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DefinitionDefinition: AI-adaptedProof: Not applicable
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The actual geometric constant in the small-ADM theorem

Definition

For the Radu ADM source choose its chart data A1,R1,ε0, with R1≥max⁡(R0,A14) and ε0>0. Require A1−1∣v∣2≤hijvivj≤A1∣v∣2 on Φ0(E3/4), and differentiated coefficients of the three remainders in its end expansion bounded by A1 (at order m≤6 their weights are rm+1, rm+2 and rm+3 for spatial, temporal and mixed remainders respectively). Supply the source extension chart Φ1:(−ε0,ε0)×E1−ε0→M~, built by interpolation between the slice unit normal and T, agreeing with the stationary chart for r>2R1, and obeying ∑i=13∣g0i∣+∣g00+1∣≤A1/(R1+r). Under J<M02 set A‾ADM=max⁡{R1,ε0−1,(M02−J)−1,sup⁡M~∑m=06(∑a,b=03∣∂mgab∣+∑a=03∣∂mTa∣)}. Here all spacetime coordinate derivatives and components are summed, and the supremum is required finite. The source's quantitative condition is a bound on this actual normalized chart package. It is not a claim that small J alone controls curvature, chart radius, horizon collar width or the distance to extremality.

Facts & Assumptions

[F1]

Radu small-ADM global and bifurcation package fixes the end and charts; The ADM-source mass and angular-momentum parameters fixes M0,J and the mass-one labels. Maximality and smooth boundary in the ADM theorem fixes the original maximal section.

[F2]

Differentiated asymptotic bounds and parameter uniformity defines componentwise spatial Cartesian differentiated decay estimates and uniform constants on the exterior chart.

[F3]

Radu, §1.1, the quantitative-coordinate paragraphs and (1.2)–(1.3), specifies the interpolated chart package and effective constant. The finite supremum of spacetime coordinate derivatives on that chart is an explicit hypothesis of the Definition, to be supplied for each application; it is not inferred from the spatial decay notation in [F2].

Justification

Every term is computed from the specified source chart, metric, field and positive parameters. The strict parameter inequality makes the inverse gap finite, and the explicit supremum condition makes the last term finite. A maximum of this finite list is a unique finite positive number. The ancillary chart and remainder conditions remain part of the package; merely writing down a maximum on an unrelated chart would not instantiate the source theorem. The chart choices and all their bounds must be supplied for each application.

Depends on

Used by · 2

Dependency tree · 2 levels

Each result is drawn at its shortest distance from this item. Arrows run from prerequisites to the items that use them; this item has a heavier outline. External source nodes link directly to the cited text. The view shows up to two dependency steps; open a prerequisite to continue.

External dependencies

Alexandru F. Radu, Rigidity of stationary black holes with small ADM angular momentum · §1.1: setup, GR and (1.1), SBS and the separate maximality paragraph; quantitative-coordinate paragraphs immediately before (1.2), equations (1.2)–(1.3), and Theorem 1.1 for mass-one application.

The quantitative package uses A_1, R_1>=max(R_0,A_1^4), epsilon_0>0, spatial metric comparability on Phi_0(E_{3/4}), and differentiated remainder coefficients bounded by A_1. Its extension Phi_1:(-epsilon_0,epsilon_0) x E_{1-epsilon_0}->Mtilde interpolates between the slice unit normal and T, agrees with the stationary chart for r>2R_1, and satisfies sum_i|g_0i|+|g_00+1|<=A_1/(R_1+r). Equation (1.3) defines Abar as the maximum of R_1, epsilon_0^{-1}, (M^2-J)^{-1} and the supremum on Mtilde of all metric and stationary-field component derivatives through spacetime order six, summed over indices.

Hypotheses: The smooth stationary Ricci-flat four-spacetime with signature (-,+,+,+), source GR/SBS, the given maximal slice with smooth boundary geometry, and J<M^2. Supply the stated chart and quantitative bounds; finite Abar is required for a bounded-geometry application. Theorem 1.1 uses mass-one data. The source M is denoted M_0 locally.

Reading limits: Retrieved arXiv HTML v1 and read §1.1 from the spacetime setup through GR, (1.1), SBS, maximality, the quantitative-coordinate paragraphs, (1.2)–(1.3), and Theorem 1.1 with its adjacent qualification. Used only to check this definition and its application hypotheses. The interpolation construction in reference [5], rigidity proof, and existence of the quantitative package for any particular spacetime were not reviewed or reconstructed.

Sources