(m,Ο€)=(E3​(m),Ο€β€²){\tilde{E}}_{3}(m,\pi)=(E_{3}(m),\pi^{\prime}). Given ff a map in Δσ21​(𝒲)\Delta_{\sigma_{21}}({\mathcal{W}}), the map E3​(f)E_{3}(f) is actually in Δσ21​(𝒲)\Delta_{\sigma_{21}}({\mathcal{W}}) and this defines E~3​(f){\tilde{E}}_{3}(f).

We have defined an endofunctor E~3{\tilde{E}}_{3} of Δσ21​(𝒲)\Delta_{\sigma_{21}}({\mathcal{W}}).

There is a commutative diagram

E2​E32​(m)\textstyle{E_{2}E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ23​E3\scriptstyle{\sigma_{23}E_{3}}E2​τ3\scriptstyle{E_{2}\tau_{3}}E3​E2​E3​(m)\textstyle{E_{3}E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​σ23\scriptstyle{E_{3}\sigma_{23}}E32​E2​(m)\textstyle{E_{3}^{2}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E32​(Ο€)\scriptstyle{E_{3}^{2}(\pi)}Ο„3​E2\scriptstyle{\tau_{3}E_{2}}E32​E1​(m)\textstyle{E_{3}^{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​σ31\scriptstyle{E_{3}\sigma_{31}}Ο„3​E1\scriptstyle{\tau_{3}E_{1}}E3​E1​E3​(m)\textstyle{E_{3}E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31​E3\scriptstyle{\sigma_{31}E_{3}}E1​E32​(m)\textstyle{E_{1}E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​τ3\scriptstyle{E_{1}\tau_{3}}E2​E32​(m)\textstyle{E_{2}E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ23​E3\scriptstyle{\sigma_{23}E_{3}}E3​E2​E3​(m)\textstyle{E_{3}E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​σ23\scriptstyle{E_{3}\sigma_{23}}E32​E2​(m)\textstyle{E_{3}^{2}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E32​(Ο€)\scriptstyle{E_{3}^{2}(\pi)}E32​E1​(m)\textstyle{E_{3}^{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​σ31\scriptstyle{E_{3}\sigma_{31}}E3​E1​E3​(m)\textstyle{E_{3}E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31​E3\scriptstyle{\sigma_{31}E_{3}}E1​E32​(m)\textstyle{E_{1}E_{3}^{2}(m)}

It follows that Ο„3\tau_{3} defines an endomorphism of E~32{\tilde{E}}_{3}^{2}. So, (E~3,Ο„3)({\tilde{E}}_{3},\tau_{3}) defines a 22-representation on Δσ21​(𝒲)\Delta_{\sigma_{21}}({\mathcal{W}}).

Let E21E_{21} denote the functor E~{\tilde{E}} of Δσ21​(𝒲)\Delta_{\sigma_{21}}({\mathcal{W}}). We have

E~3​E21​(m,Ο€)=(Β Β Β Β E3​E2​(m)βŠ•E3​E1​(m)Β Β Β E3​(Ο€)Β Β Β Β Β Β Β Β Β ,Ο€β€²),{\tilde{E}}_{3}E_{21}(m,\pi)=({\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 47.55789pt\hbox{{\hbox{\kern-47.55789pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{E_{3}E_{2}(m)\oplus E_{3}E_{1}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-13.54237pt\raise 21.03578pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.75pt\hbox{$\scriptstyle{E_{3}(\pi)}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 19.91682pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}},\pi^{\prime}),

where

Ο€β€²=(Οƒ31​E2∘E3​(Οƒ21∘E2β€‹Ο€βˆ˜Ο„2)βˆ˜Οƒ23​E2Οƒ31​E2∘E3​σ21βˆ˜Οƒ23​E10Οƒ31​E1∘E3​(Ο„1∘E1β€‹Ο€βˆ˜Οƒ21)βˆ˜Οƒ23​E1)\pi^{\prime}=\left(\begin{matrix}\sigma_{31}E_{2}\circ E_{3}(\sigma_{21}\circ E_{2}\pi\circ\tau_{2})\circ\sigma_{23}E_{2}&\sigma_{31}E_{2}\circ E_{3}\sigma_{21}\circ\sigma_{23}E_{1}\\ 0&\sigma_{31}E_{1}\circ E_{3}(\tau_{1}\circ E_{1}\pi\circ\sigma_{21})\circ\sigma_{23}E_{1}\end{matrix}\right)

and

E21​E~3​(m,Ο€)=(Β Β Β Β E2​E3​(m)βŠ•E1​E3​(m)Β Β Β Οƒ31∘E3​(Ο€)βˆ˜Οƒ23Β Β Β Β Β Β Β Β Β ,Ο€β€²β€²)E_{21}{\tilde{E}}_{3}(m,\pi)=({\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 47.55789pt\hbox{{\hbox{\kern-47.55789pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{E_{2}E_{3}(m)\oplus E_{1}E_{3}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-29.57921pt\raise 21.03578pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.75pt\hbox{$\scriptstyle{\sigma_{31}\circ E_{3}(\pi)\circ\sigma_{23}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 19.91682pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}},\pi^{\prime\prime})

where

Ο€β€²β€²=(Οƒ21​E3∘E2​(Οƒ31∘E3​(Ο€)βˆ˜Οƒ23)βˆ˜Ο„2​E3Οƒ21​E30Ο„1​E3βˆ˜Οƒ13​E1∘E1​E3β€‹Ο€βˆ˜E1​σ23βˆ˜Οƒ21​E3)).\pi^{\prime\prime}=\left(\begin{matrix}\sigma_{21}E_{3}\circ E_{2}(\sigma_{31}\circ E_{3}(\pi)\circ\sigma_{23})\circ\tau_{2}E_{3}&\sigma_{21}E_{3}\\ 0&\tau_{1}E_{3}\circ\sigma_{13}E_{1}\circ E_{1}E_{3}\pi\circ E_{1}\sigma_{23}\circ\sigma_{21}E_{3}\end{matrix}\right)\bigl).

We have commutative diagrams

E22​E3​(m)\textstyle{E_{2}^{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„2​E3\scriptstyle{\tau_{2}E_{3}}E2​σ23\scriptstyle{E_{2}\sigma_{23}}E22​E3​(m)\textstyle{E_{2}^{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​σ23\scriptstyle{E_{2}\sigma_{23}}E2​E3​E2​(m)\textstyle{E_{2}E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​E3​π\scriptstyle{E_{2}E_{3}\pi}Οƒ23​E2\scriptstyle{\sigma_{23}E_{2}}E2​E3​E1​(m)\textstyle{E_{2}E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​σ31\scriptstyle{E_{2}\sigma_{31}}Οƒ23​E1\scriptstyle{\sigma_{23}E_{1}}E2​E1​E3​(m)\textstyle{E_{2}E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ12​E3\scriptstyle{\sigma_{12}E_{3}}E1​E2​E3​(m)\textstyle{E_{1}E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​σ23\scriptstyle{E_{1}\sigma_{23}}E2​E3​E2​(m)\textstyle{E_{2}E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ23​E2\scriptstyle{\sigma_{23}E_{2}}E3​E22​(m)\textstyle{E_{3}E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​τ2\scriptstyle{E_{3}\tau_{2}}E3​E22​(m)\textstyle{E_{3}E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​E2​π\scriptstyle{E_{3}E_{2}\pi}E3​E2​E1​(m)\textstyle{E_{3}E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​σ21\scriptstyle{E_{3}\sigma_{21}}E3​E1​E2​(m)\textstyle{E_{3}E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31​E2\scriptstyle{\sigma_{31}E_{2}}E1​E3​E2​(m)\textstyle{E_{1}E_{3}E_{2}(m)}
E2​E1​E3​(m)\textstyle{E_{2}E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21​E3\scriptstyle{\sigma_{21}E_{3}}E2​σ13\scriptstyle{E_{2}\sigma_{13}}E1​E2​E3​(m)\textstyle{E_{1}E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​σ23\scriptstyle{E_{1}\sigma_{23}}E1​E3​E2​(m)\textstyle{E_{1}E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​E3​π\scriptstyle{E_{1}E_{3}\pi}Οƒ13​E2\scriptstyle{\sigma_{13}E_{2}}E1​E3​E1​(m)\textstyle{E_{1}E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​σ31\scriptstyle{E_{1}\sigma_{31}}Οƒ13​E1\scriptstyle{\sigma_{13}E_{1}}E12​E3​(m)\textstyle{E_{1}^{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„1​E3\scriptstyle{\tau_{1}E_{3}}E12​E3​(m)\textstyle{E_{1}^{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​σ13\scriptstyle{E_{1}\sigma_{13}}E2​E3​E1​(m)\textstyle{E_{2}E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ23​E1\scriptstyle{\sigma_{23}E_{1}}E3​E2​E1​(m)\textstyle{E_{3}E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​σ21\scriptstyle{E_{3}\sigma_{21}}E3​E1​E2​(m)\textstyle{E_{3}E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​E1​π\scriptstyle{E_{3}E_{1}\pi}E3​E12​(m)\textstyle{E_{3}E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​τ1\scriptstyle{E_{3}\tau_{1}}E3​E12​(m)\textstyle{E_{3}E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31​E1\scriptstyle{\sigma_{31}E_{1}}E1​E3​E1​(m)\textstyle{E_{1}E_{3}E_{1}(m)}

So, (Οƒ2300Οƒ13)\left(\begin{matrix}\sigma_{23}&0\\ 0&\sigma_{13}\end{matrix}\right) defines an isomorphism E21​E~3​(m,Ο€)β†’βˆΌE~3​E21​(m,Ο€)E_{21}{\tilde{E}}_{3}(m,\pi)\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\tilde{E}}_{3}E_{21}(m,\pi). It provides an isomorphism of functors Οƒ21,3:E21​E~3β†’βˆΌE~3​E21\sigma_{21,3}:E_{21}{\tilde{E}}_{3}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\tilde{E}}_{3}E_{21}.

Replacing 11 by 22, 22 by 33 and 33 by 11, the construction above provides a 22-representation (E~1,Ο„1)({\tilde{E}}_{1},\tau_{1}) of Δσ32​(𝒲)\Delta_{\sigma_{32}}({\mathcal{W}}) and we denote by E32E_{32} the endofunctor E~{\tilde{E}} of Ξ”32​(𝒲)\Delta_{32}({\mathcal{W}}). We have an isomorphism Οƒ32,1:E32​E~1β†’βˆΌE~1​E32\sigma_{32,1}:E_{32}{\tilde{E}}_{1}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\tilde{E}}_{1}E_{32}.

Let us now define another 22-representation. The justifications for the constructions below will be given in the proof of Proposition 4.3.12.

We define a differential category Ξ”123​(𝒲)\Delta_{123}({\mathcal{W}}). Its objects are quadruples (m,Ο€21,Ο€31,Ο€32)(m,\pi_{21},\pi_{31},\pi_{32}) where mβˆˆπ’²Β―im\in\overline{{\mathcal{W}}}^{i}, Ο€i​j:Ei​(m)β†’Ej​(m)\pi_{ij}:E_{i}(m)\to E_{j}(m) satisfy

d⁑(Ο€21)=d⁑(Ο€32)=0,d⁑(Ο€31)=Ο€21βˆ˜Ο€32d(\pi_{21})=d(\pi_{32})=0,\ d(\pi_{31})=\pi_{21}\circ\pi_{32}

and given i,j,k,l∈{1,2,3}i,j,k,l\in\{1,2,3\} with jβˆ’lβ‰₯iβˆ’k>0j-l\geq i-k>0, we have an equality between maps Ei​Ej​(m)β†’Ek​El​(m)E_{i}E_{j}(m)\to E_{k}E_{l}(m):

Οƒl​k∘El​πi​kβˆ˜Οƒi​l∘Ei​πj​l+Ek​πj​lβˆ˜Οƒj​k∘Ej​πi​kβˆ˜Οƒi​j+Ξ΄j​k​Ej​πi​lβˆ˜Οƒi​j+Ξ΄i​l​σl​k∘Ei​πj​k=0\sigma_{lk}\circ E_{l}\pi_{ik}\circ\sigma_{il}\circ E_{i}\pi_{jl}+E_{k}\pi_{jl}\circ\sigma_{jk}\circ E_{j}\pi_{ik}\circ\sigma_{ij}+\delta_{jk}E_{j}\pi_{il}\circ\sigma_{ij}+\delta_{il}\sigma_{lk}\circ E_{i}\pi_{jk}=0

where we put Οƒr​r=Ο„r\sigma_{rr}=\tau_{r}.

Note that the equality for (i,j,k,l)=(3,2,2,1)(i,j,k,l)=(3,2,2,1) is equivalent to the one for (i,j,k,l)=(2,3,1,2)(i,j,k,l)=(2,3,1,2).

We define HomΞ”123​(𝒲)⁑((m,Ο€21,Ο€31,Ο€32),(mβ€²,Ο€21β€²,Ο€31β€²,Ο€32β€²))\operatorname{Hom}\nolimits_{\Delta_{123}({\mathcal{W}})}((m,\pi_{21},\pi_{31},\pi_{32}),(m^{\prime},\pi^{\prime}_{21},\pi^{\prime}_{31},\pi^{\prime}_{32})) to be the differential submodule of Hom𝒲⁑(m,mβ€²)\operatorname{Hom}\nolimits_{\mathcal{W}}(m,m^{\prime}) of maps ff such that Ej​fβˆ˜Ο€i​j=Ο€i​jβ€²βˆ˜Ei​fE_{j}f\circ\pi_{ij}=\pi^{\prime}_{ij}\circ E_{i}f for all i>ji>j.

We define a differential endofunctor EE of Ξ”123​(𝒲)\Delta_{123}({\mathcal{W}}) by E⁑(m,Ο€21,Ο€31,Ο€32)=(mβ€²,Ο€21β€²,Ο€31β€²,Ο€32β€²)E(m,\pi_{21},\pi_{31},\pi_{32})=(m^{\prime},\pi^{\prime}_{21},\pi^{\prime}_{31},\pi^{\prime}_{32}) where

mβ€²=Β Β Β Β E3​(m)βŠ•E2​(m)βŠ•E1​(m)Β Β Β Ο€31Β Β Β Β Β Β Β Β Ο€32Β Β Β Β Β Β Β Β Ο€21Β Β Β Β Β Β Β Β Β m^{\prime}={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 55.72571pt\hbox{{\hbox{\kern-55.72571pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{E_{3}(m)\oplus E_{2}(m)\oplus E_{1}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-8.99098pt\raise 37.54272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\pi_{31}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 48.36943pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-35.22432pt\raise 19.54272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\ \pi_{32}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern-2.84526pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern 13.7711pt\raise 19.54272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\pi_{21}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 45.52417pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}}
Ο€31β€²:Β Β Β Β E32​(m)βŠ•E3​E2​(m)βŠ•E3​E1​(m)Β Β Β E1​E3​(m)βŠ•E1​E2​(m)βŠ•E12​(m)Β Β Β Β Οƒ31∘E3​π31βˆ˜Ο„3Β Β Β Β Β Β Β Β Β Β Οƒ31Β Β Β Β Β Β Β Β Β Β Ο„1∘E1​π31βˆ˜Οƒ31Β Β Β Β Β Β Β Β Β Β \pi^{\prime}_{31}:{\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 118.46088pt\hbox{{\hbox{\kern-68.17015pt\raise 28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{3}^{2}(m)\oplus E_{3}E_{2}(m)\oplus E_{3}E_{1}(m)}$}}}}}{\hbox{\kern-68.17015pt\raise-28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{1}E_{3}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-118.46088pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\sigma_{31}\circ E_{3}\pi_{31}\circ\tau_{3}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-62.59573pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-12.10573pt\raise 5.00694pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\sigma_{31}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-56.90521pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 62.59573pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\tau_{1}\circ E_{1}\pi_{31}\circ\sigma_{31}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 62.59573pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces}}}}}
Ο€32β€²:Β Β Β Β E32​(m)βŠ•E3​E2​(m)βŠ•E3​E1​(m)Β Β Β E2​E3​(m)βŠ•E22​(m)βŠ•E2​E1​(m)Β Β Β Β Οƒ32∘E3​π32βˆ˜Ο„3Β Β Β Β Β Β Β Β Β Β Οƒ32Β Β Β Β Β Β Β Β Β Β Οƒ12∘E1​π32βˆ˜Οƒ31Β Β Β Β Β Β Β Β Β Β Ο„2∘E2​π32βˆ˜Οƒ32Β Β Β Β Β Β Β Β Β Β \pi^{\prime}_{32}:{\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 118.46088pt\hbox{{\hbox{\kern-68.17015pt\raise 28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{3}^{2}(m)\oplus E_{3}E_{2}(m)\oplus E_{3}E_{1}(m)}$}}}}}{\hbox{\kern-68.17015pt\raise-28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{2}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{2}E_{1}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-118.46088pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\sigma_{32}\circ E_{3}\pi_{32}\circ\tau_{3}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-62.59573pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-50.9615pt\raise 5.00694pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\sigma_{32}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-56.90521pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 62.59573pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\sigma_{12}\circ E_{1}\pi_{32}\circ\sigma_{31}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 62.59573pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-5.69052pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\tau_{2}\circ E_{2}\pi_{32}\circ\sigma_{32}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-5.69052pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces}}}}}
Ο€21β€²:Β Β Β Β E2​E3​(m)βŠ•E22​(m)βŠ•E2​E1​(m)Β Β Β E1​E3​(m)βŠ•E1​E2​(m)βŠ•E12​(m)Β Β Β Β Οƒ31∘E3​π21βˆ˜Οƒ23Β Β Β Β Β Β Β Β Β Β Ο„1∘E1​π21βˆ˜Οƒ21Β Β Β Β Β Β Β Β Β Β Οƒ21Β Β Β Β Β Β Β Β Β Β Οƒ21∘E2​π21βˆ˜Ο„2Β Β Β Β Β Β Β Β Β Β \pi^{\prime}_{21}:{\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 122.80978pt\hbox{{\hbox{\kern-68.17015pt\raise 28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{2}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{2}E_{1}(m)}$}}}}}{\hbox{\kern-68.17015pt\raise-28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{1}E_{3}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-122.80978pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\sigma_{31}\circ E_{3}\pi_{21}\circ\sigma_{23}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-62.59573pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 62.59573pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\tau_{1}\circ E_{1}\pi_{21}\circ\sigma_{21}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 62.59573pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 13.19344pt\raise 5.00694pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\sigma_{21}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 0.0pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-60.389pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\sigma_{21}\circ E_{2}\pi_{21}\circ\tau_{2}\!}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-5.69052pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces}}}}}

We define an endomorphism Ο„\tau of E2E^{2} as follows. We have E2​(m,Ο€21,Ο€31,Ο€32)=(mβ€²β€²,Ο€21β€²β€²,Ο€31β€²β€²,Ο€32β€²β€²)E^{2}(m,\pi_{21},\pi_{31},\pi_{32})=(m^{\prime\prime},\pi^{\prime\prime}_{21},\pi^{\prime\prime}_{31},\pi^{\prime\prime}_{32}) where (ignoring differentials)

mβ€²β€²=E32​(m)βŠ•E3​E2​(m)βŠ•E3​E1​(m)βŠ•E2​E3​(m)βŠ•E22​(m)βŠ•E2​E1​(m)βŠ•E1​E3​(m)βŠ•E1​E2​(m)βŠ•E12​(m).m^{\prime\prime}=E_{3}^{2}(m)\oplus E_{3}E_{2}(m)\oplus E_{3}E_{1}(m)\oplus E_{2}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{2}E_{1}(m)\oplus E_{1}E_{3}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m).

