Vermeil's theorem

In differential geometry, Vermeil's theorem essentially states that the scalar curvature is the only (non-trivial) absolute invariant among those of prescribed type suitable for Albert Einstein’s theory of General Relativity. The theorem was proved by the German mathematician Hermann Vermeil in 1917.

Standard version of the theorem

The theorem states that the Ricci scalar $R$ [1] is the only scalar invariant (or absolute invariant) linear in the second derivatives of the metric tensor $g_{\mu \nu }$ .

Notes

Let us recall that Ricci scalar $R$ is linear in the second derivatives of the metric tensor $g_{\mu \nu }$ , quadratic in the first derivatives and contains the inverse matrix $g^{\mu \nu },$ which is a rational function of the components $g_{\mu \nu }$ .

References

Vermeil, H. (1917). "Notiz über das mittlere Krümmungsmaß einer n-fach ausgedehnten Riemann'schen Mannigfaltigkeit". Nachrichten von der Gesellschaft der Wissenschaften zu Göttingen. Mathematisch-Physikalische Klasse. 21: 334–344.
Weyl, Hermann (1922). Space, time, matter. Translated by Brose, Henry L. Courier Corporation. ISBN 0-486-60267-2. JFM 48.1059.12.

This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.

[1] Let us recall that Ricci scalar $R$ is linear in the second derivatives of the metric tensor $g_{\mu \nu }$ , quadratic in the first derivatives and contains the inverse matrix $g^{\mu \nu },$ which is a rational function of the components $g_{\mu \nu }$ .

Vermeil's theorem

Standard version of the theorem

See also

Notes

References