Semiclassical gravity is the approximation to the theory of quantum gravity in which one treats matter fields 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 \( G_{\mu \nu } \), to the expectation value of the energy–momentum tensor operator,\( T_{\mu \nu } \), of the matter fields:

\( G_{\mu\nu} = \frac{ 8 \pi G }{ c^4 } \left\langle \hat T_{\mu\nu} \right\rangle_\psi \)

where G is the gravitational constant and \( \psi \) indicates the quantum state of the matter fields.

Stress–energy tensor

There is some ambiguity in regulating the stress–energy tensor, and this depends upon the curvature. This ambiguity can be absorbed into the cosmological constant, the gravitational constant, and the quadratic couplings[1]

\( \int d^dx \,\sqrt{-g} R^2 \) and \( \int d^dx\, \sqrt{-g} R^{\mu\nu}R_{\mu\nu}. \)

There's also the other quadratic term

\( \int d^dx\, \sqrt{-g} R^{\mu\nu\rho\sigma}R_{\mu\nu\rho\sigma}, \)

but (in 4-dimensions) this term is a linear combination of the other two terms and a surface term. See Gauss–Bonnet gravity for more details.

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 diagrams 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.
Experimental status

There are cases where semiclassical gravity breaks down. For instance,[2] if M is a huge mass, then the superposition

\( \frac{1}{\sqrt{2}} \left( \left| M \text{ at } A \right\rangle + \left| M \text{ at } B \right\rangle \right) \)

where A and B are widely separated, then the expectation value of the stress–energy tensor is M/2 at A and M/2 at B, but we would never observe the metric sourced by such a distribution. Instead, we decohere into a state with the metric sourced at A and another sourced at B with a 50% chance each.

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 of cosmic inflation, which is thought to occur at the very beginnings of the big bang.

See Wald (1994) Chapter 4, section 6 "The Stress-Energy Tensor".

See Page and Geilker; Eppley and Hannah; Albers, Kiefer, and Reginatto.


Birrell, N. D. and Davies, P. C. W., Quantum fields in curved space, (Cambridge University Press, Cambridge, UK, 1982).
Don N. Page, and C. D. Geilker, "Indirect Evidence for Quantum Gravity." Physical Review Letters 47 (1981) 979–982. doi:10.1103/PhysRevLett.47.979
K. Eppley and E. Hannah, "The necessity of quantizing the gravitational field." Found. Phys. 7 (1977) 51–68. doi:10.1007/BF00715241
Mark Albers, Claus Kiefer, Marcel Reginatto, "Measurement Analysis and Quantum Gravity." Physical Review D 78 6 (2008) 064051, doi:10.1103/PhysRevD.78.064051 arXiv:0802.1978.
Robert M. Wald, Quantum Field Theory in Curved Spacetime and Black Hole Thermodynamics. University of Chicago Press, 1994.
Semiclassical gravity on

See also

Quantum field theory in curved spacetime


Theories of gravitation
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