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The exterior Schwarzschild charts do not cover the horizon-crossing extension: the regular horizon point (v, r) = (0, s)
Statement refuted
Statement refuted: "Let be the Schwarzschild exterior datum with and let be the horizon-crossing extension of Smooth horizon-crossing extension of the Schwarzschild exterior metric in the advanced chart. Then every point of lies in the image of the exterior datum under the embedding , hence in the domain of some Schwarzschild (product) chart of the datum; equivalently, every point added by the extension is reached at a bounded value of the exterior coordinate ."
The counterexample is the point
on the level set , and the following three facts refute both forms of the statement:
- : the map preserves the function , so for every , whereas .
- is a regular point of a smooth Lorentzian manifold, not a boundary artifact: at one has , the inertia is , and the Kretschmann scalar is , finite and nonzero.
- Every sequence with must have and exterior coordinate , where ; so the exterior coordinate is unbounded along the approach to , and the second form of the statement ("bounded ") fails as well.
Facts & Assumptions
Given: The exterior datum with , its tortoise function on , the extension with chart , the embedding , and the point with .
restricts to a diffeomorphism of onto the open subset of and ; on this subset the chart function of pulls back to the radial coordinate of the datum, and (Smooth horizon-crossing extension of the Schwarzschild exterior metric in the advanced chart clauses (a)-(c), The Schwarzschild exterior model datum: domain, metric, mass parameter and time orientation clauses (b)-(c)).
is smooth and nondegenerate of inertia on all of , in every spherical-polar product chart, and the Kretschmann scalar of equals on (Smooth horizon-crossing extension of the Schwarzschild exterior metric in the advanced chart clauses (a), (d), (e), Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model, Smooth covariant 2-tensor fields on a smooth manifold).
On the tortoise function satisfies ; is the inverse of the strictly increasing bijection , so for every the inequality is equivalent to for ; hence as (The natural logarithm as the inverse of the exponential function, The exponential is a continuous bijection from onto , The exponential function is strictly increasing, The derivative of at a point that is a limit point of , and differentiability on a set, Rational powers of a positive base, Intervals of : the nine order-convex forms, nondegeneracy, and length).
Counterexample
( is not in the image of the exterior datum.) Let with . By [L1], , whose third-to-second chart entry equals the radial coordinate of the datum, and because the domain of the datum is (The Schwarzschild exterior model datum: domain, metric, mass parameter and time orientation clause (b)). At the extension chart has ; if then , a contradiction. Hence , and since every product chart of the datum is a chart of , no Schwarzschild chart of the datum contains . This is clause 1.
( is a regular point.) By [L2], , which is nonzero because and ; the inertia at is , and the Kretschmann scalar there is , finite and positive. So is an interior point of a smooth nondegenerate Lorentzian four-manifold on which all stated curvature data are finite; in particular the failure of the product charts to cover is not due to being a singularity or a boundary point of the extension. This is clause 2.
(The exterior coordinate is unbounded.) Let be a sequence with . By [L1] the first chart coordinate of is and the second is ; convergence to forces and . Then . Since for all and , the argument tends to , so by [L3] and hence ; therefore . More explicitly, for every bound there is with for , whence : the exterior coordinate is unbounded above along the approach. This is clause 3.
(An approach exists.) For each integer set and , with the fixed angular point of . Then and , so the limiting assertion of step 2.1 is nonvacuous. Together with steps 1.1 and 1.2, this refutes both claimed properties at the specified regular horizon point.
Remarks
- What the counterexample says. The horizon point lies in the closure of in but not in ; it is a regular point of the extension and requires a genuinely different chart, whose existence is the content of the cited extension lemma. The refuted statement is not that the exterior chart fails somewhere — the cited lemma proves its regularity on — but that the charts of the exterior datum suffice for the extension. No value of , , or , no numerical integration and no measurement occurs.
Depends on
The Schwarzschild exterior model datum: domain, metric, mass parameter and time orientation
Smooth horizon-crossing extension of the Schwarzschild exterior metric in the advanced chart
Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
Smooth covariant 2-tensor fields on a smooth manifold
The natural logarithm as the inverse of the exponential function
The exponential is a continuous bijection from onto
The derivative of at a point that is a limit point of , and differentiability on a set
Rational powers of a positive base
Intervals of : the nine order-convex forms, nondegeneracy, and length
The exponential function is strictly increasing
Dependency tree · 2 levels
Sources
- D. Tong, General Relativity (Cambridge Part III Mathematical Tripos, Michaelmas 2019), sections 6.1.3-6.1.4: the tortoise coordinate r_* = r + 2GM log((r-2GM)/2GM), its divergence as r -> 2GM and the change to regular horizon-crossing coordinates, printed pp. 238-247 (PDF pp. 245-254)
- S. M. Carroll, Lecture Notes on General Relativity, arXiv:gr-qc/9712019v1 (1997), Ch. 7: the tortoise coordinate, Eddington-Finkelstein and Kruskal coordinates, and the statement that the Schwarzschild coordinates break down at the horizon, printed pp. 184-189 (PDF pp. 191-196)