ScalingStacks

4.4.3. Relations

Let ℳ{\mathcal{M}} be the strict monoidal pointed category generated by objects ala_{l} for 1≤l≤31\leq l\leq 3 and maps λl​m:al​am→am​al\lambda_{lm}:a_{l}a_{m}\to a_{m}a_{l} for l≤ml\leq m with relations λl​l2=0\lambda_{ll}^{2}=0 and

λm​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:ℳ→𝒰∙,al↦e,λl​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(Homℳ(al1⋯alr,am1⋯amr))⊂Hr∙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 w∈𝔖rw\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}.

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Proof. Given the defining relations for 𝒰∙{\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,…,n−1}i\in\{1,\ldots,n-1\} such that li≤li+1l_{i}\leq l_{i+1}, we put T~i=al1⋯ali−1λli,li+1ali+2⋯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,…,n−1}i_{1},\ldots,i_{r},j_{1},\ldots,j_{s}\in\{1,\ldots,n-1\} such that T~i1⋯T~ir\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r}} and T~j1⋯T~js\tilde{T}_{j_{1}}\cdots\tilde{T}_{j_{s}} are well-defined and Ti1⋯Tir=Tj1⋯TjsT_{i_{1}}\cdots T_{i_{r}}=T_{j_{1}}\cdots T_{j_{s}}, then we have T~i1⋯T~ir=T~j1⋯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~i1⋯T~ir\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r}} is well-defined and non-zero. Let w=si1⋯sir∈𝔖nw=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 w′=si1⋯sir−1w^{\prime}=s_{i_{1}}\cdots s_{i_{r-1}}. Put d=ird=i_{r} and w′=w​sdw^{\prime}=ws_{d}. Since Ti1⋯Tir≠0T_{i_{1}}\cdots T_{i_{r}}\neq 0, we have r=ℓ⁡(w)r=\ell(w). We have L~​(w)={(d,d+1)}​∐sd​(L~​(w′))\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~i1⋯T~ir−1\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r-1}} from al1⋯ald−1ald+1aldald+2⋯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~​(w′)(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)}​∐sd​(L~​(w′))\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 w∈𝔖nw\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=si1⋯sirw=s_{i_{1}}\cdots s_{i_{r}} be a reduced decomposition of ww. We show by induction on rr that T~i1⋯T~ir\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r}} is well-defined. As before, we define dd and w′w^{\prime}. By induction on rr, the element T~i1⋯T~ir−1\tilde{T}_{i_{1}}\cdots\tilde{T}_{i_{r-1}} gives a well-defined map from al1⋯ald−1ald+1aldald+2⋯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 al1⋯alna_{l_{1}}\cdots a_{l_{n}}. We deduce that T~i1⋯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 w∈𝔖rw\in{\mathfrak{S}}_{r} satisfying the assumptions of Lemma 4.4.6, we put λw=H−1​(Tw)\lambda_{w}=H^{-1}(T_{w}).

We denote by ℳ′{\mathcal{M}}^{\prime} the strict monoidal kk-linear category obtained from k⁡[ℳ]k[{\mathcal{M}}] by adding maps ε:a1​a3→1\varepsilon:a_{1}a_{3}\to 1 and η:1→a3​a1\eta:1\to a_{3}a_{1} and relations

a3​ε∘η​a3=id,ε​a1∘a1​η=ida_{3}\varepsilon\circ\eta a_{3}=\operatorname{id}\nolimits,\ \varepsilon a_{1}\circ a_{1}\eta=\operatorname{id}\nolimits
λ23=a3​a2​ε∘a3​λ12​a3∘η​a2​a3,λ13=ε​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
λ11=ε​a12∘a1​ε​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 ℳ′opp→∼ℳ′{\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,λ12↦λ23,λ23↦λ12,λ13↦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}
λ11↦λ33,λ22↦λ22,λ33↦λ11,ε↦η,η↦ε.\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

λ(1⋯n+1)∘G1⋯Gnη=λ(n+2⋯2)∘ηG1⋯Gn:G1⋯Gn→a3G1⋯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

εG1⋯Gn∘λ(2⋯n+2)=G1⋯Gnε∘λ(n+1⋯1):a1G1⋯Gna3→G1⋯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​λ13∘η​a3\displaystyle a_{3}\lambda_{13}\circ\eta a_{3} =a3​ε​a3​a1∘a3​a1​λ33​a1∘a3​a1​a3​η∘η​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​ε​a3​a1∘η​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
=λ33​a1∘a3​η\displaystyle=\lambda_{33}a_{1}\circ a_{3}\eta
λ13​a1∘a1​η\displaystyle\lambda_{13}a_{1}\circ a_{1}\eta =ε​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
=ε​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​λ11∘ε​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​λ11∘η​a1∘ε​a1∘a1​η\displaystyle=a_{3}\lambda_{11}\circ\eta a_{1}\circ\varepsilon a_{1}\circ a_{1}\eta
=a3​λ11∘η​a1\displaystyle=a_{3}\lambda_{11}\circ\eta a_{1}
λ23​a1∘a2​η\displaystyle\lambda_{23}a_{1}\circ a_{2}\eta =a3​a2​ε​a1∘a3​λ12​a3​a1∘η​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​ε​a1∘a3​a2​a1​η∘a3​λ12∘η​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​λ12∘η​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 n≥2n\geq 2. We prove the first statement of the lemma by induction on nn. We have

λ(n+2⋯2)∘ηG1⋯Gn\displaystyle\lambda_{(n+2\cdots 2)}\circ\eta G_{1}\cdots G_{n} =λ(n+2⋯3)∘(λ(23)∘ηG1)G2⋯Gn\displaystyle=\lambda_{(n+2\cdots 3)}\circ(\lambda_{(23)}\circ\eta G_{1})G_{2}\cdots G_{n}
=λ(n+2⋯3)∘(λ(12)∘G1η)G2⋯Gn\displaystyle=\lambda_{(n+2\cdots 3)}\circ(\lambda_{(12)}\circ G_{1}\eta)G_{2}\cdots G_{n}
=λ(12)∘G1(λ(n+1⋯2)∘ηG2⋯Gn)\displaystyle=\lambda_{(12)}\circ G_{1}(\lambda_{(n+1\cdots 2)}\circ\eta G_{2}\cdots G_{n})
=λ(12)∘G1(λ(1⋯n)∘G2⋯Gnη)\displaystyle=\lambda_{(12)}\circ G_{1}(\lambda_{(1\cdots n)}\circ G_{2}\cdots G_{n}\eta)
=λ(1⋯n+1)∘G1⋯Gnη\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 ℳ′{\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,λ12↦λ,λ23↦σ,λ13↦ρ,λ11↦τ1,λ22↦τ2,λ33↦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,ε↦ε1.\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 w∈𝔖rw\in{\mathfrak{S}}_{r} satisfying the assumptions of Lemma 4.4.6, we still denote by λw\lambda_{w} the element R⁡(λw)R(\lambda_{w}).

Lemma 4.4.7 has the following consequence.

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

λ(1⋯n+1)∘G1⋯Gnη1=λ(n+2⋯2)∘η1G1⋯Gn:G1⋯Gn→E1G1⋯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

ε1G1⋯Gn∘λ(2⋯n+2)=G1⋯Gnε1∘λ(n+1⋯1):F1G1⋯GnE1→G1⋯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}.

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

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2