ScalingStacks

4.4.5. 22-arrows

We assume in §4.4.5 that σ\sigma is invertible.

Given (m,ς)∈Δλ​𝒲(m,\varsigma)\in\Delta_{\lambda}{\mathcal{W}}, write E2​(m,ς)=(m′′,ς′′)E^{2}(m,\varsigma)=(m^{\prime\prime},\varsigma^{\prime\prime}). The formula (4.3.3) defines an endomorphism τ\tau of m′′m^{\prime\prime}.

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Lemma 4.4.14. Given i≥1i\geq 1, we have τ∘ςi′′=ςi′′∘E2i​F1i​τ\tau\circ\varsigma^{\prime\prime}_{i}=\varsigma^{\prime\prime}_{i}\circ E_{2}^{i}F_{1}^{i}\tau.

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Proof. Let A=τ∘ςi′′A=\tau\circ\varsigma^{\prime\prime}_{i} and B=ςi′′∘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} =λ(12)∘E22ςi∘λ(2⋯2i+2)∘λ(1⋯2i+1)\displaystyle=\lambda_{(12)}\circ E_{2}^{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
=E22ςi∘λ(1⋯2i+2)∘λ(1⋯2i+1)\displaystyle=E_{2}^{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
a12\displaystyle a_{12} =∑r=1iλ(12)∘E22ςi−1∘E2i+1F1i−1ε1∘λ(2⋯r+1)∘λ(2i+1⋯i+r+1)∘λ(1⋯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)}
=∑r=1iE22ςi−1∘E2i+1F1i−1ε1∘λ(12)∘λ(1⋯i+1)∘λ(1⋯r)∘λ(2i+1⋯i+r+1)∘λ(i+1⋯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} =∑r=1iλ(12)∘E22ςi−1∘λ(2⋯2i)∘E2iF1i−1ε1E2∘λ(1⋯r)(2i⋯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)}
=∑r=1iE22ςi−1∘λ(1⋯2i)∘E2iF1i−1ε1E2∘λ(1⋯r)(2i⋯i+r)∘λ(2​i+1,2​i+2)∘E2iF1i−1σ−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}
=∑r=1iE22ςi−1∘λ(1⋯2i)∘E2iF1i−1E2ε1∘λ(2​i,2​i+1)∘λ(2i⋯i+r)∘λ(1⋯r)∘E2iF1i−1σ−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}
=∑r=1iE22ςi−1∘E2i+1F1i−1ε1∘λ(1⋯2i+1)∘λ(2i⋯i+r)∘λ(1⋯r)∘E2iF1i−1σ−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} =∑1≤r≤i1≤s<iλ(12)∘E22ςi−2∘E2iF1i−2ε1∘λ(2⋯s+1)(2i−1⋯i+s)∘E2iF1i−1ε1E1∘λ(1⋯r)(2i⋯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)}
=∑1≤r≤i1≤s<iE22ςi−2∘E2iF1i−2ε1∘E2iF1i−1ε1E1∘λ(1⋯s+1)∘λ(1⋯r)∘λ(2i−1⋯i+s)∘λ(2i⋯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)}
=∑1≤r≤s<iE22ςi−2∘E2iF1i−2ε1∘E2iF1i−1ε1E1∘λ(2⋯r+1)∘λ(1⋯s+1)∘λ(2i⋯i+r)∘λ(2i⋯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} =σ−1∘E1E2ςi∘λ(2⋯2i+2)∘λ(1⋯2i+1)\displaystyle=\sigma^{-1}\circ E_{1}E_{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
=σ−1∘E1E2ςi∘λ(2⋯2i+2)∘λ(1⋯2i+1)∘λ(2​i+1,2​i+2)∘E2iF1iσ−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}
=σ−1∘E1E2ςi∘λ(12)∘λ(2⋯2i+2)∘λ(1⋯2i+1)∘E2iF1iσ−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}
=E1E2ςi∘λ(2⋯2i+2)∘λ(1⋯2i+1)∘E2iF1iσ−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} =∑r=1iσ−1∘E1E2ςi−1∘E1E2iF1i−1ε1∘λ(2⋯r+1)∘λ(2i+1⋯i+r+1)∘λ(1⋯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)}
=∑r=1iE2E1ςi−1∘E2E1E2i−1F1i−1ε1∘σ−1E2i−1F1iE1∘λ(1⋯2i+1)∘λ(1⋯r)∘λ(2i⋯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)}
=∑r=1iE2E1ςi−1∘E2E1E2i−1F1i−1ε1∘λ(2⋯2i+1)∘λ(1⋯r)∘λ(2i⋯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} =λ(12)∘E12ςi∘λ(2⋯2i+2)∘λ(1⋯2i+1)\displaystyle=\lambda_{(12)}\circ E_{1}^{2}\varsigma_{i}\circ\lambda_{(2\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
