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Lovelock's theorem of general relativity says that from a local gravitational action which contains only second derivatives of the four-dimensional spacetime metric, then the only possible equations of motion are the Einstein field equations. [1] [2] [3] The theorem was described by British physicist David Lovelock in 1971.
In theoretical physics, Lovelock's theory of gravity (often referred to as Lovelock gravity) is a generalization of Einstein's theory of general relativity introduced by David Lovelock in 1971. [1] It is the most general metric theory of gravity yielding conserved second order equations of motion in an arbitrary number of spacetime dimensions D .
This is a list of notable theorems. Lists of theorems and similar statements include: List of algebras; ... Łoś' theorem (model theory) Lovelock's theorem
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Pages in category "Theorems in general relativity" The following 9 pages are in this category, out of 9 total. ... Lovelock's theorem; N. No-hair theorem; P.
David Lovelock (born 1938) is a British theoretical physicist and mathematician. He is known for the Lovelock theory of gravity and Lovelock's theorem . [ 1 ] [ 2 ] [ 3 ]
Lovelock's theorem, a theorem about gravity Lovelock theory of gravity , an extension of Einstein's theory of general relativity 51663 Lovelock , a minor planet
Roger Penrose (Hawking–Penrose singularity theorems, Penrose diagrams, techniques from algebraic geometry and differential topology, Penrose limits, cosmic censorship hypotheses, Penrose inequalities, geometry of gravitational plane waves, impulsive waves, Penrose–Khan colliding plane wave, Newman–Penrose formalism, Weyl curvature ...