ScalingStacks

Proof. [02SL]

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Proof.

To prove equation (4.104) we may assume that mΛ=0m_{\Lambda}=0 and lΛ=0l_{\Lambda}=0. Let u∈N~​(Λ)ℝu\in{\widetilde{N}}(\Lambda)_{\mathbb{R}}. Then, the function c⁡(ψ)|π~Λ−1​(u)\operatorname{c}(\psi)|_{{\widetilde{\pi}}^{-1}_{\Lambda}(u)} is concave. Let Λ′∈Π\Lambda^{\prime}\in\Pi such that Λ\Lambda is a face of Λ′\Lambda^{\prime} and π~Λ−1​(u)∩c⁡(Λ′)≠∅{\widetilde{\pi}}^{-1}_{\Lambda}(u)\cap\operatorname{c}(\Lambda^{\prime})\not=\emptyset. Then, π~Λ−1​(u)∩c⁡(Λ′){\widetilde{\pi}}^{-1}_{\Lambda}(u)\cap\operatorname{c}(\Lambda^{\prime}) is a polyhedron of maximal dimension of π~Λ−1​(u){\widetilde{\pi}}^{-1}_{\Lambda}(u) and the restriction of c⁡(ψ)\operatorname{c}(\psi) to this polyhedron is constant and, by equation (4.90), agrees with ψ​(Λ)​(u)\psi(\Lambda)(u). Therefore, by concavity,

(π~Λ)∗​c⁡(ψ)​(u)=maxv∈πσ−1​(u)​c​(ψ)​(v),({\widetilde{\pi}}_{\Lambda})_{\ast}\operatorname{c}(\psi)(u)=\max_{v\in\pi^{-1}_{\sigma}(u)}\operatorname{c}(\psi)(v),

agrees with ψ​(Λ)​(u)\psi(\Lambda)(u). This proves equation (4.104).

Back in the general case when mΛm_{\Lambda} and lΛl_{\Lambda} may be different from zero, by Proposition 3.78, Proposition 3.40(4) and Lemma 4.102 we have

stab⁡((π~Λ)∗​(c⁡(ψ−mΛ−lΛ)))\displaystyle\operatorname{stab}(({\widetilde{\pi}}_{\Lambda})_{\ast}(\operatorname{c}(\psi-m_{\Lambda}-l_{\Lambda}))) =(π~Λ∨)−1​stab⁡(c⁡(ψ−mΛ−lΛ))\displaystyle=({\widetilde{\pi}}^{\vee}_{\Lambda})^{-1}\operatorname{stab}(\operatorname{c}(\psi-m_{\Lambda}-l_{\Lambda}))
=(π~Λ∨)−1​(stab⁡(c⁡(ψ))−(mΛ,lΛ))\displaystyle=({\widetilde{\pi}}^{\vee}_{\Lambda})^{-1}(\operatorname{stab}(\operatorname{c}(\psi))-(m_{\Lambda},l_{\Lambda}))
=(π~Λ∨+(mΛ,lΛ))−1​stab⁡(c⁡(ψ))\displaystyle=({\widetilde{\pi}}^{\vee}_{\Lambda}+(m_{\Lambda},l_{\Lambda}))^{-1}\operatorname{stab}(\operatorname{c}(\psi))
=(π~Λ∨+(mΛ,lΛ))−1​epi⁡(−ψ∨).\displaystyle=({\widetilde{\pi}}^{\vee}_{\Lambda}+(m_{\Lambda},l_{\Lambda}))^{-1}\operatorname{epi}(-\psi^{\vee}).

The remaining statements are clear. ∎

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