We define the endomorphism Ο„\tau of mβ€²β€²m^{\prime\prime} by

(4.3.6) Ο„=(Ο„3Οƒ23Οƒ13Ο„2Οƒ12Ο„1).\tau=\left(\begin{matrix}\tau_{3}\\ &&&\sigma_{23}\\ &&&&&&\sigma_{13}\\ \\ &&&&\tau_{2}\\ &&&&&&&\sigma_{12}\\ \\ \\ &&&&&&&&\tau_{1}\end{matrix}\right).
0P63

Proposition 4.3.12. The construction above defines a 22-representation on Ξ”123​(𝒲)\Delta_{123}({\mathcal{W}}).

We have isomorphisms of 22-representations Δσ21,3βˆ’1​Δσ21​(𝒲)β†’βˆΌΞ”123​(𝒲)\Delta_{\sigma_{21,3}^{-1}}\Delta_{\sigma_{21}}({\mathcal{W}})\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}\Delta_{123}({\mathcal{W}}) and Δσ32,1​Δσ32​(𝒲)β†’βˆΌΞ”123​(𝒲)\Delta_{\sigma_{32,1}}\Delta_{\sigma_{32}}({\mathcal{W}})\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}\Delta_{123}({\mathcal{W}}) whose underlying functors make the following diagram commutative

Δσ21,3βˆ’1​Δσ21​(𝒲)\textstyle{\Delta_{\sigma_{21,3}^{-1}}\Delta_{\sigma_{21}}({\mathcal{W}})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}∼\scriptstyle{\sim}Ο‰\scriptstyle{\omega}Ξ”123​(𝒲)\textstyle{\Delta_{123}({\mathcal{W}})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο‰\scriptstyle{\omega}Δσ32,1​Δσ32​(𝒲)\textstyle{\Delta_{\sigma_{32,1}}\Delta_{\sigma_{32}}({\mathcal{W}})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}∼\scriptstyle{\sim}Ο‰\scriptstyle{\omega}𝒲\textstyle{\mathcal{W}}
0P64

Proof. Replacing 𝒲{\mathcal{W}} by 𝒲¯i\overline{{\mathcal{W}}}^{i}, we can assume it is strongly pretriangulated and idempotent-complete.

The category Δσ21,3βˆ’1​Δσ21​(𝒲)\Delta_{\sigma_{21,3}^{-1}}\Delta_{\sigma_{21}}({\mathcal{W}}) has objects ((m,Ο€21),Ο€3)((m,\pi_{21}),\pi_{3}) where mβˆˆπ’²m\in{\mathcal{W}}, Ο€21:E2​(m)β†’E1​(m)\pi_{21}:E_{2}(m)\to E_{1}(m) and Ο€3:E~3​(m,Ο€21)β†’E21​(m,Ο€21)\pi_{3}:{\tilde{E}}_{3}(m,\pi_{21})\to E_{21}(m,\pi_{21}) satisfy

d⁑(Ο€21)=d⁑(Ο€3)=0d(\pi_{21})=d(\pi_{3})=0

and the diagram (4.3.2) commutes for Ο€21\pi_{21} and for Ο€3\pi_{3}.

For i∈{1,2}i\in\{1,2\}, let Ο€3​i\pi_{3i} be the composition of Ο€3\pi_{3} with the projection onto Ei​(m)E_{i}(m). We have d⁑(Ο€32)=0d(\pi_{32})=0 and d⁑(Ο€31)=Ο€21βˆ˜Ο€32d(\pi_{31})=\pi_{21}\circ\pi_{32}.

The commutativity of (4.3.2) for Ο€21\pi_{21} is the commutativity of

E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π21\scriptstyle{E_{2}\pi_{21}}Ο„2\scriptstyle{\tau_{2}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21\scriptstyle{\sigma_{21}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π21\scriptstyle{E_{1}\pi_{21}}E12​(m)\textstyle{E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„1\scriptstyle{\tau_{1}}E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π21\scriptstyle{E_{2}\pi_{21}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21\scriptstyle{\sigma_{21}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π21\scriptstyle{E_{1}\pi_{21}}E12​(m)\textstyle{E_{1}^{2}(m)}

The maps Ο€3​i:E3​(m)β†’Ei​(m)\pi_{3i}:E_{3}(m)\to E_{i}(m) for i∈{1,2}i\in\{1,2\} give rise to a map

(Ο€32Ο€31)∈HomΔσ21​(𝒲)⁑(E~3​(m,Ο€21),E21​(m,Ο€21))\left(\begin{matrix}\pi_{32}\\ \pi_{31}\end{matrix}\right)\in\operatorname{Hom}\nolimits_{\Delta_{\sigma_{21}}({\mathcal{W}})}({\tilde{E}}_{3}(m,\pi_{21}),E_{21}(m,\pi_{21}))

if and only if the composition

E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ23\scriptstyle{\sigma_{23}}E3​E2​(m)\textstyle{E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π21\scriptstyle{E_{3}\pi_{21}}E3​E1​(m)\textstyle{E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31\scriptstyle{\sigma_{31}}E1​E3​(m)\textstyle{E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π32\scriptstyle{E_{1}\pi_{32}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)}

is equal to the sum of the following two maps:

E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π32\scriptstyle{E_{2}\pi_{32}}E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„2\scriptstyle{\tau_{2}}E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π21\scriptstyle{E_{2}\pi_{21}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21\scriptstyle{\sigma_{21}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)}

and

E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π31\scriptstyle{E_{2}\pi_{31}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21\scriptstyle{\sigma_{21}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)}

and the following diagram commutes:

E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ23\scriptstyle{\sigma_{23}}E2​π31\scriptstyle{E_{2}\pi_{31}}E3​E2​(m)\textstyle{E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π21\scriptstyle{E_{3}\pi_{21}}E3​E1​(m)\textstyle{E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31\scriptstyle{\sigma_{31}}E1​E3​(m)\textstyle{E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π31\scriptstyle{E_{1}\pi_{31}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21\scriptstyle{\sigma_{21}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π21\scriptstyle{E_{1}\pi_{21}}E12​(m)\textstyle{E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„1\scriptstyle{\tau_{1}}E12​(m)\textstyle{E_{1}^{2}(m)}

The commutativity of (4.3.2) for Ο€3\pi_{3} is equivalent to the commutativity of the following diagrams:

E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π31\scriptstyle{E_{3}\pi_{31}}Ο„3\scriptstyle{\tau_{3}}E3​E1​(m)\textstyle{E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31\scriptstyle{\sigma_{31}}E1​E3​(m)\textstyle{E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π31\scriptstyle{E_{3}\pi_{31}}E12​(m)\textstyle{E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„1\scriptstyle{\tau_{1}}E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π31\scriptstyle{E_{3}\pi_{31}}E3​E1​(m)\textstyle{E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31\scriptstyle{\sigma_{31}}E1​E3​(m)\textstyle{E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π31\scriptstyle{E_{3}\pi_{31}}E12​(m)\textstyle{E_{1}^{2}(m)}
E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}Ο„3\scriptstyle{\tau_{3}}E3​E2​(m)\textstyle{E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ32\scriptstyle{\sigma_{32}}E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„2\scriptstyle{\tau_{2}}E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}E3​E2​(m)\textstyle{E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ32\scriptstyle{\sigma_{32}}E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}E22​(m)\textstyle{E_{2}^{2}(m)}
E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π31\scriptstyle{E_{3}\pi_{31}}Ο„3\scriptstyle{\tau_{3}}E3​E1​(m)\textstyle{E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31\scriptstyle{\sigma_{31}}E1​E3​(m)\textstyle{E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π32\scriptstyle{E_{1}\pi_{32}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ12\scriptstyle{\sigma_{12}}E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}E3​E2​(m)\textstyle{E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ32\scriptstyle{\sigma_{32}}E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π31\scriptstyle{E_{2}\pi_{31}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)}

and the vanishing of the following composition:

E32​(m)β†’Ο„3E32​(m)β†’E3​π31E3​E1​(m)β†’Οƒ31E1​E3​(m)β†’E1​π32E1​E2​(m).E_{3}^{2}(m)\xrightarrow{\tau_{3}}E_{3}^{2}(m)\xrightarrow{E_{3}\pi_{31}}E_{3}E_{1}(m)\xrightarrow{\sigma_{31}}E_{1}E_{3}(m)\xrightarrow{E_{1}\pi_{32}}E_{1}E_{2}(m).

Note that the vanishing of that composition follows from the commutativity of the diagram immediately above.

We deduce that the objects of Δσ21,3βˆ’1​Δσ21​(𝒲)\Delta_{\sigma_{21,3}^{-1}}\Delta_{\sigma_{21}}({\mathcal{W}}) can be described as quadruples (m,Ο€21,Ο€31,Ο€32)(m,\pi_{21},\pi_{31},\pi_{32}) where mβˆˆπ’²m\in{\mathcal{W}}, Ο€i​j:Ei​(m)β†’Ej​(m)\pi_{ij}:E_{i}(m)\to E_{j}(m) satisfy

d⁑(Ο€21)=d⁑(Ο€32)=0,d⁑(Ο€31)=Ο€21βˆ˜Ο€32d(\pi_{21})=d(\pi_{32})=0,\ d(\pi_{31})=\pi_{21}\circ\pi_{32}

and given i,j,k,l∈{1,2,3}i,j,k,l\in\{1,2,3\} with jβˆ’lβ‰₯iβˆ’k>0j-l\geq i-k>0, we have an equality between maps Ei​Ej​(m)β†’Ek​El​(m)E_{i}E_{j}(m)\to E_{k}E_{l}(m):

Οƒl​k∘El​πi​kβˆ˜Οƒi​l∘Ei​πj​l+Ek​πj​lβˆ˜Οƒj​k∘Ej​πi​kβˆ˜Οƒi​j+Ξ΄j​k​Ej​πi​lβˆ˜Οƒi​j+Ξ΄i​l​σl​k∘Ei​πj​k=0\sigma_{lk}\circ E_{l}\pi_{ik}\circ\sigma_{il}\circ E_{i}\pi_{jl}+E_{k}\pi_{jl}\circ\sigma_{jk}\circ E_{j}\pi_{ik}\circ\sigma_{ij}+\delta_{jk}E_{j}\pi_{il}\circ\sigma_{ij}+\delta_{il}\sigma_{lk}\circ E_{i}\pi_{jk}=0

where we put Οƒr​r=Ο„r\sigma_{rr}=\tau_{r}.

This provides an isomorphism of categories Δσ21,3βˆ’1​Δσ21​(𝒲)β†’βˆΌΞ”123​(𝒲)\Delta_{\sigma_{21,3}^{-1}}\Delta_{\sigma_{21}}({\mathcal{W}})\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}\Delta_{123}({\mathcal{W}}).

Let us now describe the action of EE on Δσ21,3βˆ’1​Δσ21​(𝒲)\Delta_{\sigma_{21,3}^{-1}}\Delta_{\sigma_{21}}({\mathcal{W}}).

We have E⁑((m,Ο€21),Ο€3)=(mβ€²,Ο€β€²)E((m,\pi_{21}),\pi_{3})=(m^{\prime},\pi^{\prime}) where

mβ€²=Β Β Β Β E~3​(m,Ο€21)βŠ•E21​(m,Ο€21)Β Β Β Ο€3Β Β Β Β Β Β Β Β Β m^{\prime}={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 54.52208pt\hbox{{\hbox{\kern-54.52208pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{{\tilde{E}}_{3}(m,\pi_{21})\oplus E_{21}(m,\pi_{21})}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-7.28957pt\raise 19.54272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\pi_{3}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 34.14313pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}}
=(Β Β Β Β E3​(m)βŠ•E2​(m)βŠ•E1​(m)Β Β Β Ο€31Β Β Β Β Β Β Β Β Ο€32Β Β Β Β Β Β Β Β Ο€21Β Β Β Β Β Β Β Β Β ,Β Β Β Β E2​E3​(m)βŠ•E22​(m)βŠ•E2​E1​(m)Β Β Β E1​E3​(m)βŠ•E1​E2​(m)βŠ•E12​(m)Β Β Β Β Οƒ31∘E3​π21βˆ˜Οƒ23Β Β Β Β Β Β Β Β Β Β Οƒ21∘E2​π21βˆ˜Ο„2Β Β Β Β Β Β Β Β Β Β Ο„1∘E1​π21βˆ˜Οƒ21Β Β Β Β Β Β Β Β Β Β Οƒ21Β Β Β Β Β Β Β Β Β Β )=({\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 55.72571pt\hbox{{\hbox{\kern-55.72571pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{E_{3}(m)\oplus E_{2}(m)\oplus E_{1}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-8.99098pt\raise 37.54272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\pi_{31}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 48.36943pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-37.27293pt\raise 19.54272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\ \ \pi_{32}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern-2.84526pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern 13.7711pt\raise 19.54272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\pi_{21}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 45.52417pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}},{\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 117.11926pt\hbox{{\hbox{\kern-68.17015pt\raise 28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{2}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{2}E_{1}(m)}$}}}}}{\hbox{\kern-68.17015pt\raise-28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{1}E_{3}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-117.11926pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\sigma_{31}\circ E_{3}\pi_{21}\circ\sigma_{23}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-56.90521pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-53.53183pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\sigma_{21}\circ E_{2}\pi_{21}\circ\tau_{2}\!\!}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 0.0pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 56.90521pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\tau_{1}\circ 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Ο€β€²:Β Β Β Β E~32​(m,Ο€21)βŠ•E~3​E21​(m,Ο€21)Β Β Β E21​E~3​(m,Ο€21)βŠ•E212​(m,Ο€21)Β Β Β Β Οƒ21,3βˆ’1∘E~3​π3βˆ˜Ο„3Β Β Β Β Β Β Β Β Β Β Ο„E21∘E21​π3βˆ˜Οƒ21,3βˆ’1Β Β Β Β Β Β Β Β Β Β Οƒ21,3βˆ’1Β Β Β Β Β Β Β Β Β Β \pi^{\prime}:{\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 99.85797pt\hbox{{\hbox{\kern-58.43185pt\raise 28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{{\tilde{E}}_{3}^{2}(m,\pi_{21})\oplus{\tilde{E}}_{3}E_{21}(m,\pi_{21})}$}}}}}{\hbox{\kern-62.73737pt\raise-28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{21}{\tilde{E}}_{3}(m,\pi_{21})\oplus E_{21}^{2}(m,\pi_{21})}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-99.85797pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-2.62502pt\hbox{$\scriptstyle{\sigma_{21,3}^{-1}\circ{\tilde{E}}_{3}\pi_{3}\circ\tau_{3}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-42.67891pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 42.67891pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.86725pt\hbox{$\scriptstyle{\tau_{E_{21}}\circ E_{21}\pi_{3}\circ\sigma_{21,3}^{-1}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 42.67891pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-17.97343pt\raise 7.10612pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-2.13391pt\hbox{$\scriptstyle{\sigma_{21,3}^{-1}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-36.98839pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces}}}}}
=Β Β Β Β E32​(m)βŠ•E3​E2​(m)βŠ•E3​E1​(m)Β Β Β E2​E3​(m)βŠ•E1​E3​(m)βŠ•E22​(m)βŠ•E2​E1​(m)βŠ•E1​E2​(m)βŠ•E12​(m)Β Β Β Οƒ32∘E3​π32βˆ˜Ο„3Β Β Β Β Β Β Β Β Οƒ31∘E3​π31βˆ˜Ο„3Β Β Β Β Β Β Β Β Οƒ32Β Β Β Β Β Β Β Β Β Ο„2∘E2​π32βˆ˜Οƒ32Β Β Β Β Β Β Β Β Β Β Οƒ12∘E1​π32βˆ˜Οƒ31Β Β Β Β Β Β Β Β Β Β Οƒ31Β Β Β Β Β Β Β Β Β Β Ο„1∘E1​π21βˆ˜Οƒ31Β Β Β Β Β Β Β Β Β Β ={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 161.73352pt\hbox{{\hbox{\kern-68.17015pt\raise 42.67891pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{3}^{2}(m)\oplus E_{3}E_{2}(m)\oplus E_{3}E_{1}(m)}$}}}}}{\hbox{\kern-142.45137pt\raise-42.67891pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{2}E_{3}(m)\oplus E_{1}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{2}E_{1}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 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0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 36.41922pt\raise-8.54361pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\!\!\sigma_{12}\circ E_{1}\pi_{32}\circ\sigma_{31}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 28.4526pt\raise-34.14313pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 16.79288pt\raise 15.47916pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\!\!\sigma_{31}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-71.13152pt\raise-34.14313pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 91.83302pt\raise 5.89168pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\tau_{1}\circ E_{1}\pi_{21}\circ\sigma_{31}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 142.26303pt\raise-34.14313pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces}}}}}

Via the isomorphism of categories above, this corresponds to the functor EE on Ξ”123​(𝒲)\Delta_{123}({\mathcal{W}}).

The endomorphism Ο„\tau of E2​((m,Ο€21),Ο€3)E^{2}((m,\pi_{21}),\pi_{3}) is

E~32​(m,Ο€21)βŠ•E~3​E21​(m,Ο€21)βŠ•E21​E~3​(m,Ο€21)βŠ•E212​(m,Ο€21)\textstyle{{\tilde{E}}_{3}^{2}(m,\pi_{21})\oplus{\tilde{E}}_{3}E_{21}(m,\pi_{21})\oplus E_{21}{\tilde{E}}_{3}(m,\pi_{21})\oplus E_{21}^{2}(m,\pi_{21})}E~32​(m,Ο€21)βŠ•E~3​E21​(m,Ο€21)βŠ•E21​E~3​(m,Ο€21)βŠ•E212​(m,Ο€21)\textstyle{{\tilde{E}}_{3}^{2}(m,\pi_{21})\oplus{\tilde{E}}_{3}E_{21}(m,\pi_{21})\oplus E_{21}{\tilde{E}}_{3}(m,\pi_{21})\oplus E_{21}^{2}(m,\pi_{21})}Ο„3\scriptstyle{\tau_{3}}Ο„E21\scriptstyle{\tau_{E_{21}}}Οƒ21,3\scriptstyle{\sigma_{21,3}}
=Β Β Β Β E32​(m)βŠ•E3​E2​(m)βŠ•E3​E1​(m)βŠ•E2​E3​(m)βŠ•E1​E3​(m)βŠ•E22​(m)βŠ•E2​E1​(m)βŠ•E1​E2​(m)βŠ•E12​(m)Β Β Β E32​(m)βŠ•E3​E2​(m)βŠ•E3​E1​(m)βŠ•E2​E3​(m)βŠ•E1​E3​(m)βŠ•E22​(m)βŠ•E2​E1​(m)βŠ•E1​E2​(m)βŠ•E12​(m)Β Β Β Β Ο„3Β Β Β Β Β Β Β Β Β Β Οƒ23Β Β Β Β Β Β Β Β Β Β Οƒ13Β Β Β Β Β Β Β Β Β Β Ο„2Β Β Β Β Β Β Β Β Β Β Ο„1Β Β Β Β Β Β Β Β Β Β Οƒ12Β Β Β Β Β Β Β Β Β Β ={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 246.90207pt\hbox{{\hbox{\kern-216.73259pt\raise 28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{3}^{2}(m)\oplus E_{3}E_{2}(m)\oplus E_{3}E_{1}(m)\oplus E_{2}E_{3}(m)\oplus E_{1}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{2}E_{1}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}$}}}}}{\hbox{\kern-216.73259pt\raise-28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{3}^{2}(m)\oplus E_{3}E_{2}(m)\oplus E_{3}E_{1}(m)\oplus E_{2}E_{3}(m)\oplus E_{1}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{2}E_{1}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-246.90207pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\tau_{3}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-233.31137pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-131.60667pt\raise 5.00694pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\sigma_{23}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-176.40616pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-68.4296pt\raise-5.00694pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\sigma_{13}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-119.50095pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 46.15977pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\tau_{2}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 59.75047pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 224.77559pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\tau_{1}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 224.77559pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 121.31334pt\raise 5.00694pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\sigma_{12}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 108.1199pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces}}}}}

This coincides with the endomorphism Ο„\tau of the endofunctor E2E^{2} of Ξ”123​(𝒲)\Delta_{123}({\mathcal{W}}).

