In differential geometry, the Einstein tensor (named after Albert Einstein; also known as the trace-reversed Ricci tensor) is used to express the curvature of a pseudo-Riemannian manifold. In general relativity, it occurs in the Einstein field equations for gravitation that describe spacetime curvature in a manner consistent with energy and momentum conservation.
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The Einstein tensor is symmetric
The Ricci tensor depends only on the metric tensor, so the Einstein tensor can be defined directly with just the metric tensor. However, this expression is complex and rarely quoted in textbooks. The complexity of this expression can be shown using the formula for the Ricci tensor in terms of Christoffel symbols:
where is the Kronecker tensor and the Christoffel symbol is defined as
Before cancellations, this formula results in individual terms. Cancellations bring this number down somewhat.
In the special case of a locally inertial reference frame near a point, the first derivatives of the metric tensor vanish and the component form of the Einstein tensor is considerably simplified:
where square brackets conventionally denote antisymmetrization over bracketed indices, i.e.
The special case of n = 4 dimensions in physics (3 space, 1 time) gives , the trace of the Einstein tensor, as the negative of , the Ricci tensor's trace. Thus another name for the Einstein tensor is the trace-reversed Ricci tensor.
Use in general relativity
From the explicit form of the Einstein tensor, the Einstein tensor is a nonlinear function of the metric tensor, but is linear in the second partial derivatives of the metric. As a symmetric order-2 tensor, the Einstein tensor has 10 independent components in a 4-dimensional space. It follows that the Einstein field equations are a set of 10 quasilinear second-order partial differential equations for the metric tensor.
The contracted Bianchi identities can also be easily expressed with the aid of the Einstein tensor:
The (contracted) Bianchi identities automatically ensure the covariant conservation of the stress–energy tensor in curved spacetimes:
The physical significance of the Einstein tensor is highlighted by this identity. In terms of the densitized stress tensor contracted on a Killing vector , an ordinary conservation law holds:
David Lovelock has shown that, in a four-dimensional differentiable manifold, the Einstein tensor is the only tensorial and divergence-free function of the and at most their first and second partial derivatives.
However, the Einstein field equation is not the only equation which satisfies the three conditions:
- Resemble but generalize Newton–Poisson gravitational equation
- Apply to all coordinate systems, and
- Guarantee local covariant conservation of energy–momentum for any metric tensor.
Many alternative theories have been proposed, such as the Einstein–Cartan theory, that also satisfy the above conditions.
- Lovelock, D. (1971). "The Einstein Tensor and Its Generalizations". Journal of Mathematical Physics. 12 (3): 498–502. Bibcode:1971JMP....12..498L. doi:10.1063/1.1665613. Archived from the original on 2013-02-24.
- Lovelock, D. (1969). "The uniqueness of the Einstein field equations in a four-dimensional space". Archive for Rational Mechanics and Analysis. 33 (1): 54–70. Bibcode:1969ArRMA..33...54L. doi:10.1007/BF00248156.
- Farhoudi, M. (2009). "Lovelock Tensor as Generalized Einstein Tensor". General Relativity and Gravitation. 41 (1): 17–29. arXiv:gr-qc/9510060. Bibcode:2009GReGr..41..117F. doi:10.1007/s10714-008-0658-9.
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- Ohanian, Hans C.; Remo Ruffini (1994). Gravitation and Spacetime (Second ed.). W. W. Norton & Company. ISBN 978-0-393-96501-8.
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