ScalingStacks

Proof. [04NV]

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Proof.

We show that siΟƒs^{\sigma}_{i} is an equation for DiD_{i} on 𝔛σ\mathfrak{X}_{\sigma}; the proof is analogous for sjΟƒs^{\sigma}_{j}.

On ZZ, Wiσ|Z=div(h){W_{i}^{\sigma}}_{|Z}=\textrm{div}(h) and siσs^{\sigma}_{i} is a non-zero global section, which means that

β„’iΟƒ|Z(Z)=π’ͺZ(WiΟƒ)(Z)={fβˆˆπ’¦(Z)|div(f)+div(h)β©Ύ0}\displaystyle{\mathscr{L}^{\sigma}_{i}}_{|Z}(Z)=\mathcal{O}_{Z}({W^{\sigma}_{i}})(Z)=\{f\in\mathcal{K}(Z)\,|\,\textrm{div}(f)+\textrm{div}(h)\geqslant 0\} →≃π’ͺZ​(Z)=k\displaystyle\xrightarrow{\simeq}\mathcal{O}_{Z}(Z)=k
f\displaystyle f ↦f​h\displaystyle\mapsto fh
siΟƒ\displaystyle s^{\sigma}_{i} ↦siσ​h=λ∈kΓ—.\displaystyle\mapsto s^{\sigma}_{i}h=\lambda\in k^{\times}.

Let 𝒰\mathcal{U} be an open cover of π’³βˆ–(βˆͺiβ€²βˆ‰JβˆͺLΟƒDiβ€²)\mathscr{X}\setminus\big(\cup_{i^{\prime}\notin J\cup L_{\sigma}}D_{i^{\prime}}\big) such that Di|U=div(gU){D_{i}}_{|U}=\textrm{div}(g_{U}) for any Uβˆˆπ’°U\in\mathcal{U}; this is possible as DiD_{i} is a Cartier divisor. On UU, WiΟƒ|U=βˆ’Di|U=div(gUβˆ’1){W^{\sigma}_{i}}_{|U}=-{D_{i}}_{|U}=\textrm{div}(g_{U}^{-1}) and

β„’iσ​(π”›Οƒβˆ©U)\displaystyle\mathscr{L}^{\sigma}_{i}(\mathfrak{X}_{\sigma}\cap U) →≃π’ͺ𝔛σ​(π”›Οƒβˆ©U)\displaystyle\xrightarrow{\simeq}\mathcal{O}_{\mathfrak{X}_{\sigma}}(\mathfrak{X}_{\sigma}\cap U)
f\displaystyle f ↦f​gUβˆ’1\displaystyle\mapsto fg_{U}^{-1}
siΟƒ\displaystyle s^{\sigma}_{i} ↦siσ​gUβˆ’1∈π’ͺ𝔛σ×​(π”›Οƒβˆ©U),\displaystyle\mapsto s^{\sigma}_{i}g_{U}^{-1}\in\mathcal{O}_{\mathfrak{X}_{\sigma}}^{\times}(\mathfrak{X}_{\sigma}\cap U),

where siσ​gUβˆ’1s^{\sigma}_{i}g_{U}^{-1} is a regular invertible function on π”›Οƒβˆ©U\mathfrak{X}_{\sigma}\cap U, as its reduction to ZZ is invertible. Finally, the section siΟƒs^{\sigma}_{i} is defined globally on 𝒳/Z^\widehat{\mathscr{X}_{/Z}} and on each open π”›Οƒβˆ©U\mathfrak{X}_{\sigma}\cap U gives a local equation of the divisor DiD_{i}, hence it is a equation for DiD_{i} on 𝔛σ\mathfrak{X}_{\sigma}. ∎

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