The category Δσ32,1​Δσ32​(𝒲)\Delta_{\sigma_{32,1}}\Delta_{\sigma_{32}}({\mathcal{W}}) has objects pairs ((m,Ο€32),Ο€1)((m,\pi_{32}),\pi_{1}) where mβˆˆπ’²m\in{\mathcal{W}}, Ο€32:E3​(m)β†’E2​(m)\pi_{32}:E_{3}(m)\to E_{2}(m) and Ο€1:E32​(m,Ο€32)β†’E~1​(m,Ο€32)\pi_{1}:E_{32}(m,\pi_{32})\to{\tilde{E}}_{1}(m,\pi_{32}) satisfy

d⁑(Ο€32)=d⁑(Ο€1)=0d(\pi_{32})=d(\pi_{1})=0

and the diagram (4.3.2) commutes for Ο€32\pi_{32} and for Ο€1\pi_{1}.

For i∈{2,3}i\in\{2,3\}, let Ο€i​1\pi_{i1} be the composition of the inclusion Ei​(m)β†’E32​(m)E_{i}(m)\to E_{32}(m) with Ο€1\pi_{1}. We have d⁑(Ο€21)=0d(\pi_{21})=0 and d⁑(Ο€31)=Ο€21βˆ˜Ο€32d(\pi_{31})=\pi_{21}\circ\pi_{32}.

As in the case of the category Δσ21,3βˆ’1​Δσ21​(𝒲)\Delta_{\sigma_{21,3}^{-1}}\Delta_{\sigma_{21}}({\mathcal{W}}), the objects of Δσ32,1​Δσ32​(𝒲)\Delta_{\sigma_{32,1}}\Delta_{\sigma_{32}}({\mathcal{W}}) can be described as quadruples (m,Ο€21,Ο€31,Ο€32)(m,\pi_{21},\pi_{31},\pi_{32}) where mβˆˆπ’²m\in{\mathcal{W}}, Ο€i​j:Ei​(m)β†’Ej​(m)\pi_{ij}:E_{i}(m)\to E_{j}(m) satisfy

d⁑(Ο€21)=d⁑(Ο€32)=0,d⁑(Ο€31)=Ο€21βˆ˜Ο€32,d(\pi_{21})=d(\pi_{32})=0,\ d(\pi_{31})=\pi_{21}\circ\pi_{32},

the composition

E3​E2​(m)β†’E3​π21E3​E1​(m)β†’Οƒ31E1​E3​(m)β†’E1​π32E1​E2​(m)β†’Οƒ12E2​E1​(m)E_{3}E_{2}(m)\xrightarrow{E_{3}\pi_{21}}E_{3}E_{1}(m)\xrightarrow{\sigma_{31}}E_{1}E_{3}(m)\xrightarrow{E_{1}\pi_{32}}E_{1}E_{2}(m)\xrightarrow{\sigma_{12}}E_{2}E_{1}(m)

is equal to the sum of the following two maps

E3​E2​(m)β†’Οƒ32E2​E3​(m)β†’E2​π32E22​(m)β†’Ο„2E22​(m)β†’E2​π21E2​E1​(m)E_{3}E_{2}(m)\xrightarrow{\sigma_{32}}E_{2}E_{3}(m)\xrightarrow{E_{2}\pi_{32}}E_{2}^{2}(m)\xrightarrow{\tau_{2}}E_{2}^{2}(m)\xrightarrow{E_{2}\pi_{21}}E_{2}E_{1}(m)

and

E3​E2​(m)β†’Οƒ32E2​E3​(m)β†’E2​π31E2​E1​(m),E_{3}E_{2}(m)\xrightarrow{\sigma_{32}}E_{2}E_{3}(m)\xrightarrow{E_{2}\pi_{31}}E_{2}E_{1}(m),

the following diagrams commute

E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„3\scriptstyle{\tau_{3}}E3​π31\scriptstyle{E_{3}\pi_{31}}E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}E3​E2​(m)\textstyle{E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ32\scriptstyle{\sigma_{32}}E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π31\scriptstyle{E_{2}\pi_{31}}E3​E1​(m)\textstyle{E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31\scriptstyle{\sigma_{31}}E1​E3​(m)\textstyle{E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π32\scriptstyle{E_{1}\pi_{32}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ12\scriptstyle{\sigma_{12}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)}
E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}Ο„3\scriptstyle{\tau_{3}}E3​E2​(m)\textstyle{E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ32\scriptstyle{\sigma_{32}}E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„2\scriptstyle{\tau_{2}}E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}E3​E2​(m)\textstyle{E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ32\scriptstyle{\sigma_{32}}E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π32\scriptstyle{E_{3}\pi_{32}}E22​(m)\textstyle{E_{2}^{2}(m)}
E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π31\scriptstyle{E_{3}\pi_{31}}Ο„3\scriptstyle{\tau_{3}}E3​E1​(m)\textstyle{E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31\scriptstyle{\sigma_{31}}E1​E3​(m)\textstyle{E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π31\scriptstyle{E_{3}\pi_{31}}E12​(m)\textstyle{E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„1\scriptstyle{\tau_{1}}E32​(m)\textstyle{E_{3}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π31\scriptstyle{E_{3}\pi_{31}}E3​E1​(m)\textstyle{E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31\scriptstyle{\sigma_{31}}E1​E3​(m)\textstyle{E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π31\scriptstyle{E_{3}\pi_{31}}E12​(m)\textstyle{E_{1}^{2}(m)}
E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π21\scriptstyle{E_{2}\pi_{21}}Ο„2\scriptstyle{\tau_{2}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21\scriptstyle{\sigma_{21}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π21\scriptstyle{E_{1}\pi_{21}}E12​(m)\textstyle{E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„1\scriptstyle{\tau_{1}}E22​(m)\textstyle{E_{2}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π21\scriptstyle{E_{2}\pi_{21}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21\scriptstyle{\sigma_{21}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π21\scriptstyle{E_{1}\pi_{21}}E12​(m)\textstyle{E_{1}^{2}(m)}
E2​E3​(m)\textstyle{E_{2}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E2​π31\scriptstyle{E_{2}\pi_{31}}Οƒ23\scriptstyle{\sigma_{23}}E2​E1​(m)\textstyle{E_{2}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ21\scriptstyle{\sigma_{21}}E1​E2​(m)\textstyle{E_{1}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π21\scriptstyle{E_{1}\pi_{21}}E12​(m)\textstyle{E_{1}^{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο„1\scriptstyle{\tau_{1}}E3​E2​(m)\textstyle{E_{3}E_{2}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E3​π21\scriptstyle{E_{3}\pi_{21}}E3​E1​(m)\textstyle{E_{3}E_{1}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒ31\scriptstyle{\sigma_{31}}E1​E3​(m)\textstyle{E_{1}E_{3}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}E1​π31\scriptstyle{E_{1}\pi_{31}}E12​(m)\textstyle{E_{1}^{2}(m)}

and the following composition vanishes:

E3​E2​(m)β†’E3​π21E3​E1​(m)β†’Οƒ31E1​E3​(m)β†’E1​π31E12​(m)β†’Ο„1E12​(m).E_{3}E_{2}(m)\xrightarrow{E_{3}\pi_{21}}E_{3}E_{1}(m)\xrightarrow{\sigma_{31}}E_{1}E_{3}(m)\xrightarrow{E_{1}\pi_{31}}E_{1}^{2}(m)\xrightarrow{\tau_{1}}E_{1}^{2}(m).

The vanishing of that composition follows from the commutativity of the diagram immediately above.

This description of objects provides an isomorphism of categories Δσ32,1​Δσ32​(𝒲)β†’βˆΌΞ”123​(𝒲)\Delta_{\sigma_{32,1}}\Delta_{\sigma_{32}}({\mathcal{W}})\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}\Delta_{123}({\mathcal{W}}).

Let us now describe the action of EE on Δσ32,1​Δσ32​(𝒲)\Delta_{\sigma_{32,1}}\Delta_{\sigma_{32}}({\mathcal{W}}).

We have E⁑((m,Ο€32),Ο€1)=(mβ€²,Ο€β€²)E((m,\pi_{32}),\pi_{1})=(m^{\prime},\pi^{\prime}) where

mβ€²=Β Β Β Β E32​(m,Ο€32)βŠ•E~1​(m,Ο€32)Β Β Β Ο€1Β Β Β Β Β Β Β Β Β m^{\prime}={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 53.411pt\hbox{{\hbox{\kern-53.411pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{E_{32}(m,\pi_{32})\oplus{\tilde{E}}_{1}(m,\pi_{32})}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-7.28957pt\raise 19.54272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\pi_{1}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 34.14313pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}}
=(Β Β Β Β E3​(m)βŠ•E2​(m)βŠ•E1​(m)Β Β Β Ο€31Β Β Β Β Β Β Β Β Ο€32Β Β Β Β Β Β Β Β Ο€21Β Β Β Β Β Β Β Β Β ,Β Β Β Β E32​(m)βŠ•E3​E2​(m)βŠ•E3​E1​(m)Β Β Β E2​E3​(m)βŠ•E22​(m)βŠ•E2​E1​(m)Β Β Β Β Οƒ32∘E3​π32βˆ˜Ο„3Β Β Β Β Β Β Β Β Β Β Ο„2∘E2​π32βˆ˜Οƒ32Β Β Β Β Β Β Β Β Β Β Οƒ12∘E1​π32βˆ˜Οƒ31Β Β Β Β Β Β Β Β Β Β Οƒ32Β Β Β Β Β Β Β Β Β Β )=({\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 55.72571pt\hbox{{\hbox{\kern-55.72571pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{E_{3}(m)\oplus E_{2}(m)\oplus E_{1}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-8.99098pt\raise 37.54272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\pi_{31}}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 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0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\!\!\tau_{2}\circ E_{2}\pi_{32}\circ\sigma_{32}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 0.0pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 56.90521pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.89168pt\hbox{$\scriptstyle{\sigma_{12}\circ 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Ο€β€²:Β Β Β Β E322​(m,Ο€32)βŠ•E32​E~1​(m,Ο€32)Β Β Β E~1​E32​(m,Ο€32)βŠ•E~12​(m,Ο€32)Β Β Β Β Οƒ32,1∘E32​π1βˆ˜Ο„E32Β Β Β Β Β Β Β Β Β Β Ο„1∘E~1​π1βˆ˜Οƒ32,1Β Β Β Β Β Β Β Β Β Β Οƒ32,1Β Β Β Β Β Β Β Β Β Β \pi^{\prime}:{\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 113.15536pt\hbox{{\hbox{\kern-62.73737pt\raise 28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{32}^{2}(m,\pi_{32})\oplus E_{32}{\tilde{E}}_{1}(m,\pi_{32})}$}}}}}{\hbox{\kern-58.43185pt\raise-28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{{\tilde{E}}_{1}E_{32}(m,\pi_{32})\oplus{\tilde{E}}_{1}^{2}(m,\pi_{32})}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-113.15536pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.1389pt\hbox{$\scriptstyle{\sigma_{32,1}\circ E_{32}\pi_{1}\circ\tau_{E_{32}}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-42.67891pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 42.67891pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-2.62502pt\hbox{$\scriptstyle{\tau_{1}\circ{\tilde{E}}_{1}\pi_{1}\circ\sigma_{32,1}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 42.67891pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-17.97343pt\raise 5.49306pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-0.52084pt\hbox{$\scriptstyle{\sigma_{32,1}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-36.98839pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces}}}}}
=Β Β Β Β E32​(m)βŠ•E3​E2​(m)βŠ•E2​E3​(m)βŠ•E22​(m)βŠ•E3​E1​(m)βŠ•E2​E1​(m)Β Β Β E1​E3​(m)βŠ•E1​E2​(m)βŠ•E12​(m)Β Β Β Οƒ31∘E3​π31βˆ˜Ο„3Β Β Β Β Β Β Β Β Β Οƒ31Β Β Β Β Β Β Β Β Β Ο„1∘E1​π31βˆ˜Οƒ31Β Β Β Β Β Β Β Β Οƒ31∘E3​π21βˆ˜Οƒ23Β Β Β Β Β Β Β Β Β Οƒ21∘E2​π21βˆ˜Ο„2Β Β Β Β Β Β Β Β Β Οƒ21Β Β Β Β Β Β Β Β Ο„1∘E1​π31βˆ˜Οƒ21Β Β Β Β Β Β Β Β Β ={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 161.73352pt\hbox{{\hbox{\kern-142.45137pt\raise 42.67891pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{3}^{2}(m)\oplus E_{3}E_{2}(m)\oplus E_{2}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{3}E_{1}(m)\oplus E_{2}E_{1}(m)}$}}}}}{\hbox{\kern-68.17015pt\raise-42.67891pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{1}E_{3}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 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Via the isomorphism of categories above, this corresponds to the functor EE on Ξ”123​(𝒲)\Delta_{123}({\mathcal{W}}).

The endomorphism Ο„\tau of E2​((m,Ο€32),Ο€1)E^{2}((m,\pi_{32}),\pi_{1}) is

E322​(m,Ο€32)βŠ•E32​E~1​(m,Ο€32)βŠ•E~1​E32​(m,Ο€32)βŠ•E~12​(m,Ο€32)\textstyle{E_{32}^{2}(m,\pi_{32})\oplus E_{32}{\tilde{E}}_{1}(m,\pi_{32})\oplus{\tilde{E}}_{1}E_{32}(m,\pi_{32})\oplus{\tilde{E}}_{1}^{2}(m,\pi_{32})}E322​(m,Ο€32)βŠ•E32​E~1​(m,Ο€32)βŠ•E~1​E32​(m,Ο€32)βŠ•E~12​(m,Ο€32)\textstyle{E_{32}^{2}(m,\pi_{32})\oplus E_{32}{\tilde{E}}_{1}(m,\pi_{32})\oplus{\tilde{E}}_{1}E_{32}(m,\pi_{32})\oplus{\tilde{E}}_{1}^{2}(m,\pi_{32})}Ο„E32\scriptstyle{\tau_{E_{32}}}Ο„1\scriptstyle{\tau_{1}}Οƒ32,1βˆ’1\scriptstyle{\sigma_{32,1}^{-1}}
=Β Β Β Β E32​(m)βŠ•E3​E2​(m)βŠ•E2​E3​(m)βŠ•E22​(m)βŠ•E3​E1​(m)βŠ•E2​E1​(m)βŠ•E1​E3​(m)βŠ•E1​E2​(m)βŠ•E12​(m)Β Β Β E32​(m)βŠ•E3​E2​(m)βŠ•E2​E3​(m)βŠ•E22​(m)βŠ•E3​E1​(m)βŠ•E2​E1​(m)βŠ•E1​E3​(m)βŠ•E1​E2​(m)βŠ•E12​(m)Β Β Β Β Ο„3Β Β Β Β Β Β Β Β Β Β Οƒ23Β Β Β Β Β Β Β Β Β Β Οƒ13Β Β Β Β Β Β Β Β Β Β Ο„2Β Β Β Β Β Β Β Β Β Β Ο„1Β Β Β Β Β Β Β Β Β Β Οƒ12Β Β Β Β Β Β Β Β Β Β ={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 246.90207pt\hbox{{\hbox{\kern-216.73259pt\raise 28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{3}^{2}(m)\oplus E_{3}E_{2}(m)\oplus E_{2}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{3}E_{1}(m)\oplus E_{2}E_{1}(m)\oplus E_{1}E_{3}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}$}}}}}{\hbox{\kern-216.73259pt\raise-28.4526pt\hbox{\hbox{\kern 0.0pt\raise-2.82002pt\hbox{$\textstyle{E_{3}^{2}(m)\oplus E_{3}E_{2}(m)\oplus E_{2}E_{3}(m)\oplus E_{2}^{2}(m)\oplus E_{3}E_{1}(m)\oplus E_{2}E_{1}(m)\oplus E_{1}E_{3}(m)\oplus E_{1}E_{2}(m)\oplus E_{1}^{2}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-246.90207pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\tau_{3}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-233.31137pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-163.21272pt\raise 5.00694pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\sigma_{23}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-176.40616pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 39.10896pt\raise 5.00694pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\sigma_{13}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-5.69052pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern-76.18643pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\tau_{2}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern-62.59573pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 224.77559pt\raise 0.0pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\tau_{1}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 224.77559pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces{}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 96.01418pt\raise 5.00694pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.00694pt\hbox{$\scriptstyle{\sigma_{12}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 51.21469pt\raise-19.91682pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces{\hbox{\lx@xy@drawline@}}\ignorespaces}}}}}

This coincides with the endomorphism Ο„\tau of the endofunctor E2E^{2} of Ξ”123​(𝒲)\Delta_{123}({\mathcal{W}}). ∎

4.4. Dual diagonal action

4.4.1. Category

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 𝒲{\mathcal{W}} and a closed morphism of functors Ξ»:F1​E2β†’E2​F1\lambda:F_{1}E_{2}\to E_{2}F_{1} such that diagrams (4.2.1) commute. As in Β§4.2.1, we have maps ΞΌi,j=ΞΌ(i,i),(j,j):E2i​F1i​E2j​F1jβ†’E2i+j​F1i+j\mu_{i,j}=\mu_{(i,i),(j,j)}:E_{2}^{i}F_{1}^{i}E_{2}^{j}F_{1}^{j}\to E_{2}^{i+j}F_{1}^{i+j}.

We define a differential category Δλ​𝒲\Delta_{\lambda}{\mathcal{W}}. Its objects are pairs (m,Ο‚)(m,\varsigma) where mβˆˆπ’²Β―im\in\overline{{\mathcal{W}}}^{i} and Ο‚=(Ο‚i)iβ‰₯1\varsigma=(\varsigma_{i})_{i\geq 1}, Ο‚i∈Z​Hom𝒲¯i⁑(E2i​F1i​(m),m)\varsigma_{i}\in Z\operatorname{Hom}\nolimits_{\overline{{\mathcal{W}}}^{i}}(E_{2}^{i}F_{1}^{i}(m),m), satisfies that

  • β€’

    for all i,jβ‰₯1i,j\geq 1, we have Ο‚i∘E2i​F1i​ςj=Ο‚i+j∘μi,j\varsigma_{i}\circ E_{2}^{i}F_{1}^{i}\varsigma_{j}=\varsigma_{i+j}\circ\mu_{i,j}

  • β€’

    Ο‚i∘Tr​F1i=Ο‚i∘E2i​Tr\varsigma_{i}\circ T_{r}F_{1}^{i}=\varsigma_{i}\circ E_{2}^{i}T_{r} for all 1≀r<i1\leq r<i.

We define HomΔλ​𝒲⁑((m,Ο‚),(mβ€²,Ο‚β€²))\operatorname{Hom}\nolimits_{\Delta_{\lambda}{\mathcal{W}}}((m,\varsigma),(m^{\prime},\varsigma^{\prime})) to be the differential submodule of Hom𝒲¯i⁑(m,mβ€²)\operatorname{Hom}\nolimits_{\overline{{\mathcal{W}}}^{i}}(m,m^{\prime}) of elements ff such that for all iβ‰₯1i\geq 1, the following diagram commutes

E2i​F1i​(m)\textstyle{E_{2}^{i}F_{1}^{i}(m)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο‚i\scriptstyle{\varsigma_{i}}E2i​F1i​f\scriptstyle{E_{2}^{i}F_{1}^{i}f}m\textstyle{m\ignorespaces\ignorespaces\ignorespaces\ignorespaces}f\scriptstyle{f}E2i​F1i​(mβ€²)\textstyle{E_{2}^{i}F_{1}^{i}(m^{\prime})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο‚iβ€²\scriptstyle{\varsigma^{\prime}_{i}}mβ€²\textstyle{m^{\prime}}

The composition of maps is defined to be that of 𝒲¯i\overline{{\mathcal{W}}}^{i}.

