Einstein-Hilbert effect

from Wikipedia, the free encyclopedia

The Einstein-Hilbert effect is a mathematical expression from the general theory of relativity , which was first given by David Hilbert . From this effect , the leave Einstein's field equations with the principle of least action derived.

Mathematically, the Einstein-Hilbert effect is formulated as follows:

It is

The requirement that the variation in effect vanish for every variation in the metric provides the equations

where denotes the components of the Ricci tensor .

These are the field equations in a vacuum in the absence of particles and fields and in the case of vanishing vacuum energy density . The right-hand side of the field equations, the components of the energy-momentum tensor , is obtained by varying the part of the effect that describes matter according to the metric. The pre-factor

prior to the Einstein-Hilbert action determines the strength, with the energy and pulse the gravitational produce.

In order to get the cosmological constant in the field equations, the effect can be given a term

Add. Such a term can also be understood as a component of the energy-momentum tensor, which has the advantage that it provides a physical justification for the cosmological constant. Today (2016) there are a large number of models that try to explain a cosmological constant through the matter content of the universe with varying degrees of success.