ScalingStacks

0P6A

Proof. We have

E1​λ∘ρ​E2∘F1​σ=E_{1}\lambda\circ\rho E_{2}\circ F_{1}\sigma=
=E1​E2​F1​ε1∘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​ε1∘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​ε1∘E1​λ​F1​E1∘E1​F1​λ​E1∘E1​τ1​E2​E1∘η1​F1​E2​E1∘ε1​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​ε1∘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​ε1∘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​ε1∘E1​E2​F1​ε1​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​ε1∘E1​E2​F1​ε1​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​ε1∘E1​E2​F1​ε1​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∘E2​ρ∘λ​E1.\displaystyle=\sigma F_{1}\circ E_{2}\rho\circ\lambda E_{1}.

We have

ρ​F1∘F1​ρ∘τ1​E1\displaystyle\rho F_{1}\circ F_{1}\rho\circ\tau_{1}E_{1} =ε1​E1​F12∘F1​ε1​E12​F12∘τ1​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}
=ε1​E1​F12∘F1​ε1​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}
=ε1​E1​F12∘F1​ε1​E12​F12∘F12​(τ1​E1∘E1​τ1∘τ1​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}
=ε1​E1​F12∘F1​ε1​E12​F12∘F12​(E1​τ1∘τ1​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}
=ε1​E1​F12∘F1​ε1​E12​F12∘F12​(E1​τ1∘τ1​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​τ1∘ρ​F1∘F1​ρ.\displaystyle=E_{1}\tau_{1}\circ\rho F_{1}\circ F_{1}\rho.

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

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2