ScalingStacks

Proposition 6.27 . [02WL]

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Proposition 6.27.

With the previous hypothesis and notations, the equality

(6.28) hL¯1tor⁡(XΣ1)=(d+1)!​λK​∫H∨​(ΔΨ)(A∗​ψL¯,s)∨​d​volM1=(d+1)!​λK​∫H∨​(ΔΨ)H∗∨​(ψL¯,s∨−u)​d​volM1\operatorname{h}^{\operatorname{tor}}_{{\overline{L}}_{1}}(X_{\Sigma_{1}})=(d+1)!\lambda_{K}\int_{H^{\vee}(\Delta_{\Psi})}(A^{\ast}\psi_{{\overline{L}},s})^{\vee}\,\text{\rm d}\operatorname{vol}_{M_{1}}\\ =(d+1)!\lambda_{K}\int_{H^{\vee}(\Delta_{\Psi})}H^{\vee}_{\ast}(\psi^{\vee}_{{\overline{L}},s}-u)\,\text{\rm d}\operatorname{vol}_{M_{1}}

holds. Moreover

(6.29) hL¯1tor⁡(XΣ1)−hL¯tor⁡(Y)=(d+1)!​λK​∫H∨​(ΔΨ)(A∗​Ψ)∨​d​volM1=(d+1)!​∫H∨​(ΔΨ)H∗∨​(ιΔΨ−λK​u)​d​volM1,\operatorname{h}^{\operatorname{tor}}_{{\overline{L}}_{1}}(X_{\Sigma_{1}})-\operatorname{h}^{\operatorname{tor}}_{{\overline{L}}}(Y)=(d+1)!\lambda_{K}\int_{H^{\vee}(\Delta_{\Psi})}(A^{\ast}\Psi)^{\vee}\,\text{\rm d}\operatorname{vol}_{M_{1}}\\ =(d+1)!\int_{H^{\vee}(\Delta_{\Psi})}H^{\vee}_{\ast}(\iota_{\Delta_{\Psi}}-\lambda_{K}u)\,\text{\rm d}\operatorname{vol}_{M_{1}},

where ιΔΨ\iota_{\Delta_{\Psi}} is the indicator function of ΔΨ\Delta_{\Psi} (Example 3.16).

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