0P65

Remark 4.4.1. The structure of objects in Δλ​𝒲\Delta_{\lambda}{\mathcal{W}} can be described graphically as follows:

[Uncaptioned image]
0P66

Remark 4.4.2. The maps ΞΌi,j\mu_{i,j} make A=⨁iβ‰₯0E2i​F1iA=\bigoplus_{i\geq 0}E_{2}^{i}F_{1}^{i} into a monoid in the monoidal category of endofunctors of 𝒲¯i\overline{{\mathcal{W}}}^{i}, when 𝒲¯i\overline{{\mathcal{W}}}^{i} has enough direct sums. If 𝒲¯i\overline{{\mathcal{W}}}^{i} has enough colimits, we have an induced monoid AΒ―=⨁iβ‰₯0(E2i​F1i)βŠ—HiβŠ—HioppHi\bar{A}=\bigoplus_{i\geq 0}(E_{2}^{i}F_{1}^{i})\otimes_{H_{i}\otimes H_{i}^{\operatorname{opp}\nolimits}}H_{i}. Now, the category Δλ​𝒲\Delta_{\lambda}{\mathcal{W}} is the category of AΒ―\bar{A}-modules in 𝒲¯i\overline{{\mathcal{W}}}^{i}.

0P67

Remark 4.4.3. Let us define a lax bi-22-representation Ei,j=E2j​F1iE_{i,j}=E_{2}^{j}F_{1}^{i} on 𝒲{\mathcal{W}} as deduced from the one defined in Β§4.2.1 by applying the swap automorphism of 𝒰×𝒰{\mathcal{U}}\times{\mathcal{U}} (cf Remark 4.2.3).

There is a faithful differential functor Δλ​𝒲→ΔE​𝒲,(m,Ο‚)↦(m,Ο‚1)\Delta_{\lambda}{\mathcal{W}}\to\Delta_{E}{\mathcal{W}},\ (m,\varsigma)\mapsto(m,\varsigma_{1}).

4.4.2. Adjoint

We assume F1F_{1} has a right adjoint E1E_{1} and denote by Ξ΅1\varepsilon_{1} and Ξ·1\eta_{1} the counit and unit of the adjunction. We denote by Ο„1\tau_{1} the endomorphism of E12E_{1}^{2} corresponding by adjunction to the endomorphism Ο„1\tau_{1} of F12F_{1}^{2}. The pair (E1,Ο„1)(E_{1},\tau_{1}) provides an action of 𝒰{\mathcal{U}} on 𝒲{\mathcal{W}}.

0P68

Remark 4.4.4. The maps Ξ·1\eta_{1}, Ξ΅1\varepsilon_{1}, the relations they satisfy, and Ξ»\lambda, Οƒ\sigma and ρ\rho are described graphically as:

[Uncaptioned image]

We denote by Οƒ\sigma the composition

(4.4.1) Οƒ:E2​E1β†’Ξ·1​E2​E1E1​F1​E2​E1β†’E1​λ​E2E1​E2​F1​E1β†’E1​E2​Ρ1E1​E2\sigma:E_{2}E_{1}\xrightarrow{\eta_{1}E_{2}E_{1}}E_{1}F_{1}E_{2}E_{1}\xrightarrow{E_{1}\lambda E_{2}}E_{1}E_{2}F_{1}E_{1}\xrightarrow{E_{1}E_{2}\varepsilon_{1}}E_{1}E_{2}

and by ρ\rho the composition

(4.4.2) ρ:F1​E1β†’F1​E1​η1F1​E12​F1β†’F1​τ1​F1F1​E12​F1β†’Ξ΅1​E1​F1E1​F1.\rho:F_{1}E_{1}\xrightarrow{F_{1}E_{1}\eta_{1}}F_{1}E_{1}^{2}F_{1}\xrightarrow{F_{1}\tau_{1}F_{1}}F_{1}E_{1}^{2}F_{1}\xrightarrow{\varepsilon_{1}E_{1}F_{1}}E_{1}F_{1}.

The diagram (4.3.1) is commutative.

0P69

Lemma 4.4.5. We have

E1β€‹Ξ»βˆ˜Οβ€‹E2∘F1​σ=σ​F1∘E2β€‹Οβˆ˜Ξ»β€‹E1​ and ​ρ​F1∘F1β€‹Οβˆ˜Ο„1​E1=E1​τ1βˆ˜Οβ€‹F1∘F1​ρ.E_{1}\lambda\circ\rho E_{2}\circ F_{1}\sigma=\sigma F_{1}\circ E_{2}\rho\circ\lambda E_{1}\text{ and }\rho F_{1}\circ F_{1}\rho\circ\tau_{1}E_{1}=E_{1}\tau_{1}\circ\rho F_{1}\circ F_{1}\rho.
0P6A

Proof. We have

E1β€‹Ξ»βˆ˜Οβ€‹E2∘F1​σ=E_{1}\lambda\circ\rho E_{2}\circ F_{1}\sigma=
=E1​E2​F1​Ρ1∘E1​λ​F1​E1∘F1​E12​F1​λ​E1∘F1​τ1​F12​E2​E1∘F1​E1​η1​F1​E2​E1∘F1​η1​E2​E2\displaystyle=E_{1}E_{2}F_{1}\varepsilon_{1}\circ E_{1}\lambda F_{1}E_{1}\circ F_{1}E_{1}^{2}F_{1}\lambda E_{1}\circ F_{1}\tau_{1}F_{1}^{2}E_{2}E_{1}\circ F_{1}E_{1}\eta_{1}F_{1}E_{2}E_{1}\circ F_{1}\eta_{1}E_{2}E_{2}
=E1​E2​F1​Ρ1∘E1​λ​F1​E1∘F1​E12​F1​λ​E1∘F1​E12​τ1​E2​E1∘F1​E1​η1​F1​E2​E1∘F1​η1​E2​E2\displaystyle=E_{1}E_{2}F_{1}\varepsilon_{1}\circ E_{1}\lambda F_{1}E_{1}\circ F_{1}E_{1}^{2}F_{1}\lambda E_{1}\circ F_{1}E_{1}^{2}\tau_{1}E_{2}E_{1}\circ F_{1}E_{1}\eta_{1}F_{1}E_{2}E_{1}\circ F_{1}\eta_{1}E_{2}E_{2}
=E1​E2​F1​Ρ1∘E1​λ​F1​E1∘E1​F1​λ​E1∘E1​τ1​E2​E1∘η1​F1​E2​E1∘Ρ1​F1​E2​E1∘F1​η1​E2​E2\displaystyle=E_{1}E_{2}F_{1}\varepsilon_{1}\circ E_{1}\lambda F_{1}E_{1}\circ E_{1}F_{1}\lambda E_{1}\circ E_{1}\tau_{1}E_{2}E_{1}\circ\eta_{1}F_{1}E_{2}E_{1}\circ\varepsilon_{1}F_{1}E_{2}E_{1}\circ F_{1}\eta_{1}E_{2}E_{2}
=E1​E2​F1​Ρ1∘E1​λ​F1​E1∘E1​F1​λ​E1∘E1​τ1​E2​E1∘η1​F1​E2​E1\displaystyle=E_{1}E_{2}F_{1}\varepsilon_{1}\circ E_{1}\lambda F_{1}E_{1}\circ E_{1}F_{1}\lambda E_{1}\circ E_{1}\tau_{1}E_{2}E_{1}\circ\eta_{1}F_{1}E_{2}E_{1}
=E1​E2​F1​Ρ1∘E1​E2​τ1​E1∘E1​λ​F1​E1∘E1​F1​λ​E1∘η1​F1​E2​E1\displaystyle=E_{1}E_{2}F_{1}\varepsilon_{1}\circ E_{1}E_{2}\tau_{1}E_{1}\circ E_{1}\lambda F_{1}E_{1}\circ E_{1}F_{1}\lambda E_{1}\circ\eta_{1}F_{1}E_{2}E_{1}
=E1​E2​F1​Ρ1∘E1​E2​F1​Ρ1​E1​F1∘E1​E2​F12​E1​η1∘E1​E2​τ1​E1∘E1​λ​F1​E1∘E1​F1​λ​E1∘η1​F1​E2​E1\displaystyle=E_{1}E_{2}F_{1}\varepsilon_{1}\circ E_{1}E_{2}F_{1}\varepsilon_{1}E_{1}F_{1}\circ E_{1}E_{2}F_{1}^{2}E_{1}\eta_{1}\circ E_{1}E_{2}\tau_{1}E_{1}\circ E_{1}\lambda F_{1}E_{1}\circ E_{1}F_{1}\lambda E_{1}\circ\eta_{1}F_{1}E_{2}E_{1}
=E1​E2​F1​Ρ1∘E1​E2​F1​Ρ1​E1​F1∘E1​E2​τ1​E12​F1∘E1​E2​F12​E1​η1∘E1​λ​F1​E1∘E1​F1​λ​E1∘η1​F1​E2​E1\displaystyle=E_{1}E_{2}F_{1}\varepsilon_{1}\circ E_{1}E_{2}F_{1}\varepsilon_{1}E_{1}F_{1}\circ E_{1}E_{2}\tau_{1}E_{1}^{2}F_{1}\circ E_{1}E_{2}F_{1}^{2}E_{1}\eta_{1}\circ E_{1}\lambda F_{1}E_{1}\circ E_{1}F_{1}\lambda E_{1}\circ\eta_{1}F_{1}E_{2}E_{1}
=E1​E2​F1​Ρ1∘E1​E2​F1​Ρ1​E1​F1∘E1​E2​F12​τ1​F1∘E1​E2​F12​E1​η1∘E1​λ​F1​E1∘E1​F1​λ​E1∘η1​F1​E2​E1\displaystyle=E_{1}E_{2}F_{1}\varepsilon_{1}\circ E_{1}E_{2}F_{1}\varepsilon_{1}E_{1}F_{1}\circ E_{1}E_{2}F_{1}^{2}\tau_{1}F_{1}\circ E_{1}E_{2}F_{1}^{2}E_{1}\eta_{1}\circ E_{1}\lambda F_{1}E_{1}\circ E_{1}F_{1}\lambda E_{1}\circ\eta_{1}F_{1}E_{2}E_{1}
=σ​F1∘E2β€‹Οβˆ˜Ξ»β€‹E1.\displaystyle=\sigma F_{1}\circ E_{2}\rho\circ\lambda E_{1}.

We have

ρ​F1∘F1β€‹Οβˆ˜Ο„1​E1\displaystyle\rho F_{1}\circ F_{1}\rho\circ\tau_{1}E_{1} =Ξ΅1​E1​F12∘F1​Ρ1​E12​F12βˆ˜Ο„1​E13​F12∘F12​E1​τ1​F12∘F12​E12​η1​F1∘F12​τ1​F1∘F12​E1​η1\displaystyle=\varepsilon_{1}E_{1}F_{1}^{2}\circ F_{1}\varepsilon_{1}E_{1}^{2}F_{1}^{2}\circ\tau_{1}E_{1}^{3}F_{1}^{2}\circ F_{1}^{2}E_{1}\tau_{1}F_{1}^{2}\circ F_{1}^{2}E_{1}^{2}\eta_{1}F_{1}\circ F_{1}^{2}\tau_{1}F_{1}\circ F_{1}^{2}E_{1}\eta_{1}
=Ξ΅1​E1​F12∘F1​Ρ1​E12​F12∘F12​τ1​E1​F12∘F12​E1​τ1​F12∘F12​E12​η1​F1∘F12​τ1​F1∘F12​E1​η1\displaystyle=\varepsilon_{1}E_{1}F_{1}^{2}\circ F_{1}\varepsilon_{1}E_{1}^{2}F_{1}^{2}\circ F_{1}^{2}\tau_{1}E_{1}F_{1}^{2}\circ F_{1}^{2}E_{1}\tau_{1}F_{1}^{2}\circ F_{1}^{2}E_{1}^{2}\eta_{1}F_{1}\circ F_{1}^{2}\tau_{1}F_{1}\circ F_{1}^{2}E_{1}\eta_{1}
=Ξ΅1​E1​F12∘F1​Ρ1​E12​F12∘F12​(Ο„1​E1∘E1​τ1βˆ˜Ο„1​E1)​F12∘F12​E12​η1​F1∘F12​E1​η1\displaystyle=\varepsilon_{1}E_{1}F_{1}^{2}\circ F_{1}\varepsilon_{1}E_{1}^{2}F_{1}^{2}\circ F_{1}^{2}(\tau_{1}E_{1}\circ E_{1}\tau_{1}\circ\tau_{1}E_{1})F_{1}^{2}\circ F_{1}^{2}E_{1}^{2}\eta_{1}F_{1}\circ F_{1}^{2}E_{1}\eta_{1}
=Ξ΅1​E1​F12∘F1​Ρ1​E12​F12∘F12​(E1​τ1βˆ˜Ο„1​E1∘E1​τ1)​F12∘F12​E12​η1​F1∘F12​E1​η1\displaystyle=\varepsilon_{1}E_{1}F_{1}^{2}\circ F_{1}\varepsilon_{1}E_{1}^{2}F_{1}^{2}\circ F_{1}^{2}(E_{1}\tau_{1}\circ\tau_{1}E_{1}\circ E_{1}\tau_{1})F_{1}^{2}\circ F_{1}^{2}E_{1}^{2}\eta_{1}F_{1}\circ F_{1}^{2}E_{1}\eta_{1}
=Ξ΅1​E1​F12∘F1​Ρ1​E12​F12∘F12​(E1​τ1βˆ˜Ο„1​E1)​F12∘F12​E13​τ1∘F12​E12​η1​F1∘F12​E1​η1\displaystyle=\varepsilon_{1}E_{1}F_{1}^{2}\circ F_{1}\varepsilon_{1}E_{1}^{2}F_{1}^{2}\circ F_{1}^{2}(E_{1}\tau_{1}\circ\tau_{1}E_{1})F_{1}^{2}\circ F_{1}^{2}E_{1}^{3}\tau_{1}\circ F_{1}^{2}E_{1}^{2}\eta_{1}F_{1}\circ F_{1}^{2}E_{1}\eta_{1}
=E1​τ1βˆ˜Οβ€‹F1∘F1​ρ.\displaystyle=E_{1}\tau_{1}\circ\rho F_{1}\circ F_{1}\rho.

∎

4.4.3. Relations

Let β„³{\mathcal{M}} be the strict monoidal pointed category generated by objects ala_{l} for 1≀l≀31\leq l\leq 3 and maps Ξ»l​m:al​amβ†’am​al\lambda_{lm}:a_{l}a_{m}\to a_{m}a_{l} for l≀ml\leq m with relations Ξ»l​l2=0\lambda_{ll}^{2}=0 and

Ξ»m​n​l∘m​λl​n∘λl​m​n=n​λl​m∘λl​n​m∘l​λm​n​ for ​l≀m≀n.\lambda_{mn}l\circ m\lambda_{ln}\circ\lambda_{lm}n=n\lambda_{lm}\circ\lambda_{ln}m\circ l\lambda_{mn}\text{ for }l\leq m\leq n.
0P6B

Lemma 4.4.6. We have a pointed faithful strict monoidal functor

H:β„³β†’π’°βˆ™,al↦e,Ξ»l​m↦τ.H:{\mathcal{M}}\to{\mathcal{U}}^{\bullet},\ a_{l}\mapsto e,\ \lambda_{lm}\mapsto\tau.

Given l1,…,lr,m1,…,mr∈{1,2,3}l_{1},\ldots,l_{r},m_{1},\ldots,m_{r}\in\{1,2,3\}, the non-zero elements of H(Homβ„³(al1β‹―alr,am1β‹―amr))βŠ‚Hrβˆ™H(\operatorname{Hom}\nolimits_{\mathcal{M}}(a_{l_{1}}\cdots a_{l_{r}},a_{m_{1}}\cdots a_{m_{r}}))\subset H_{r}^{\bullet} are those TwT_{w} with wβˆˆπ”–rw\in{\mathfrak{S}}_{r} such that for all i,j∈{1,…,r}i,j\in\{1,\ldots,r\} with i<ji<j and w⁑(i)>w⁑(j)w(i)>w(j), we have li≀ljl_{i}\leq l_{j}.

0P6C

Proof. Given the defining relations for π’°βˆ™{\mathcal{U}}^{\bullet}, the construction of the lemma does define (uniquely) a monoidal functor HH.

Fix l1,…,ln∈{1,…,3}l_{1},\ldots,l_{n}\in\{1,\ldots,3\}. Given i∈{1,…,nβˆ’1}i\in\{1,\ldots,n-1\} such that li≀li+1l_{i}\leq l_{i+1}, we put T~i=al1β‹―aliβˆ’1Ξ»li,li+1ali+2β‹―aln\tilde{T}_{i}=a_{l_{1}}\cdots a_{l_{i-1}}\lambda_{l_{i},l_{i+1}}a_{l_{i+2}}\cdots a_{l_{n}}. Note that T~i​T~i+1​T~i\tilde{T}_{i}\tilde{T}_{i+1}\tilde{T}_{i} is well-defined if and only if li≀li+1≀li+2l_{i}\leq l_{i+1}\leq l_{i+2}, hence if and only if T~i+1​T~i​T~i+1\tilde{T}_{i+1}\tilde{T}_{i}\tilde{T}_{i+1} is well-defined. As a consequence, given i1,…,ir,j1,…,js∈{1,…,nβˆ’1}i_{1},\ldots,i_{r},j_{1},\ldots,j_{s}\in\{1,\ldots,n-1\} such that T~i1β‹―T~ir\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r}} and T~j1β‹―T~js\tilde{T}_{j_{1}}\cdots\tilde{T}_{j_{s}} are well-defined and Ti1β‹―Tir=Tj1β‹―TjsT_{i_{1}}\cdots T_{i_{r}}=T_{j_{1}}\cdots T_{j_{s}}, then we have T~i1β‹―T~ir=T~j1β‹―T~js\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r}}=\tilde{T}_{j_{1}}\cdots\tilde{T}_{j_{s}}. This shows the faithfulness of HH.

Consider i1,…,iri_{1},\ldots,i_{r} such that T~i1β‹―T~ir\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r}} is well-defined and non-zero. Let w=si1β‹―sirβˆˆπ”–nw=s_{i_{1}}\cdots s_{i_{r}}\in{\mathfrak{S}}_{n}. We show by induction on rr that given (i,j)∈L~​(w)(i,j)\in\tilde{L}(w), we have li≀ljl_{i}\leq l_{j}.

Let wβ€²=si1β‹―sirβˆ’1w^{\prime}=s_{i_{1}}\cdots s_{i_{r-1}}. Put d=ird=i_{r} and wβ€²=w​sdw^{\prime}=ws_{d}. Since Ti1β‹―Tirβ‰ 0T_{i_{1}}\cdots T_{i_{r}}\neq 0, we have r=ℓ⁑(w)r=\ell(w). We have L~​(w)={(d,d+1)}β€‹βˆsd​(L~​(wβ€²))\tilde{L}(w)=\{(d,d+1)\}\coprod s_{d}(\tilde{L}(w^{\prime})) by Lemma 3.2.3. We have a well-defined map T~i1β‹―T~irβˆ’1\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r-1}} from al1β‹―aldβˆ’1ald+1aldald+2β‹―alna_{l_{1}}\cdots a_{l_{d-1}}a_{l_{d+1}}a_{l_{d}}a_{l_{d+2}}\cdots a_{l_{n}}. It follows by induction that given (i,j)∈L~​(wβ€²)(i,j)\in\tilde{L}(w^{\prime}), we have lsd​(i)≀lsd​(j)l_{s_{d}(i)}\leq l_{s_{d}(j)}. Since L~​(w)={(d,d+1)}β€‹βˆsd​(L~​(wβ€²))\tilde{L}(w)=\{(d,d+1)\}\coprod s_{d}(\tilde{L}(w^{\prime})) (Lemma 3.2.3), we deduce that li≀ljl_{i}\leq l_{j} for all (i,j)∈L~​(w)(i,j)\in\tilde{L}(w).

