ScalingStacks

0P6I

Proof. We have

d⁡((ςi′)11)\displaystyle d((\varsigma^{\prime}_{i})_{11}) =E2ςi∘d(τ2E2i−1∘⋯∘E2i−1τ2)F1i∘λ(i+1⋯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)}
=∑r=1iE2ςi∘λ(1⋯r)(r+1⋯i+1)∘λ(i+1⋯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)}
=∑r=1iE2ςi∘λ(1⋯r)(r+1⋯i+1)∘λ(i+1⋯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)}
=∑r=1iE2ςi∘λ(1⋯r)(2i+1⋯i+r+1)∘λ(i+1⋯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)}
=E2ςi∘λ(1⋯i)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(1\cdots i)}
(ςi′)12∘E2i​F1i​π=(\varsigma^{\prime}_{i})_{12}\circ E_{2}^{i}F_{1}^{i}\pi=
=∑r=1iE2ςi−1∘E2iF1i−1ς1∘λ(2​i,2​i+1)∘E2iF1i−1ε1F1E2∘E2iF1iη1E2∘λ(1⋯r)(2i⋯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)}
=∑r=1iE2ςi∘λ(i+1⋯2i)∘λ(2​i,2​i+1)∘λ(1⋯r)(2i⋯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)}
=E2ςi∘λ(1⋯i)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(1\cdots i)}
=d⁡((ςi′)11).\displaystyle=d((\varsigma^{\prime}_{i})_{11}).
d⁡((ςi′)22)\displaystyle d((\varsigma^{\prime}_{i})_{22}) =E1ςi∘λ(1⋯i+1)∘E2id(ρF1i−1∘F1ρF1i−2∘⋯∘F1i−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)
=∑r=1iE1ςi∘λ(1⋯i+r)∘E2iF1r−1η1F1i−r∘E2iF1r−1ε1F1i−r∘λ(i+r+1⋯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)}
=∑r=1iE1ςi∘λ(i+r+1⋯2)∘η1E2iF1i−1∘E2iF1i−1ε1∘λ(2i⋯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)}
=∑r=1iE1ςi∘λ(i+r+1⋯i+2)∘λ(i+2⋯2)∘η1E2iF1i−1∘E2iF1i−1ε1∘λ(2i⋯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)}
=∑r=1iE1ςi∘λ(2⋯r+1)∘λ(i+2⋯2)∘η1E2iF1i−1∘E2iF1i−1ε1∘λ(2i⋯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)}
=E1ςi∘λ(i+2⋯2)∘η1E2iF1i−1∘E2iF1i−1ε1∘λ(2i⋯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)}
π∘(ςi′)12\displaystyle\pi\circ(\varsigma^{\prime}_{i})_{12} =∑r=1iE1ς1∘λ(12)∘E2η1∘E2ςi−1∘E2iF1i−1ε1∘λ(1⋯r)(2i⋯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)}
=∑r=1iE1ς1∘λ(23)∘η1E2∘E2ςi−1∘E2iF1i−1ε1∘λ(1⋯r)(2i⋯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)}
=∑r=1iE1ς1∘E1E2F1ςi−1∘λ23∘η1E2iF1i−1∘E2iF1i−1ε1∘λ(1⋯r)(2i⋯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)}
=∑r=1iE1ςi∘λ(i+2⋯3)∘λ23∘λ(3⋯r+2)∘η1E2iF1i−1∘E2iF1i−1ε1∘λ(2i⋯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)}
=E1ςi∘λ(i+2⋯2)∘η1E2iF1i−1∘E2iF1i−1ε1∘λ(2i⋯i+r)=d((ςi′)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⁡((ςi′)12)=A+Bd((\varsigma^{\prime}_{i})_{12})=A+B

