ScalingStacks

Proof. [04NY]

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Proof.

By Eq. 1.2.4 we have ui∞=−ui0−∑m∈Lσ​σ′(C⋅Dm)​umu_{i_{\infty}}=-u_{i_{0}}-\sum_{m\in L_{\sigma\sigma^{\prime}}}(C\cdot D_{m})u_{m}, so

for i∈Lσ​σ′, Wiσ′\displaystyle\textrm{for $i\in L_{\sigma\sigma^{\prime}}$, }\quad W^{\sigma^{\prime}}_{i} =−det(Δ,(ul)l∈Lσ​σ′∖{i},ui∞)det(ui,(ul)l∈Lσ​σ′∖{i},ui∞)\displaystyle=-\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{\infty}})}{\det(u_{i},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{\infty}})}
=−det(Δ,(ul)l∈Lσ​σ′∖{i},ui0)det(ui,(ul)l∈Lσ​σ′∖{i},ui0)−∑m∈Lσ​σ′(C⋅Dm)​det(Δ,(ul)l∈Lσ​σ′∖{i},um)det(ui,(ul)l∈Lσ​σ′∖{i},ui0)\displaystyle=-\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{0}})}{\det(u_{i},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{0}})}-\sum_{m\in L_{\sigma\sigma^{\prime}}}(C\cdot D_{m})\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{m})}{\det(u_{i},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{0}})}
=Wiσ−(C⋅Di)​det(Δ,(ul)l∈Lσ​σ′∖{i},ui)det(ui,(ul)l∈Lσ​σ′∖{i},ui0)=Wiσ−(C⋅Di)​Wi0σ;\displaystyle=W^{\sigma}_{i}-(C\cdot D_{i})\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i})}{\det(u_{i},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{0}})}=W^{\sigma}_{i}-(C\cdot D_{i})W^{\sigma}_{i_{0}};
for i=i∞, Wi∞σ′\displaystyle\textrm{for $i=i_{\infty}$, }\quad W^{\sigma^{\prime}}_{i_{\infty}} =det(Δ,(ul)l∈Lσ​σ′)det(ui∞,(ul)l∈Lσ​σ′)=−det(Δ,(ul)l∈Lσ​σ′)det(ui0,(ul)l∈Lσ​σ′)=−Wi0σ.\displaystyle=\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}})}{\det(u_{i_{\infty}},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}})}=-\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}})}{\det(u_{i_{0}},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}})}=-W^{\sigma}_{i_{0}}.

For j∈Jj\in J

∑i∈Lσ′λj,i​Wiσ′\displaystyle\sum_{i\in L_{\sigma^{\prime}}}\lambda_{j,i}W^{\sigma^{\prime}}_{i} =−λj,i∞​Wi0σ+∑i∈Lσ​σ′λj,i​(Wiσ−(C⋅Di)​Wi0σ)\displaystyle=-\lambda_{j,i_{\infty}}W^{\sigma}_{i_{0}}+\sum_{i\in L_{\sigma\sigma^{\prime}}}\lambda_{j,i}\left(W^{\sigma}_{i}-(C\cdot D_{i})W^{\sigma}_{i_{0}}\right)
=(−λj,i∞−∑i∈Lσ​σ′λj,i​(C⋅Di)−λj,i0)​Wi0σ+∑i∈Lσλj,i​Wiσ\displaystyle=\Big(-\lambda_{j,i_{\infty}}-\sum_{i\in L_{\sigma\sigma^{\prime}}}\lambda_{j,i}(C\cdot D_{i})-\lambda_{j,i_{0}}\Big)W^{\sigma}_{i_{0}}+\sum_{i\in L_{\sigma}}\lambda_{j,i}W^{\sigma}_{i}
=(C⋅Dj)Wi0σ+∑i∈Lσλi,jWiσby Eq. 2.1.7\displaystyle=(C\cdot D_{j})W^{\sigma}_{i_{0}}+\sum_{i\in L_{\sigma}}\lambda_{i,j}W^{\sigma}_{i}\hskip 30.0pt\textrm{by \lx@cref{creftype~refnum}{equ fan}}
Wjσ′\displaystyle W^{\sigma^{\prime}}_{j} =−Dj−∑l∈Lλj,l​Dl−∑i∈Lσ′λj,i​Wiσ′\displaystyle=-D_{j}-\sum_{l\in L}\lambda_{j,l}D_{l}-\sum_{i\in L_{\sigma^{\prime}}}\lambda_{j,i}W^{\sigma^{\prime}}_{i}
=−Dj−∑l∈Lλj,l​Dl−∑i∈Lσλj,i​Wiσ−(C⋅Dj)​Wi0σ=Wjσ−(C⋅Dj)​Wi0σ.\displaystyle=-D_{j}-\sum_{l\in L}\lambda_{j,l}D_{l}-\sum_{i\in L_{\sigma}}\lambda_{j,i}W^{\sigma}_{i}-(C\cdot D_{j})W^{\sigma}_{i_{0}}=W^{\sigma}_{j}-(C\cdot D_{j})W^{\sigma}_{i_{0}}.

These relations can be summed up as (Wiσ′Wi∞σ′Wjσ′)=Mℬ′​ℬ​(WiσWi0σWjσ)\left(\begin{matrix}W^{\sigma^{\prime}}_{i}\\ W^{\sigma^{\prime}}_{i_{\infty}}\\ W^{\sigma^{\prime}}_{j}\end{matrix}\right)=M_{\mathcal{B}^{\prime}\mathcal{B}}\left(\begin{matrix}W^{\sigma}_{i}\\ W^{\sigma}_{i_{0}}\\ W^{\sigma}_{j}\end{matrix}\right), i.e. Wσ′=(Mℬ′​ℬ⊗Id)WσW^{\sigma^{\prime}}=(M_{\mathcal{B}^{\prime}\mathcal{B}}\otimes\Id)W^{\sigma}. ∎

Original source context: S2.SS1.E7

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