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Verified constant-density static star and vacuum exterior

Physical scope

Exact constant-density family in the adopted static Lambda=0 model for 0<u<8/9, including regular center and explicit C1 piecewise-C2 vacuum matching; the bound is family-specific, with no realistic causal EOS, general Buchdahl conclusion, empirical claim, or stability result.

Statement

Assume the constant-density preparation Specified constant-density star and vacuum boundary model and the exact ZF+ACω mathematical convention used by Exact regular constant-density solution with verified matching. Put a=1−u and B(r)=1−ur2/R2. For 0≤r≤R, the adopted model has the explicit profiles M(r)=MR(r/R)3,b(r)=B(r)2,P(r)=ε0B(r)−a3a−B(r),eϕ(r)=3a−B(r)2. For r≥R, set M(r)=MR, b(r)=1−2GMR/(c2r), P(r)=0, ε(r)=0, and eϕ(r)=b(r). Then the interior is a regular static Einstein-fluid solution through the center, the exterior is vacuum, and the join at r=R is C1 and piecewise C2 with no delta-supported surface stress. The central pressure is finite and equals P(0)=ε0(1−a)/(3a−1). This conclusion is specific to the constant-density branch 0<u<8/9.

Facts & Assumptions

Given: The constant-density EOS, ρ0>0, R>0, u∈(0,8/9), the adopted static Einstein-fluid model, and the exact current mathematical supplier under ZF+ACω.

[F1]

Specified constant-density star and vacuum boundary model supplies ε0=ρ0c2, MR=4πρ0R3/3, u=2GMR/(c2R)∈(0,8/9), and the constant EOS on IP=(0,∞) together with its smooth extension E^ to an open interval containing zero, so the interior boundary value P(R)=0 is defined. It prescribes the vacuum exterior separately from the fluid EOS.

[F2]

Exact regular constant-density solution with verified matching: under those parameters and the geometry of Smooth static spherical geometry and state domain, the displayed M,b,P,eϕ solve the interior Einstein/conservation equations, extend to a C2 Cartesian center, and match to the exterior at r=R as a C1 piecewise-C2 metric with no distributional surface stress; the bound is only for this family.

[A1]

The Einstein equation and constant-density boundary preparation in [F1] are adopted physical premises, not observations.

Proof

1.1givenF1algebra

Since u<8/9, a=1−u>1/3. For 0≤r≤R, a≤B(r)≤1, so b=B2>0 and 3a−B(r)≥3a−1>0. Thus the stated interior pressure and lapse are finite, P(R)=0, and P(0)=ε0(1−a)/(3a−1).

2.1A1F1F2step 1.1∎

The inputs in [F1] meet the hypotheses of [F2] exactly. That mathematical result verifies the mass, lapse, pressure, and vacuum equations and the regular center and interface; therefore these fields solve the adopted physical model. The discontinuous density at the boundary is part of the stated piecewise model, and the verified C1 matching supplies no delta-supported surface stress.

Depends on

Dependency tree · 2 levels

Sources