where

A\displaystyle A =∑1≤s<r≤iE2ςi−1∘E2iF1i−1ε1∘λ(1⋯s)(s+1⋯r)(2i⋯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)}
=∑1≤s<r≤iE2ςi−1∘λ(s+1⋯r)∘E2iF1i−1ε1∘λ(1⋯s)(2i⋯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)}
=∑1≤s<r≤iE2ςi−1∘λ(i+r−1⋯s+i)∘E2iF1i−1ε1∘λ(1⋯s)(2i⋯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)}
=∑1≤s<r≤iE2ςi−1∘E2iF1i−1ε1∘λ(1⋯s)(2i⋯i+r)(i+r−1⋯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=∑1≤r′≤i1≤s′≤i−r′E2ςi−1∘E2iF1i−1ε1∘λ(1⋯r′)(2i⋯i+r′+s′)(i+r′+s′−1⋯i+r′)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⁡((ςi′)12)=0d((\varsigma^{\prime}_{i})_{12})=0.

We have shown that d⁡(ςi′)=0d(\varsigma^{\prime}_{i})=0,

Fix r∈{1,…,i}r\in\{1,\ldots,i\}. We put br=E2ςi−1∘E2iFi−1ε1∘λ(1⋯r)(2i⋯i+r):E2iF1iE1(m)→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,…,i−1}s\in\{1,\ldots,i-1\}.

If s>rs>r, we have

br​(Ts⊗1)\displaystyle b_{r}(T_{s}\otimes 1) =E2ςi−1∘λ(s,s+1)∘E2iFi−1∘λ(1⋯r)(2i⋯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)}
=E2ςi−1∘λ(i+s−1,i+s)∘E2iFi−1∘λ(1⋯r)(2i⋯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)}
=E2ςi−1∘E2iFi−1∘λ(i+s−1,i+s)λ(1⋯r)(2i⋯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)}
=E2ςi−1∘E2iFi−1∘λ(1⋯r)(2i⋯i+r)λ(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​(1⊗Ts).\displaystyle=b_{r}(1\otimes T_{s}).

If s<r−1s<r-1, we have

br​(1⊗Ts)\displaystyle b_{r}(1\otimes T_{s}) =E2ςi−1∘λ(i+s,i+s+1)∘E2iFi−1∘λ(1⋯r)(2i⋯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)}
=E2ςi−1∘λ(s+1,s+2)∘E2iFi−1∘λ(1⋯r)(2i⋯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)}
=E2ςi−1∘E2iFi−1∘λ(s+1,s+2)∘λ(1⋯r)(2i⋯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)}
=E2ςi−1∘E2iFi−1∘λ(1⋯r)(2i⋯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​(Ts⊗1).\displaystyle=b_{r}(T_{s}\otimes 1).

We have

br(Tr−1⊗1)=E2ςi−1∘E2iFi−1∘λ(1⋯r)(2i⋯i+r)∘λ(r−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(1⊗Tr)=E2ςi−1∘E2iFi−1∘λ(1⋯r)(2i⋯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(1⊗Tr−1)=E2ςi−1∘E2iFi−1∘λ(1⋯r)(2i⋯i+r−1)=br−1(Tr−1⊗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 (ςi)12​(1⊗Ts)=(ςi)12​(Ts⊗1)(\varsigma_{i})_{12}(1\otimes T_{s})=(\varsigma_{i})_{12}(T_{s}\otimes 1).

We have

(ςi′)11​(Ts⊗1)\displaystyle(\varsigma^{\prime}_{i})_{11}(T_{s}\otimes 1) =E2ςi∘λ(s+1,s+2)∘λ(1⋯2i+1)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(s+1,s+2)}\circ\lambda_{(1\cdots 2i+1)}
=E2ςi∘λ(i+s+1,i+s+2)∘λ(1⋯2i+1)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(i+s+1,i+s+2)}\circ\lambda_{(1\cdots 2i+1)}
=E2ςi∘λ(1⋯2i+1)λ(i+s,i+s+1)\displaystyle=E_{2}\varsigma_{i}\circ\lambda_{(1\cdots 2i+1)}\lambda_{(i+s,i+s+1)}
=(ςi′)11​(1⊗Ts).\displaystyle=(\varsigma^{\prime}_{i})_{11}(1\otimes T_{s}).

