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A geodesic limit for sufficiently small self-gravitating bodies

Ehlers and Geroch proved a geodesic-limit theorem that permits a small body to carry its own gravitational field. Around a prescribed timelike curve, their hypotheses require arbitrarily localized nonzero bodies satisfying the dominant energy condition, with metrics and connections arbitrarily close to a smooth background. Under those conditions the limiting curve must be a geodesic of that background. The proof also applies to a conserved symmetric matter tensor satisfying the same support and energy conditions.

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What is recorded here?

Ehlers and Geroch proved a geodesic-limit theorem that permits a small body to carry its own gravitational field. Around a prescribed timelike curve, their hypotheses require arbitrarily localized nonzero bodies satisfying the dominant energy condition, with metrics and connections arbitrarily close to a smooth background. Under those conditions the limiting curve must be a geodesic of that background. The proof also applies to a conserved symmetric matter tensor satisfying the same support and energy conditions.

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Scientific scope

This is a conditional limiting theorem. It neither makes arbitrary finite bodies exact geodesics nor supplies a uniform long-time self-force error bound. Its metric-closeness hypotheses exclude unrestricted strong self-gravity; the authors explicitly exclude black holes and singular regions. The stronger tidal bound and charged-body extension discussed in the paper are not established general-relativistic results here. The 2003 preprint and 2004 publication identity are distinguished.

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People and systems

Jürgen Ehlers; Robert Geroch

These are the listed authors of the cited contribution sources. Paper authorship does not quantify individual effort. An incomplete list is explicitly marked; same names are not automatically merged.

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English catalogue narrative

A geodesic limit for sufficiently small self-gravitating bodies

Ehlers and Geroch proved a geodesic-limit theorem that permits a small body to carry its own gravitational field. Around a prescribed timelike curve, their hypotheses require arbitrarily localized nonzero bodies satisfying the dominant energy condition, with metrics and connections arbitrarily close to a smooth background. Under those conditions the limiting curve must be a geodesic of that background. The proof also applies to a conserved symmetric matter tensor satisfying the same support and energy conditions.

Scientific scope

This is a conditional limiting theorem. It neither makes arbitrary finite bodies exact geodesics nor supplies a uniform long-time self-force error bound. Its metric-closeness hypotheses exclude unrestricted strong self-gravity; the authors explicitly exclude black holes and singular regions. The stronger tidal bound and charged-body extension discussed in the paper are not established general-relativistic results here. The 2003 preprint and 2004 publication identity are distinguished.

Reading status

This is a source-linked WRS catalogue note. A full explanatory guide and independent scientific reconstruction have not been completed for this entry. Read the identified original work for its complete narrative and arguments.

People and systems

Jürgen Ehlers; Robert Geroch

These are the listed authors of the cited contribution sources. Paper authorship does not quantify individual effort. An incomplete list is explicitly marked; same names are not automatically merged.

Original sources