Proposition

Corollary 10 ([Strict direction for compact variations]). On the original weakly asymptotically flat exterior, choose a smooth majorant B≥|K| equal to Cr^ -1-q far out and apply Lemma 9 ([The decaying Neumann problem and strictification]). …

Corollary 10 ([Strict direction for compact variations]). On the original weakly asymptotically flat exterior, choose a smooth majorant B≥|K| equal to Cr-1-q far out and apply Lemma 9 ([The decaying Neumann problem and strictification]). Consider the tangent direction (g',K',α',Dm')=(2φg,φK,0,0) at purely electric data, transporting v by the metric square root. On an active ray μm+Jm(v)=0 , the derivative C'=2(μm+Jm(v))' satisfies C' =2k(-Δφ+K(∇φ,v)) +4(n-2)cn2φ|E|2 ≥2kρ0, C'/ρ0⟶2k. At a marginal boundary θ+'=-k . The energy derivative is finite, the momentum derivative is zero, and φ=O2(r2-n ) .

Prove 1Disprove 0Cited as proposition 1Chain graphAdd Your Proof

Add Your Proof1

Prove
A smooth radial majorant on the end can be patched to a sufficiently large smooth function on the core; it need not reproduce higher derivatives of K . Differentiate and . The derivative of the overall factor e^ -2δφ multiplies the active value zero. The drift term is O(r^ -n-q ) , and the electric term divided by ρ_0 tends to zero. The assertions now follow from , , and .