ScalingStacks

Proof of Lemma 3.4 . [01A5]

Original official author HTML, exact retained edition. Historical TeX conversion verdicts remain unchanged. Cited-edition alignment and mathematical self-containment are not assessed.

Complete original source context · Original author HTML

Proof of Lemma 3.4.

Note first that ψ\psi may be assumed to be a model function by

Lemma 3.5.

Let ν\nu be a positive Radon measure on XX and let φ\varphi be a bounded θ\theta-psh function. Then we have

∫φ​ν=infψ≥φ∫ψ​ν\int\varphi\nu=\inf_{\psi\geq\varphi}\int\psi\nu

where ψ\psi ranges over all θ\theta-psh model functions such that ψ≥φ\psi\geq\varphi.

Since we already know that (φ1,…,φp)↦M⁡(φ1,…,φp)(\varphi_{1},\dots,\varphi_{p})\mapsto\MAC(\varphi_{1},\dots,\varphi_{p}) is continuous along decreasing nets, we may by regularization assume that all φi\varphi_{i} and χi\chi_{i} are also model functions. Integration by parts (3.1) then yields

∫ψ​M⁡(χ1,χ2,…,χp)−∫ψ​M⁡(φ1,χ2,…,χp)==∫(χ1−φ1)​M⁡(ψ,χ2,…,χp)−∫(χ1−φ1)​M⁡(0,χ2,…,χp)\int\psi\MAC(\chi_{1},\chi_{2},\dots,\chi_{p})-\int\psi\MAC(\varphi_{1},\chi_{2},\dots,\chi_{p})=\\ =\int(\chi_{1}-\varphi_{1})\MAC(\psi,\chi_{2},\dots,\chi_{p})-\int(\chi_{1}-\varphi_{1})\MAC(0,\chi_{2},\dots,\chi_{p})

hence

∫ψ​M⁡(χ1,…,χp)≥∫ψ​M⁡(φ1,χ2,…,χp)+∫(φ1−χ1)​M⁡(0,χ2,…,χp).\int\psi\MAC(\chi_{1},\dots,\chi_{p})\geq\int\psi\MAC(\varphi_{1},\chi_{2},\dots,\chi_{p})+\int(\varphi_{1}-\chi_{1})\MAC(0,\chi_{2},\dots,\chi_{p}).

We similarly have

∫ψ​M⁡(φ1,χ2,χ3,…,χp)\displaystyle\int\psi\MAC(\varphi_{1},\chi_{2},\chi_{3},\dots,\chi_{p}) ≥∫ψ​M⁡(φ1,φ2,χ3,…,χp)\displaystyle\geq\int\psi\MAC(\varphi_{1},\varphi_{2},\chi_{3},\dots,\chi_{p})
+∫(φ2−χ2)M(φ1,0,χ3,…,χp).\displaystyle+\int(\varphi_{2}-\chi_{2})\MAC(\varphi_{1},0,\chi_{3},\dots,\chi_{p}).

Iterating this argument and summing up then yields the desired result. ∎

Original mathematics by the credited authors. Source-backed reader collection; mathematical self-containment is not assessed.