Consider now wβˆˆπ”–nw\in{\mathfrak{S}}_{n} such that given (i,j)∈L~​(w)(i,j)\in\tilde{L}(w), we have li≀ljl_{i}\leq l_{j}. Let w=si1β‹―sirw=s_{i_{1}}\cdots s_{i_{r}} be a reduced decomposition of ww. We show by induction on rr that T~i1β‹―T~ir\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r}} is well-defined. As before, we define dd and wβ€²w^{\prime}. By induction on rr, the element T~i1β‹―T~irβˆ’1\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r-1}} gives a well-defined map from al1β‹―aldβˆ’1ald+1aldald+2β‹―alna_{l_{1}}\cdots a_{l_{d-1}}a_{l_{d+1}}a_{l_{d}}a_{l_{d+2}}\cdots a_{l_{n}}. Since (d,d+1)∈L~​(w)(d,d+1)\in\tilde{L}(w), it follows that ld≀ld+1l_{d}\leq l_{d+1}, hence T~d\tilde{T}_{d} is a well-defined map from al1β‹―alna_{l_{1}}\cdots a_{l_{n}}. We deduce that T~i1β‹―T~ir\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r}}. This shows that TwT_{w} is in the image of HH. ∎

Given l1,…,lr,m1,…,mr∈{1,2,3}l_{1},\ldots,l_{r},m_{1},\ldots,m_{r}\in\{1,2,3\} and wβˆˆπ”–rw\in{\mathfrak{S}}_{r} satisfying the assumptions of Lemma 4.4.6, we put Ξ»w=Hβˆ’1​(Tw)\lambda_{w}=H^{-1}(T_{w}).

We denote by β„³β€²{\mathcal{M}}^{\prime} the strict monoidal kk-linear category obtained from k⁑[β„³]k[{\mathcal{M}}] by adding maps Ξ΅:a1​a3β†’1\varepsilon:a_{1}a_{3}\to 1 and Ξ·:1β†’a3​a1\eta:1\to a_{3}a_{1} and relations

a3β€‹Ξ΅βˆ˜Ξ·β€‹a3=id,Ρ​a1∘a1​η=ida_{3}\varepsilon\circ\eta a_{3}=\operatorname{id}\nolimits,\ \varepsilon a_{1}\circ a_{1}\eta=\operatorname{id}\nolimits
Ξ»23=a3​a2β€‹Ξ΅βˆ˜a3​λ12​a3βˆ˜Ξ·β€‹a2​a3,Ξ»13=Ρ​a3​a1∘a1​λ33​a1∘a1​a3​η\lambda_{23}=a_{3}a_{2}\varepsilon\circ a_{3}\lambda_{12}a_{3}\circ\eta a_{2}a_{3},\ \lambda_{13}=\varepsilon a_{3}a_{1}\circ a_{1}\lambda_{33}a_{1}\circ a_{1}a_{3}\eta
Ξ»11=Ρ​a12∘a1​Ρ​a3​a12∘a12​λ33​a12∘a12​a3​η​a1∘a12​η.\lambda_{11}=\varepsilon a_{1}^{2}\circ a_{1}\varepsilon a_{3}a_{1}^{2}\circ a_{1}^{2}\lambda_{33}a_{1}^{2}\circ a_{1}^{2}a_{3}\eta a_{1}\circ a_{1}^{2}\eta.

There is a monoidal duality, i.e. a monoidal equivalence β„³β€²oppβ†’βˆΌβ„³β€²{\mathcal{M}}^{\prime{\operatorname{opp}\nolimits}}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\mathcal{M}}^{\prime} given by

a1↦a3,a2↦a2,a3↦a1,Ξ»12↦λ23,Ξ»23↦λ12,Ξ»13↦λ13a_{1}\mapsto a_{3},\ a_{2}\mapsto a_{2},\ a_{3}\mapsto a_{1},\ \lambda_{12}\mapsto\lambda_{23},\ \lambda_{23}\mapsto\lambda_{12},\ \lambda_{13}\mapsto\lambda_{13}
Ξ»11↦λ33,Ξ»22↦λ22,Ξ»33↦λ11,Ρ↦η,η↦Ρ.\lambda_{11}\mapsto\lambda_{33},\ \lambda_{22}\mapsto\lambda_{22},\ \lambda_{33}\mapsto\lambda_{11},\ \varepsilon\mapsto\eta,\ \eta\mapsto\varepsilon.
0P6D

Lemma 4.4.7. Let G1,…,Gn∈{a1,a2,a3}G_{1},\ldots,G_{n}\in\{a_{1},a_{2},a_{3}\}. We have

Ξ»(1β‹―n+1)∘G1β‹―GnΞ·=Ξ»(n+2β‹―2)∘ηG1β‹―Gn:G1β‹―Gnβ†’a3G1β‹―Gna1\lambda_{(1\cdots n+1)}\circ G_{1}\cdots G_{n}\eta=\lambda_{(n+2\cdots 2)}\circ\eta G_{1}\cdots G_{n}:G_{1}\cdots G_{n}\to a_{3}G_{1}\cdots G_{n}a_{1}

and

Ξ΅G1β‹―Gn∘λ(2β‹―n+2)=G1β‹―GnΡ∘λ(n+1β‹―1):a1G1β‹―Gna3β†’G1β‹―Gn.\varepsilon G_{1}\cdots G_{n}\circ\lambda_{(2\cdots n+2)}=G_{1}\cdots G_{n}\varepsilon\circ\lambda_{(n+1\cdots 1)}:a_{1}G_{1}\cdots G_{n}a_{3}\to G_{1}\cdots G_{n}.
0P6E

Proof. We have

a3​λ13βˆ˜Ξ·β€‹a3\displaystyle a_{3}\lambda_{13}\circ\eta a_{3} =a3​Ρ​a3​a1∘a3​a1​λ33​a1∘a3​a1​a3β€‹Ξ·βˆ˜Ξ·β€‹a3\displaystyle=a_{3}\varepsilon a_{3}a_{1}\circ a_{3}a_{1}\lambda_{33}a_{1}\circ a_{3}a_{1}a_{3}\eta\circ\eta a_{3}
=a3​Ρ​a3​a1βˆ˜Ξ·β€‹a32​a1∘λ33​a1∘a3​η\displaystyle=a_{3}\varepsilon a_{3}a_{1}\circ\eta a_{3}^{2}a_{1}\circ\lambda_{33}a_{1}\circ a_{3}\eta
=Ξ»33​a1∘a3​η\displaystyle=\lambda_{33}a_{1}\circ a_{3}\eta
Ξ»13​a1∘a1​η\displaystyle\lambda_{13}a_{1}\circ a_{1}\eta =Ρ​a3​a12∘a1​λ33​a12∘a1​a3​η​a1∘a1​η\displaystyle=\varepsilon a_{3}a_{1}^{2}\circ a_{1}\lambda_{33}a_{1}^{2}\circ a_{1}a_{3}\eta a_{1}\circ a_{1}\eta
=Ρ​a3​a12∘a1​a32​λ11∘a1​a3​η​a1∘a1​η\displaystyle=\varepsilon a_{3}a_{1}^{2}\circ a_{1}a_{3}^{2}\lambda_{11}\circ a_{1}a_{3}\eta a_{1}\circ a_{1}\eta
=a3​λ11βˆ˜Ξ΅β€‹a3​a12∘a1​a3​η​a1∘a1​η\displaystyle=a_{3}\lambda_{11}\circ\varepsilon a_{3}a_{1}^{2}\circ a_{1}a_{3}\eta a_{1}\circ a_{1}\eta
=a3​λ11βˆ˜Ξ·β€‹a1βˆ˜Ξ΅β€‹a1∘a1​η\displaystyle=a_{3}\lambda_{11}\circ\eta a_{1}\circ\varepsilon a_{1}\circ a_{1}\eta
=a3​λ11βˆ˜Ξ·β€‹a1\displaystyle=a_{3}\lambda_{11}\circ\eta a_{1}
Ξ»23​a1∘a2​η\displaystyle\lambda_{23}a_{1}\circ a_{2}\eta =a3​a2​Ρ​a1∘a3​λ12​a3​a1βˆ˜Ξ·β€‹a2​a3​a1∘a2​η\displaystyle=a_{3}a_{2}\varepsilon a_{1}\circ a_{3}\lambda_{12}a_{3}a_{1}\circ\eta a_{2}a_{3}a_{1}\circ a_{2}\eta
=a3​a2​Ρ​a1∘a3​a2​a1β€‹Ξ·βˆ˜a3​λ12βˆ˜Ξ·β€‹a2\displaystyle=a_{3}a_{2}\varepsilon a_{1}\circ a_{3}a_{2}a_{1}\eta\circ a_{3}\lambda_{12}\circ\eta a_{2}
=a3​λ12βˆ˜Ξ·β€‹a2\displaystyle=a_{3}\lambda_{12}\circ\eta a_{2}

It follows that the first statement of the lemma holds when n=1n=1. Consider now nβ‰₯2n\geq 2. We prove the first statement of the lemma by induction on nn. We have

Ξ»(n+2β‹―2)∘ηG1β‹―Gn\displaystyle\lambda_{(n+2\cdots 2)}\circ\eta G_{1}\cdots G_{n} =Ξ»(n+2β‹―3)∘(Ξ»(23)∘ηG1)G2β‹―Gn\displaystyle=\lambda_{(n+2\cdots 3)}\circ(\lambda_{(23)}\circ\eta G_{1})G_{2}\cdots G_{n}
=Ξ»(n+2β‹―3)∘(Ξ»(12)∘G1Ξ·)G2β‹―Gn\displaystyle=\lambda_{(n+2\cdots 3)}\circ(\lambda_{(12)}\circ G_{1}\eta)G_{2}\cdots G_{n}
=Ξ»(12)∘G1(Ξ»(n+1β‹―2)∘ηG2β‹―Gn)\displaystyle=\lambda_{(12)}\circ G_{1}(\lambda_{(n+1\cdots 2)}\circ\eta G_{2}\cdots G_{n})
=Ξ»(12)∘G1(Ξ»(1β‹―n)∘G2β‹―GnΞ·)\displaystyle=\lambda_{(12)}\circ G_{1}(\lambda_{(1\cdots n)}\circ G_{2}\cdots G_{n}\eta)
=Ξ»(1β‹―n+1)∘G1β‹―GnΞ·\displaystyle=\lambda_{(1\cdots n+1)}\circ G_{1}\cdots G_{n}\eta

The second statement of the lemma follows by applying the duality of β„³β€²{\mathcal{M}}^{\prime}. ∎

Lemmas 4.4.5 and 4.4.6 show that there is a kk-linear monoidal functor R:ℳ′→𝒲R:{\mathcal{M}}^{\prime}\to{\mathcal{W}}

a1↦F1,a2↦E2,a3↦E1,Ξ»12↦λ,Ξ»23↦σ,Ξ»13↦ρ,Ξ»11↦τ1,Ξ»22↦τ2,Ξ»33↦τ1a_{1}\mapsto F_{1},\ a_{2}\mapsto E_{2},\ a_{3}\mapsto E_{1},\ \lambda_{12}\mapsto\lambda,\lambda_{23}\mapsto\sigma,\ \lambda_{13}\mapsto\rho,\ \lambda_{11}\mapsto\tau_{1},\ \lambda_{22}\mapsto\tau_{2},\ \lambda_{33}\mapsto\tau_{1}
η↦η1,Ρ↦Ρ1.\eta\mapsto\eta_{1},\ \varepsilon\mapsto\varepsilon_{1}.

Given l1,…,lr,m1,…,mr∈{1,2,3}l_{1},\ldots,l_{r},m_{1},\ldots,m_{r}\in\{1,2,3\} and wβˆˆπ”–rw\in{\mathfrak{S}}_{r} satisfying the assumptions of Lemma 4.4.6, we still denote by Ξ»w\lambda_{w} the element R⁑(Ξ»w)R(\lambda_{w}).

Lemma 4.4.7 has the following consequence.

0P6F

Lemma 4.4.8. Let G1,…,Gn∈{E1,E2,F1}G_{1},\ldots,G_{n}\in\{E_{1},E_{2},F_{1}\}. We have

Ξ»(1β‹―n+1)∘G1β‹―GnΞ·1=Ξ»(n+2β‹―2)∘η1G1β‹―Gn:G1β‹―Gnβ†’E1G1β‹―GnF1\lambda_{(1\cdots n+1)}\circ G_{1}\cdots G_{n}\eta_{1}=\lambda_{(n+2\cdots 2)}\circ\eta_{1}G_{1}\cdots G_{n}:G_{1}\cdots G_{n}\to E_{1}G_{1}\cdots G_{n}F_{1}

and

Ξ΅1G1β‹―Gn∘λ(2β‹―n+2)=G1β‹―GnΞ΅1∘λ(n+1β‹―1):F1G1β‹―GnE1β†’G1β‹―Gn.\varepsilon_{1}G_{1}\cdots G_{n}\circ\lambda_{(2\cdots n+2)}=G_{1}\cdots G_{n}\varepsilon_{1}\circ\lambda_{(n+1\cdots 1)}:F_{1}G_{1}\cdots G_{n}E_{1}\to G_{1}\cdots G_{n}.

4.4.4. 11-arrows

Let (m,Ο‚)βˆˆΞ”Ξ»β€‹π’²(m,\varsigma)\in\Delta_{\lambda}{\mathcal{W}}. Let Ο€=π⁑(Ο‚)\pi=\pi(\varsigma) be the composition

Ο€:E2​(m)β†’E2​η1E2​E1​F1​(m)→σ​F1E1​E2​F1​(m)β†’E1​ς1E1​(m).\pi:E_{2}(m)\xrightarrow{E_{2}\eta_{1}}E_{2}E_{1}F_{1}(m)\xrightarrow{\sigma F_{1}}E_{1}E_{2}F_{1}(m)\xrightarrow{E_{1}\varsigma_{1}}E_{1}(m).

Note that Ο€\pi is also equal to the composition

Ο€:E2​(m)β†’Ξ·1​E2E1​F1​E2​(m)β†’E1​λE1​E2​F1​(m)β†’E1​ς1E1​(m)\pi:E_{2}(m)\xrightarrow{\eta_{1}E_{2}}E_{1}F_{1}E_{2}(m)\xrightarrow{E_{1}\lambda}E_{1}E_{2}F_{1}(m)\xrightarrow{E_{1}\varsigma_{1}}E_{1}(m)

since E1​λ​E1​F1∘η1​E2​E1​F1∘E2​η1=E1​E2​F1​η1∘E1β€‹Ξ»βˆ˜Ξ·1​E2E_{1}\lambda E_{1}F_{1}\circ\eta_{1}E_{2}E_{1}F_{1}\circ E_{2}\eta_{1}=E_{1}E_{2}F_{1}\eta_{1}\circ E_{1}\lambda\circ\eta_{1}E_{2} and E1​E2​F1​η1∘E1​E2​F1​Ρ1=idE1​E2​F1E_{1}E_{2}F_{1}\eta_{1}\circ E_{1}E_{2}F_{1}\varepsilon_{1}=\operatorname{id}\nolimits_{E_{1}E_{2}F_{1}}.

The pair (m,Ο€)(m,\pi) defines an object of Δσ​𝒲\Delta_{\sigma}{\mathcal{W}}. We obtain a faithful differential functor Ξ“:Δλ​𝒲→Δσ​𝒲,(m,Ο‚)↦(m,Ο€)\Gamma:\Delta_{\lambda}{\mathcal{W}}\to\Delta_{\sigma}{\mathcal{W}},\ (m,\varsigma)\mapsto(m,\pi).

0P6G

Remark 4.4.9. The construction of Ο€\pi from Ο‚1\varsigma_{1} is illustrated below.

[Uncaptioned image]

We define now a differential functor E:Δλ​𝒲→Δλ​𝒲E:\Delta_{\lambda}{\mathcal{W}}\to\Delta_{\lambda}{\mathcal{W}}.

Let (m,Ο‚)βˆˆΞ”Ξ»β€‹π’²(m,\varsigma)\in\Delta_{\lambda}{\mathcal{W}}. Let mβ€²=Β Β Β Β E2​(m)βŠ•E1​(m)   π         m^{\prime}={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 35.11345pt\hbox{{\hbox{\kern-35.11345pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise-2.5pt\hbox{$\textstyle{E_{2}(m)\oplus E_{1}(m)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-6.76079pt\raise 19.04272pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.50694pt\hbox{$\scriptstyle{\pi}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 19.91682pt\raise 8.53578pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}} where Ο€=π⁑(Ο‚1)\pi=\pi(\varsigma_{1}). Given iβ‰₯1i\geq 1, we define

Ο‚iβ€²=(E2Ο‚i∘λ(1β‹―2i+1)βˆ‘r=1iE2Ο‚iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―r)(2iβ‹―i+r)0E1Ο‚i∘λ(1β‹―2i+1)):E2i​F1i​(mβ€²)β†’mβ€²\varsigma^{\prime}_{i}=\left(\begin{matrix}E_{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+1)}&\sum_{r=1}^{i}E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}\\ 0&E_{1}\varsigma_{i}\circ\lambda_{(1\cdots 2i+1)}\end{matrix}\right):E_{2}^{i}F_{1}^{i}(m^{\prime})\to m^{\prime}
0P6H

Lemma 4.4.10. (mβ€²,Ο‚β€²)(m^{\prime},\varsigma^{\prime}) is an object of Δλ​𝒲\Delta_{\lambda}{\mathcal{W}}.

