In the theory of general relativity, a stress–energy–momentum pseudotensor, such as the Landau–Lifshitz pseudotensor, is an extension of the non-gravitational stress–energy tensor that incorporates the energy–momentum of gravity. It allows the energy–momentum of a system of gravitating matter to be defined. In particular it allows the total of matter plus the gravitating energy–momentum to form a conserved current within the framework of general relativity, so that the total energy–momentum crossing the hypersurface of any compact space–timehypervolume vanishes. Some people have objected to this derivation on the grounds that pseudotensors are inappropriate objects in general relativity, but the conservation law only requires the use of the 4-divergence of a pseudotensor which is, in this case, a tensor. Also, most pseudotensors are sections of jet bundles, which are now recognized as perfectly valid objects in GR.
Landau–Lifshitz pseudotensor
The use of the Landau–Lifshitz pseudotensor, a stress–energy–momentum pseudotensor for combined matter plus gravity, allows the energy–momentum conservation laws to be extended into general relativity. Subtraction of the matter stress–energy–momentum tensor from the combined pseudotensor results in the gravitational stress–energy–momentum pseudotensor.
that it be constructed entirely from the metric tensor, so as to be purely geometrical or gravitational in origin.
that it be index symmetric, i.e.,
that, when added to the stress–energy tensor of matter,, its total 4-divergence vanishes so that we have a conserved expression for the total stress–energy–momentum.
Examining the 4 requirement conditions we can see that the first 3 are relatively easy to demonstrate:
Since the Einstein tensor,, is itself constructed from the metric, so therefore is
Since the Einstein tensor,, is symmetric so is since the additional terms are symmetric by inspection.
The Landau–Lifshitz pseudotensor is constructed so that when added to the stress–energy tensor of matter,, its total 4-divergence vanishes:. This follows from the cancellation of the Einstein tensor,, with the stress–energy tensor, by the Einstein field equations; the remaining term vanishes algebraically due the commutativity of partial derivatives applied across antisymmetric indices.
The Landau–Lifshitz pseudotensor appears to include second derivative terms in the metric, but in fact the explicit second derivative terms in the pseudotensor cancel with the implicit second derivative terms contained within the Einstein tensor,. This is more evident when the pseudotensor is directly expressed in terms of the metric tensor or the Levi-Civita connection; only the first derivative terms in the metric survive and these vanish where the frame is locally inertial at any chosen point. As a result, the entire pseudotensor vanishes locally , which demonstrates the delocalisation of gravitational energy–momentum.
Cosmological constant
When the Landau–Lifshitz pseudotensor was formulated it was commonly assumed that the cosmological constant,, was zero. Nowadays we don't make that assumption, and the expression needs the addition of a term, giving: This is necessary for consistency with the Einstein field equations.
This pseudotensor was originally developed by Albert Einstein. Paul Dirac showed that the mixed Einstein pseudotensor satisfies a conservation law Clearly this pseudotensor for gravitational stress–energy is constructed exclusively from the metric tensor and its first derivatives. Consequently, it vanishes at any event when the coordinate system is chosen to make the first derivatives of the metric vanish because each term in the pseudotensor is quadratic in the first derivatives of the metric. However it is not symmetric, and is therefore not suitable as a basis for defining the angular momentum.