- Semiclassical gravity
Semiclassical gravity is the approximation to the theory of
quantum gravity in which one treatsmatter field s as being quantum and the gravitational field as being classical.In semiclassical gravity, matter is represented by quantum matter fields that propagate according to the theory of quantum fields in curved spacetime. The spacetime in which the fields propagate is classical but dynamical. The curvature of the spacetime is given by the "semiclassical Einstein equations", which relate the curvature of the spacetime, given by the
Einstein tensor , to the expectation value of the energy-momentum tensor operator, , of the matter fields::
where "G" is Newton's constant and indicates the quantum state of the matter fields.
Since the theory of quantum gravity is not yet known, it is difficult to say what is the regime of validity of semiclassical gravity. However, one can formally show that semiclassical gravity could be deduced from quantum gravity by considering "N" copies of the quantum matter fields, and taking the limit of "N" going to infinity while keeping the product "GN" constant. At diagrammatic level, semiclassical gravity corresponds to summing all
Feynman diagram s which do not have loops of gravitons (but have an arbitrary number of matter loops). Semiclassical gravity can also be deduced from an axiomatic approach.The most important applications of semiclassical gravity are to understand the
Hawking radiation of black holes and the generation of random gaussian-distributed perturbations in the theory ofcosmic inflation , which is thought to occur at the very beginnings of the big bang.* Birrell, N. D. and Davies, P. C. W., "Quantum fields in curved space", (Cambridge University Press, Cambridge, UK, 1982).
References
* [http://xstructure.inr.ac.ru/x-bin/theme3.py?level=1&index1=-43587 Semiclassical gravity on arxiv.org]
* Kiefer, Claus [http://arxiv.org/abs/gr-qc/9312015 The semiclassical approximation to quantum gravity]
Wikimedia Foundation. 2010.