0P6I

Proof. We have

d⁑((Ο‚iβ€²)11)\displaystyle d((\varsigma^{\prime}_{i})_{11}) =E2Ο‚i∘d(Ο„2E2iβˆ’1βˆ˜β‹―βˆ˜E2iβˆ’1Ο„2)F1i∘λ(i+1β‹―2i+1)\displaystyle=E_{2}\varsigma_{i}\circ d(\tau_{2}E_{2}^{i-1}\circ\cdots\circ E_{2}^{i-1}\tau_{2})F_{1}^{i}\circ\lambda_{(i+1\cdots 2i+1)}
=βˆ‘r=1iE2Ο‚i∘λ(1β‹―r)(r+1β‹―i+1)∘λ(i+1β‹―2i+1)\displaystyle=\sum_{r=1}^{i}E_{2}\varsigma_{i}\circ\lambda_{(1\cdots r)(r+1\cdots i+1)}\circ\lambda_{(i+1\cdots 2i+1)}
=βˆ‘r=1iE2Ο‚i∘λ(1β‹―r)(r+1β‹―i+1)∘λ(i+1β‹―2i+1)\displaystyle=\sum_{r=1}^{i}E_{2}\varsigma_{i}\circ\lambda_{(1\cdots r)(r+1\cdots i+1)}\circ\lambda_{(i+1\cdots 2i+1)}
=βˆ‘r=1iE2Ο‚i∘λ(1β‹―r)(2i+1β‹―i+r+1)∘λ(i+1β‹―2i+1)\displaystyle=\sum_{r=1}^{i}E_{2}\varsigma_{i}\circ\lambda_{(1\cdots r)(2i+1\cdots i+r+1)}\circ\lambda_{(i+1\cdots 2i+1)}
=E2Ο‚i∘λ(1β‹―i)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(1\cdots i)}
(Ο‚iβ€²)12∘E2i​F1i​π=(\varsigma^{\prime}_{i})_{12}\circ E_{2}^{i}F_{1}^{i}\pi=
=βˆ‘r=1iE2Ο‚iβˆ’1∘E2iF1iβˆ’1Ο‚1∘λ(2​i,2​i+1)∘E2iF1iβˆ’1Ξ΅1F1E2∘E2iF1iΞ·1E2∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varsigma_{1}\circ\lambda_{(2i,2i+1)}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}F_{1}E_{2}\circ E_{2}^{i}F_{1}^{i}\eta_{1}E_{2}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=βˆ‘r=1iE2Ο‚i∘λ(i+1β‹―2i)∘λ(2​i,2​i+1)∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{2}\varsigma_{i}\circ\lambda_{(i+1\cdots 2i)}\circ\lambda_{(2i,2i+1)}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=E2Ο‚i∘λ(1β‹―i)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(1\cdots i)}
=d⁑((Ο‚iβ€²)11).\displaystyle=d((\varsigma^{\prime}_{i})_{11}).
d⁑((Ο‚iβ€²)22)\displaystyle d((\varsigma^{\prime}_{i})_{22}) =E1Ο‚i∘λ(1β‹―i+1)∘E2id(ρF1iβˆ’1∘F1ρF1iβˆ’2βˆ˜β‹―βˆ˜F1iβˆ’1ρ)\displaystyle=E_{1}\varsigma_{i}\circ\lambda_{(1\cdots i+1)}\circ E_{2}^{i}d(\rho F_{1}^{i-1}\circ F_{1}\rho F_{1}^{i-2}\circ\cdots\circ F_{1}^{i-1}\rho)
=βˆ‘r=1iE1Ο‚i∘λ(1β‹―i+r)∘E2iF1rβˆ’1Ξ·1F1iβˆ’r∘E2iF1rβˆ’1Ξ΅1F1iβˆ’r∘λ(i+r+1β‹―2i+1)\displaystyle=\sum_{r=1}^{i}E_{1}\varsigma_{i}\circ\lambda_{(1\cdots i+r)}\circ E_{2}^{i}F_{1}^{r-1}\eta_{1}F_{1}^{i-r}\circ E_{2}^{i}F_{1}^{r-1}\varepsilon_{1}F_{1}^{i-r}\circ\lambda_{(i+r+1\cdots 2i+1)}
=βˆ‘r=1iE1Ο‚i∘λ(i+r+1β‹―2)∘η1E2iF1iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}\varsigma_{i}\circ\lambda_{(i+r+1\cdots 2)}\circ\eta_{1}E_{2}^{i}F_{1}^{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2i\cdots i+r)}
=βˆ‘r=1iE1Ο‚i∘λ(i+r+1β‹―i+2)∘λ(i+2β‹―2)∘η1E2iF1iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}\varsigma_{i}\circ\lambda_{(i+r+1\cdots i+2)}\circ\lambda_{(i+2\cdots 2)}\circ\eta_{1}E_{2}^{i}F_{1}^{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2i\cdots i+r)}
=βˆ‘r=1iE1Ο‚i∘λ(2β‹―r+1)∘λ(i+2β‹―2)∘η1E2iF1iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}\varsigma_{i}\circ\lambda_{(2\cdots r+1)}\circ\lambda_{(i+2\cdots 2)}\circ\eta_{1}E_{2}^{i}F_{1}^{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2i\cdots i+r)}
=E1Ο‚i∘λ(i+2β‹―2)∘η1E2iF1iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(2iβ‹―i+1)\displaystyle=E_{1}\varsigma_{i}\circ\lambda_{(i+2\cdots 2)}\circ\eta_{1}E_{2}^{i}F_{1}^{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2i\cdots i+1)}
Ο€βˆ˜(Ο‚iβ€²)12\displaystyle\pi\circ(\varsigma^{\prime}_{i})_{12} =βˆ‘r=1iE1Ο‚1∘λ(12)∘E2Ξ·1∘E2Ο‚iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}\varsigma_{1}\circ\lambda_{(12)}\circ E_{2}\eta_{1}\circ E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=βˆ‘r=1iE1Ο‚1∘λ(23)∘η1E2∘E2Ο‚iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}\varsigma_{1}\circ\lambda_{(23)}\circ\eta_{1}E_{2}\circ E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=βˆ‘r=1iE1Ο‚1∘E1E2F1Ο‚iβˆ’1∘λ23∘η1E2iF1iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}\varsigma_{1}\circ E_{1}E_{2}F_{1}\varsigma_{i-1}\circ\lambda_{23}\circ\eta_{1}E_{2}^{i}F_{1}^{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=βˆ‘r=1iE1Ο‚i∘λ(i+2β‹―3)∘λ23∘λ(3β‹―r+2)∘η1E2iF1iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}\varsigma_{i}\circ\lambda_{(i+2\cdots 3)}\circ\lambda_{23}\circ\lambda_{(3\cdots r+2)}\circ\eta_{1}E_{2}^{i}F_{1}^{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2i\cdots i+r)}
=E1Ο‚i∘λ(i+2β‹―2)∘η1E2iF1iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(2iβ‹―i+r)=d((Ο‚iβ€²)22).\displaystyle=E_{1}\varsigma_{i}\circ\lambda_{(i+2\cdots 2)}\circ\eta_{1}E_{2}^{i}F_{1}^{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2i\cdots i+r)}=d((\varsigma^{\prime}_{i})_{22}).

We have

d⁑((Ο‚iβ€²)12)=A+Bd((\varsigma^{\prime}_{i})_{12})=A+B

where

A\displaystyle A =βˆ‘1≀s<r≀iE2Ο‚iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―s)(s+1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{1\leq s<r\leq i}E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots s)(s+1\cdots r)(2i\cdots i+r)}
=βˆ‘1≀s<r≀iE2Ο‚iβˆ’1∘λ(s+1β‹―r)∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―s)(2iβ‹―i+r)\displaystyle=\sum_{1\leq s<r\leq i}E_{2}\varsigma_{i-1}\circ\lambda_{(s+1\cdots r)}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots s)(2i\cdots i+r)}
=βˆ‘1≀s<r≀iE2Ο‚iβˆ’1∘λ(i+rβˆ’1β‹―s+i)∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―s)(2iβ‹―i+r)\displaystyle=\sum_{1\leq s<r\leq i}E_{2}\varsigma_{i-1}\circ\lambda_{(i+r-1\cdots s+i)}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots s)(2i\cdots i+r)}
=βˆ‘1≀s<r≀iE2Ο‚iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―s)(2iβ‹―i+r)(i+rβˆ’1β‹―i+s)\displaystyle=\sum_{1\leq s<r\leq i}E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots s)(2i\cdots i+r)(i+r-1\cdots i+s)}

and

B=βˆ‘1≀r′≀i1≀s′≀iβˆ’rβ€²E2Ο‚iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―rβ€²)(2iβ‹―i+rβ€²+sβ€²)(i+rβ€²+sβ€²βˆ’1β‹―i+rβ€²)B=\sum_{\begin{subarray}{c}1\leq r^{\prime}\leq i\\ 1\leq s^{\prime}\leq i-r^{\prime}\end{subarray}}E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots r^{\prime})(2i\cdots i+r^{\prime}+s^{\prime})(i+r^{\prime}+s^{\prime}-1\cdots i+r^{\prime})}

So A=BA=B and d⁑((Ο‚iβ€²)12)=0d((\varsigma^{\prime}_{i})_{12})=0.

We have shown that d⁑(Ο‚iβ€²)=0d(\varsigma^{\prime}_{i})=0,

Fix r∈{1,…,i}r\in\{1,\ldots,i\}. We put br=E2Ο‚iβˆ’1∘E2iFiβˆ’1Ξ΅1∘λ(1β‹―r)(2iβ‹―i+r):E2iF1iE1(m)β†’E2(m)b_{r}=E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}:E_{2}^{i}F_{1}^{i}E_{1}(m)\to E_{2}(m).

Consider s∈{1,…,iβˆ’1}s\in\{1,\ldots,i-1\}.

If s>rs>r, we have

br​(TsβŠ—1)\displaystyle b_{r}(T_{s}\otimes 1) =E2Ο‚iβˆ’1∘λ(s,s+1)∘E2iFiβˆ’1∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=E_{2}\varsigma_{i-1}\circ\lambda_{(s,s+1)}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=E2Ο‚iβˆ’1∘λ(i+sβˆ’1,i+s)∘E2iFiβˆ’1∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=E_{2}\varsigma_{i-1}\circ\lambda_{(i+s-1,i+s)}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=E2Ο‚iβˆ’1∘E2iFiβˆ’1∘λ(i+sβˆ’1,i+s)Ξ»(1β‹―r)(2iβ‹―i+r)\displaystyle=E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(i+s-1,i+s)}\lambda_{(1\cdots r)(2i\cdots i+r)}
=E2Ο‚iβˆ’1∘E2iFiβˆ’1∘λ(1β‹―r)(2iβ‹―i+r)Ξ»(i+s,i+s+1)\displaystyle=E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}\lambda_{(i+s,i+s+1)}
=br​(1βŠ—Ts).\displaystyle=b_{r}(1\otimes T_{s}).

If s<rβˆ’1s<r-1, we have

br​(1βŠ—Ts)\displaystyle b_{r}(1\otimes T_{s}) =E2Ο‚iβˆ’1∘λ(i+s,i+s+1)∘E2iFiβˆ’1∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=E_{2}\varsigma_{i-1}\circ\lambda_{(i+s,i+s+1)}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=E2Ο‚iβˆ’1∘λ(s+1,s+2)∘E2iFiβˆ’1∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=E_{2}\varsigma_{i-1}\circ\lambda_{(s+1,s+2)}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=E2Ο‚iβˆ’1∘E2iFiβˆ’1∘λ(s+1,s+2)∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(s+1,s+2)}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=E2Ο‚iβˆ’1∘E2iFiβˆ’1∘λ(1β‹―r)(2iβ‹―i+r)∘λ(s,s+1)\displaystyle=E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}\circ\lambda_{(s,s+1)}
=br​(TsβŠ—1).\displaystyle=b_{r}(T_{s}\otimes 1).

We have

br(Trβˆ’1βŠ—1)=E2Ο‚iβˆ’1∘E2iFiβˆ’1∘λ(1β‹―r)(2iβ‹―i+r)∘λ(rβˆ’1,r)=0b_{r}(T_{r-1}\otimes 1)=E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}\circ\lambda_{(r-1,r)}=0
br(1βŠ—Tr)=E2Ο‚iβˆ’1∘E2iFiβˆ’1∘λ(1β‹―r)(2iβ‹―i+r)∘λ(i+r,i+r+1)=0b_{r}(1\otimes T_{r})=E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}\circ\lambda_{(i+r,i+r+1)}=0
br(1βŠ—Trβˆ’1)=E2Ο‚iβˆ’1∘E2iFiβˆ’1∘λ(1β‹―r)(2iβ‹―i+rβˆ’1)=brβˆ’1(Trβˆ’1βŠ—1).b_{r}(1\otimes T_{r-1})=E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{i-1}\circ\lambda_{(1\cdots r)(2i\cdots i+r-1)}=b_{r-1}(T_{r-1}\otimes 1).

We have shown that (Ο‚i)12​(1βŠ—Ts)=(Ο‚i)12​(TsβŠ—1)(\varsigma_{i})_{12}(1\otimes T_{s})=(\varsigma_{i})_{12}(T_{s}\otimes 1).

We have

(Ο‚iβ€²)11​(TsβŠ—1)\displaystyle(\varsigma^{\prime}_{i})_{11}(T_{s}\otimes 1) =E2Ο‚i∘λ(s+1,s+2)∘λ(1β‹―2i+1)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(s+1,s+2)}\circ\lambda_{(1\cdots 2i+1)}
=E2Ο‚i∘λ(i+s+1,i+s+2)∘λ(1β‹―2i+1)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(i+s+1,i+s+2)}\circ\lambda_{(1\cdots 2i+1)}
=E2Ο‚i∘λ(1β‹―2i+1)Ξ»(i+s,i+s+1)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+1)}\lambda_{(i+s,i+s+1)}
=(Ο‚iβ€²)11​(1βŠ—Ts).\displaystyle=(\varsigma^{\prime}_{i})_{11}(1\otimes T_{s}).

Similarly,

(Ο‚iβ€²)22​(TsβŠ—1)=(Ο‚iβ€²)11​(1βŠ—Ts).(\varsigma^{\prime}_{i})_{22}(T_{s}\otimes 1)=(\varsigma^{\prime}_{i})_{11}(1\otimes T_{s}).

So Ο‚i​(1βŠ—Ts)=Ο‚i​(TsβŠ—1)\varsigma_{i}(1\otimes T_{s})=\varsigma_{i}(T_{s}\otimes 1).

Let l∈{1,2}l\in\{1,2\}. We have

(Ο‚i+jβ€²)l​l∘μi​j=El​ςi+j∘λw(\varsigma^{\prime}_{i+j})_{ll}\circ\mu_{ij}=E_{l}\varsigma_{i+j}\circ\lambda_{w}

where w⁑(r)=rw(r)=r and w⁑(i+r)=i+r+j+1w(i+r)=i+r+j+1 for 1≀r≀i1\leq r\leq i, w⁑(2​i+r)=i+rw(2i+r)=i+r and w⁑(2​i+j+r)=2​i+j+r+1w(2i+j+r)=2i+j+r+1 for 1≀r≀j1\leq r\leq j and w⁑(2​i+2​j+1)=i+j+1w(2i+2j+1)=i+j+1.

We have

(Ο‚iβ€²)l​l∘(Ο‚jβ€²)l​l\displaystyle(\varsigma^{\prime}_{i})_{ll}\circ(\varsigma^{\prime}_{j})_{ll} =ElΟ‚i∘ElE2iF1iΟ‚j∘λ(1β‹…2​i+1)∘λ(2i+1β‹―2i+2j+1)\displaystyle=E_{l}\varsigma_{i}\circ E_{l}E_{2}^{i}F_{1}^{i}\varsigma_{j}\circ\lambda_{(1\cdot 2i+1)}\circ\lambda_{(2i+1\cdots 2i+2j+1)}
=ElΟ‚i+j∘λwβ€²βˆ˜Ξ»(1β‹…2​i+1)∘λ(2i+1β‹―2i+2j+1)\displaystyle=E_{l}\varsigma_{i+j}\circ\lambda_{w^{\prime}}\circ\lambda_{(1\cdot 2i+1)}\circ\lambda_{(2i+1\cdots 2i+2j+1)}

where w′​(r)=rw^{\prime}(r)=r for 1≀r≀i+11\leq r\leq i+1, w′​(i+1+r)=i+j+1+rw^{\prime}(i+1+r)=i+j+1+r for 1≀r≀i1\leq r\leq i, w′​(1+2​i+r)=1+i+rw^{\prime}(1+2i+r)=1+i+r and w′​(1+2​i+j+r)=1+2​i+j+rw^{\prime}(1+2i+j+r)=1+2i+j+r for 1≀r≀j1\leq r\leq j.

It follows that (Ο‚i+jβ€²)l​l∘μi​j=(Ο‚iβ€²)l​l∘(Ο‚jβ€²)l​l(\varsigma^{\prime}_{i+j})_{ll}\circ\mu_{ij}=(\varsigma^{\prime}_{i})_{ll}\circ(\varsigma^{\prime}_{j})_{ll}.

Given l≀l′≀1l\leq l^{\prime}\leq 1, we put blβ€²,l=E2Ο‚lβ€²βˆ’1∘E2lβ€²Flβ€²βˆ’1Ξ΅1∘λ(1β‹―l)(2lβ€²β‹―lβ€²+l):E2lβ€²F1lβ€²E1(m)β†’E2(m)b_{l^{\prime},l}=E_{2}\varsigma_{l^{\prime}-1}\circ E_{2}^{l^{\prime}}F_{l^{\prime}-1}\varepsilon_{1}\circ\lambda_{(1\cdots l)(2l^{\prime}\cdots l^{\prime}+l)}:E_{2}^{l^{\prime}}F_{1}^{l^{\prime}}E_{1}(m)\to E_{2}(m). We denote by wl1,l2w_{l_{1},l_{2}} the permutation of 𝔖l1+l2{\mathfrak{S}}_{l_{1}+l_{2}} given by s↦s+l2s\mapsto s+l_{2} for 1≀s≀l11\leq s\leq l_{1} and s↦sβˆ’l1s\mapsto s-l_{1} for l1+1≀s≀l1+l2l_{1}+1\leq s\leq l_{1}+l_{2}.

Consider r∈{1,…,i}r\in\{1,\ldots,i\}. We have

bi,r∘(Ο‚jβ€²)22\displaystyle b_{i,r}\circ(\varsigma^{\prime}_{j})_{22} =E2Ο‚iβˆ’1∘E2iF1iβˆ’1Ο‚j∘E2iF1iβˆ’1Ξ΅1E2jF1j∘λ(1β‹―r)(2iβ‹―i+r)∘λ(2i+1β‹―2i+2j+1)\displaystyle=E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varsigma_{j}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{2}^{j}F_{1}^{j}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}\circ\lambda_{(2i+1\cdots 2i+2j+1)}
=E2Ο‚i+jβˆ’1∘λwiβˆ’1,j∘E2iF1iβˆ’1Ξ΅1E2jF1j∘λ(2i+1β‹―2i+2j+1)∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=E_{2}\varsigma_{i+j-1}\circ\lambda_{w_{i-1,j}}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{2}^{j}F_{1}^{j}\circ\lambda_{(2i+1\cdots 2i+2j+1)}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=E2Ο‚i+jβˆ’1∘E2iΞ»wiβˆ’1,jF1j∘E2iF1iβˆ’1E2jF1jβˆ’1Ξ΅1∘λ(2i+2jβ‹―2i)∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=E_{2}\varsigma_{i+j-1}\circ E_{2}^{i}\lambda_{w_{i-1,j}}F_{1}^{j}\circ E_{2}^{i}F_{1}^{i-1}E_{2}^{j}F_{1}^{j-1}\varepsilon_{1}\circ\lambda_{(2i+2j\cdots 2i)}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=E2Ο‚i+jβˆ’1∘E2iΞ»wiβˆ’1,jF1j∘E2iF1iβˆ’1E2jF1jβˆ’1Ξ΅1∘λ(2i+2jβ‹―i+r)\displaystyle=E_{2}\varsigma_{i+j-1}\circ E_{2}^{i}\lambda_{w_{i-1,j}}F_{1}^{j}\circ E_{2}^{i}F_{1}^{i-1}E_{2}^{j}F_{1}^{j-1}\varepsilon_{1}\circ\lambda_{(2i+2j\cdots i+r)}
=E2Ο‚i+jβˆ’1∘E2i+jF1i+jβˆ’1Ξ΅1∘E2iΞ»wiβˆ’1,jF1j+1E1∘λ(2i+2jβ‹―i+r)\displaystyle=E_{2}\varsigma_{i+j-1}\circ E_{2}^{i+j}F_{1}^{i+j-1}\varepsilon_{1}\circ E_{2}^{i}\lambda_{w_{i-1,j}}F_{1}^{j+1}E_{1}\circ\lambda_{(2i+2j\cdots i+r)}
=E2Ο‚i+jβˆ’1∘E2i+jF1i+jβˆ’1Ξ΅1∘λ(2i+2jβ‹―i+j+r)∘E2iΞ»wi,jF1jE1\displaystyle=E_{2}\varsigma_{i+j-1}\circ E_{2}^{i+j}F_{1}^{i+j-1}\varepsilon_{1}\circ\lambda_{(2i+2j\cdots i+j+r)}\circ E_{2}^{i}\lambda_{w_{i,j}}F_{1}^{j}E_{1}
=bi+j,r∘μi,j.\displaystyle=b_{i+j,r}\circ\mu_{i,j}.

