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Coupled reduced Einstein–Maxwell local evolution

Statement

Assume ACω. Let s≥5 be an integer and let U=(gab,pab,qabi,ei,bi) be the finite-dimensional first-order state on the 2π-periodic three-torus, with pab=∇ˉ0gab and qabi=∇ˉigab for a fixed smooth background connection ∇ˉ. The component Sobolev spaces Hs are those of Periodic high-Sobolev state spaces. Assume an open admissible state set O on which g is Lorentzian, g00<0, the inverse spatial block (gij) is positive definite, the lapse is positive, and the chosen state variables and coefficients are smooth. Let K⋐int⁡K′⋐O be compact sets and R≥0. Assume the draft local symmetric-hyperbolic supplier Exact periodic positive symmetric-hyperbolic supplier with its stated integer-s, coefficient, compact-state, choice and norm hypotheses. Then the harmonic-coordinate reduced Einstein equation with source Tab=μ0−1(FacFbc−14gabFcdFcd), coupled to the six source-free Maxwell field-strength evolution equations, is a smooth quasilinear symmetric-hyperbolic system. For every initial state U0∈Hs taking values in K and satisfying ∥U0∥Hs≤R, its reduced system has a local solution with the regularity and compact-state bounds of Exact periodic positive symmetric-hyperbolic supplier. No Einstein or Maxwell constraint is assumed in this reduced-system statement.

Facts & Assumptions

Given: The fixed source-free Einstein–Maxwell equations, the positive symmetric Maxwell reduction, a smooth background connection, the admissible compact state sets, and the draft local solver interface.

[L1]

Draft definition Electrovacuum tensor Cauchy system fixes the curvature/sign convention, κ>0, μ0>0, Λ∈R, the trace-free Maxwell stress Tab=μ0−1Qab(g,F), and the equations Gab+Λgab=κTab, dF=d⋆gF=0. The item file is listed in batch 6; its status is draft and its verification precheck is pending; this use is conditional on the actual draft statement.

[L2]

Draft periodic-state definition Periodic high-Sobolev state spaces uses T2π3=R3/(2πZ)3 and the real componentwise Fourier norm ∥u∥Hs2=∑k∈Z3(1+∣k∣2)s∣u^(k)∣2, under ACω. Its item file is listed in batch 6; its status is draft and its verification precheck is pending; this use remains conditional on that actual draft.

[L3]

Draft result Exact periodic positive symmetric-hyperbolic supplier: for s≥5, smooth periodic symmetric matrices Aμ and smooth B on an open finite-dimensional state set, a time matrix uniformly positive on compact admissible neighborhoods, and bounded Hs initial data valued in K⋐int⁡K′, there is a common T>0 and a solution on (−T,T) with L∞Hs∩CHs−1, ∂sU∈L∞Hs−1 and values in K′. Its proof applies the current GR existence, uniqueness/stability and smooth-persistence suppliers. The draft file is listed in batch-6 inventory and its precheck is pending; this conclusion remains conditional.

[F1]

Positive symmetric Maxwell field-strength reduction gives the six-dimensional Maxwell principal block S(ξ), which is symmetric, has norm ∣ξ∣, and has positive time matrix α−1I6.

[L4]

Principal part of the reduced Einstein operator and its first-order symmetric hyperbolic reduction gives the reduced metric wave block with time matrix diag⁡(I,−g00I,gijI) and states that a smooth algebraic stress map of additional first-order matter variables introduces no metric principal-derivative coupling.

[L5]

Draft initial-data interface Harmonic initial data relative to a fixed smooth background uses a fixed smooth positive reference γ and sets gij=hij, g00=−1, g0i=0, ∂0gij=2Kij, ∂0g00=−2tr⁡hK, and ∂0g0i=hijhkℓ(Γ(h)jkℓ−Γ(γ)jkℓ). Its actual proof gives the required H=0 and Hs regularity. The item file is listed in batch 6 and its precheck is pending; this use remains conditional.

Proof

1.1givenL4F1algebra

In the admissible open state set, g00<0 and (gij)>0 make the metric time matrix in [L4] positive definite. On a compact K′, its least eigenvalue is bounded below by a positive constant. The lapse condition gives the Maxwell time matrix α−1I6>0, also uniformly on K′. Therefore the combined time matrix is the block sum of these two positive matrices.

1.2givenL1F1L4algebra

For a spatial covector ξ, the metric wave spatial matrices are symmetric by [L4], while the Maxwell spatial matrices are symmetric by [F1]; the shift contributes a scalar identity block and preserves symmetry. The Einstein stress Q(g,F) is algebraic in (g,g−1,F), so its components contain no derivatives of U. The Maxwell tetrad and Hodge coefficients depend smoothly on (g,g−1), and their derivatives multiply only the state components; because p,q are included in U, these are smooth zero-order terms. There are no off-diagonal derivative blocks between the metric and Maxwell equations.

2.1step 1.1step 1.2givenL2L3L5construct∎

Keep the arbitrary compact sets K⋐int⁡K′⋐O and bound R fixed as in the Statement. Steps 1.1–1.2 verify the coefficient hypotheses throughout O, so they hold on a neighborhood of this K′, independently of any particular initial jet. Choose a compact time slab containing zero in its interior and lying inside the smooth background's time domain. On its product with the torus and K′, smoothness bounds each coefficient derivative and compactness gives a uniform positive lower bound for the combined time matrix. Every U0 in the Statement belongs to the bounded class of [L2]; thus [L3] applies to these same K,K′,R and gives a common local interval and the asserted bounds for every such U0. The orthogonal harmonic jet in [L5] is included whenever it belongs to this bounded class, but no harmonic, derivative-compatibility, Einstein or Maxwell constraint is required for the reduced solver.

Depends on

Dependency tree · 2 levels

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