Similarly,

(ςi′)22​(Ts⊗1)=(ςi′)11​(1⊗Ts).(\varsigma^{\prime}_{i})_{22}(T_{s}\otimes 1)=(\varsigma^{\prime}_{i})_{11}(1\otimes T_{s}).

So ςi​(1⊗Ts)=ςi​(Ts⊗1)\varsigma_{i}(1\otimes T_{s})=\varsigma_{i}(T_{s}\otimes 1).

Let l∈{1,2}l\in\{1,2\}. We have

(ςi+j′)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

(ςi′)l​l∘(ςj′)l​l\displaystyle(\varsigma^{\prime}_{i})_{ll}\circ(\varsigma^{\prime}_{j})_{ll} =Elςi∘ElE2iF1iςj∘λ(1⋅2​i+1)∘λ(2i+1⋯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)}
=Elςi+j∘λw′∘λ(1⋅2​i+1)∘λ(2i+1⋯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 (ςi+j′)l​l∘μi​j=(ςi′)l​l∘(ςj′)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 bl′,l=E2ςl′−1∘E2l′Fl′−1ε1∘λ(1⋯l)(2l′⋯l′+l):E2l′F1l′E1(m)→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↦s−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∘(ςj′)22\displaystyle b_{i,r}\circ(\varsigma^{\prime}_{j})_{22} =E2ςi−1∘E2iF1i−1ςj∘E2iF1i−1ε1E2jF1j∘λ(1⋯r)(2i⋯i+r)∘λ(2i+1⋯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)}
=E2ςi+j−1∘λwi−1,j∘E2iF1i−1ε1E2jF1j∘λ(2i+1⋯2i+2j+1)∘λ(1⋯r)(2i⋯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)}
=E2ςi+j−1∘E2iλwi−1,jF1j∘E2iF1i−1E2jF1j−1ε1∘λ(2i+2j⋯2i)∘λ(1⋯r)(2i⋯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)}
=E2ςi+j−1∘E2iλwi−1,jF1j∘E2iF1i−1E2jF1j−1ε1∘λ(2i+2j⋯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)}
=E2ςi+j−1∘E2i+jF1i+j−1ε1∘E2iλwi−1,jF1j+1E1∘λ(2i+2j⋯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)}
=E2ςi+j−1∘E2i+jF1i+j−1ε1∘λ(2i+2j⋯i+j+r)∘E2iλwi,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

(ςi′)11∘bj,r\displaystyle(\varsigma^{\prime}_{i})_{11}\circ b_{j,r} =E2ςi∘E2i+1F1iςj−1∘λ(1⋯2i+1)∘E2iF1iE2jF1j−1ε1∘λ(2i+1⋯2i+r)(2i+2j⋯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)}
=E2ςi+j−1∘E2i+1λwi,j−1F1j−1∘λ(1⋯2i+1)∘E2iF1iE2jF1j−1ε1∘λ(2i+1⋯2i+r)(2i+2j⋯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)}
=E2ςi+j−1∘E2i+jF1i+j−1ε1∘E2i+1λwi,j−1F1jE1∘λ(1⋯2i+1)∘λ(2i+1⋯2i+r)(2i+2j⋯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)}
=E2ςi+j−1∘E2i+jF1i+j−1ε1∘λ(1⋯i+r)(2i+2j⋯2i+j+r)∘E2iλwi,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,j≥1i,j\geq 1, we have ςi∘E2i​F1i​ςj=ςi+j∘μi,j\varsigma_{i}\circ E_{2}^{i}F_{1}^{i}\varsigma_{j}=\varsigma_{i+j}\circ\mu_{i,j}. ∎

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

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2