Consider r∈{1,…,j}r\in\{1,\ldots,j\}. We have

(Ο‚iβ€²)11∘bj,r\displaystyle(\varsigma^{\prime}_{i})_{11}\circ b_{j,r} =E2Ο‚i∘E2i+1F1iΟ‚jβˆ’1∘λ(1β‹―2i+1)∘E2iF1iE2jF1jβˆ’1Ξ΅1∘λ(2i+1β‹―2i+r)(2i+2jβ‹―2i+j+r)\displaystyle=E_{2}\varsigma_{i}\circ E_{2}^{i+1}F_{1}^{i}\varsigma_{j-1}\circ\lambda_{(1\cdots 2i+1)}\circ E_{2}^{i}F_{1}^{i}E_{2}^{j}F_{1}^{j-1}\varepsilon_{1}\circ\lambda_{(2i+1\cdots 2i+r)(2i+2j\cdots 2i+j+r)}
=E2Ο‚i+jβˆ’1∘E2i+1Ξ»wi,jβˆ’1F1jβˆ’1∘λ(1β‹―2i+1)∘E2iF1iE2jF1jβˆ’1Ξ΅1∘λ(2i+1β‹―2i+r)(2i+2jβ‹―2i+j+r)\displaystyle=E_{2}\varsigma_{i+j-1}\circ E_{2}^{i+1}\lambda_{w_{i,j-1}}F_{1}^{j-1}\circ\lambda_{(1\cdots 2i+1)}\circ E_{2}^{i}F_{1}^{i}E_{2}^{j}F_{1}^{j-1}\varepsilon_{1}\circ\lambda_{(2i+1\cdots 2i+r)(2i+2j\cdots 2i+j+r)}
=E2Ο‚i+jβˆ’1∘E2i+jF1i+jβˆ’1Ξ΅1∘E2i+1Ξ»wi,jβˆ’1F1jE1∘λ(1β‹―2i+1)∘λ(2i+1β‹―2i+r)(2i+2jβ‹―2i+j+r)\displaystyle=E_{2}\varsigma_{i+j-1}\circ E_{2}^{i+j}F_{1}^{i+j-1}\varepsilon_{1}\circ E_{2}^{i+1}\lambda_{w_{i,j-1}}F_{1}^{j}E_{1}\circ\lambda_{(1\cdots 2i+1)}\circ\lambda_{(2i+1\cdots 2i+r)(2i+2j\cdots 2i+j+r)}
=E2Ο‚i+jβˆ’1∘E2i+jF1i+jβˆ’1Ξ΅1∘λ(1β‹―i+r)(2i+2jβ‹―2i+j+r)∘E2iΞ»wi,jF1jE1\displaystyle=E_{2}\varsigma_{i+j-1}\circ E_{2}^{i+j}F_{1}^{i+j-1}\varepsilon_{1}\circ\lambda_{(1\cdots i+r)(2i+2j\cdots 2i+j+r)}\circ E_{2}^{i}\lambda_{w_{i,j}}F_{1}^{j}E_{1}
=bi+j,j+r∘μi,j.\displaystyle=b_{i+j,j+r}\circ\mu_{i,j}.

It follows that for all i,jβ‰₯1i,j\geq 1, we have Ο‚i∘E2i​F1i​ςj=Ο‚i+j∘μi,j\varsigma_{i}\circ E_{2}^{i}F_{1}^{i}\varsigma_{j}=\varsigma_{i+j}\circ\mu_{i,j}. ∎

0P6J

Remark 4.4.11. The graphical description of Ο‚β€²\varsigma^{\prime} is the following:

[Uncaptioned image]

Given f∈HomΔλ​𝒲⁑((m,Ο‚),(m~,Ο‚~))f\in\operatorname{Hom}\nolimits_{\Delta_{\lambda}{\mathcal{W}}}((m,\varsigma),(\tilde{m},\tilde{\varsigma})), we put E⁑(f)=(E2​(f)00E1​(f))E(f)=\left(\begin{matrix}E_{2}(f)&0\\ 0&E_{1}(f)\end{matrix}\right).

0P6K

Lemma 4.4.12. We have E⁑(f)∈HomΔλ​𝒲⁑(E⁑(m,Ο‚),E⁑(m~,Ο‚~))E(f)\in\operatorname{Hom}\nolimits_{\Delta_{\lambda}{\mathcal{W}}}(E(m,\varsigma),E(\tilde{m},\tilde{\varsigma})). The construction makes EE into a differential endofunctor of Δλ​𝒲\Delta_{\lambda}{\mathcal{W}}.

0P6L

Proof. The lemma follows from the commutativity of the following diagram:

E2i​F1i​E2​(m)βŠ•E2i​F1i​E1​(m)\textstyle{E_{2}^{i}F_{1}^{i}E_{2}(m)\oplus E_{2}^{i}F_{1}^{i}E_{1}(m)}E2​(m)βŠ•E1​(m)\textstyle{E_{2}(m)\oplus E_{1}(m)}E2i​F1i​E2​(m~)βŠ•E2i​F1i​E1​(m~)\textstyle{E_{2}^{i}F_{1}^{i}E_{2}(\tilde{m})\oplus E_{2}^{i}F_{1}^{i}E_{1}(\tilde{m})}E2​(m~)βŠ•E1​(m~)\textstyle{E_{2}(\tilde{m})\oplus E_{1}(\tilde{m})}E2Ο‚i∘λ(1β‹―2i+1)\scriptstyle{E_{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+1)}}E1Ο‚i∘λ(1β‹―2i+1)\scriptstyle{E_{1}\varsigma_{i}\circ\lambda_{(1\cdots 2i+1)}}βˆ‘r=1iE2Ο‚iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―r)(2iβ‹―i+r)\scriptstyle{\sum_{r=1}^{i}E_{2}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}}E2i​F1i​E2​f\scriptstyle{E_{2}^{i}F_{1}^{i}E_{2}f}E2i​F1i​E1​f\scriptstyle{E_{2}^{i}F_{1}^{i}E_{1}f}E2​f\scriptstyle{E_{2}f}E1​f\scriptstyle{E_{1}f}E2Ο‚~i∘λ(1β‹―2i+1)\scriptstyle{E_{2}\tilde{\varsigma}_{i}\circ\lambda_{(1\cdots 2i+1)}}E1Ο‚~i∘λ(1β‹―2i+1)\scriptstyle{E_{1}\tilde{\varsigma}_{i}\circ\lambda_{(1\cdots 2i+1)}}βˆ‘r=1iE2Ο‚~iβˆ’1∘E2iF1iβˆ’1Ξ΅1∘λ(1β‹―r)(2iβ‹―i+r)\scriptstyle{\sum_{r=1}^{i}E_{2}\tilde{\varsigma}_{i-1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}}

∎

0P6M

Lemma 4.4.13. We have Eβˆ˜Ξ“=Ξ“βˆ˜EE\circ\Gamma=\Gamma\circ E.

0P6N

Proof. Let (m,Ο‚)βˆˆΞ”Ξ»β€‹π’²(m,\varsigma)\in\Delta_{\lambda}{\mathcal{W}}. We have E⁑(m,Ο€)=(mβ€²,Ο€β€²)E(m,\pi)=(m^{\prime},\pi^{\prime}) where mβ€²=cone⁑(Ο€)m^{\prime}=\operatorname{cone}\nolimits(\pi) and Ο€β€²\pi^{\prime} is given in Β§4.3.2. We have Ξ“βˆ˜E⁑(m,Ο‚)=(mβ€²,Ο€β€²β€²)\Gamma\circ E(m,\varsigma)=(m^{\prime},\pi^{\prime\prime}) where

Ο€12β€²β€²=E1​E2​Ρ1∘E1​λ​E1∘η1​E2​E1=Οƒ,Ο€21β€²β€²=0\pi^{\prime\prime}_{12}=E_{1}E_{2}\varepsilon_{1}\circ E_{1}\lambda E_{1}\circ\eta_{1}E_{2}E_{1}=\sigma,\ \pi^{\prime\prime}_{21}=0
Ο€11β€²β€²\displaystyle\pi^{\prime\prime}_{11} =E1​E2​ς1∘E1​E2β€‹Ξ»βˆ˜E1​λ​E2∘E1​F1​τ2∘η1​E22\displaystyle=E_{1}E_{2}\varsigma_{1}\circ E_{1}E_{2}\lambda\circ E_{1}\lambda E_{2}\circ E_{1}F_{1}\tau_{2}\circ\eta_{1}E_{2}^{2}
=E1​E2​ς1∘E1​E2β€‹Ξ»βˆ˜E1​λ​E2∘η1​E22βˆ˜Ο„2\displaystyle=E_{1}E_{2}\varsigma_{1}\circ E_{1}E_{2}\lambda\circ E_{1}\lambda E_{2}\circ\eta_{1}E_{2}^{2}\circ\tau_{2}
=E1​E2​ς1∘E1​E2β€‹Ξ»βˆ˜Οƒβ€‹F1​E2∘E2​η1​E2βˆ˜Ο„2\displaystyle=E_{1}E_{2}\varsigma_{1}\circ E_{1}E_{2}\lambda\circ\sigma F_{1}E_{2}\circ E_{2}\eta_{1}E_{2}\circ\tau_{2}
=Οƒβˆ˜E2​E1​ς1∘E2​E1β€‹Ξ»βˆ˜E2​η1​E2βˆ˜Ο„2\displaystyle=\sigma\circ E_{2}E_{1}\varsigma_{1}\circ E_{2}E_{1}\lambda\circ E_{2}\eta_{1}E_{2}\circ\tau_{2}
=Ο€11β€²\displaystyle=\pi^{\prime}_{11}
Ο€22β€²β€²\displaystyle\pi^{\prime\prime}_{22} =E12​ς1∘E12β€‹Ξ»βˆ˜E1​ρ​E2∘E1​F1β€‹Οƒβˆ˜Ξ·1​E2​E1\displaystyle=E_{1}^{2}\varsigma_{1}\circ E_{1}^{2}\lambda\circ E_{1}\rho E_{2}\circ E_{1}F_{1}\sigma\circ\eta_{1}E_{2}E_{1}
=E12​ς1∘E12β€‹Ξ»βˆ˜E1​ρ​E2∘η1​E1​E2βˆ˜Οƒ\displaystyle=E_{1}^{2}\varsigma_{1}\circ E_{1}^{2}\lambda\circ E_{1}\rho E_{2}\circ\eta_{1}E_{1}E_{2}\circ\sigma
=E12​ς1∘E12β€‹Ξ»βˆ˜Ο„1​F1​E2∘E1​η1​E2βˆ˜Οƒ\displaystyle=E_{1}^{2}\varsigma_{1}\circ E_{1}^{2}\lambda\circ\tau_{1}F_{1}E_{2}\circ E_{1}\eta_{1}E_{2}\circ\sigma
=Ο„1∘E12​ς1∘E12β€‹Ξ»βˆ˜E1​η1​E2βˆ˜Οƒ\displaystyle=\tau_{1}\circ E_{1}^{2}\varsigma_{1}\circ E_{1}^{2}\lambda\circ E_{1}\eta_{1}E_{2}\circ\sigma
=Ο€22β€²\displaystyle=\pi^{\prime}_{22}

It follows that Ο€β€²β€²=Ο€β€²\pi^{\prime\prime}=\pi^{\prime}. ∎

4.4.5. 22-arrows

We assume in Β§4.4.5 that Οƒ\sigma is invertible.

Given (m,Ο‚)βˆˆΞ”Ξ»β€‹π’²(m,\varsigma)\in\Delta_{\lambda}{\mathcal{W}}, write E2​(m,Ο‚)=(mβ€²β€²,Ο‚β€²β€²)E^{2}(m,\varsigma)=(m^{\prime\prime},\varsigma^{\prime\prime}). The formula (4.3.3) defines an endomorphism Ο„\tau of mβ€²β€²m^{\prime\prime}.

0P6P

Lemma 4.4.14. Given iβ‰₯1i\geq 1, we have Ο„βˆ˜Ο‚iβ€²β€²=Ο‚iβ€²β€²βˆ˜E2i​F1i​τ\tau\circ\varsigma^{\prime\prime}_{i}=\varsigma^{\prime\prime}_{i}\circ E_{2}^{i}F_{1}^{i}\tau.

0P6Q

Proof. Let A=Ο„βˆ˜Ο‚iβ€²β€²A=\tau\circ\varsigma^{\prime\prime}_{i} and B=Ο‚iβ€²β€²βˆ˜E2i​F1i​τB=\varsigma^{\prime\prime}_{i}\circ E_{2}^{i}F_{1}^{i}\tau.

We have

a21=a22=a31=a32=a33=a34=a41=a42=a43=0a_{21}=a_{22}=a_{31}=a_{32}=a_{33}=a_{34}=a_{41}=a_{42}=a_{43}=0
a11\displaystyle a_{11} =Ξ»(12)∘E22Ο‚i∘λ(2β‹―2i+2)∘λ(1β‹―2i+1)\displaystyle=\lambda_{(12)}\circ E_{2}^{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
=E22Ο‚i∘λ(1β‹―2i+2)∘λ(1β‹―2i+1)\displaystyle=E_{2}^{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
a12\displaystyle a_{12} =βˆ‘r=1iΞ»(12)∘E22Ο‚iβˆ’1∘E2i+1F1iβˆ’1Ξ΅1∘λ(2β‹―r+1)∘λ(2i+1β‹―i+r+1)∘λ(1β‹―2i+1)\displaystyle=\sum_{r=1}^{i}\lambda_{(12)}\circ E_{2}^{2}\varsigma_{i-1}\circ E_{2}^{i+1}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2\cdots r+1)}\circ\lambda_{(2i+1\cdots i+r+1)}\circ\lambda_{(1\cdots 2i+1)}
=βˆ‘r=1iE22Ο‚iβˆ’1∘E2i+1F1iβˆ’1Ξ΅1∘λ(12)∘λ(1β‹―i+1)∘λ(1β‹―r)∘λ(2i+1β‹―i+r+1)∘λ(i+1β‹―2i+1)\displaystyle=\sum_{r=1}^{i}E_{2}^{2}\varsigma_{i-1}\circ E_{2}^{i+1}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(12)}\circ\lambda_{(1\cdots i+1)}\circ\lambda_{(1\cdots r)}\circ\lambda_{(2i+1\cdots i+r+1)}\circ\lambda_{(i+1\cdots 2i+1)}
=0\displaystyle=0
a13\displaystyle a_{13} =βˆ‘r=1iΞ»(12)∘E22Ο‚iβˆ’1∘λ(2β‹―2i)∘E2iF1iβˆ’1Ξ΅1E2∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}\lambda_{(12)}\circ E_{2}^{2}\varsigma_{i-1}\circ\lambda_{(2\cdots 2i)}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{2}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=βˆ‘r=1iE22Ο‚iβˆ’1∘λ(1β‹―2i)∘E2iF1iβˆ’1Ξ΅1E2∘λ(1β‹―r)(2iβ‹―i+r)∘λ(2​i+1,2​i+2)∘E2iF1iβˆ’1Οƒβˆ’1\displaystyle=\sum_{r=1}^{i}E_{2}^{2}\varsigma_{i-1}\circ\lambda_{(1\cdots 2i)}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{2}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}\circ\lambda_{(2i+1,2i+2)}\circ E_{2}^{i}F_{1}^{i-1}\sigma^{-1}
=βˆ‘r=1iE22Ο‚iβˆ’1∘λ(1β‹―2i)∘E2iF1iβˆ’1E2Ξ΅1∘λ(2​i,2​i+1)∘λ(2iβ‹―i+r)∘λ(1β‹―r)∘E2iF1iβˆ’1Οƒβˆ’1\displaystyle=\sum_{r=1}^{i}E_{2}^{2}\varsigma_{i-1}\circ\lambda_{(1\cdots 2i)}\circ E_{2}^{i}F_{1}^{i-1}E_{2}\varepsilon_{1}\circ\lambda_{(2i,2i+1)}\circ\lambda_{(2i\cdots i+r)}\circ\lambda_{(1\cdots r)}\circ E_{2}^{i}F_{1}^{i-1}\sigma^{-1}
=βˆ‘r=1iE22Ο‚iβˆ’1∘E2i+1F1iβˆ’1Ξ΅1∘λ(1β‹―2i+1)∘λ(2iβ‹―i+r)∘λ(1β‹―r)∘E2iF1iβˆ’1Οƒβˆ’1\displaystyle=\sum_{r=1}^{i}E_{2}^{2}\varsigma_{i-1}\circ E_{2}^{i+1}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots 2i+1)}\circ\lambda_{(2i\cdots i+r)}\circ\lambda_{(1\cdots r)}\circ E_{2}^{i}F_{1}^{i-1}\sigma^{-1}
a14\displaystyle a_{14} =βˆ‘1≀r≀i1≀s<iΞ»(12)∘E22Ο‚iβˆ’2∘E2iF1iβˆ’2Ξ΅1∘λ(2β‹―s+1)(2iβˆ’1β‹―i+s)∘E2iF1iβˆ’1Ξ΅1E1∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{\begin{subarray}{c}1\leq r\leq i\\ 1\leq s<i\end{subarray}}\lambda_{(12)}\circ E_{2}^{2}\varsigma_{i-2}\circ E_{2}^{i}F_{1}^{i-2}\varepsilon_{1}\circ\lambda_{(2\cdots s+1)(2i-1\cdots i+s)}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=βˆ‘1≀r≀i1≀s<iE22Ο‚iβˆ’2∘E2iF1iβˆ’2Ξ΅1∘E2iF1iβˆ’1Ξ΅1E1∘λ(1β‹―s+1)∘λ(1β‹―r)∘λ(2iβˆ’1β‹―i+s)∘λ(2iβ‹―i+r)\displaystyle=\sum_{\begin{subarray}{c}1\leq r\leq i\\ 1\leq s<i\end{subarray}}E_{2}^{2}\varsigma_{i-2}\circ E_{2}^{i}F_{1}^{i-2}\varepsilon_{1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(1\cdots s+1)}\circ\lambda_{(1\cdots r)}\circ\lambda_{(2i-1\cdots i+s)}\circ\lambda_{(2i\cdots i+r)}
=βˆ‘1≀r≀s<iE22Ο‚iβˆ’2∘E2iF1iβˆ’2Ξ΅1∘E2iF1iβˆ’1Ξ΅1E1∘λ(2β‹―r+1)∘λ(1β‹―s+1)∘λ(2iβ‹―i+r)∘λ(2iβ‹―i+s+1)\displaystyle=\sum_{1\leq r\leq s<i}E_{2}^{2}\varsigma_{i-2}\circ E_{2}^{i}F_{1}^{i-2}\varepsilon_{1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(2\cdots r+1)}\circ\lambda_{(1\cdots s+1)}\circ\lambda_{(2i\cdots i+r)}\circ\lambda_{(2i\cdots i+s+1)}
a23\displaystyle a_{23} =Οƒβˆ’1∘E1E2Ο‚i∘λ(2β‹―2i+2)∘λ(1β‹―2i+1)\displaystyle=\sigma^{-1}\circ E_{1}E_{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
=Οƒβˆ’1∘E1E2Ο‚i∘λ(2β‹―2i+2)∘λ(1β‹―2i+1)∘λ(2​i+1,2​i+2)∘E2iF1iΟƒβˆ’1\displaystyle=\sigma^{-1}\circ E_{1}E_{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}\circ\lambda_{(2i+1,2i+2)}\circ E_{2}^{i}F_{1}^{i}\sigma^{-1}
=Οƒβˆ’1∘E1E2Ο‚i∘λ(12)∘λ(2β‹―2i+2)∘λ(1β‹―2i+1)∘E2iF1iΟƒβˆ’1\displaystyle=\sigma^{-1}\circ E_{1}E_{2}\varsigma_{i}\circ\lambda_{(12)}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}\circ E_{2}^{i}F_{1}^{i}\sigma^{-1}
=E1E2Ο‚i∘λ(2β‹―2i+2)∘λ(1β‹―2i+1)∘E2iF1iΟƒβˆ’1\displaystyle=E_{1}E_{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}\circ E_{2}^{i}F_{1}^{i}\sigma^{-1}
a24\displaystyle a_{24} =βˆ‘r=1iΟƒβˆ’1∘E1E2Ο‚iβˆ’1∘E1E2iF1iβˆ’1Ξ΅1∘λ(2β‹―r+1)∘λ(2i+1β‹―i+r+1)∘λ(1β‹―2i+1)\displaystyle=\sum_{r=1}^{i}\sigma^{-1}\circ E_{1}E_{2}\varsigma_{i-1}\circ E_{1}E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2\cdots r+1)}\circ\lambda_{(2i+1\cdots i+r+1)}\circ\lambda_{(1\cdots 2i+1)}
=βˆ‘r=1iE2E1Ο‚iβˆ’1∘E2E1E2iβˆ’1F1iβˆ’1Ξ΅1βˆ˜Οƒβˆ’1E2iβˆ’1F1iE1∘λ(1β‹―2i+1)∘λ(1β‹―r)∘λ(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{2}E_{1}\varsigma_{i-1}\circ E_{2}E_{1}E_{2}^{i-1}F_{1}^{i-1}\varepsilon_{1}\circ\sigma^{-1}E_{2}^{i-1}F_{1}^{i}E_{1}\circ\lambda_{(1\cdots 2i+1)}\circ\lambda_{(1\cdots r)}\circ\lambda_{(2i\cdots i+r)}
=βˆ‘r=1iE2E1Ο‚iβˆ’1∘E2E1E2iβˆ’1F1iβˆ’1Ξ΅1∘λ(2β‹―2i+1)∘λ(1β‹―r)∘λ(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{2}E_{1}\varsigma_{i-1}\circ E_{2}E_{1}E_{2}^{i-1}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2\cdots 2i+1)}\circ\lambda_{(1\cdots r)}\circ\lambda_{(2i\cdots i+r)}
a44\displaystyle a_{44} =Ξ»(12)∘E12Ο‚i∘λ(2β‹―2i+2)∘λ(1β‹―2i+1)\displaystyle=\lambda_{(12)}\circ E_{1}^{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
=E12Ο‚i∘λ(1β‹―2i+2)∘λ(1β‹―2i+1)\displaystyle=E_{1}^{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}