=E12ςi∘λ(1⋯2i+2)∘λ(1⋯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} =E22ςi∘λ(2⋯2i+2)∘λ(1⋯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)}
=E22ςi∘λ(1⋯2i+2)∘λ(1⋯2i+1)\displaystyle=E_{2}^{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+2)}\circ\lambda_{(1\cdots 2i+1)}
b13\displaystyle b_{13} =∑r=1iE22ςi−1∘E2i+1F1i−1ε1∘λ(2⋯r+1)∘λ(2i+1⋯i+r+1)∘λ(1⋯2i+1)∘E2iF1iσ−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}
=∑r=1iE22ςi−1∘E2i+1F1i−1ε1∘λ(1⋯2i+1)∘λ(2i⋯i+r)∘λ(1⋯r)∘E2iF1iσ−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} =∑1≤r≤i1≤s<iE22ςi−2∘E2iF1i−2ε1∘λ(2⋯s+1)(2i−1⋯i+s)∘E2iF1i−1ε1E1∘λ(1⋯r)(2i⋯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)}
=∑1≤r≤i1≤s<iE22ςi−2∘E2iF1i−2ε1∘E2iF1i−1ε1E1∘λ(2​i+1,2​i+2)∘λ(2⋯s+1)(2i−1⋯i+s)∘λ(1⋯r)(2i⋯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)}
=∑1≤r≤i1≤s<iE22ςi−2∘E2iF1i−2ε1∘E2iF1i−1ε1E1∘λ(2​i−1,2​i)∘λ(2⋯s+1)(2i−1⋯i+s)∘λ(1⋯r)(2i⋯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)}
=∑1≤s<r≤iE22ςi−2∘E2iF1i−2ε1∘E2iF1i−1ε1E1∘λ(2⋯s+1)∘λ(1⋯r)∘λ(2i⋯i+s)∘λ(2i⋯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)}
=∑1≤r′≤s′≤iE22ςi−2∘E2iF1i−2ε1∘E2iF1i−1ε1E1∘λ(2⋯r′+1)∘λ(1⋯s′+1)∘λ(2i⋯i+r′)∘λ(2i⋯i+s′+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=E2E1ςi∘λ(2⋯2i+2)∘λ(1⋯2i+1)∘E2iF1iσ−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} =∑r=1iE2E1ςi−1∘λ(2⋯2i)∘E2iF1i−1ε1E1∘λ(1⋯r)(2i⋯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)}
=∑r=1iE2E1ςi−1∘λ(2⋯2i)∘E2iF1i−1E1ε1∘λ(2​i,2​i+1)∘λ(1⋯r)(2i⋯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)}
=∑r=1iE2E1ςi−1∘E2iF1i−1E1ε1∘λ(2⋯2i+1)∘λ(1⋯r)(2i⋯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} =∑r=1iE1E2ςi−1∘E1E2iF1i−1ε1∘λ(2⋯r+1)∘λ(2i+1⋯i+r+1)∘λ(1⋯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)}
=∑r=1iE1E2ςi−1∘E1E2iF1i−1ε1∘λ(1⋯2i+2)∘λ(1⋯r)∘λ(2i⋯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)}
=∑r=1iE1E2ςi−1∘λ(1⋯2i)∘E2iF1i−1E1ε1∘λ(2​i,2​i+1)∘λ(2​i+1,2​i+2)∘λ(1⋯r)∘λ(2i⋯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)}
=∑r=1iE1E2ςi−1∘λ(1⋯2i)∘E2iF1i−1ε1E1∘λ(2​i+1,2​i+2)∘λ(2​i+1,2​i+2)∘λ(1⋯r)∘λ(2i⋯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} =E12ςi∘λ(2⋯2i+2)∘λ(1⋯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)}
=E12ςi∘λ(1⋯2i+2)∘λ(1⋯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 τ\tau defines an endomorphism of E2​(m,ς)E^{2}(m,\varsigma) for all (m,ς)∈Δλ​𝒲(m,\varsigma)\in\Delta_{\lambda}{\mathcal{W}}. The functor Γ\Gamma is faithful, Γ​E2=E2​Γ\Gamma E^{2}=E^{2}\Gamma (Lemma 4.4.13) and τ\tau commutes with Γ\Gamma. It follows that τ\tau is functorial.

Theorem 4.3.8 has the following consequence.

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Theorem 4.4.15. The data (Δλ​𝒲,E,τ)(\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 τ\tau.

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

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

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2