We have

b21=b12=b22=b31=b32=b33=b41=b42=b43=0b_{21}=b_{12}=b_{22}=b_{31}=b_{32}=b_{33}=b_{41}=b_{42}=b_{43}=0
b11\displaystyle b_{11} =E22Ο‚i∘λ(2β‹―2i+2)∘λ(1β‹―2i+1)∘λ(2​i+1,2​i+2)\displaystyle=E_{2}^{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}\circ\lambda_{(2i+1,2i+2)}
=E22Ο‚i∘λ(1β‹―2i+2)∘λ(1β‹―2i+1)\displaystyle=E_{2}^{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
b13\displaystyle b_{13} =βˆ‘r=1iE22Ο‚iβˆ’1∘E2i+1F1iβˆ’1Ξ΅1∘λ(2β‹―r+1)∘λ(2i+1β‹―i+r+1)∘λ(1β‹―2i+1)∘E2iF1iΟƒβˆ’1\displaystyle=\sum_{r=1}^{i}E_{2}^{2}\varsigma_{i-1}\circ E_{2}^{i+1}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2\cdots r+1)}\circ\lambda_{(2i+1\cdots i+r+1)}\circ\lambda_{(1\cdots 2i+1)}\circ E_{2}^{i}F_{1}^{i}\sigma^{-1}
=βˆ‘r=1iE22Ο‚iβˆ’1∘E2i+1F1iβˆ’1Ξ΅1∘λ(1β‹―2i+1)∘λ(2iβ‹―i+r)∘λ(1β‹―r)∘E2iF1iΟƒβˆ’1\displaystyle=\sum_{r=1}^{i}E_{2}^{2}\varsigma_{i-1}\circ E_{2}^{i+1}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots 2i+1)}\circ\lambda_{(2i\cdots i+r)}\circ\lambda_{(1\cdots r)}\circ E_{2}^{i}F_{1}^{i}\sigma^{-1}
b14\displaystyle b_{14} =βˆ‘1≀r≀i1≀s<iE22Ο‚iβˆ’2∘E2iF1iβˆ’2Ξ΅1∘λ(2β‹―s+1)(2iβˆ’1β‹―i+s)∘E2iF1iβˆ’1Ξ΅1E1∘λ(1β‹―r)(2iβ‹―i+r)∘λ(2​i+1,2​i+2)\displaystyle=\sum_{\begin{subarray}{c}1\leq r\leq i\\ 1\leq s<i\end{subarray}}E_{2}^{2}\varsigma_{i-2}\circ E_{2}^{i}F_{1}^{i-2}\varepsilon_{1}\circ\lambda_{(2\cdots s+1)(2i-1\cdots i+s)}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}\circ\lambda_{(2i+1,2i+2)}
=βˆ‘1≀r≀i1≀s<iE22Ο‚iβˆ’2∘E2iF1iβˆ’2Ξ΅1∘E2iF1iβˆ’1Ξ΅1E1∘λ(2​i+1,2​i+2)∘λ(2β‹―s+1)(2iβˆ’1β‹―i+s)∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{\begin{subarray}{c}1\leq r\leq i\\ 1\leq s<i\end{subarray}}E_{2}^{2}\varsigma_{i-2}\circ E_{2}^{i}F_{1}^{i-2}\varepsilon_{1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(2i+1,2i+2)}\circ\lambda_{(2\cdots s+1)(2i-1\cdots i+s)}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=βˆ‘1≀r≀i1≀s<iE22Ο‚iβˆ’2∘E2iF1iβˆ’2Ξ΅1∘E2iF1iβˆ’1Ξ΅1E1∘λ(2​iβˆ’1,2​i)∘λ(2β‹―s+1)(2iβˆ’1β‹―i+s)∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{\begin{subarray}{c}1\leq r\leq i\\ 1\leq s<i\end{subarray}}E_{2}^{2}\varsigma_{i-2}\circ E_{2}^{i}F_{1}^{i-2}\varepsilon_{1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(2i-1,2i)}\circ\lambda_{(2\cdots s+1)(2i-1\cdots i+s)}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=βˆ‘1≀s<r≀iE22Ο‚iβˆ’2∘E2iF1iβˆ’2Ξ΅1∘E2iF1iβˆ’1Ξ΅1E1∘λ(2β‹―s+1)∘λ(1β‹―r)∘λ(2iβ‹―i+s)∘λ(2iβ‹―i+r)\displaystyle=\sum_{1\leq s<r\leq i}E_{2}^{2}\varsigma_{i-2}\circ E_{2}^{i}F_{1}^{i-2}\varepsilon_{1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(2\cdots s+1)}\circ\lambda_{(1\cdots r)}\circ\lambda_{(2i\cdots i+s)}\circ\lambda_{(2i\cdots i+r)}
=βˆ‘1≀r′≀s′≀iE22Ο‚iβˆ’2∘E2iF1iβˆ’2Ξ΅1∘E2iF1iβˆ’1Ξ΅1E1∘λ(2β‹―rβ€²+1)∘λ(1β‹―sβ€²+1)∘λ(2iβ‹―i+rβ€²)∘λ(2iβ‹―i+sβ€²+1)\displaystyle=\sum_{1\leq r^{\prime}\leq s^{\prime}\leq i}E_{2}^{2}\varsigma_{i-2}\circ E_{2}^{i}F_{1}^{i-2}\varepsilon_{1}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(2\cdots r^{\prime}+1)}\circ\lambda_{(1\cdots s^{\prime}+1)}\circ\lambda_{(2i\cdots i+r^{\prime})}\circ\lambda_{(2i\cdots i+s^{\prime}+1)}
b23=E2E1Ο‚i∘λ(2β‹―2i+2)∘λ(1β‹―2i+1)∘E2iF1iΟƒβˆ’1b_{23}=E_{2}E_{1}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}\circ E_{2}^{i}F_{1}^{i}\sigma^{-1}
b24\displaystyle b_{24} =βˆ‘r=1iE2E1Ο‚iβˆ’1∘λ(2β‹―2i)∘E2iF1iβˆ’1Ξ΅1E1∘λ(1β‹―r)(2iβ‹―i+r)∘λ(2​i+1,2​i+2)\displaystyle=\sum_{r=1}^{i}E_{2}E_{1}\varsigma_{i-1}\circ\lambda_{(2\cdots 2i)}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}\circ\lambda_{(2i+1,2i+2)}
=βˆ‘r=1iE2E1Ο‚iβˆ’1∘λ(2β‹―2i)∘E2iF1iβˆ’1E1Ξ΅1∘λ(2​i,2​i+1)∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{2}E_{1}\varsigma_{i-1}\circ\lambda_{(2\cdots 2i)}\circ E_{2}^{i}F_{1}^{i-1}E_{1}\varepsilon_{1}\circ\lambda_{(2i,2i+1)}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
=βˆ‘r=1iE2E1Ο‚iβˆ’1∘E2iF1iβˆ’1E1Ξ΅1∘λ(2β‹―2i+1)∘λ(1β‹―r)(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{2}E_{1}\varsigma_{i-1}\circ E_{2}^{i}F_{1}^{i-1}E_{1}\varepsilon_{1}\circ\lambda_{(2\cdots 2i+1)}\circ\lambda_{(1\cdots r)(2i\cdots i+r)}
b34\displaystyle b_{34} =βˆ‘r=1iE1E2Ο‚iβˆ’1∘E1E2iF1iβˆ’1Ξ΅1∘λ(2β‹―r+1)∘λ(2i+1β‹―i+r+1)∘λ(1β‹―2i+1)∘λ(2​i+1,2​i+2)\displaystyle=\sum_{r=1}^{i}E_{1}E_{2}\varsigma_{i-1}\circ E_{1}E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(2\cdots r+1)}\circ\lambda_{(2i+1\cdots i+r+1)}\circ\lambda_{(1\cdots 2i+1)}\circ\lambda_{(2i+1,2i+2)}
=βˆ‘r=1iE1E2Ο‚iβˆ’1∘E1E2iF1iβˆ’1Ξ΅1∘λ(1β‹―2i+2)∘λ(1β‹―r)∘λ(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}E_{2}\varsigma_{i-1}\circ E_{1}E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}\circ\lambda_{(1\cdots 2i+2)}\circ\lambda_{(1\cdots r)}\circ\lambda_{(2i\cdots i+r)}
=βˆ‘r=1iE1E2Ο‚iβˆ’1∘λ(1β‹―2i)∘E2iF1iβˆ’1E1Ξ΅1∘λ(2​i,2​i+1)∘λ(2​i+1,2​i+2)∘λ(1β‹―r)∘λ(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}E_{2}\varsigma_{i-1}\circ\lambda_{(1\cdots 2i)}\circ E_{2}^{i}F_{1}^{i-1}E_{1}\varepsilon_{1}\circ\lambda_{(2i,2i+1)}\circ\lambda_{(2i+1,2i+2)}\circ\lambda_{(1\cdots r)}\circ\lambda_{(2i\cdots i+r)}
=βˆ‘r=1iE1E2Ο‚iβˆ’1∘λ(1β‹―2i)∘E2iF1iβˆ’1Ξ΅1E1∘λ(2​i+1,2​i+2)∘λ(2​i+1,2​i+2)∘λ(1β‹―r)∘λ(2iβ‹―i+r)\displaystyle=\sum_{r=1}^{i}E_{1}E_{2}\varsigma_{i-1}\circ\lambda_{(1\cdots 2i)}\circ E_{2}^{i}F_{1}^{i-1}\varepsilon_{1}E_{1}\circ\lambda_{(2i+1,2i+2)}\circ\lambda_{(2i+1,2i+2)}\circ\lambda_{(1\cdots r)}\circ\lambda_{(2i\cdots i+r)}
=0\displaystyle=0
b44\displaystyle b_{44} =E12Ο‚i∘λ(2β‹―2i+2)∘λ(1β‹―2i+1)∘λ(2​i+1,2​i+2)\displaystyle=E_{1}^{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}\circ\lambda_{(2i+1,2i+2)}
=E12Ο‚i∘λ(1β‹―2i+2)∘λ(1β‹―2i+1)\displaystyle=E_{1}^{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}

We deduce that A=BA=B and the lemma follows. ∎

Lemma 4.4.14 shows that Ο„\tau defines an endomorphism of E2​(m,Ο‚)E^{2}(m,\varsigma) for all (m,Ο‚)βˆˆΞ”Ξ»β€‹π’²(m,\varsigma)\in\Delta_{\lambda}{\mathcal{W}}. The functor Ξ“\Gamma is faithful, Γ​E2=E2​Γ\Gamma E^{2}=E^{2}\Gamma (Lemma 4.4.13) and Ο„\tau commutes with Ξ“\Gamma. It follows that Ο„\tau is functorial.

Theorem 4.3.8 has the following consequence.

0P6R

Theorem 4.4.15. The data (Δλ​𝒲,E,Ο„)(\Delta_{\lambda}{\mathcal{W}},E,\tau) is an idempotent-complete strongly pretriangulated 22-representation.

The following proposition is a consequence of Lemma 4.4.13 and the construction of Ο„\tau.

0P6S

Proposition 4.4.16. The functor Ξ“:Δλ​𝒲→Δσ​𝒲\Gamma:\Delta_{\lambda}{\mathcal{W}}\to\Delta_{\sigma}{\mathcal{W}} induces a morphism of 22-representations.

4.5. Tensor product and internal Hom\operatorname{Hom}\nolimits

Let us give two applications of the construction of Β§4.3. Let (𝒱1,E1,Ο„1)({\mathcal{V}}_{1},E_{1},\tau_{1}) and (𝒱2,E2,Ο„2)({\mathcal{V}}_{2},E_{2},\tau_{2}) be idempotent-complete strongly pretriangulated 22-representations.

We view 𝒱1βŠ—π’±2{\mathcal{V}}_{1}\otimes{\mathcal{V}}_{2} as endowed with two strictly commuting actions of 𝒰{\mathcal{U}} given by (E1βŠ—1,Ο„1βŠ—1)(E_{1}\otimes 1,\tau_{1}\otimes 1) and (1βŠ—E2,1βŠ—Ο„2)(1\otimes E_{2},1\otimes\tau_{2}): the isomorphism Οƒ:(1βŠ—E2)∘(E1βŠ—1)β†’βˆΌ(E1βŠ—1)∘(1βŠ—E2)\sigma:(1\otimes E_{2})\circ(E_{1}\otimes 1)\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}(E_{1}\otimes 1)\circ(1\otimes E_{2}) is the identity.

We define the tensor product 22-representation

𝒱1βŠ—β—‹π’±2=Δσ(𝒱1βŠ—π’±2).{\mathcal{V}}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{2}=\Delta_{\sigma}({\mathcal{V}}_{1}\otimes{\mathcal{V}}_{2}).

Given (Ξ¦i,Ο†i):𝒱i→𝒱iβ€²(\Phi_{i},\varphi_{i}):{\mathcal{V}}_{i}\to{\mathcal{V}}^{\prime}_{i} a morphism of 22-representations for i∈{1,2}i\in\{1,2\}, Proposition 4.3.9 provides a morphism of 22-representations 𝒱1βŠ—β—‹π’±2→𝒱′1βŠ—β—‹π’±β€²2{\mathcal{V}}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{2}\to{\mathcal{V}}^{\prime}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}^{\prime}_{2}.

Given 𝒱1{\mathcal{V}}_{1}, 𝒱2{\mathcal{V}}_{2} and 𝒱3{\mathcal{V}}_{3} 22-representations, Proposition 4.3.12 provides an isomorphism

(𝒱1βŠ—β—‹π’±2)βŠ—β—‹π’±3β†’βˆΌπ’±1βŠ—β—‹(𝒱2βŠ—β—‹π’±3)({\mathcal{V}}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{2}){\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{3}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\mathcal{V}}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}({\mathcal{V}}_{2}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{3})

that commutes with forgetful functors Ο‰\omega.

Since the forgetful functors Ο‰\omega are faithful, we deduce that idempotent-complete strongly pretriangulated 22-representations form a monoidal 22-category.

Consider now Hom⁑(𝒱1,𝒱2)\operatorname{Hom}\nolimits({\mathcal{V}}_{1},{\mathcal{V}}_{2}). It is endowed with two strictly commuting structures of 22-representations: the first one is given by ((Ξ¦β†¦Ξ¦βˆ˜E1),Φ​τ1)((\Phi\mapsto\Phi\circ E_{1}),\Phi\tau_{1}) and the second one by ((Φ↦E2∘Φ),Ο„2​Φ)((\Phi\mapsto E_{2}\circ\Phi),\tau_{2}\Phi). The isomorphism Οƒ\sigma is the identity.

We define the internal Hom\operatorname{Hom}\nolimits 22-representation

ℋ​ℋ​o​m​(𝒱1,𝒱2)=Δ​Hom⁑(𝒱1,𝒱2).{\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}_{1},{\mathcal{V}}_{2})=\Delta\operatorname{Hom}\nolimits({\mathcal{V}}_{1},{\mathcal{V}}_{2}).

The category ℋ​ℋ​o​m​(𝒱1,𝒱2){\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}_{1},{\mathcal{V}}_{2}) has objects pairs (Ξ¦,Ο€)(\Phi,\pi) where Ξ¦:𝒱1→𝒱2Β―i\Phi:{\mathcal{V}}_{1}\to\overline{{\mathcal{V}}_{2}}^{i} is a differential functor and Ο€:E2​Φ→Φ​E1\pi:E_{2}\Phi\to\Phi E_{1} is a closed natural transformation of functors such that

Ο„1β€‹Ξ¦βˆ˜Ο€β€‹E1∘E2​π=π​E1∘E2β€‹Ο€βˆ˜Ο„2​Φ:E22​Φ→Φ​E12.\tau_{1}\Phi\circ\pi E_{1}\circ E_{2}\pi=\pi E_{1}\circ E_{2}\pi\circ\tau_{2}\Phi:E_{2}^{2}\Phi\to\Phi E_{1}^{2}.

Note that Hom𝒰⁑(𝒱1,𝒱2)\operatorname{Hom}\nolimits_{\mathcal{U}}({\mathcal{V}}_{1},{\mathcal{V}}_{2}) is the full subcategory of ℋ​ℋ​o​m​(𝒱1,𝒱2){\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}_{1},{\mathcal{V}}_{2}) with objects pairs (Ξ¦,Ο€)(\Phi,\pi) where Ξ¦\Phi takes values in 𝒱2{\mathcal{V}}_{2} and Ο€\pi is invertible.

Given (Ξ¦1,Ο†1):𝒱1′→𝒱1(\Phi_{1},\varphi_{1}):{\mathcal{V}}^{\prime}_{1}\to{\mathcal{V}}_{1} and (Ξ¦2,Ο†2):𝒱2→𝒱2β€²(\Phi_{2},\varphi_{2}):{\mathcal{V}}_{2}\to{\mathcal{V}}^{\prime}_{2} two morphisms of 22-representations, Proposition 4.3.9 provides a morphism of 22-representations ℋ​ℋ​o​m​(𝒱1,𝒱2)→ℋ​ℋ​o​m​(𝒱1β€²,𝒱2β€²){\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}_{1},{\mathcal{V}}_{2})\to{\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}^{\prime}_{1},{\mathcal{V}}^{\prime}_{2}).

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

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2